S p e ctro m ete rs Ocean Optics pioneered the concept of ... - NDN
S p e ctro m ete rs Ocean Optics pioneered the concept of ... - NDN
S p e ctro m ete rs Ocean Optics pioneered the concept of ... - NDN
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Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
<strong>Ocean</strong> <strong>Optics</strong> <strong>pioneered</strong> <strong>the</strong> <strong>concept</strong><br />
<strong>of</strong> modular, miniature spe<strong>ctro</strong>scopy<br />
to <strong>of</strong>fer more flexibility in your<br />
optical sensing applications. Our line<br />
<strong>of</strong> spe<strong>ctro</strong>m<strong>ete</strong>r models ranges from<br />
<strong>the</strong> world’s most popular generalpurpose<br />
miniature spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> to<br />
compact, scientific-grade units that<br />
perform as well as most high-priced<br />
laboratory-grade systems.<br />
Our spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> address <strong>the</strong> needs<br />
<strong>of</strong> use<strong>rs</strong> across a wide range <strong>of</strong> industries<br />
and disciplines involved in basic<br />
research and science discovery, OEM<br />
development and industrial process<br />
control. Our expertise comes from<br />
assisting you in designing <strong>the</strong><br />
optimum spe<strong>ctro</strong>scopy system for<br />
your needs, a service we’ve provided<br />
for more than 150,000 applications.<br />
Tip<br />
If you placed every spe<strong>ctro</strong>m<strong>ete</strong>r<br />
we’ve sold atop each o<strong>the</strong>r, <strong>the</strong><br />
stack would reach nearly 20,000 feet<br />
– about <strong>the</strong> height <strong>of</strong> Alaska’s Mt.<br />
Denali, <strong>the</strong> tallest mountain in North<br />
America.
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
STS Series OEM Microspe<strong>ctro</strong>m<strong>ete</strong>r<br />
Amazing Full-Spectrum Performance in a Tiny Footprint<br />
NEW<br />
FOR 2011<br />
The STS introduces a family <strong>of</strong> compact, low-cost spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> that’s<br />
ideal for embedding into OEM devices. At just 40 mm x 42 mm x<br />
24 mm (1.6” x 1.7” x 0.9”), <strong>the</strong> STS provides full spectral analysis with<br />
low stray light, high signal to noise ratio and optical resolution <strong>of</strong><br />
~1.5 nm (FWHM) – remarkable performance for a spe<strong>ctro</strong>m<strong>ete</strong>r that<br />
size. The STS is an especially attractive option for high-intensity applications<br />
such as LED characterization and absorbance/transmission<br />
measurements, yet ve<strong>rs</strong>atile enough for an extensive range <strong>of</strong> spectral<br />
sensing requirements.<br />
Key Features<br />
Full Spectral Analysis in a Small Footprint<br />
CMOS-based unit is less than 50 mm (2”) square, weighs just 68 g<br />
(2.4 oz.)<br />
Ideal for OEM Devices<br />
Compact unit available at low cost and reproducible in large<br />
production quantities<br />
Remarkable Performance<br />
Meets or exceeds optical resolution, stability, sensitivity and o<strong>the</strong>r<br />
performance criteria associated with larger, more expensive spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Built-in Shutter<br />
Convenient feature for making dark measurements<br />
Physical<br />
Dimensions:<br />
40 mm x 42 mm x 24 mm<br />
Weight:<br />
68 g (2.4 oz. ), incl. 0.5 m 400 µm fiber<br />
Operating temperature: 0-50 °C, 5 °C change/hour ramp<br />
Storage temperature: -20 to +75 °C<br />
D<strong>ete</strong>ctor<br />
D<strong>ete</strong>ctor type:<br />
ELIS1024, 1024 pixel linear CMOS<br />
D<strong>ete</strong>ctor range: 200-1100 nm (uncoated)<br />
Pixels/size: 1024, 7.8 x 125 µm<br />
Pixel well depth: 800,000 e-<br />
Optical Bench<br />
Design:<br />
Crossed Czerny Turner, focal length 28 mm<br />
Entrance aperture: Shaped aperture<br />
Gratings:<br />
600 l/mm<br />
Fiber optic connector: Fixed<br />
Quantum efficiency: 60% (@ 675 nm)<br />
Spe<strong>ctro</strong>scopic<br />
Wavelength range: VIS (350-800 nm), NIR (650-1100 nm)<br />
Optical resolution: 1.2-1.4 nm FWHM (w/15 µm slit)<br />
Signal-to-noise ratio: 2000:1 (maximum signal)<br />
A/D resolution: 14 bits<br />
Dark noise:<br />
STS Series OEM Microspe<strong>ctro</strong>m<strong>ete</strong>r<br />
Amazing Full-Spectrum Performance in a Tiny Footprint<br />
Robust Optical Bench Design<br />
At <strong>the</strong> heart <strong>of</strong> <strong>the</strong> STS is a CMOS d<strong>ete</strong>ctor in a crossed Czerny Turner optical bench. The bench<br />
is distinguished by custom-molded collimating and focusing mirro<strong>rs</strong> and a 600 lines/mm<br />
groove density grating that projects spectra onto <strong>the</strong> d<strong>ete</strong>ctor.<br />
The unit achieves significantly better optical resolution and produces less stray light than most<br />
filter-based and o<strong>the</strong>r spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> <strong>of</strong> its size. In addition, <strong>the</strong> STS is available with a built-in<br />
shutter for making dark measurements much simpler than manually blocking <strong>the</strong> light or<br />
turning <strong>of</strong>f/on your light source.<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
STS takes advantage <strong>of</strong> recent advances in CMOS d<strong>ete</strong>cto<strong>rs</strong> that elevate optoele<strong>ctro</strong>nic<br />
performance and improve system reproducibility. It uses a 1024-element ELIS-1024 linear image sensor that’s responsive from 200-1100 nm and has<br />
great sensitivity (6.74V/lux-second typical). This new generation <strong>of</strong> CMOS d<strong>ete</strong>cto<strong>rs</strong> <strong>of</strong>fe<strong>rs</strong> excellent performance with great value.<br />
STS Options<br />
We <strong>of</strong>fer STS models for 350-800 nm (STS-VIS) and 650-1100 nm (STS-NIR) applications; a UV model is in development. Each unit has a fixed optical<br />
bench configuration, although use<strong>rs</strong> can select from slit sizes ranging from 15 µm to 200 µm.<br />
The device also has a 0.5 m length optical fiber (200 µm or 400 µm diam<strong>ete</strong>r) that’s fixed to <strong>the</strong> STS entrance aperture to optimize signal collection efficiency.<br />
The STS is fully operational in SpectraSuite spe<strong>ctro</strong>scopy s<strong>of</strong>tware – including <strong>the</strong> shutter control. S<strong>of</strong>tware is priced separately.<br />
Markets and Applications<br />
The STS is conceived as a low-cost, high-performance spe<strong>ctro</strong>m<strong>ete</strong>r for OEM and high-volume applications where one or more wavelengths are being<br />
monitored and custome<strong>rs</strong> seek a highly reproducible result. Life sciences, medical diagnostics, solid state lighting and environmental analysis are<br />
among <strong>the</strong> industries where STS is an attractive alternative to filter-based optical sensing systems and o<strong>the</strong>r microspe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong>.<br />
STS has very good optical resolution, wavelength and <strong>the</strong>rmal stability, making it a great choice for LED and light source characterization, as well as<br />
absorbance/transmission measurements in process and o<strong>the</strong>r industries.<br />
Sample Results with STS OEM Microspe<strong>ctro</strong>m<strong>ete</strong>r<br />
Spectral Output <strong>of</strong> Xenon Flash Lamp<br />
Spectral Emission Lines <strong>of</strong> Mercury Argon Source<br />
www.oceanoptics.com Tel: +1 727-733-2447 5
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Torus Concave Grating Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
New Spe<strong>ctro</strong>m<strong>ete</strong>r Delive<strong>rs</strong> Low Stray Light and High Throughput<br />
NEW<br />
FOR 2011<br />
Torus introduces a family <strong>of</strong> aberration-corrected concave diffraction<br />
grating spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> that delive<strong>rs</strong> low stray light, high throughput<br />
and excellent <strong>the</strong>rmal stability for a wide range <strong>of</strong> research and OEM<br />
applications.<br />
Our fi<strong>rs</strong>t Torus model is a Visible spe<strong>ctro</strong>m<strong>ete</strong>r (360-825 nm) whose<br />
spectral range and low stray light render it especially useful for measuring<br />
color, while its increased sensitivity and throughput make it<br />
ideal for low light level applications.<br />
Like most <strong>Ocean</strong> <strong>Optics</strong> spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong>, Torus interfaces with a<br />
computer via <strong>the</strong> USB port and couples to our line <strong>of</strong> SMA 905-terminated<br />
optical fibe<strong>rs</strong>, light sources and accessories. Spe<strong>ctro</strong>m<strong>ete</strong>r<br />
operation is as simple as installing SpectraSuite spe<strong>ctro</strong>scopy<br />
s<strong>of</strong>tware and <strong>the</strong>n connecting <strong>the</strong> USB cable from <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r<br />
to <strong>the</strong> computer. Wavelength calibration coefficients unique to each<br />
spe<strong>ctro</strong>m<strong>ete</strong>r are programmed into a memory chip right on <strong>the</strong> unit;<br />
<strong>the</strong> s<strong>of</strong>tware simply reads <strong>the</strong>se values from <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r.<br />
Key Features<br />
Concave Grating-based Spe<strong>ctro</strong>m<strong>ete</strong>r<br />
Toroidal diffraction grating ensures low stray light and high<br />
throughput<br />
Visible Wavelength Range<br />
Fi<strong>rs</strong>t <strong>of</strong> a family <strong>of</strong> concave grating spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> ideal for a range<br />
<strong>of</strong> applications from 360-825 nm<br />
Low Stray Light with Excellent Throughput<br />
Provides viable alternative to standard miniature spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
for applications such as dosimetry, high-concentration absorbance<br />
measurements and precision light metrology<br />
Physical<br />
Dimensions:<br />
Weight:<br />
Operating temp.: -10 to +50 °C<br />
D<strong>ete</strong>ctor<br />
D<strong>ete</strong>ctor type: Sony ILX511B<br />
D<strong>ete</strong>ctor range: 200-1100 nm<br />
Pixels: 2048<br />
Pixel well depth: ~62,500 e-<br />
Optical Bench<br />
Design:<br />
Flat field<br />
Focal length:<br />
85 mm<br />
Entrance aperture:<br />
149.9 mm x 119.4 mm x 63.5 mm (5.9 in. x 4.7 in. x<br />
2.5 in.)<br />
954 g (2.1 lb.)<br />
5, 10, 25, 50 or 100 µm wide slit or fiber with user-selectable<br />
aperture (tested at F3 and F4)<br />
Gratings:<br />
Toroidal concave holographic (blazed @ 400 nm)<br />
Mechanical interface 8-32 threaded holes at base (3 places)<br />
Optical input interface: SMA 905 fiber connector and C-mount lens adapter<br />
Spe<strong>ctro</strong>scopic<br />
Wavelength range: 360-825 nm<br />
Optical resolution: ≤1.5 nm FWHM over <strong>the</strong> spectral range<br />
Signal-to-noise ratio: 250:1 (at full signal)<br />
A/D resolution: 16 bits<br />
Dark noise:<br />
50 RMS counts, 300 counts peak to peak<br />
Dynamic range: 2 x 10 8 (system); 1300:1 (single acquisition)<br />
Integration time: 1 ms-20 s<br />
Stray light:<br />
0.03% @ 400 nm<br />
Corrected linearity: >99.8%<br />
Ele<strong>ctro</strong>nics<br />
Power consumption: 250 mA @ 5 VDC<br />
Power options: USB or GPIO port<br />
Data transfer speed: Full spectrum every 1 ms with USB 2.0 port, 15 ms with<br />
USB 1.1 port, 200 ms with serial port<br />
Connector:<br />
USB or GPIO port<br />
Inputs/Outputs: Yes, 8 onboard digital user-programmable GPIOs<br />
Analog channels: 0<br />
Breakout box: Supported<br />
Trigger modes: 4 modes<br />
Strobe functions: Yes<br />
Computer Requirements<br />
Computer interface: USB 2.0, RS-232<br />
Operating systems: Any supported by OmniDriver/SeaBreeze or RS-232<br />
Compliance<br />
CE mark:<br />
Yes<br />
RoHS:<br />
Yes<br />
S<strong>of</strong>tware<br />
Operating s<strong>of</strong>tware: SpectraSuite support (extra)<br />
Dev. s<strong>of</strong>tware: OmniDriver/SeaBreeze driver (extra)<br />
6 www.oceanoptics.com Tel: +1 727-733-2447
Torus Concave Grating Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Low Stray Light, High Throughput<br />
Concave Grating Design<br />
Reflective concave gratings are concave mirro<strong>rs</strong> that dispe<strong>rs</strong>e light; <strong>the</strong> concavity <strong>of</strong> <strong>the</strong> grating reflects and focuses <strong>the</strong> light and <strong>the</strong> grating groove<br />
pattern dispe<strong>rs</strong>es <strong>the</strong> light. These aberration-corrected concave gratings are known for <strong>the</strong>ir low stray light and high efficiency. The toroidal (<strong>the</strong> radius<br />
<strong>of</strong> curvature in <strong>the</strong> focusing and dispe<strong>rs</strong>ion directions are different) grating used in Torus fur<strong>the</strong>r enhances <strong>the</strong> aberration correction and efficiency.<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
For our Visible Torus spe<strong>ctro</strong>m<strong>ete</strong>r, we use a variable line spacing grating with 550 (+/-2) grooves/mm groove density at center and a blaze wavelength<br />
<strong>of</strong> 400 nm. Blaze wavelength is <strong>the</strong> wavelength <strong>of</strong> maximum diffraction efficiency and depends on bench design and o<strong>the</strong>r considerations.<br />
Next Generation <strong>of</strong> High-value Miniature Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Torus is <strong>the</strong> fi<strong>rs</strong>t <strong>of</strong> a new line <strong>of</strong> <strong>Ocean</strong> <strong>Optics</strong> spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> distinguished by scientific-grade spectral performance in <strong>the</strong> compact, flexible bench<br />
design that is our hallmark.<br />
Like our flagship USB2000+ Spe<strong>ctro</strong>m<strong>ete</strong>r, Torus uses a Sony ILX511B linear CCD-array d<strong>ete</strong>ctor. However <strong>the</strong> Torus debuts a novel flat field optical<br />
bench design. The Torus has <strong>the</strong> same robust, high-speed ele<strong>ctro</strong>nics that distinguish <strong>the</strong> USB2000+, but with improved throughput and less stray<br />
light due to <strong>the</strong> aberration-corrected toroidal grating. What’s more, Torus has good <strong>the</strong>rmal stability – wavelength drift is mitigated and peak shape<br />
stays <strong>the</strong> same over a wide temperature range. As a result, Torus makes possible precision metrology, fluorescence and absorbance applications with<br />
demanding stray light and <strong>the</strong>rmal stability requirements.<br />
Typical Applications<br />
Torus works well for applications where low stray light, high throughput and great <strong>the</strong>rmal stability are necessary. Here are some examples:<br />
- Trace gas amounts in <strong>the</strong> atmosphere<br />
- Absorbance <strong>of</strong> optically dense solutions (<strong>the</strong> smaller <strong>the</strong> amount <strong>of</strong> stray light present, <strong>the</strong> higher <strong>the</strong> absorbance values that can be measured)<br />
- Precision measurement <strong>of</strong> LEDs, lase<strong>rs</strong> and o<strong>the</strong>r light sources<br />
- Medical dosimetry in tissue and biological media<br />
- Fluorescence from solid surfaces, backscattering and fluorescence in solutions and powde<strong>rs</strong><br />
Torus Options<br />
Our initial Torus <strong>of</strong>fering is responsive from 360-825 nm and is available with <strong>the</strong> same optical bench accessories – slits, order-sorting filte<strong>rs</strong> and <strong>the</strong><br />
like – as our USB2000+ Spe<strong>ctro</strong>m<strong>ete</strong>r. The Torus accommodates SMA 905-terminated optical fibe<strong>rs</strong>, light sources and accessories. Free-space optical<br />
coupling is accommodated with standard C-mount adapte<strong>rs</strong>. Torus is fully operational in SpectraSuite s<strong>of</strong>tware and is compatible with our OmniDriver<br />
and SeaBreeze s<strong>of</strong>tware development platforms. S<strong>of</strong>tware is priced separately.<br />
Sample Results with Torus Spe<strong>ctro</strong>m<strong>ete</strong>r<br />
Tungsten Halogen Source<br />
Spectral Emission Lines <strong>of</strong> Argon Source<br />
www.oceanoptics.com Tel: +1 727-733-2447 7
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Unde<strong>rs</strong>tanding <strong>Ocean</strong> <strong>Optics</strong> Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Helpful Hints in Choosing <strong>the</strong> Optimum Spe<strong>ctro</strong>m<strong>ete</strong>r Model<br />
Spe<strong>ctro</strong>scopy is a technique in which <strong>the</strong> design criteria exist as a set <strong>of</strong> trade-<strong>of</strong>fs. The optimal spe<strong>ctro</strong>m<strong>ete</strong>r depends entirely upon <strong>the</strong> application –<br />
and your budget. The design process begins by asking a series <strong>of</strong> questions: What are you trying to measure? How fast do you need <strong>the</strong> measurement?<br />
Where is <strong>the</strong> sample? Who will be operating <strong>the</strong> instrument? And <strong>the</strong>n <strong>the</strong>re’s <strong>the</strong> most important question <strong>of</strong> all: Why are you making <strong>the</strong> measurements?<br />
Armed with <strong>the</strong> answe<strong>rs</strong> to those questions, we can help guide you to <strong>the</strong> best spe<strong>ctro</strong>m<strong>ete</strong>r, at <strong>the</strong> best value, for your application. Here’s a quick<br />
guide to your primary choices:<br />
Spe<strong>ctro</strong>m<strong>ete</strong>r Models at a Glance<br />
Spe<strong>ctro</strong>m<strong>ete</strong>r Family Most Popular D<strong>ete</strong>ctor Type Typical Use<br />
USB<br />
USB2000+, USB4000,<br />
CHEMUSB and Jaz<br />
Linear CCD arrays<br />
General-purpose and educational; applications include absorbance,<br />
emission and color<br />
HR HR2000+, HR4000 Linear CCD arrays Characterization <strong>of</strong> lase<strong>rs</strong> and atomic emission lines<br />
QE65000 QE65000 Back-thinned, TE-cooled CCD array High-sensitivity, low light-level applications such as<br />
fluorescence and Raman<br />
Maya Maya2000 Pro Back-thinned CCD array High-sensitivity applications; also, deep UV<br />
NIR<br />
NIRQuest512,<br />
NIRQuest256-2.5<br />
InGaAs linear array<br />
Wide range <strong>of</strong> NIR applications from 900-2500 nm<br />
Mid-IR SIR models InGaAs, Mercury Cadmium Telluride<br />
(MCT), o<strong>the</strong><strong>rs</strong><br />
High-speed and transient-event applications from<br />
900-6500 nm; especially suited for laser applications<br />
Fourier Transform ANIR models InGaAs, MCT Materials identification, gas d<strong>ete</strong>ction and process control from<br />
900-4500 nm<br />
We also <strong>of</strong>fer new spe<strong>ctro</strong>m<strong>ete</strong>r options for OEM integration (<strong>the</strong> STS family) and for<br />
applications where low stray light, high <strong>the</strong>rmal stability and wavelength accuracy are<br />
important (Torus family).<br />
Spe<strong>ctro</strong>m<strong>ete</strong>r Configuration Types<br />
Throughout this catalog we describe <strong>the</strong> lion’s share <strong>of</strong> our spe<strong>ctro</strong>m<strong>ete</strong>r models in one<br />
<strong>of</strong> three ways:<br />
- User-configured describes spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> for which <strong>the</strong> user selects <strong>the</strong> optimum<br />
combination <strong>of</strong> optical bench components, including gratings, slits, filte<strong>rs</strong> and more.<br />
These built-to-suit spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> <strong>of</strong>fer maximum flexibility.<br />
- Preconfigured spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> have all <strong>the</strong> optical bench components already<br />
selected. We <strong>of</strong>fer <strong>the</strong>se “preset” spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> for general UV-VIS and VIS-NIR<br />
applications, extended-range (UV-NIR) use, fluorescence and irradiance. These models<br />
typically are in stock and ready to ship at time <strong>of</strong> order.<br />
- The term Spe<strong>ctro</strong>m<strong>ete</strong>r Systems most <strong>of</strong>ten applies to an application-specific,<br />
spe<strong>ctro</strong>scopy-based instrument that <strong>of</strong>ten includes sampling accessories, s<strong>of</strong>tware<br />
and <strong>the</strong> like. Our primary system models are in Raman, LIBS and metrology and are<br />
covered elsewhere in this catalog.<br />
All spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> are available with an extensive selection <strong>of</strong> complementary<br />
accessories.<br />
8 www.oceanoptics.com Tel: +1 727-733-2447
USB Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> Overview<br />
Choosing <strong>the</strong> Best USB2000+ or USB4000 Option for Your Application<br />
<strong>Ocean</strong> <strong>Optics</strong> USB-series spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> are ve<strong>rs</strong>atile performe<strong>rs</strong> for a wide array <strong>of</strong> applications. Although our flagship USB2000+ and USB4000<br />
spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> have comparable ele<strong>ctro</strong>nics and architecture, <strong>the</strong>y do have one very important difference: <strong>the</strong>ir linear CCD array d<strong>ete</strong>cto<strong>rs</strong>. In addition,<br />
USB2000+ and USB4000 spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> are available in application-ready (preconfigured for specific application types) and build-your-own (userconfigured<br />
for maximum flexibility) ve<strong>rs</strong>ions.<br />
Comparing <strong>the</strong> USB2000+ and USB4000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
The USB2000+ has a 2048-element Sony ILX511B d<strong>ete</strong>ctor and <strong>the</strong> USB4000 has <strong>the</strong> 3648-element Toshiba TCD1304AP d<strong>ete</strong>ctor. Both are linear silicon<br />
CCD arrays, with an effective range <strong>of</strong> 200-1100 nm, and are available with <strong>the</strong> same optical bench accessory options (quartz window for UV performance,<br />
order-sorting filte<strong>rs</strong> and so on).<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Advantages <strong>of</strong> <strong>the</strong> USB2000+<br />
- Its Sony ILX511B d<strong>ete</strong>ctor is coated with a phosphor for better response in <strong>the</strong> UV,<br />
making it especially useful for applications below 350 nm.<br />
- It has a faster minimum integration time – 1 ms compared with 3.8 ms for <strong>the</strong><br />
USB4000. That’s an advantage for applications involving transient events such as<br />
measuring a pulsed light source.<br />
- In applications where you have a considerable amount <strong>of</strong> light, its faster integration<br />
time helps you avoid saturating <strong>the</strong> d<strong>ete</strong>ctor.<br />
Advantages <strong>of</strong> <strong>the</strong> USB4000<br />
- It has better response at wavelengths beyond 400 nm, making it a good choice for<br />
VIS-Shortwave NIR applications.<br />
- Its signal to noise ratio (300:1) and sensitivity (130 photons/count @ 400 nm) are<br />
slightly better than that for <strong>the</strong> USB2000+. This is important in low-light level<br />
applications.<br />
- It’s slightly less expensive than <strong>the</strong> USB2000+. Both systems <strong>of</strong>fer great value at a<br />
reasonable price. But if you’re equipping a lab with multiple units and are primarily<br />
working in <strong>the</strong> VIS-NIR, <strong>the</strong> per-unit savings you realize could be applied to completing<br />
your order with our light sources, accessories and o<strong>the</strong>r complementary products.<br />
USB Series Spe<strong>ctro</strong>m<strong>ete</strong>r Models at a Glance<br />
You can configure a USB2000+ or USB4000 with gratings and optical bench accessories for a myriad <strong>of</strong> application possibilities. Or, over <strong>the</strong> next<br />
several pages, investigate one <strong>of</strong> <strong>the</strong> nearly 10 different application-ready USB2000+/USB4000 systems described in <strong>the</strong> table below:<br />
General Use<br />
Best for USB2000+ Series USB4000 Series<br />
USB2000+UV-VIS<br />
USB2000+VIS-NIR<br />
USB4000-UV-VIS<br />
USB4000-VIS-NIR<br />
Extended range (200-1050 nm) USB2000+XR1 USB4000-XR1<br />
Fluorescence No preconfigured models USB4000-FL (several excitation wavelength options)<br />
Irradiance USB2000+RAD No preconfigured models<br />
www.oceanoptics.com Tel: +1 727-733-2447 9
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
USB2000+UV-VIS and USB2000+VIS-NIR<br />
Application-ready Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> for <strong>the</strong> UV-VIS and VIS-NIR<br />
A typical USB2000+ UV-VIS setup might<br />
include components such as XSR Optical<br />
Fiber Assemblies, a DH2000 Deuterium<br />
Tungsten Halogen Light Source and a<br />
CUV-UV-10 Cuvette Holder.<br />
We <strong>of</strong>fer general-purpose UV-VIS and VIS-NIR spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> – where all<br />
<strong>of</strong> <strong>the</strong> optical bench accessories are already selected – for basic<br />
spe<strong>ctro</strong>scopy applications such as measuring absorbance in solutions<br />
and reflectance <strong>of</strong> solids.<br />
Each spe<strong>ctro</strong>m<strong>ete</strong>r has a 2048-element Sony ILX511B d<strong>ete</strong>ctor with a<br />
multibandpass order-sorting filter and 25 µm slit for optical resolution<br />
to ~1.5 nm (FWHM). The USB2000+-UV-VIS cove<strong>rs</strong> <strong>the</strong> 200-850 nm<br />
wavelength range and <strong>the</strong> USB2000+VIS-NIR cove<strong>rs</strong> 350-1000 nm.<br />
Like all USB2000+ series spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong>, <strong>the</strong> USB2000+UV-VIS and VIS-<br />
NIR feature an amazingly small footprint and <strong>of</strong>fer plug-and-play<br />
capabilities and a simplified interface that operates without external<br />
power. Simply plug your USB2000+UV-VIS or VIS-NIR into an available<br />
USB port on your computer and you eliminate <strong>the</strong> need for analog<br />
converte<strong>rs</strong>. SpectraSuite spe<strong>ctro</strong>scopy s<strong>of</strong>tware (priced separately)<br />
operates on Windows, Macintosh and Linux operating systems and<br />
provides a range <strong>of</strong> basic and advanced spe<strong>ctro</strong>scopy functions.<br />
Key Features<br />
- Preset with optical bench accessories and gratings for general-use applications<br />
in <strong>the</strong> UV-VIS (200-850 nm) and VIS-NIR (350-100 nm)<br />
- 25 µm slit ensures good optical resolution (~1.5 nm FWHM)<br />
- Both models are in stock and ready to ship<br />
USB2000+UV-VIS and USB2000+VIS-NIR spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> are a great<br />
choice for researche<strong>rs</strong> and o<strong>the</strong><strong>rs</strong> who handle a variety <strong>of</strong> basic<br />
spe<strong>ctro</strong>scopy measurements in <strong>the</strong> cou<strong>rs</strong>e <strong>of</strong> <strong>the</strong>ir work.<br />
- Covered by <strong>Ocean</strong> <strong>Optics</strong>’ exclusive 3-year warranty<br />
- Can be combined with our light sources and sampling accessories for<br />
absorbance, reflectance and emission measurements<br />
Specifications USB2000+UV-VIS USB2000+VIS-NIR<br />
Dimensions: 89.1 mm x 63.3 mm x 34.4 mm 89.1 mm x 63.3 mm x 34.4 mm<br />
Weight: 190 g 190 g<br />
Computer interface: USB (RS-232 available on side connector) USB (RS-232 available on side connector)<br />
Spe<strong>ctro</strong>m<strong>ete</strong>r channels: Master spe<strong>ctro</strong>m<strong>ete</strong>r channel only Master spe<strong>ctro</strong>m<strong>ete</strong>r channel only<br />
D<strong>ete</strong>ctor: 2048-element linear silicon CCD array 2048-element linear silicon CCD array<br />
Integration time: 1 ms - 20 seconds 1 ms - 20 seconds<br />
Useable range: 200-850 nm (grating-dependent) 350-1000 nm (grating-dependent)<br />
Dynamic range: 2 x 10 8 (system), 1300:1 (single acquisition) 2 x 10 8 (system), 1300:1 (single acquisition)<br />
Sensitivity:<br />
75 photons/count; also, 2.9 x 10 17 joule/count<br />
2.9 x 10 17 watts/count (for 1-second integration)<br />
75 photons/count; also, 2.9 x 10 17 joule/count<br />
2.9 x 10 17 watts/count (for 1-second integration)<br />
Signal-to-noise ratio: 250:1 (at full signal) 250:1 (at full signal)<br />
Dark noise: 50 (RMS) 50 (RMS)<br />
Grating: 600 lines/mm, set to 200-850 nm (blazed at 300 nm) 600 lines/mm, set to 350-1000 nm (blazed at 500 nm)<br />
Slit: 25 µm width (height is 1000 µm) 25 µm width (height is 1000 µm)<br />
Focal length: 42 mm (input); 68 mm (output) 42 mm (input); 68 mm (output)<br />
Order-sorting:<br />
Single-piece, multi-bandpass d<strong>ete</strong>ctor coating to eliminate<br />
second-order effects from 200-850 nm<br />
Single-piece, multi-bandpass d<strong>ete</strong>ctor coating to eliminate second-order<br />
effects from 350-1000 nm<br />
Resolution: 1.5 nm (FWHM) 1.5 nm (FWHM)<br />
Stray light:<br />
< 0.05% at 600 nm<br />
< 0.10% at 435 nm<br />
< 0.05% at 600 nm<br />
< 0.10% at 435 nm<br />
< 0.10% at 250 nm<br />
Fiber optic connector: SMA 905 to single-strand optical fiber (0.22 NA) SMA 905 to single-strand optical fiber (0.22 NA)<br />
10 www.oceanoptics.com Tel: +1 727-733-2447
USB4000-UV-VIS and USB4000-VIS-NIR<br />
Application-ready Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> for <strong>the</strong> UV-VIS and VIS-NIR<br />
The USB4000-UV-VIS and USB4000-VIS-NIR are reliable, robust<br />
spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> that have a 3648-element linear CCD array d<strong>ete</strong>ctor<br />
for good signal to noise performance and enhanced ele<strong>ctro</strong>nics for<br />
controlling <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r and accessories.<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Each spe<strong>ctro</strong>m<strong>ete</strong>r has a 3648-element Toshiba TCD1304AP d<strong>ete</strong>ctor<br />
with a multibandpass order-sorting filter and 25 µm slit for optical<br />
resolution to ~1.5 nm (FWHM). The USB4000-UV-VIS cove<strong>rs</strong> <strong>the</strong><br />
200-850 nm wavelength range and <strong>the</strong> USB4000-VIS-NIR cove<strong>rs</strong> 350-<br />
1000 nm. Operating s<strong>of</strong>tware (priced separately) is SpectraSuite, a<br />
comprehensive program that operates on Windows, Macintosh and<br />
Linux operating systems.<br />
Although <strong>the</strong> USB4000-UV-VIS and USB4000-VIS-NIR have a<br />
preconfigured optical bench, <strong>the</strong>re’s still flexibility built in to your setup<br />
possibilities. That’s because <strong>the</strong>se spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> are compatible with<br />
our entire range <strong>of</strong> SMA 905-terminated fiber optic accessories.<br />
Changing your sampling setup is as easy as unscrewing a connector<br />
and adding new components or accessories – including light sources,<br />
cuvette holde<strong>rs</strong>, flow cells and fiber optic probes and assemblies.<br />
UB4000-UV-VIS and USB4000-VIS-NIR spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> are among <strong>the</strong> most popular miniature spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> in <strong>the</strong> world and make a great choice for<br />
a variety <strong>of</strong> basic absorbance, reflectance and emission applications. And both models are in stock and ready to ship today.<br />
Specifications USB4000-UV-VIS USB4000-VIS-NIR<br />
Dimensions: 89.1 mm x 63.3 mm x 34.4 mm 89.1 mm x 63.3 mm x 34.4 mm<br />
Weight: 190 g 190 g<br />
Computer interface: Unive<strong>rs</strong>al Serial Bus (RS-232 available on side connector) Unive<strong>rs</strong>al Serial Bus (RS-232 available on side connector)<br />
Spe<strong>ctro</strong>m<strong>ete</strong>r channels: Master spe<strong>ctro</strong>m<strong>ete</strong>r channel only Master spe<strong>ctro</strong>m<strong>ete</strong>r channel only<br />
D<strong>ete</strong>ctor: Toshiba TCD1304AP Linear CCD array Toshiba TCD1304AP Linear CCD array<br />
Integration time: 1 ms-65 seconds 1 ms-65 seconds<br />
Useable range: 200-850 nm (grating-dependent) 350-1000 nm (grating-dependent)<br />
Dynamic range: 2 x 10 8 (system), 1300:1 for a single acquisition 2 x 10 8 (system), 1300:1 for a single acquisition<br />
Sensitivity: 130 photons/count at 400 nm; 60 photons/count at 600 nm 130 photons/count at 400 nm; 60 photons/count at 600 nm<br />
Signal-to-noise ratio: 300:1 (at full signal) 300:1 (at full signal)<br />
Dark noise: 50 (RMS) 50 (RMS)<br />
Grating: 600 l/mm, set to 200-850 mm (blazed at 300 nm) 600 l/mm, set to 350-1000 nm (blazed at 500 nm)<br />
Slit: 1000 µm x 25 µm 1000 µm x 25 µm<br />
Focal length: 42 mm (input); 68 mm (output) 42 mm (input); 68 mm (output)<br />
Order-sorting:<br />
Single-piece, multi-bandpass d<strong>ete</strong>ctor coating to eliminate<br />
second-order effects from 200-850 nm<br />
Single-piece, multi-bandpass d<strong>ete</strong>ctor coating to eliminate secondorder<br />
effects from 350-1000 nm<br />
Resolution: 1.5 nm (FWHM) 1.5 nm (FWHM)<br />
Stray light:
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
USB Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Extended Range XR Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Our XR-Series USB Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> are responsive across a wide<br />
spectral range and provide you optical resolution <strong>of</strong> ~2.0 nm<br />
(FWHM) with <strong>the</strong> convenience <strong>of</strong> a single, monolithic unit that cove<strong>rs</strong><br />
wavelengths from ~200-1050 nm.<br />
The XR option is now available for our USB2000+ (USB2000+XR1)<br />
and USB4000 (USB4000-XR1) Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> and can be configured<br />
into custom systems (specify GRATING_#XR1). The extended-range<br />
grating is also available in a portable Jaz Spe<strong>ctro</strong>m<strong>ete</strong>r configuration<br />
(see JAZ-EL200-XR1 in <strong>the</strong> Jaz section).<br />
With <strong>the</strong> XR Series, <strong>the</strong>re’s no more need to daisy-chain multiple<br />
spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> to enable UV-NIR coverage. Thanks to <strong>the</strong> XR’s<br />
500-lines/mm groove density grating, you have <strong>the</strong> advantage <strong>of</strong><br />
broader spectral coverage as well as good optical resolution.<br />
This grating delive<strong>rs</strong> 850 nm <strong>of</strong> spectral range and is blazed at<br />
250 nm. And, because <strong>the</strong>ir optical bench designs are not affected,<br />
<strong>the</strong> USB2000+ and USB4000 experience no trade-<strong>of</strong>f in performance<br />
with <strong>the</strong> new grating.<br />
XR Extended Range Grating Efficiency<br />
Specifications USB2000+XR1 USB4000-XR1<br />
Spe<strong>ctro</strong>m<strong>ete</strong>r type:<br />
USB2000+ advanced USB4000 general-purpose<br />
ele<strong>ctro</strong>nics spe<strong>ctro</strong>m<strong>ete</strong>r spe<strong>ctro</strong>m<strong>ete</strong>r<br />
Grating:<br />
Grating #31, 500 l/mm,<br />
blazed at 250 nm<br />
Grating #31, 500 l/mm,<br />
blazed at 250 nm<br />
Spectral range: 200-1050 nm 200-1050 nm<br />
Entrance slit: 25 µm 25 µm<br />
Optical resolution (FWHM): ~1.7-2.1 nm ~1.7-2.0 nm<br />
Order-sorting filter: Yes Yes<br />
D<strong>ete</strong>ctor collection lens: No No<br />
Note: Dimensions, d<strong>ete</strong>ctor and ele<strong>ctro</strong>nics specifications are comparable to<br />
<strong>the</strong> specifications for <strong>the</strong> USB2000+ Spe<strong>ctro</strong>m<strong>ete</strong>r and its application-ready<br />
ve<strong>rs</strong>ions.<br />
Technical Tip<br />
What applications are XR-Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> best for?<br />
Solar irradiance measurements, atomic emission line analysis, plasma analysis, process applications and more.<br />
How are you able to provide <strong>the</strong> extended range option in USB-series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong>?<br />
The diffraction grating provides coverage from 200-1050 nm, but that’s only part <strong>of</strong> <strong>the</strong> story. The broad range doesn’t<br />
do you much good if you are unable to manage higher-order spectral sorting. So we developed a proprietary orde<strong>rs</strong>orting<br />
filter that is applied directly to <strong>the</strong> d<strong>ete</strong>ctor to eliminate second- and third-order effects.<br />
Why select a 25 µm slit as <strong>the</strong> standard option in <strong>the</strong> XR-series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong>?<br />
Selecting a 25 µm slit allows us to maintain good optical resolution across <strong>the</strong> entire spectral range. Also, unless your application involves low<br />
levels <strong>of</strong> light, <strong>the</strong> slit width is appropriate.<br />
12 www.oceanoptics.com Tel: +1 727-733-2447
USB4000-FL Fluorescence Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Preconfigured Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> for Fluorescence<br />
The USB4000-FL, USB4000-FL-450 and USB4000-FL-395<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> are preconfigured for fluorescence measurements<br />
from 360-1100 nm. Each spe<strong>ctro</strong>m<strong>ete</strong>r comes with a 200 µm slit and<br />
d<strong>ete</strong>ctor collection lens for increased light throughput and features<br />
plug-and-play operation, a high-performance 3648-element CCDarray<br />
d<strong>ete</strong>ctor and fast USB 2.0 connectivity.<br />
There are three USB4000-FL options:<br />
- USB4000-FL<br />
Our basic fluorescence spe<strong>ctro</strong>m<strong>ete</strong>r can be combined with<br />
various excitation sources and accessories for probe- and cuvettebased<br />
setups. We <strong>of</strong>fer an extensive range <strong>of</strong> separate LEDs for<br />
excitation.<br />
- USB4000-FL-450 and USB4000-FL-395<br />
These models <strong>of</strong>fer all <strong>the</strong> advantages <strong>of</strong> our USB4000-FL, but<br />
with a direct-attach 470 nm LED (pictured) or 395 nm LED for<br />
excitation. The LED connects to <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r via a 10-pin<br />
connector. The spe<strong>ctro</strong>m<strong>ete</strong>r powe<strong>rs</strong> and controls (through<br />
s<strong>of</strong>tware) <strong>the</strong> LED. The direct-attach LED option provides you with<br />
a convenient, small-footprint package for your single-wavelength<br />
excitation needs.<br />
Filtering Options<br />
USB4000-FLs can be used with our LVF-series Linear Variable Filte<strong>rs</strong><br />
for simple yet effective separation <strong>of</strong> excitation and fluorescence<br />
energy. Use our LVF-L Linear Variable Low-pass Filter to fine-tune<br />
your excitation source for maximum signal with minimum overlap;<br />
our LVF-H Linear Variable High-pass Filter can be effective on <strong>the</strong><br />
d<strong>ete</strong>ction side. Additional blocking filter options are also available.<br />
Physical<br />
Dimensions:<br />
89.1 mm x 63.3 mm x 34. 4 mm (spe<strong>ctro</strong>m<strong>ete</strong>r only);<br />
89.1 mm x 120.3 mm x 34.4 mm (spe<strong>ctro</strong>m<strong>ete</strong>r w/LED)<br />
190 g (spe<strong>ctro</strong>m<strong>ete</strong>r only); 310 g (spe<strong>ctro</strong>m<strong>ete</strong>r w/LED)<br />
Weight:<br />
D<strong>ete</strong>ctor Specifications<br />
D<strong>ete</strong>ctor:<br />
Toshiba TCD1304AP Linear CCD array<br />
D<strong>ete</strong>ctor range: 200-1100 nm<br />
Pixels:<br />
3648 pixels<br />
Pixel size:<br />
8 μm x 200 μm<br />
Pixel well depth: 100,000 ele<strong>ctro</strong>ns<br />
Sensitivity:<br />
130 photons/count at 400 nm; 60 photons/count at 600 nm<br />
Optical Bench<br />
Design:<br />
f/4, Asymmetrical crossed Czerny-Turner<br />
Focal length:<br />
42 mm (input); 68 mm (output)<br />
Entrance aperture: 200 µm wide slit<br />
Grating:<br />
Grating #3 -- groove density 600 l/mm, set to<br />
360-1000 nm, 500 nm blaze<br />
D<strong>ete</strong>ctor collection<br />
lens:<br />
Fiber optic connector:<br />
Yes, L4<br />
SMA 905 to 0.22 numerical aperture single-strand optical<br />
fiber<br />
Spe<strong>ctro</strong>scopic<br />
Wavelength range: 360-1000 nm<br />
Optical resolution: ~10.0 nm FWHM<br />
Signal-to-noise ratio: 300:1 (at full signal)<br />
A/D resolution: 16 bit<br />
Dark noise:<br />
50 RMS counts<br />
Dynamic range: 2 x 10 8 (system), 1300:1 for a single acquisition<br />
Integration time: 3.8 ms-10 seconds<br />
Stray light:<br />
99.8%<br />
LED Specifications for USB4000-FL-450 and USB4000-FL-395<br />
Wavelength:<br />
460-490 nm (USB4000-FL-450) and 380-410 nm<br />
(USB4000-FL-395)<br />
Power consumption: 60 mA @ 5 VDC<br />
Power output:<br />
60 µW (minimum) into a 600 µm fiber<br />
Stability:<br />
+/-1.0% drift after 2-minute warm-up period<br />
Ele<strong>ctro</strong>nics<br />
Power consumption: 250 mA @ 5 VDC<br />
Data transfer speed: Full scans to memory every 5 ms with USB 2.0 port<br />
Inputs/Outputs: Yes, 8 onboard digital user-programmable GPIOs<br />
Analog channels: No<br />
Auto nulling:<br />
Yes<br />
Trigger modes: 4 modes<br />
Strobe functions: Yes<br />
Connector:<br />
22-pin connector<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
www.oceanoptics.com Tel: +1 727-733-2447 13
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
USB2000+RAD Spe<strong>ctro</strong>m<strong>ete</strong>r<br />
Preconfigured for Irradiance Measurements<br />
The USB2000+RAD Spe<strong>ctro</strong>radiom<strong>ete</strong>r is a preconfigured<br />
combination <strong>of</strong> a powerful 2-MHz analog-to-digital (A/D) converter,<br />
programmable ele<strong>ctro</strong>nics, a 2048-element CCD-array d<strong>ete</strong>ctor,<br />
a high-speed USB 2.0 port and cosine corrector. This innovative<br />
combination produces our fastest spe<strong>ctro</strong>m<strong>ete</strong>r yet and provides<br />
resolution to 0.35 nm (FWHM). The USB2000+RAD allows use<strong>rs</strong> to<br />
capture and store a full spectrum into memory every millisecond<br />
when <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r is interfaced to a computer via a USB 2.0 port.<br />
This spe<strong>ctro</strong>radiom<strong>ete</strong>r system features a USB2000+ Spe<strong>ctro</strong>m<strong>ete</strong>r<br />
and attached CC-3-DA cosine corrector that does not require in-field<br />
NIST-traceable UV-VIS calibration as it is precalibrated by <strong>Ocean</strong><br />
<strong>Optics</strong> with our SPEC-CAL-UV radiometric calibration service for UV<br />
spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong>. The USB2000+RAD is preconfigured and is ready for<br />
measurement "out <strong>of</strong> <strong>the</strong> box" so that installation and measurement<br />
is fast, accurate and convenient.<br />
Features<br />
- Programmable microcontroller<br />
- 1,000 full spectra per second<br />
- Modular design<br />
- Automatically reads wavelength calibration coefficients <strong>of</strong> <strong>the</strong><br />
spe<strong>ctro</strong>m<strong>ete</strong>r and configures operating s<strong>of</strong>tware<br />
- RoHS and CE compliant<br />
Specifications<br />
Physical<br />
Dimensions:<br />
Weight:<br />
D<strong>ete</strong>ctor<br />
D<strong>ete</strong>ctor:<br />
D<strong>ete</strong>ctor range:<br />
Pixels:<br />
Pixel size:<br />
Pixel well depth:<br />
Sensitivity:<br />
Optical Bench<br />
Design:<br />
Focal length:<br />
Entrance aperture:<br />
Grating:<br />
D<strong>ete</strong>ctor collection<br />
lens:<br />
Collimating and focusing<br />
mirror:<br />
UV enhanced window:<br />
Fiber optic connector:<br />
89.1 mm x 63.3 mm x 34.4 mm<br />
190 g<br />
Sony ILX511 linear silicon CCD array<br />
200-1100 nm<br />
2048 pixels<br />
14 μm x 200 μm<br />
~62,500 ele<strong>ctro</strong>ns<br />
75 photons/count at 400 nm; 41 photons/count at 600 nm<br />
f/4, Symmetrical crossed Czerny-Turner<br />
42 mm input; 68 mm output<br />
50 µm wide slit<br />
Grating # 2 groove density 600 l/mm, set to 250-800 nm<br />
(400 nm blaze)<br />
Yes, L2<br />
Standard<br />
UV2 quarrtz window<br />
SMA 905 to 0.22 numerical aperture single-strand<br />
optical fiber<br />
Spe<strong>ctro</strong>scopic<br />
Wavelength range: 200 - 850 nm<br />
Optical resolution: ~2.0 FWHM<br />
Signal-to-noise ratio: 250:1 (at full signal)<br />
A/D resolution: 16 bit<br />
Dark noise:<br />
50 RMS counts<br />
Dynamic range: 2 x 10 8 (system); 1300:1 for a single acquisition<br />
Integration time: 1 ms to 65 seconds (20 s typical)<br />
Stray light:<br />
USB User-configured Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> Overview<br />
Optimizing <strong>the</strong> USB2000+ and USB4000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> for Your Application<br />
With standard USB2000+ and USB4000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong>, you select <strong>the</strong> optimum combination <strong>of</strong> optical bench options -- gratings, slits, filte<strong>rs</strong>, mirro<strong>rs</strong><br />
and more – to optimize <strong>the</strong> system for your application. Hundreds <strong>of</strong> different setups can be configured for each model.<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
With <strong>the</strong> exception <strong>of</strong> <strong>the</strong> d<strong>ete</strong>ctor, <strong>the</strong> USB2000+ and USB4000 use identical optical bench accessories. The Jaz Spe<strong>ctro</strong>m<strong>ete</strong>r uses virtually <strong>the</strong> same<br />
lineup <strong>of</strong> accessories as well (see <strong>the</strong> Jaz section for details).<br />
USB2000+/USB4000 Optical Bench Options<br />
Maximum flexibility is available with USB2000+ and USB4000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong>. Here are <strong>the</strong> optical bench accessories available for your spe<strong>ctro</strong>m<strong>ete</strong>r:<br />
1<br />
SMA 905 Connector<br />
Light from a fiber ente<strong>rs</strong> <strong>the</strong> optical bench through <strong>the</strong><br />
SMA 905 Connector. The SMA 905 bulkhead provides<br />
a precise locus for <strong>the</strong> end <strong>of</strong> <strong>the</strong> optical fiber, fixed slit,<br />
absorbing filter and fiber clad mode aperture.<br />
4<br />
8<br />
2<br />
3<br />
4<br />
5<br />
6<br />
Fixed Entrance Slit: specify slit size<br />
Light passes through <strong>the</strong> installed slit, which acts as <strong>the</strong><br />
entrance aperture. Slits come in various widths from<br />
5 µm to 200 µm. The slit is fixed in <strong>the</strong> SMA 905 bulkhead<br />
to sit against <strong>the</strong> end <strong>of</strong> a fiber.<br />
Longpass Absorbing Filter: optional<br />
If selected, an absorbing filter is installed between <strong>the</strong> slit<br />
and <strong>the</strong> clad mode aperture in <strong>the</strong> SMA 905 bulkhead.<br />
The filter is used to limit bandwidth <strong>of</strong> light entering<br />
spe<strong>ctro</strong>m<strong>ete</strong>r or to balance color.<br />
Collimating Mirror: specify standard or SAG+<br />
The collimating mirror is matched to <strong>the</strong> 0.22 numerical<br />
aperture <strong>of</strong> our optical fiber. Light reflects from this<br />
mirror, as a collimated beam, toward <strong>the</strong> grating. You can<br />
opt to install a standard mirror or a UV absorbing SAG+<br />
mirror.<br />
Grating & Wavelength Range: specify grating<br />
& starting wavelength<br />
We install <strong>the</strong> grating on a platform that we <strong>the</strong>n rotate<br />
to select <strong>the</strong> starting wavelength you’ve specified. Then<br />
we permanently fix <strong>the</strong> grating in place to eliminate<br />
mechanical shifts or drift.<br />
Focusing Mirror: specify standard or SAG+<br />
This mirror focuses fi<strong>rs</strong>t-order spectra on <strong>the</strong> d<strong>ete</strong>ctor<br />
plane. Both <strong>the</strong> collimating and focusing mirro<strong>rs</strong> are<br />
made in-house to guarantee <strong>the</strong> highest reflectance and<br />
<strong>the</strong> lowest stray light possible. You can opt to install a<br />
standard or SAG+ mirror.<br />
7<br />
8<br />
9<br />
10<br />
6<br />
3<br />
1<br />
2<br />
5<br />
L2/L4 D<strong>ete</strong>ctor Collection Lens: optional<br />
This cylindrical lens, made in-house to ensure aberration-free<br />
performance, is fixed to <strong>the</strong> d<strong>ete</strong>ctor to focus <strong>the</strong> light from <strong>the</strong><br />
tall slit onto <strong>the</strong> shorter d<strong>ete</strong>ctor elements. It increases lightcollection<br />
efficiency.<br />
D<strong>ete</strong>ctor<br />
We <strong>of</strong>fer a 2048-element Sony ILX511B and 3648-element<br />
Toshiba TCD1304AP linear CCD array d<strong>ete</strong>ctor. Each pixel<br />
responds to <strong>the</strong> wavelength <strong>of</strong> light that strikes it. Ele<strong>ctro</strong>nics<br />
bring <strong>the</strong> compl<strong>ete</strong> spectrum to <strong>the</strong> s<strong>of</strong>tware.<br />
OFLV Variable Longpass Order-sorting Filter:<br />
optional<br />
Our proprietary filte<strong>rs</strong> precisely block second- and third-order<br />
light from reaching specific d<strong>ete</strong>ctor elements.<br />
UV2/UV4 D<strong>ete</strong>ctor Upgrade: optional<br />
When selected, <strong>the</strong> d<strong>ete</strong>ctor’s standard BK7 window is<br />
replaced with a quartz window to enhance <strong>the</strong> performance <strong>of</strong><br />
<strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r for applications
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
USB2000+ Spe<strong>ctro</strong>m<strong>ete</strong>r<br />
User-configured for Maximum Flexibility<br />
The USB2000+ Spe<strong>ctro</strong>m<strong>ete</strong>r is a clever combination <strong>of</strong> technologies:<br />
a powerful 2-MHz analog-to-digital (A/D) converter, programmable<br />
ele<strong>ctro</strong>nics, a 2048-element CCD-array d<strong>ete</strong>ctor and a high-speed USB<br />
2.0 port.<br />
This innovative design produces our fastest spe<strong>ctro</strong>m<strong>ete</strong>r and<br />
provides resolution to 0.35 nm (FWHM). The USB2000+ allows use<strong>rs</strong><br />
to capture and store a full spectrum into memory every millisecond<br />
(that’s 1,000 full spectra every second) when <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r is<br />
interfaced to a computer via a USB 2.0 port. The USB2000+ is perfect<br />
for chemical, biochemical and o<strong>the</strong>r applications where fast reactions<br />
need to be monitored.<br />
Features<br />
- 1,000 full spectra/second<br />
- Programmable microcontroller<br />
- Modular design – hundreds <strong>of</strong> configurations possible<br />
- Built-to-suit wavelength range and resolution<br />
- Automatically reads <strong>the</strong> wavelength calibration coefficients <strong>of</strong> <strong>the</strong><br />
spe<strong>ctro</strong>m<strong>ete</strong>r and configures operating s<strong>of</strong>tware<br />
- USB-to-PC interface; no external power requirements<br />
- RoHS and CE compliance<br />
Programmable Microcontroller<br />
The USB2000+ has an onboard programmable microcontroller that<br />
provides flexibility in controlling <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r and accessories.<br />
Through a 22-pin connector, you can implement all operating<br />
param<strong>ete</strong><strong>rs</strong> in <strong>the</strong> s<strong>of</strong>tware, such as controlling external light sources,<br />
creating processes and routines and retrieving data from external<br />
devices. The USB2000+ gives you access to 10 user-programmable<br />
digital I/Os for interfacing to o<strong>the</strong>r equipment and a pulse generator<br />
for triggering o<strong>the</strong>r devices.<br />
16 www.oceanoptics.com Tel: +1 727-733-2447<br />
Physical<br />
Dimensions:<br />
89.1 mm x 63.3 mm x 34.4 mm<br />
Weight:<br />
190 g<br />
D<strong>ete</strong>ctor<br />
D<strong>ete</strong>ctor:<br />
Sony ILX511B linear silicon CCD array<br />
D<strong>ete</strong>ctor range: 200-1100 nm<br />
Pixels:<br />
2048 pixels<br />
Pixel size:<br />
14 μm x 200 μm<br />
Pixel well depth: ~62,500 ele<strong>ctro</strong>ns<br />
Sensitivity:<br />
75 photons/count at 400 nm; 41 photons/count at 600 nm<br />
Optical Bench<br />
Design:<br />
f/4, Symmetrical crossed Czerny-Turner<br />
Focal length:<br />
42 mm input; 68 mm output<br />
Entrance aperture: 5, 10, 25, 50, 100 or 200 µm wide slits or fiber (no slit)<br />
Grating options: 14 different gratings, UV through Shortwave NIR<br />
XR grating option: Yes<br />
D<strong>ete</strong>ctor collection Yes, L2<br />
lens option:<br />
OFLV filter options: OFLV-200-850; OFLV-350-1000<br />
O<strong>the</strong>r bench filter Longpass OF-1 filte<strong>rs</strong><br />
options:<br />
Collimating and focusing<br />
Standard or SAG+<br />
mirro<strong>rs</strong>:<br />
UV enhanced window: Yes, UV2 quartz window<br />
Fiber optic connector: SMA 905 to 0.22 numerical aperture single-strand optical<br />
fiber<br />
Spe<strong>ctro</strong>scopic<br />
Wavelength range: Grating dependent<br />
Optical resolution: ~0.3-10.0 nm FWHM<br />
Signal-to-noise ratio: 250:1 (at full signal)<br />
A/D resolution: 16 bit<br />
Dark noise:<br />
50 RMS counts<br />
Dynamic range: 2 x 10 8 (system); 1300:1 for a single acquisition<br />
Integration time: 1 ms to 65 seconds (20 seconds typical)<br />
Stray light:<br />
If you’re looking for an economical, ve<strong>rs</strong>atile spe<strong>ctro</strong>m<strong>ete</strong>r, you’ll find<br />
<strong>the</strong> USB4000 to be an exceptional solution. This compact, modular<br />
unit packs a 3648-element Toshiba linear CCD-array d<strong>ete</strong>ctor to<br />
provide you increased signal-to-noise and enhanced ele<strong>ctro</strong>nics for<br />
control <strong>of</strong> <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r as well as its accessories.<br />
The USB4000 Spe<strong>ctro</strong>m<strong>ete</strong>r is distinguished by its enhanced ele<strong>ctro</strong>nics:<br />
16-bit A/D resolution with auto nulling feature (an enhanced<br />
electrical dark-signal correction); EEPROM storage <strong>of</strong> calibration<br />
coefficients for simple spe<strong>ctro</strong>m<strong>ete</strong>r start-up; 8 programmable GPIO<br />
signals for controlling peripheral devices; and an ele<strong>ctro</strong>nic shutter –<br />
a handy feature to prevent d<strong>ete</strong>ctor saturation.<br />
The USB4000 couples easily via an SMA 905 connector to our line <strong>of</strong><br />
spe<strong>ctro</strong>scopic accessories. Direct-attach accessories are available, as<br />
well as discr<strong>ete</strong> light sources, optical fibe<strong>rs</strong>, sampling devices such<br />
as cuvette holde<strong>rs</strong> and flow cells, and many more. In most instances,<br />
changing <strong>the</strong> sampling system from one experiment setup to<br />
ano<strong>the</strong>r is as easy as unscrewing a connector and swapping out<br />
accessories.<br />
Features<br />
- Programmable microcontroller<br />
- Modular design<br />
- Automatically reads wavelength calibration coefficients <strong>of</strong> <strong>the</strong><br />
spe<strong>ctro</strong>m<strong>ete</strong>r and configures operating s<strong>of</strong>tware<br />
- RoHS and CE compliant<br />
USB4000 Spe<strong>ctro</strong>m<strong>ete</strong>r<br />
User-Configured to be Flexible<br />
Physical<br />
Dimensions:<br />
89.1 mm x 63.3 mm x 34.4 mm<br />
Weight:<br />
190 g<br />
D<strong>ete</strong>ctor<br />
D<strong>ete</strong>ctor:<br />
Toshiba TCD1304AP linear CCD array<br />
D<strong>ete</strong>ctor range: 200-1100 nm<br />
Pixels:<br />
3648 pixels<br />
Pixel size:<br />
8 μm x 200 μm<br />
Pixel well depth: 100,000 ele<strong>ctro</strong>ns<br />
Sensitivity:<br />
130 photons/count at 400 nm; 60 photons/count at<br />
600 nm<br />
Optical Bench<br />
Design:<br />
f/4, Asymmetrical crossed Czerny-Turner<br />
Focal length:<br />
42 mm (input); 68 mm (output)<br />
Entrance aperture: 5, 10, 25, 50, 100 or 200 µm wide slits or fiber (no slit)<br />
Grating:<br />
15 different gratings, UV through Shortwave NIR<br />
OFLV filter:<br />
OFLV-200-850, OFLV-350-1000<br />
UV enhanced window: Yes, UV4 quartz window<br />
Fiber optic connector: SMA 905 to 0.22 numerical aperture single-strand optical<br />
fiber<br />
Spe<strong>ctro</strong>scopic<br />
Wavelength range: Grating dependent<br />
Optical resolution: ~1.5 nm FWHM<br />
Signal-to-noise ratio: 300:1 (at full signal)<br />
A/D resolution: 16 bit<br />
Dark noise:<br />
50 RMS counts<br />
Integration time: 3.8 ms-10 seconds<br />
Dynamic range: 2 x 10 8 (system), 1300:1 for a single acquisition<br />
Stray light:<br />
99.8%<br />
Ele<strong>ctro</strong>nics<br />
Power consumption: 250 mA @ 5 VDC<br />
Data transfer speed: Full spectrum to memory every 5 ms with USB 2.0 port<br />
Inputs/Outputs: Yes, 8 onboard digital user-programmable GPIOs<br />
Breakout box compatible:<br />
Yes, with <strong>the</strong> USB-ADP-BB adapter<br />
Trigger modes: 4 modes<br />
Strobe functions: Yes<br />
Connector:<br />
22-pin connector<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Fun Fact: Our USB Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> are among <strong>the</strong> most popular selling miniature spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> on <strong>the</strong> market and can trace <strong>the</strong>ir<br />
lineage to <strong>the</strong> S1000 – <strong>the</strong> world’s fi<strong>rs</strong>t miniature spe<strong>ctro</strong>m<strong>ete</strong>r -- which we introduced in 1992. The fi<strong>rs</strong>t miniature spe<strong>ctro</strong>m<strong>ete</strong>r we<br />
sold went to a researcher at Los Alamos National Laboratories, whose work involved plutonium. Yea<strong>rs</strong> later we tracked down that fi<strong>rs</strong>t<br />
spe<strong>ctro</strong>m<strong>ete</strong>r and now display it at company headquarte<strong>rs</strong>.<br />
www.oceanoptics.com Tel: +1 727-733-2447 17
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
USB User-configured Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Bench Accessories for USB2000+/USB4000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
The magic behind our USB2000+ and USB4000 miniature spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> is <strong>the</strong> options you can select to configure your optical bench to perfectly suit<br />
your unique application needs. By consulting with an <strong>Ocean</strong> <strong>Optics</strong> Applications Scientist, you can choose <strong>the</strong> optimum combination <strong>of</strong> aperture size,<br />
d<strong>ete</strong>ctor accessories, filte<strong>rs</strong>, gratings and more.<br />
SMA 905 Connecto<strong>rs</strong><br />
This precision connector aligns to <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r’s entrance slit and ensures concentricity <strong>of</strong> <strong>the</strong><br />
fiber. For an upgrade fee, we replace <strong>the</strong> standard SMA 905 Connector with a connector <strong>of</strong> your<br />
choice. Call us for details on custom connecto<strong>rs</strong> and adapte<strong>rs</strong>.<br />
Fixed Entrance Slits<br />
Our entrance slits are rectangular apertures that are 1 mm tall and come in varying widths from<br />
5 µm to 200 µm. Smaller slit sizes achieve <strong>the</strong> best optical resolution.<br />
Slit Description USB2000+ Pixel Resolution USB4000 Pixel Resolution<br />
SLIT-5 5-µm wide x 1-mm high ~3.0 pixels ~5.3 pixels<br />
SLIT-10 10-µm wide x 1-mm high ~3.2 pixels ~5.7 pixels<br />
SLIT-25 25-µm wide x 1-mm high ~4.2 pixels ~7.5 pixels<br />
SLIT-50 50-µm wide x 1-mm high ~6.5 pixels ~11.6 pixels<br />
SLIT-100 100-µm wide x 1-mm high ~12 pixels ~21 pixels<br />
SLIT-200 200-µm wide x 1-mm high ~24 pixels ~42 pixels<br />
Longpass Absorbing Filte<strong>rs</strong><br />
Whe<strong>the</strong>r you select a Longpass Absorbing or Blocking Filter, each has a transmission band and a<br />
blocking band to restrict radiation to a certain wavelength region. This helps eliminate second- and<br />
third-order effects. Filte<strong>rs</strong> are installed permanently.<br />
OF1-WG305<br />
OF1-GG375<br />
OF1-GG395<br />
OF1-GG475<br />
OF1-OG515<br />
OF1-OG550<br />
OF1-OG590<br />
Item<br />
Description<br />
Longpass filter; transmits light >305 nm<br />
Longpass filter; transmits light >375 nm<br />
Longpass filter, installed, transmits light >395 nm<br />
Longpass filter; transmits light >475 nm<br />
Longpass filter; transmits light >515 nm<br />
Longpass filter; transmits light >550 nm<br />
Longpass filter: transmits light >590 nm<br />
Collimating and Focusing Mirro<strong>rs</strong><br />
You can replace our standard aluminum-coated reflective mirro<strong>rs</strong> with our proprietary UV-absorbing<br />
SAG+ Mirro<strong>rs</strong>. These increase reflectance in <strong>the</strong> VIS-NIR range while increasing your spe<strong>ctro</strong>m<strong>ete</strong>r’s<br />
sensitivity. They also absorb nearly all UV light – reducing <strong>the</strong> effects <strong>of</strong> excitation scattering in<br />
fluorescence measurements.<br />
Item Code: SAG+UPG<br />
Grating and Wavelength Range<br />
With a choice <strong>of</strong> 15 gratings, you can easily customize <strong>the</strong> spectral range and most efficient region<br />
<strong>of</strong> your USB Series Spe<strong>ctro</strong>m<strong>ete</strong>r. Our gratings are permanently fixed in place at <strong>the</strong> time <strong>of</strong> manufacture<br />
and are available in both ruled and holographic ve<strong>rs</strong>ions. See page 21 for grating options<br />
and efficiency curves and consult and <strong>Ocean</strong> <strong>Optics</strong> Applications Scientist for details.<br />
18 www.oceanoptics.com Tel: +1 727-733-2447
USB User-configured Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
D<strong>ete</strong>cto<strong>rs</strong> and Accessories for USB2000+/USB4000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
D<strong>ete</strong>cto<strong>rs</strong><br />
The USB2000+ has a 2048-element Sony ILX511B d<strong>ete</strong>ctor and <strong>the</strong> USB4000 has a 3648-element<br />
Toshiba TCD1304AP d<strong>ete</strong>ctor. Both are linear silicon CCD arrays with an effective range <strong>of</strong><br />
200-1100 nm. D<strong>ete</strong>cto<strong>rs</strong> come with BK7 or quartz windows; order-sorting filte<strong>rs</strong> and collection<br />
lenses are optional.<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
D<strong>ete</strong>ctor Collection Lenses<br />
These cylindrical lenses ensure aberration-free performance and are fixed to <strong>the</strong> d<strong>ete</strong>ctor’s window<br />
to focus light from <strong>the</strong> tall slit onto <strong>the</strong> shorter d<strong>ete</strong>ctor elements. The L2 (for <strong>the</strong> USB2000+) and<br />
L4 (USB4000) increase light collection efficiency and help reduce stray light. They also are useful for<br />
low-light level applications where a large-diam<strong>ete</strong>r fiber is being used.<br />
D<strong>ete</strong>cto<strong>rs</strong> with OFLV Filte<strong>rs</strong><br />
OFLV Variable Longpass Order-sorting Filte<strong>rs</strong> are applied to <strong>the</strong> d<strong>ete</strong>ctor’s window to eliminate second- and third-order effects. We use a patented<br />
coating technology to apply <strong>the</strong> filter to <strong>the</strong> substrate.<br />
UV2 and UV4 D<strong>ete</strong>ctor Window Upgrades<br />
For any application
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
USB User-Configured Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Choosing <strong>the</strong> Right Grating<br />
Groove Density<br />
The Groove density (mm -1 ) <strong>of</strong> a grating d<strong>ete</strong>rmines its dispe<strong>rs</strong>ion, while <strong>the</strong> angle<br />
<strong>of</strong> <strong>the</strong> groove d<strong>ete</strong>rmines <strong>the</strong> most efficient region <strong>of</strong> <strong>the</strong> spectrum. The greater<br />
<strong>the</strong> groove density, <strong>the</strong> better <strong>the</strong> optical resolution possible, but <strong>the</strong> more truncated<br />
<strong>the</strong> spectral range.<br />
Spectral Range<br />
Spectral range (bandwidth) is <strong>the</strong> dispe<strong>rs</strong>ion <strong>of</strong> <strong>the</strong> grating across <strong>the</strong> linear array<br />
and is a function <strong>of</strong> <strong>the</strong> groove density. When you choose a starting wavelength<br />
for a spe<strong>ctro</strong>m<strong>ete</strong>r, you add its spectral range to <strong>the</strong> starting wavelength to<br />
d<strong>ete</strong>rmine <strong>the</strong> wavelength range. For several gratings, <strong>the</strong> Spectral Range <strong>of</strong> a<br />
grating varies according to <strong>the</strong> starting wavelength range. The rule <strong>of</strong> thumb is<br />
this: <strong>the</strong> higher <strong>the</strong> starting wavelength, <strong>the</strong> more truncated <strong>the</strong> spectral range.<br />
Blaze Wavelength<br />
For ruled gratings, <strong>the</strong> blaze wavelength is <strong>the</strong> peak wavelength in an efficiency<br />
curve. For holographic gratings, it is <strong>the</strong> most efficient wavelength region.<br />
Best Efficiency ( >30%)<br />
All ruled or holographically etched gratings optimize fi<strong>rs</strong>t-order spectra at certain<br />
wavelength regions; <strong>the</strong> “best” or most efficient region is <strong>the</strong> range where efficiency<br />
is >30%. In some cases, gratings have a greater spectral range than is<br />
efficiently diffracted. For example, Grating 1 has about a 650 nm spectral range,<br />
but is most efficient from 200-575 nm. In this case, wavelengths >575 nm will<br />
have lower intensity due to <strong>the</strong> grating’s reduced efficiency.<br />
Note: Although <strong>the</strong> spectral range <strong>of</strong> a spe<strong>ctro</strong>m<strong>ete</strong>r with Grating 13 is broad, <strong>the</strong> d<strong>ete</strong>ctor will respond to light only from 300-1100 nm. Also, because<br />
<strong>the</strong> grating has broad spectral range, optical resolution 30%)
USB User-Configured Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Gratings for USB2000+/USB4000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
The graphs below are grating efficiency curves for gratings with groove densities <strong>of</strong> 500, 600, 1200, 1800 and 2400 mm -1 . Additional information is<br />
available at www.oceanoptics.com/Products/bench_grating_usb.asp.<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Groove Density <strong>of</strong> 600 mm -1 Groove Density <strong>of</strong> 1200 mm -1<br />
Relative Efficiency<br />
Relative Efficiency<br />
Grating #1 Grating #2 Grating #3 Grating #4 Grating #14<br />
Grating #5 Grating #6 Grating #9<br />
Groove Density <strong>of</strong> 1800 mm -1<br />
Groove Density <strong>of</strong> 2400 mm -1<br />
Relative Efficiency<br />
Relative Efficiency<br />
Grating #10 Grating #11<br />
Grating #7 Grating #12<br />
Grating Selection Tips:<br />
Groove Density <strong>of</strong> 500 mm -1<br />
- These efficiency curves relate only to <strong>the</strong> grating. System response<br />
is affected by a number <strong>of</strong> variables, including d<strong>ete</strong>ctor response.<br />
- Grating selection <strong>of</strong>ten involves trade-<strong>of</strong>fs. For example, gratings<br />
with very high groove density (lines/mm -1 ) allow greater optical<br />
resolution but at <strong>the</strong> expense <strong>of</strong> a truncated spectral range. If<br />
<strong>the</strong> user is characterizing two or three closely aligned laser wavelengths,<br />
such a trade-<strong>of</strong>f <strong>of</strong> resolution for range might be acceptable.<br />
For o<strong>the</strong>r applications, a wider range with good resolution<br />
would make better sense.<br />
Relative Efficiency<br />
- The XR grating (#31) is a good option for broad spectral coverage<br />
(200-1050 nm) without sacrificing optical resolution (~2.0 nm<br />
FHWM with a 25 µm slit). For efficiency <strong>of</strong> Grating #8 (3600 mm -1 ),<br />
visit our website.<br />
Grating #31 (XR)<br />
www.oceanoptics.com Tel: +1 727-733-2447 21
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
USB Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Predicted Ranges and Resolution<br />
These illustrations demonstrate <strong>the</strong> predicted range and resolution <strong>of</strong> a USB4000 Spe<strong>ctro</strong>m<strong>ete</strong>r with a 25 µm entrance slit and various gratings.<br />
600 mm -1 Grating and 25 µm Slit<br />
680 1.36<br />
350<br />
1200 mm -1 Grating and 25 µm Slit<br />
670<br />
1.34<br />
330<br />
0.65<br />
SPECTRAL RANGE (nm)<br />
660<br />
650<br />
640<br />
630<br />
620<br />
610<br />
600<br />
590<br />
1.32<br />
1.30<br />
1.28<br />
1.26<br />
1.24<br />
1.22<br />
RESOLUTION (nm)<br />
SPECTRAL RANGE (nm)<br />
310<br />
290<br />
270<br />
250<br />
230<br />
210<br />
190<br />
170<br />
0.60<br />
0.55<br />
0.50<br />
0.45<br />
0.40<br />
0.35<br />
RESOLUTION (nm)<br />
580<br />
1.20<br />
200 300 400 500 600 700 800 900 1000<br />
150<br />
0.30<br />
200 300 400 500 600 700 800 900 1000<br />
STARTING WAVELENGTH (nm)<br />
STARTING WAVELENGTH (nm)<br />
Example: If <strong>the</strong> starting wavelength is 250 nm, <strong>the</strong>n <strong>the</strong> range is<br />
~667 nm, providing a 250-917 nm wavelength range and 1.34 nm<br />
optical resolution (FWHM). Gratings for <strong>the</strong> USB Bench that have groove<br />
densities <strong>of</strong> 600 mm -1 are Grating 1, 2, 3, 4 and 14.<br />
Example: If <strong>the</strong> starting wavelength is 350 nm, <strong>the</strong>n <strong>the</strong> range is<br />
~310 nm, providing a 350-660 nm wavelength range and 0.63 nm<br />
optical resolution (FWHM). Gratings for <strong>the</strong> USB Bench that have groove<br />
densities <strong>of</strong> 1200 mm -1 are Grating 5, 6 and 9.<br />
SPECTRAL RANGE (nm)<br />
220<br />
220<br />
200<br />
180<br />
160<br />
140<br />
120<br />
1800 mm -1 Grating and 25 µm Slit<br />
0.45<br />
0.40<br />
0.35<br />
0.30<br />
0.25<br />
RESOLUTION (nm)<br />
SPECTRAL RANGE (nm)<br />
160<br />
150<br />
140<br />
130<br />
120<br />
110<br />
100<br />
90<br />
2400 mm -1 Grating and 25 µm Slit<br />
0.32<br />
0.30<br />
0.28<br />
0.26<br />
0.24<br />
0.22<br />
0.20<br />
0.18<br />
RESOLUTION (nm)<br />
100<br />
200<br />
0.20<br />
300 400 500 600 700 800<br />
STARTING WAVELENGTH (nm)<br />
80<br />
0.16<br />
200 300 400 500 600 700 800 900 1000<br />
STARTING WAVELENGTH (nm)<br />
Example: If <strong>the</strong> starting wavelength is 400 nm, <strong>the</strong>n <strong>the</strong> range is<br />
~190 nm, providing a 400-590 nm wavelength range and 0.38 nm<br />
optical resolution (FWHM). Gratings for <strong>the</strong> USB Bench that have groove<br />
densities <strong>of</strong> 1800 mm -1 are Grating 10 and 11.<br />
Example: If <strong>the</strong> starting wavelength is 300 nm, <strong>the</strong>n <strong>the</strong> range is<br />
~140 nm, providing a 300-440 nm wavelength range and 0.29 nm<br />
optical resolution (FWHM). Gratings for <strong>the</strong> USB Bench that have groove<br />
densities <strong>of</strong> 2400 mm -1 are Grating 7 and 12.<br />
Technical Tip<br />
Light striking a grating is diffracted into multiple angles that vary with wavelength. For example, fi<strong>rs</strong>t order light at<br />
200 nm is diffracted at angle #1 and at angle #2, which is twice as large as #1. Angle #2 is <strong>the</strong> same as <strong>the</strong> fi<strong>rs</strong>t order<br />
angle taken by light at twice <strong>the</strong> wavelength, or 400 nm. If <strong>the</strong> application requires signal at 400 nm and light at<br />
200 nm is present, <strong>the</strong>n <strong>the</strong> signal at <strong>the</strong> pixel in question will include contributions from both wavelengths. Second<br />
order light can be removed by using bandpass blocking filte<strong>rs</strong>, which are moved into and out <strong>of</strong> <strong>the</strong> light path.<br />
Ano<strong>the</strong>r approach is <strong>the</strong> use <strong>of</strong> linear variable filte<strong>rs</strong>, which can be designed to provide <strong>the</strong> optimum blocking at each pixel in an array.<br />
22 www.oceanoptics.com Tel: +1 727-733-2447
USB Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
USB Direct-Attach Accessories<br />
We <strong>of</strong>fer a variety <strong>of</strong> compact, modular Direct-Attach Accessories that enable you to make your USB Series Spe<strong>ctro</strong>m<strong>ete</strong>r a custom-tailored solution for<br />
your unique application needs. Each accessory is designed and manufactured to be robust and provide yea<strong>rs</strong> <strong>of</strong> reliable service.<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
USB-ISS-UV-VIS<br />
Sampling System<br />
This clever, integrated sampling system is a direct-attach sample holder and deuterium tungsten light<br />
source for 200-1100 nm. You can control <strong>the</strong> USB-ISS-UV-VIS’s shutter through s<strong>of</strong>tware. A separate<br />
5V power supply is included.<br />
Item Code: USB-ISS-UV-VIS<br />
USB-ISS-VIS<br />
Sampling System<br />
The USB-ISS-VIS is a snap-on cuvette holder and visible light source combination that holds a 1-cm<br />
square cuvette and features a range <strong>of</strong> 390-900 nm. The system’s light source features a long-life<br />
tungsten bulb and multiple violet light emitting diodes. Powered via USB.<br />
Item Code: USB-ISS-VIS<br />
USB-LS Series<br />
Integrated LEDs<br />
Turn your USB2000+ or USB4000 into a spe<strong>ctro</strong>fluorom<strong>ete</strong>r by adding an integrated LED module. Standard<br />
ve<strong>rs</strong>ions are available with 395 nm and 470 nm excitation wavelengths; <strong>the</strong> 470 nm LED module is<br />
also available with a 4-20 mA output.<br />
Item Code: USB-LS-395, USB-LS-450, USB-LS-450-4-20<br />
USB-FHS<br />
Snap-On Filter Holder<br />
The USB-FHS is a combination light source filter holder that is optimized for 390-900 nm measurements.<br />
It can be used for fast, convenient absorbance and transmission measurements <strong>of</strong> square and round<br />
filte<strong>rs</strong> up to 2”. The USB-FHS features long-life tungsten bulbs and multiple violet light emitting diodes.<br />
Powered via USB.<br />
Item Code: USB-FHS<br />
USB-BP<br />
Portable Battery Pack<br />
The USB-BP is a portable Lithium Ion battery pack that gives you up to eight hou<strong>rs</strong> <strong>of</strong> continuous power<br />
to your USB Spe<strong>ctro</strong>m<strong>ete</strong>r and any additional direct-attach accessories. This battery pack delive<strong>rs</strong><br />
2 amp-hou<strong>rs</strong> at 5 volts through its two lithium cells. The USB-BP charges in three hou<strong>rs</strong> with its<br />
included charger.<br />
Item Code: USB-BP<br />
www.oceanoptics.com Tel: +1 727-733-2447 23
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
USB Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Adapte<strong>rs</strong>, Cables and O<strong>the</strong>r Accessories<br />
Adapte<strong>rs</strong>, Cables and Device Control<br />
Item Code<br />
ACC-CON-US4<br />
USB-ADP-BB<br />
USB-ADP-PC<br />
USB-ADP-PC-E<br />
USB-ADP-PX2<br />
USB-AOUT<br />
USB-CBL-0.5M<br />
USB-CBL-1<br />
USB-CBL-MINI<br />
Description<br />
Spe<strong>ctro</strong>m<strong>ete</strong>r accessory connector for external triggering on USB4000s<br />
Adapter to connect USB4000 to HR4000 Breakout Box<br />
Cable and adapter block to connect from serial port on spe<strong>ctro</strong>m<strong>ete</strong>r to serial port on computer; included with USB-CBL-PS power supply<br />
European ve<strong>rs</strong>ion <strong>of</strong> USB-ADP-PC<br />
Adapter block and cable to connect PX-2 Pulsed Xenon Lamp or LS-type LED to USB4000<br />
4-20 mA Analog Output Module for USB4000, USB2000+ Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
USB cable, 0.5 m length, for spe<strong>ctro</strong>m<strong>ete</strong>r-to-PC interface<br />
USB cable, 1 m length, for spe<strong>ctro</strong>m<strong>ete</strong>r-to-PC interface<br />
Mini USB cable for spe<strong>ctro</strong>m<strong>ete</strong>r-to-PC interface<br />
Power Supplies<br />
Item Code<br />
Description<br />
USB-CBL-PS 5 VDC power supply for spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> in Serial mode<br />
USB-BP<br />
Direct-attach Lithium Ion battery pack for USB2000+/USB4000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
WT-12V<br />
Regulated 12 VDC Power Supply (1.5A, 110/220 VAC)<br />
WT-12V-E 12 VDC Power Supply (800 mA, 220 V)<br />
WT-12V-R Regulated 12 VDC Power Supply (2.5 A, 110 V)<br />
WT-12V-R-E Regulated 12 VDC Power Supply (2.5 A, 220 V)<br />
WT-24V 24 VDC Power Supply (110 V)<br />
Note: Each <strong>Ocean</strong> <strong>Optics</strong> sales region provides power supplies applicable to your part <strong>of</strong> <strong>the</strong> world.<br />
Miscellaneous Spe<strong>ctro</strong>m<strong>ete</strong>r Accessories<br />
Item Code<br />
SPEC-CADDY1500<br />
SPEC-CADDY1520<br />
SPEC-CADDY1560<br />
USB-CUT<br />
STEADIQ-UV<br />
STEADIQ-VIS<br />
Description<br />
Rugged, water-tight Pelican case for spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> and accessories; dimensions are 16.75" x 11.18" x 6.12" (42.5 x 28.4 x 15.5 cm)<br />
Rugged, water-tight Pelican case for spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> and accessories; dimensions are 18.06" x 12.89" x 6.72" (45.9 x 32.7 x 17.1 cm)<br />
Rugged, water-tight Pelican case for spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> and accessories; dimensions are 20.37" x 15.43" x 9.00" (51.7 x 39.2 x 22.9 cm)<br />
Demonstration USB Spe<strong>ctro</strong>m<strong>ete</strong>r with cutaway open optical bench; non-functioning spe<strong>ctro</strong>m<strong>ete</strong>r that's ideal as a teaching tool<br />
Cooler-like, environmentally controlled enclosure compatible with USB2000+/USB4000 and o<strong>the</strong>r spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong>; cove<strong>rs</strong> 200-1100 nm<br />
wavelength range<br />
Cooler-like, environmentally controlled enclosure compatible with USB2000+/USB4000 and o<strong>the</strong>r spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong>; cove<strong>rs</strong> 400-2500 nm<br />
wavelength range<br />
Note: Accessories specific to <strong>the</strong> Jaz Spe<strong>ctro</strong>m<strong>ete</strong>r are available in <strong>the</strong> Jaz section. Also, additional information on SteadiQ is available at <strong>the</strong> end <strong>of</strong> <strong>the</strong><br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> section.<br />
24 www.oceanoptics.com Tel: +1 727-733-2447
Application Notes<br />
Extended-range Measurement <strong>of</strong> a Deuterium-Halogen Light Source<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Broad UV-NIR spectral coverage can be achieved in a miniature spe<strong>ctro</strong>m<strong>ete</strong>r configured with our XR-1 Extended Range grating, which is<br />
responsive from 200-1050 nm. Our USB2000+ Spe<strong>ctro</strong>m<strong>ete</strong>r with an XR-1 grating maintains good optical resolution over <strong>the</strong> UV-NIR range, making<br />
it useful for applications such as measuring <strong>the</strong> relative output <strong>of</strong> a combination deuterium-halogen light source.<br />
Introduction<br />
The ability to provide UV-NIR coverage in a single miniature<br />
spe<strong>ctro</strong>m<strong>ete</strong>r has always been a challenge. Trade-<strong>of</strong>fs inherent<br />
to most diffraction gratings – most noticeably, <strong>the</strong> effect <strong>of</strong> blaze<br />
angle on <strong>the</strong> efficiency <strong>of</strong> <strong>the</strong> diffraction – can pose challenges<br />
for certain applications. While gratings were available that diffracted<br />
over a wide range, this came at <strong>the</strong> expense <strong>of</strong> decreased<br />
optical resolution and increased problems associated with<br />
second- and third-order overlap.<br />
Newer gratings such as <strong>the</strong> XR-1 provide good efficiency over<br />
a wider wavelength range (200-1050 nm) than is o<strong>the</strong>rwise<br />
possible with standard gratings. What’s more, good optical<br />
resolution (
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
HR Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
High Resolution Miniature Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Our HR Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> combine optics and ele<strong>ctro</strong>nics that are<br />
ideal for applications demanding high resolution and fast<br />
measurements. Popular for laser characterization, gas absorbance and<br />
emission line analysis, our HR Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> are especially<br />
useful where fast reactions need to be monitored.<br />
We <strong>of</strong>fer two HR-series models, HR2000+ and HR4000, in both<br />
application-ready (preconfigured for specific application types) and<br />
build-your-own (user-configured for maximum flexibility) ve<strong>rs</strong>ions.<br />
Also, <strong>the</strong> HR2000+ and HR4000 have comparable ele<strong>ctro</strong>nics and<br />
architecture, but different linear CCD array d<strong>ete</strong>cto<strong>rs</strong>.<br />
HR Optical Bench<br />
Our HR Optical Bench is responsive from 200-1100 nm and can be<br />
configured to address your application needs through customization<br />
<strong>of</strong> gratings, mirror coatings, d<strong>ete</strong>ctor window and aperture size. Its<br />
onboard A/D converter allows you to capture and transfer up to one<br />
full spectrum into memory every millisecond when interfaced via USB to your computer.<br />
The HR2000+ has a 2048-element Sony ILX511B d<strong>ete</strong>ctor and <strong>the</strong> HR4000 has <strong>the</strong> 3648-element Toshiba TCD1304AP d<strong>ete</strong>ctor. Both are linear silicon<br />
CCD arrays, with an effective range <strong>of</strong> 200-1100 nm, and are available with <strong>the</strong> same optical bench accessory options (quartz window for UV performance,<br />
order-sorting filte<strong>rs</strong> and so on). The HR2000+ has slightly better response in <strong>the</strong> UV and faster integration time; <strong>the</strong> HR4000 has an ele<strong>ctro</strong>nic<br />
shutter feature.<br />
Onboard Microcontroller<br />
The HR Series feature an onboard microcontroller that provides you considerable flexibility in controlling your spe<strong>ctro</strong>m<strong>ete</strong>r and accessories. Through<br />
its 30-pin connector, you can control <strong>the</strong> HR’s operating param<strong>ete</strong><strong>rs</strong> and light sources, create processes and retrieve information on external objects.<br />
Ten user-programmable digital inputs/outputs allow you to interface with o<strong>the</strong>r equipment or a triggering device.<br />
Plug and Play USB Operation<br />
The HR Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> interface easily to a PC, PLC or o<strong>the</strong>r embedded controller via USB 2.0 or RS-232 serial port. Data unique to your spe<strong>ctro</strong>m<strong>ete</strong>r<br />
is programmed into a memory chip inside that is read by our spe<strong>ctro</strong>m<strong>ete</strong>r operating s<strong>of</strong>tware – enabling hot-swapping between compute<strong>rs</strong>.<br />
Ele<strong>ctro</strong>nic Shutter<br />
HR4000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> comes with an ele<strong>ctro</strong>nic shutter for control <strong>of</strong> integration time from 10 µs-4 ms – an especially useful option for measuring<br />
transient events such as laser pulses. In free-running mode, <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r integration time is 3.8 ms-20 s.<br />
HR Series Spe<strong>ctro</strong>m<strong>ete</strong>r Models at a Glance<br />
You can configure an HR2000+ or HR4000 with gratings and optical bench accessories for a wide range <strong>of</strong> applications, or you can select from one <strong>of</strong><br />
several application-ready HR2000+/HR4000s described in <strong>the</strong> table below:<br />
Best for HR2000+ Series HR4000 Series<br />
High resolution over extended range (200-1050 nm) HR2000+CG HR4000CG-UV-NIR<br />
High resolution and enhanced sensitivity over extended<br />
range (200-1050 nm)<br />
HR2000+ES<br />
NA<br />
26 www.oceanoptics.com Tel: +1 727-733-2447
HR2000+CG Application-ready Spe<strong>ctro</strong>m<strong>ete</strong>r<br />
Preconfigured for High Resolution over Extended Range<br />
HR2000+CG<br />
The HR2000+CG Composite Grating Spe<strong>ctro</strong>m<strong>ete</strong>r is preconfigured<br />
with our HC-1 Grating. This proprietary variable-blazed grating was<br />
specifically designed to provide full spectral output throughout <strong>the</strong><br />
200-1100 nm range.<br />
Also, <strong>the</strong> HR2000+CG optical bench is preconfigured with a 5 µm<br />
slit for excellent optical resolution and our OFLV-200-1100 Variable<br />
Longpass Order-sorting Filter to eliminate second- and third-order<br />
effects.<br />
The HR2000+CG is ideal for biological and chemical applications<br />
where fast measurements and high resolution are needed.<br />
Features<br />
- Wide range from 200-1100 nm<br />
- High resolution (1.0 nm FHWM) over entire available range<br />
- Captures 1,000 full scans per second<br />
- Programmable microcontroller<br />
HR2000CG Radiometric Spectra<br />
Physical<br />
Dimensions:<br />
148.6 mm x 104.8 mm x 45.1 mm<br />
Weight:<br />
570 g<br />
D<strong>ete</strong>ctor<br />
D<strong>ete</strong>ctor:<br />
Sony ILX511B linear silicon CCD array<br />
D<strong>ete</strong>ctor range: 200-1100 nm<br />
Pixels:<br />
2048 pixels<br />
Pixel size:<br />
14 μm x 200 μm<br />
Pixel well depth: ~62,500 ele<strong>ctro</strong>ns<br />
Sensitivity:<br />
75 photons/count at 400 nm; 41 photons/count at 600 nm<br />
Optical Bench<br />
Design:<br />
f/4, Symmetrical crossed Czerny-Turner<br />
Focal length:<br />
101.6 mm input and output<br />
Entrance aperture: 5 µm wide slit<br />
Grating:<br />
HC-1<br />
OFLV filter:<br />
OFLV-200-1100<br />
UV enhanced window: Yes, UV2 quartz window<br />
Fiber optic connector: SMA 905 to 0.22 numerical aperture single-strand fiber<br />
Spe<strong>ctro</strong>scopic<br />
Optical resolution: 1.0 nm FWHM<br />
Signal-to-noise ratio: 250:1 (at full signal)<br />
A/D resolution: 14 bit<br />
Dark noise:<br />
12 RMS counts<br />
Dynamic range: 2 x 10 9 (system); 1300:1 for a single acquisition<br />
Integration time: 1 ms to 65 seconds<br />
Stray light:<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
HR2000+ES Application-ready Spe<strong>ctro</strong>m<strong>ete</strong>r<br />
Preconfigured for High Resolution and Sensitivity<br />
HR2000+ES<br />
The HR2000+ES Spe<strong>ctro</strong>m<strong>ete</strong>r is a preconfigured system for<br />
enhanced sensitivity. This system integrates a high-resolution<br />
optical bench with a powerful 2-MHz A/D converter, programmable<br />
ele<strong>ctro</strong>nics and a 2048-element CCD-array d<strong>ete</strong>ctor for optical<br />
resolution to ~1.33 nm (FWHM).<br />
The HR2000+ES has a slightly larger entrance slit (10 µm) and an L2<br />
d<strong>ete</strong>ctor collection lens for additional sensitivity in extended-range<br />
applications. We also include a UV2 quartz window for UV transmission<br />
and <strong>the</strong> OFLV-200-1100 Variable Longpass Order-sorting Filter<br />
to eliminate second- and third-order effects.<br />
Features<br />
- 1,000 full spectra per second<br />
- Programmable microcontroller<br />
- High-resolution bench<br />
- Plug and play operation<br />
Sample Applications for HR2000+CG/HR2000+ES<br />
- Thin film measurements <strong>of</strong> various substrates<br />
- Plasma monitoring<br />
- Reflectance <strong>of</strong> nanoparticles<br />
- Analysis <strong>of</strong> phospho<strong>rs</strong><br />
- Characterization <strong>of</strong> lase<strong>rs</strong><br />
- Solar irradiance<br />
- Spectral output <strong>of</strong> light sources<br />
Physical<br />
Dimensions:<br />
148.6 mm x 104.8 mm x 45.1 mm<br />
Weight:<br />
570 g<br />
D<strong>ete</strong>ctor<br />
D<strong>ete</strong>ctor:<br />
Sony ILX511B linear silicon CCD-array<br />
D<strong>ete</strong>ctor range: 200-1100 nm<br />
Pixels:<br />
2048 pixels<br />
Pixel size:<br />
14 μm x 200 μm<br />
Pixel well depth: ~62,500 ele<strong>ctro</strong>ns<br />
Sensitivity:<br />
75 photons/count at 400 nm; 41 photons/count at 600 nm<br />
Optical Bench<br />
Design:<br />
f/4, Symmetrical crossed Czerny-Turner<br />
Focal length:<br />
101.6 mm input and output<br />
Entrance aperture: 10 µm wide slit<br />
Grating:<br />
HC-1 provides 200-1100 nm range<br />
D<strong>ete</strong>ctor collection Yes, L2<br />
lens:<br />
OFLV filter:<br />
OFLV 200-1100 nm<br />
UV enhanced window: Yes, UV2 quartz window<br />
Fiber optic connector: SMA 905 to 0.22 numerical aperture single-strand<br />
optical fiber<br />
Spe<strong>ctro</strong>scopic<br />
Wavelength range: 200-1100 nm<br />
Optical resolution: ~1.33 nm FWHM<br />
Signal-to-noise ratio: 250:1 (at full signal)<br />
A/D resolution: 14 bit<br />
Dark noise:<br />
12 RMS counts<br />
Dynamic range: 2 x 10 8 (system); 1300:1 for a single acquisition<br />
Integration time: 1 ms-65 seconds (20 s typical)<br />
Stray light:<br />
HR4000CG-UV-NIR<br />
Our HR4000CG-UV-NIR Composite Grating Spe<strong>ctro</strong>m<strong>ete</strong>r uses our<br />
HC-1 Grating and provides full spectral output at <strong>the</strong> 200-1100 nm<br />
ranges with best efficiency at 200-1050 nm.<br />
This preconfigured system has an OFLV variable Longpass<br />
Order-sorting filter that eliminates second- and third-order effects<br />
and utilizes a 5 µm entrance slit for improved optical<br />
resolution performance.<br />
Features<br />
- Wide range <strong>of</strong> 200-1100 nm<br />
- High resolution (0.75 nm FWHM)<br />
- Installed HC-1 composite grating and order-sorting filter<br />
µW/cm^2/nm<br />
700<br />
600<br />
500<br />
400<br />
300<br />
200<br />
100<br />
Solar Irradiance Spectrum<br />
0<br />
200 300 400 500 600 700 800 900 1000<br />
WAVELENGTH (nm)<br />
HR4000CG-UV-NIR Spe<strong>ctro</strong>m<strong>ete</strong>r<br />
Preconfigured for High Resolution and Extended Range<br />
Physical<br />
Dimensions:<br />
148.6 mm x 104.8 mm x 45.1 mm<br />
Weight:<br />
570 g<br />
D<strong>ete</strong>ctor<br />
D<strong>ete</strong>ctor:<br />
Toshiba TCD1304AP linear CCD array<br />
D<strong>ete</strong>ctor range: 200-1100 nm<br />
Pixels:<br />
3648 pixels<br />
Pixel size:<br />
8 μm x 200 μm<br />
Pixel well depth: ~100,000 ele<strong>ctro</strong>ns<br />
Sensitivity:<br />
130 photons/count at 400 nm; 60 photons/count at 600 nm<br />
Optical Bench<br />
Design:<br />
f/4, Symmetrical crossed Czerny-Turner<br />
Focal length:<br />
101.6 mm input and output<br />
Entrance aperture: 5 µm wide slit<br />
Grating:<br />
HC-1<br />
D<strong>ete</strong>ctor collection Yes, L4<br />
lens:<br />
OFLV filter:<br />
OFLV 200-1100 nm<br />
UV enhanced window: Yes, UV4 quartz window<br />
Fiber optic connector: SMA 905 to 0.22 numerical aperture single-strand optical<br />
fiber<br />
Spe<strong>ctro</strong>scopic<br />
Wavelength range: 200-1100 nm (Grating dependent)<br />
Optical resolution: 0.75 nm FWHM<br />
Signal-to-noise ratio: 250:1 (at full signal)<br />
A/D resolution: 14 bit<br />
Dark noise:<br />
12 RMS counts<br />
Dynamic range: 2 x 10 8 (system); 1300:1 for a single acquisition<br />
Integration time: 3.8 ms-10 seconds<br />
Stray light:<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
HR User-configured Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> Overview<br />
Optimizing <strong>the</strong> HR2000+ and HR4000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> for Your Application<br />
All components within <strong>the</strong> HR Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> are fixed in place at <strong>the</strong> time <strong>of</strong> manufacture and designed to give you yea<strong>rs</strong> <strong>of</strong> reliable performance.<br />
Select <strong>the</strong> optical bench options to configure a system to perfectly suit your unique application needs.<br />
With <strong>the</strong> exception <strong>of</strong> <strong>the</strong> d<strong>ete</strong>ctor, <strong>the</strong> HR2000+ and HR4000 use identical optical bench accessories. By consulting with an <strong>Ocean</strong> <strong>Optics</strong> Applications<br />
Scientist, you can choose <strong>the</strong> optimum combination <strong>of</strong> aperture size, d<strong>ete</strong>ctor accessories, filte<strong>rs</strong>, gratings and more.<br />
HR Optical Bench Options<br />
Maximum flexibility is available with HR2000+ and HR4000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong>. Here are <strong>the</strong> optical bench accessories available for your spe<strong>ctro</strong>m<strong>ete</strong>r:<br />
1<br />
SMA 905 Connector<br />
Light from a fiber ente<strong>rs</strong> <strong>the</strong> optical bench through <strong>the</strong><br />
SMA 905 Connector. The SMA 905 bulkhead provides<br />
a precise locus for <strong>the</strong> end <strong>of</strong> <strong>the</strong> optical fiber, fixed slit,<br />
absorbing filter and fiber clad mode aperture.<br />
9<br />
8<br />
7<br />
4<br />
2<br />
Fixed Entrance Slit: specify slit size<br />
Light passes through <strong>the</strong> installed slit, which acts as <strong>the</strong><br />
entrance aperture. Slits come in various widths from<br />
5 µm to 200 µm. The slit is fixed in <strong>the</strong> SMA 905 bulkhead<br />
to sit against <strong>the</strong> end <strong>of</strong> a fiber.<br />
10<br />
5<br />
6<br />
3<br />
4<br />
5<br />
6<br />
Longpass Absorbing Filter: optional<br />
If selected, an absorbing filter is installed between <strong>the</strong> slit<br />
and <strong>the</strong> clad mode aperture in <strong>the</strong> SMA 905 bulkhead.<br />
The filter is used to limit <strong>the</strong> bandwidth <strong>of</strong> light entering<br />
<strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r or to balance color.<br />
Collimating Mirror: specify standard or SAG+<br />
The collimating mirror is matched to <strong>the</strong> 0.22 numerical<br />
aperture <strong>of</strong> our optical fiber. Light reflects from this<br />
mirror, as a collimated beam, toward <strong>the</strong> grating. You can<br />
opt to install a standard mirror or a UV absorbing SAG+<br />
mirror.<br />
Grating & Wavelength Range: specify grating<br />
& starting wavelength<br />
We install <strong>the</strong> grating on a platform that we <strong>the</strong>n rotate<br />
to select <strong>the</strong> starting wavelength you’ve specified. Then<br />
we permanently fix <strong>the</strong> grating in place to eliminate<br />
mechanical shifts or drift.<br />
Focusing Mirror: specify standard or SAG+<br />
This mirror focuses fi<strong>rs</strong>t-order spectra on <strong>the</strong> d<strong>ete</strong>ctor<br />
plane. Both <strong>the</strong> collimating and focusing mirro<strong>rs</strong> are<br />
made in-house to guarantee <strong>the</strong> highest reflectance and<br />
<strong>the</strong> lowest stray light possible. You can opt to install a<br />
standard or SAG+ mirror.<br />
7<br />
8<br />
9<br />
10<br />
1<br />
3<br />
2<br />
L2/L4 D<strong>ete</strong>ctor Collection Lens: optional<br />
One <strong>of</strong> <strong>the</strong>se cylindrical lenses, made in-house to ensure<br />
aberration-free performance, is fixed to <strong>the</strong> d<strong>ete</strong>ctor to focus<br />
<strong>the</strong> light from <strong>the</strong> tall slit onto <strong>the</strong> shorter d<strong>ete</strong>ctor elements.<br />
This increases light-collection efficiency. The L2 is for <strong>the</strong><br />
HR2000+; <strong>the</strong> L4 is for <strong>the</strong> HR4000.<br />
D<strong>ete</strong>ctor<br />
We <strong>of</strong>fer a 2048-element Sony ILX511B and 3648-element<br />
Toshiba TCD1304AP linear CCD array d<strong>ete</strong>ctor. Each pixel<br />
responds to <strong>the</strong> wavelength <strong>of</strong> light that strikes it. Ele<strong>ctro</strong>nics<br />
bring <strong>the</strong> compl<strong>ete</strong> spectrum to <strong>the</strong> s<strong>of</strong>tware.<br />
OFLV Variable Longpass Order-sorting Filter:<br />
optional<br />
Our proprietary filte<strong>rs</strong> precisely block second- and third-order<br />
light from reaching specific d<strong>ete</strong>ctor elements.<br />
UV2/UV4 D<strong>ete</strong>ctor Upgrade: optional<br />
When selected, <strong>the</strong> d<strong>ete</strong>ctor’s standard BK7 window is<br />
replaced with a quartz window to enhance <strong>the</strong> performance <strong>of</strong><br />
<strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r for applications
HR2000+<br />
One <strong>of</strong> our most popular items, <strong>the</strong> HR2000+ Spe<strong>ctro</strong>m<strong>ete</strong>r features<br />
a high-resolution optical bench, a powerful 2-MHz analog-to-digital<br />
(A/D) converter, programmable ele<strong>ctro</strong>nics, a 2048-element CCDarray<br />
d<strong>ete</strong>ctor and a high-speed USB 2.0 port.<br />
This innovative combination produces an extremely fast<br />
spe<strong>ctro</strong>m<strong>ete</strong>r and provides resolution to 0.035 nm (FWHM).<br />
The HR2000+ allows use<strong>rs</strong> to capture and store a full spectrum into<br />
memory every millisecond (that’s 1,000 full spectra every second)<br />
when <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r is interfaced to a computer via a USB 2.0 port.<br />
The HR2000+ is perfect for chemical, biochemical and o<strong>the</strong>r<br />
applications where fast reactions need to be monitored and fine<br />
spectral features need to be resolved.<br />
The HR2000+ interfaces to a computer via USB 2.0 or RS-232 serial<br />
port. When combined with <strong>the</strong> Remora Network Adapter, <strong>the</strong> USB<br />
interface allows communication via E<strong>the</strong>rnet and/or wireless network.<br />
When using <strong>the</strong> serial port, <strong>the</strong> HR2000+ requires a single 5-volt<br />
power supply (not included). Data unique to each spe<strong>ctro</strong>m<strong>ete</strong>r are<br />
programmed into a memory chip on <strong>the</strong> HR2000+; SpectraSuite<br />
s<strong>of</strong>tware reads <strong>the</strong>se values for easy setup.<br />
Features<br />
- 1,000 full spectra per second<br />
- Programmable microcontroller<br />
- High-resolution performance<br />
- Multiple bench and interface options<br />
HR2000+ Spe<strong>ctro</strong>m<strong>ete</strong>r<br />
User-Configured for Flexibility<br />
Physical<br />
Dimensions:<br />
148.6 mm x 104.8 mm x 45.1 mm<br />
Weight:<br />
570 g<br />
D<strong>ete</strong>ctor<br />
D<strong>ete</strong>ctor:<br />
Sony ILX511B linear silicon CCD-array<br />
D<strong>ete</strong>ctor range: 200-1100 nm<br />
Pixels:<br />
2048 pixels<br />
Pixel size:<br />
14 μm x 200 μm<br />
Pixel well depth: ~62,500 ele<strong>ctro</strong>ns<br />
Sensitivity:<br />
75 photons/count at 400 nm; 41 photons/count at 600 nm<br />
Optical Bench<br />
Design:<br />
f/4, Symmetrical crossed Czerny-Turner<br />
Focal length:<br />
101.6 mm input and output<br />
Entrance aperture: 5, 10, 25, 50, 100 or 200 µm wide slits or fiber (no slit)<br />
Grating options: 14 different gratings, UV through Shortwave NIR<br />
HC-1 grating option: Provides 200-1100 nm range<br />
D<strong>ete</strong>ctor collection Yes, L2<br />
lens option:<br />
OFLV filter options: OFLV 200-1100 nm<br />
O<strong>the</strong>r bench filter Longpass OF-1 filte<strong>rs</strong><br />
options:<br />
Collimating and focusing<br />
Standard or SAG+UPG-HR<br />
mirro<strong>rs</strong>:<br />
UV enhanced window: Yes, UV2 quartz window<br />
Fiber optic connector: SMA 905 to 0.22 numerical aperture single-strand<br />
optical fiber<br />
Spe<strong>ctro</strong>scopic<br />
Wavelength range: Grating dependent<br />
Optical resolution: ~0.035-6.8 nm FWHM<br />
Signal-to-noise ratio: 250:1 (at full signal)<br />
A/D resolution: 14 bit<br />
Dark noise:<br />
12 RMS counts<br />
Dynamic range: 2 x 10 8 (system); 1300:1 for a single acquisition<br />
Integration time: 1 ms-65 seconds (20 s typical)<br />
Stray light:<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
HR4000 Spe<strong>ctro</strong>m<strong>ete</strong>r<br />
User-Configured for Flexibility<br />
HR4000<br />
Inside <strong>the</strong> HR4000 Spe<strong>ctro</strong>m<strong>ete</strong>r is a 3648-element CCD-array<br />
Toshiba d<strong>ete</strong>ctor that enables optical resolution as precise as<br />
0.02 nm (FWHM). Responsive from 200-1100 nm, <strong>the</strong> HR4000 can be<br />
customized for your setup needs through a choice <strong>of</strong> gratings, slits<br />
and o<strong>the</strong>r optical bench options.<br />
The HR4000 gives you <strong>the</strong> freedom to set integration time and<br />
features an ele<strong>ctro</strong>nic shutter that helps minimize saturation – even<br />
with 3.8 ms integration.<br />
The HR4000 interfaces easily with your computer or PLC through<br />
USB 2.0 or RS-232 ports. And, with its 10 user-programmable digital<br />
inputs/outputs, <strong>the</strong> HR4000 <strong>of</strong>fe<strong>rs</strong> unparalleled connectivity with<br />
external equipment.<br />
Features<br />
- Onboard microcontroller and ele<strong>ctro</strong>nic shutter<br />
- 0.02 nm optical resolution (FWHM) possible<br />
- Choice <strong>of</strong> configurations and accessories<br />
Technical Tip<br />
The dynamic range <strong>of</strong> a system is<br />
<strong>the</strong> full scale signal divided by <strong>the</strong><br />
minimum resolvable signal. For our<br />
spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong>, <strong>the</strong> minimum<br />
resolvable signal is <strong>the</strong> standard<br />
deviation <strong>of</strong> <strong>the</strong> dark signal. A<br />
common misunde<strong>rs</strong>tanding is to interchange dynamic range and<br />
A/D resolution. However, a dynamic range measurement includes<br />
<strong>the</strong> system’s minimum noise level (e.g., d<strong>ete</strong>ctor readout noise<br />
and ele<strong>ctro</strong>nic noise). It’s most applicable to low light level<br />
applications because it defines minimum d<strong>ete</strong>ctable signal.<br />
Physical<br />
Dimensions:<br />
148.6 mm x 104.8 mm x 45.1 mm<br />
Weight:<br />
570 g<br />
D<strong>ete</strong>ctor<br />
D<strong>ete</strong>ctor:<br />
Toshiba TCD1304AP linear CCD array<br />
D<strong>ete</strong>ctor range: 200-1100 nm<br />
Pixels:<br />
3648 pixels<br />
Pixel size:<br />
8 μm x 200 μm<br />
Pixel well depth: ~100,000 ele<strong>ctro</strong>ns<br />
Sensitivity:<br />
130 photons/count at 400 nm; 60 photons/count at 600 nm<br />
Optical Bench<br />
Design:<br />
f/4, Symmetrical crossed Czerny-Turner<br />
Focal length:<br />
101.6 mm input and output<br />
Entrance aperture: 5, 10, 25, 50, 100 or 200 µm wide slits or fiber (no slit)<br />
Grating options: 14 different gratings, UV through Shortwave NIR<br />
HC-1 grating option: Provides 200-1050 nm range (best efficiency)<br />
D<strong>ete</strong>ctor collection Yes, L4<br />
lens option:<br />
OFLV filter options: OFLV-200-1100<br />
O<strong>the</strong>r bench filter Longpass OF-1 filte<strong>rs</strong><br />
options:<br />
Collimating and focusing<br />
Standard or SAG+UPG-HR<br />
mirro<strong>rs</strong>:<br />
UV enhanced window: Yes, UV4 quartz window<br />
Fiber optic connector: SMA 905 to 0.22 numerical aperture single-strand<br />
optical fiber<br />
Spe<strong>ctro</strong>scopic<br />
Wavelength range: Grating dependent<br />
Optical resolution: ~0.02-8.4 nm FWHM<br />
Signal-to-noise ratio: 300:1 (at full signal)<br />
A/D resolution: 14 bit<br />
Dark noise:<br />
12 RMS counts<br />
Dynamic range: 2 x 10 8 (system); 1300:1 for a single acquisition<br />
Integration time: 3.8 ms-10 seconds<br />
Stray light:<br />
HR User-Configured Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Bench Accessories for HR2000+/HR4000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
The magic behind our HR2000+ and HR4000 miniature spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> is <strong>the</strong> options you can select to configure your optical bench to perfectly suit<br />
your unique application needs. By consulting with an <strong>Ocean</strong> <strong>Optics</strong> Applications Scientist, you can choose <strong>the</strong> optimum combination <strong>of</strong> aperture size,<br />
d<strong>ete</strong>ctor accessories, filte<strong>rs</strong>, gratings and more.<br />
Product Section<br />
SMA 905 Connector<br />
Our entrance slits are rectangular apertures that are 1 mm tall and come in varying widths from<br />
5 µm to 200 µm. Smaller slit sizes achieve <strong>the</strong> best optical resolution.<br />
Fixed Entrance Slits<br />
Our entrance slits are rectangular apertures that are 1 mm tall and come in varying widths from<br />
5 µm to 200 µm. Smaller slit sizes achieve <strong>the</strong> best optical resolution.<br />
Slit Description HR2000+<br />
Pixel Resolution<br />
SLIT-5 5-µm wide x 1-mm high ~1.5 pixels ~2.0 pixels<br />
SLIT-10 10-µm wide x 1-mm high ~2.0 pixels ~3.7 pixels<br />
SLIT-25 25-µm wide x 1-mm high ~2.5 pixels ~4.4 pixels<br />
SLIT-50 50-µm wide x 1-mm high ~4.2 pixels ~7.4 pixels<br />
SLIT-100 100-µm wide x 1-mm high ~8.0 pixels ~14.0 pixels<br />
SLIT-200 200-µm wide x 1-mm high ~15.3 pixels ~26.8 pixels<br />
HR4000<br />
Pixel Resolution<br />
Longpass Absorbing Filter<br />
Whe<strong>the</strong>r you select a Longpass Absorbing or Blocking Filter, each has a transmission band and a<br />
blocking band to restrict radiation to a certain wavelength region. This helps eliminate second- and<br />
third-order effects. Filte<strong>rs</strong> are installed permanently.<br />
OF1-WG305<br />
OF1-GG375<br />
OF1-GG395<br />
OF1-GG475<br />
OF1-OG515<br />
OF1-OG550<br />
OF1-OG590<br />
Item<br />
Description<br />
Longpass filter; transmits light >305 nm<br />
Longpass filter; transmits light >375 nm<br />
Longpass filter, installed, transmits light >395 nm<br />
Longpass filter; transmits light >475 nm<br />
Longpass filter; transmits light >515 nm<br />
Longpass filter; transmits light >550 nm<br />
Longpass filter: transmits light >590 nm<br />
Collimating and Focusing Mirro<strong>rs</strong><br />
You can replace our standard aluminum-coated reflective mirro<strong>rs</strong> with our UV-absorbing SAG+<br />
Mirro<strong>rs</strong>. These mirro<strong>rs</strong> increase reflectance in <strong>the</strong> VIS-NIR range while increasing your spe<strong>ctro</strong>m<strong>ete</strong>r’s<br />
sensitivity. They also absorb nearly all UV light – reducing <strong>the</strong> effects <strong>of</strong> excitation scattering in<br />
fluorescence measurements. They have excellent reflectivity (more than 95% across <strong>the</strong> VIS-NIR).<br />
Item Code: SAG+UPG-HR<br />
Grating and Wavelength Range<br />
With a choice <strong>of</strong> 14 gratings, you can easily customize <strong>the</strong> spectral range and most efficient region<br />
<strong>of</strong> your HR Series Spe<strong>ctro</strong>m<strong>ete</strong>r. Our gratings are permanently fixed in place at <strong>the</strong> time <strong>of</strong> manufacture<br />
and are available in both ruled and holographic ve<strong>rs</strong>ions. See page 36 for grating options and<br />
efficiency curves and consult an <strong>Ocean</strong> <strong>Optics</strong> Applications Scientist for details.<br />
www.oceanoptics.com Tel: +1 727-733-2447 33
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
HR User-configured Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
D<strong>ete</strong>cto<strong>rs</strong> and Accessories for HR2000+/HR4000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
D<strong>ete</strong>cto<strong>rs</strong><br />
The HR2000+ utilizes <strong>the</strong> Sony ILX511B linear silicon CCD array d<strong>ete</strong>ctor. Our HR4000 High-resolution<br />
Spe<strong>ctro</strong>m<strong>ete</strong>r utilizes <strong>the</strong> Toshiba TCD1304AP linear CCD array d<strong>ete</strong>ctor, which has some ele<strong>ctro</strong>nic<br />
advances over <strong>the</strong> Sony, such as an ele<strong>ctro</strong>nic shutter. Both are linear silicon CCD arrays, with<br />
an effective range <strong>of</strong> 200-1100 nm, and with <strong>the</strong> same dynamic range (1300:1). The Toshiba d<strong>ete</strong>ctor<br />
has a slightly better SNR <strong>of</strong> 300:1 ve<strong>rs</strong>us 250:1.<br />
L2 and L4 D<strong>ete</strong>ctor Collection Lens<br />
These cylindrical lenses ensure aberration-free performance and are fixed to <strong>the</strong> d<strong>ete</strong>ctor’s<br />
window to focus light from <strong>the</strong> tall slit onto <strong>the</strong> shorter d<strong>ete</strong>ctor elements. The L2 and L4 increase<br />
light collection efficiency and help reduce stray light. They are also useful in configurations with<br />
large-diam<strong>ete</strong>r fibe<strong>rs</strong> for low light-level applications.<br />
D<strong>ete</strong>cto<strong>rs</strong> with OFLV Filte<strong>rs</strong><br />
OFLV Variable Longpass Order-sorting Filte<strong>rs</strong> are applied to <strong>the</strong> d<strong>ete</strong>ctor’s window to eliminate second- and third-order effects. We use a patented<br />
coating technology to apply <strong>the</strong> filter to <strong>the</strong> substrate.<br />
UV2 and UV4 D<strong>ete</strong>ctor Window Upgrades<br />
For any application
HR User-Configured Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Choosing <strong>the</strong> Right Grating<br />
Groove Density<br />
The Groove density (mm -1 ) <strong>of</strong> a grating d<strong>ete</strong>rmines its dispe<strong>rs</strong>ion, while <strong>the</strong> angle<br />
<strong>of</strong> <strong>the</strong> groove d<strong>ete</strong>rmines <strong>the</strong> most efficient region <strong>of</strong> <strong>the</strong> spectrum. The greater<br />
<strong>the</strong> groove density, <strong>the</strong> better <strong>the</strong> optical resolution possible, but <strong>the</strong> more truncated<br />
<strong>the</strong> spectral range.<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Spectral Range<br />
The dispe<strong>rs</strong>ion <strong>of</strong> <strong>the</strong> grating across <strong>the</strong> linear array is also expressed as <strong>the</strong> “size”<br />
<strong>of</strong> <strong>the</strong> spectra on <strong>the</strong> array. The spectral range (bandwidth) is a function <strong>of</strong> <strong>the</strong><br />
groove density and does not change. When you choose a starting wavelength<br />
for a spe<strong>ctro</strong>m<strong>ete</strong>r, you add its spectral range to <strong>the</strong> starting wavelength to<br />
d<strong>ete</strong>rmine <strong>the</strong> wavelength range. For several gratings, <strong>the</strong> spectral range <strong>of</strong> a<br />
grating varies according to <strong>the</strong> starting wavelength range. The rule <strong>of</strong> thumb is<br />
this: <strong>the</strong> higher <strong>the</strong> starting wavelength, <strong>the</strong> more truncated <strong>the</strong> spectral range.<br />
Blaze Wavelength<br />
For ruled gratings, <strong>the</strong> blaze wavelength is <strong>the</strong> peak wavelength in an efficiency<br />
curve. For holographic gratings, it is <strong>the</strong> most efficient wavelength region.<br />
Best Efficiency ( >30%)<br />
All ruled or holographically etched gratings optimize fi<strong>rs</strong>t-order spectra at certain<br />
wavelength regions; <strong>the</strong> “best” or “most efficient” region is <strong>the</strong> range where<br />
efficiency is >30%. In some cases, gratings have a greater spectral range than is<br />
efficiently diffracted. For example, Grating 1 has about a 650 nm spectral range,<br />
but is most efficient from 200-575 nm. In this case, wavelengths >575 nm will<br />
have lower intensity due to <strong>the</strong> grating’s reduced efficiency.<br />
Grating and Wavelength Range<br />
With a choice <strong>of</strong> 14 gratings, you can easily customize your HR Series Spe<strong>ctro</strong>m<strong>ete</strong>r through its groove density, spectral range and blaze wavelength.<br />
Our gratings are permanently fixed in place at <strong>the</strong> time <strong>of</strong> manufacture and we <strong>of</strong>fer both ruled and holographic ve<strong>rs</strong>ions. Questions about which one<br />
is best for you? Contact an <strong>Ocean</strong> <strong>Optics</strong> Applications Scientist for details.<br />
Grating<br />
Number<br />
Intended<br />
Use<br />
Groove<br />
Density<br />
Spectral<br />
Range<br />
Blaze<br />
Wavelength<br />
HC-1 UV-NIR 300/600 variable 900 nm Variable 200-1100 nm<br />
H1 UV 600 425-445 nm 300 nm 200-575 nm<br />
H2 UV-VIS 600 415-445 nm 400 nm 250-800 nm<br />
H3 VIS-Color 600 410-440 nm 500 nm 350-850 nm<br />
H4 NIR 600 410-430 nm 750 nm 530-1100 nm<br />
H5 UV-VIS 1200 205-220 nm Holographic UV 200-400 nm<br />
H6 NIR 1200 140-195 nm 750 nm 500-1100 nm<br />
H7 UV-VIS 2400 72-102 nm Holographic UV 200-500 nm<br />
H9 VIS-NIR 1200 165-205 nm Holographic VIS 400-800 nm<br />
H10 UV-VIS 1800 95-140 nm Holographic UV 200-635 nm<br />
H11 UV-VIS 1800 75-135 nm Holographic VIS 320-720 nm<br />
H12 UV-VIS 2400 60-100 nm Holographic VIS 260-780 nm<br />
H13 UV-NIR 300 800-900 nm 500 nm 300-1100 nm<br />
H14 NIR 600 410-420 nm 1000 nm 650-1100 nm<br />
Best<br />
Efficiency (>30%)<br />
www.oceanoptics.com Tel: +1 727-733-2447 35
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
HR User-Configured Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Gratings for HR2000+/HR4000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
The graphs below are grating efficiency curves for gratings with groove densities <strong>of</strong> 600, 1200, 1800 and 2400 mm -1 (<strong>the</strong> HC-1 has variable groove<br />
density). Additional information is available at www.oceanoptics.com/Products/bench_grating_hr.asp.<br />
Groove Density <strong>of</strong> 600 mm -1 Groove Density <strong>of</strong> 1200 mm -1<br />
Relative Efficiency<br />
Relative Efficiency<br />
Grating #1 Grating #2 Grating #3 Grating #4 Grating #14<br />
Grating #5 Grating #6 Grating #9<br />
Groove Density <strong>of</strong> 1800 mm -1<br />
Groove Density <strong>of</strong> 2400 mm -1<br />
Relative Efficiency<br />
Relative Efficiency<br />
Grating #10 Grating #11<br />
Grating #7 Grating #12<br />
Grating Selection Tips:<br />
Variable Groove Density <strong>of</strong> 600 mm -1 /300 mm -1<br />
- These efficiency curves relate only to <strong>the</strong> grating. System response<br />
is affected by a number <strong>of</strong> variables, including d<strong>ete</strong>ctor response.<br />
- Grating selection <strong>of</strong>ten involves trade-<strong>of</strong>fs. For example, gratings<br />
with very high groove density (mm -1 ) allow greater optical resolution<br />
but at <strong>the</strong> expense <strong>of</strong> a truncated spectral range. If <strong>the</strong> user is<br />
characterizing two or three closely aligned laser wavelengths, such<br />
a trade-<strong>of</strong>f <strong>of</strong> resolution for range might be acceptable. For o<strong>the</strong>r<br />
applications, a wider range with good resolution would make<br />
better sense.<br />
Absolute Efficiency (%)<br />
- The HC-1 grating is a good option for broad spectral coverage<br />
(200-1100 nm) without sacrificing optical resolution.<br />
HC-1<br />
36 www.oceanoptics.com Tel: +1 727-733-2447
HR User-Configured Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Predicted Ranges & Resolution<br />
Predicted Ranges & Resolution<br />
These graphs demonstrate <strong>the</strong> range and resolution <strong>of</strong> your “HR” Bench Spe<strong>ctro</strong>m<strong>ete</strong>r with a 5 µm slit. See our website for additional graphs <strong>of</strong> ranges<br />
and resolutions for every slit size.<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
“HR” Bench with Sony D<strong>ete</strong>ctor: HR2000+<br />
“HR” Bench with Toshiba D<strong>ete</strong>ctor: HR4000<br />
SPECTRAL RANGE (nm)<br />
450<br />
445<br />
440<br />
435<br />
430<br />
425<br />
420<br />
415<br />
410<br />
600 mm -1 Grating and 5 µm Slit<br />
0.33<br />
0.32<br />
0.31<br />
0.30<br />
RESOLUTION (nm)<br />
Example:<br />
If <strong>the</strong> starting<br />
wavelength is 400 nm,<br />
<strong>the</strong>n <strong>the</strong> range is<br />
~437 nm, providing<br />
a 400-837 nm<br />
wavelength range and<br />
0.32 nm resolution.<br />
SPECTRAL RANGE (nm)<br />
450<br />
445<br />
440<br />
435<br />
430<br />
425<br />
420<br />
415<br />
410<br />
600 mm -1 Grating and 5 µm Slit<br />
0.245<br />
0.240<br />
0.235<br />
0.230<br />
0.225<br />
RESOLUTION (nm)<br />
Example:<br />
If <strong>the</strong> starting<br />
wavelength is 400 nm,<br />
<strong>the</strong>n <strong>the</strong> range is<br />
~437 nm, providing<br />
a 400-837 nm<br />
wavelength range and<br />
0.239 nm resolution.<br />
405<br />
400<br />
0.293<br />
200 400 600 800 1000<br />
STARTING WAVELENGTH (nm)<br />
405<br />
400<br />
0.220<br />
200 400 600 800 1000<br />
STARTING WAVELENGTH (nm)<br />
SPECTRAL RANGE (nm)<br />
220<br />
210<br />
200<br />
190<br />
180<br />
170<br />
160<br />
150<br />
1200 mm -1 Grating and 5 µm Slit<br />
0.16<br />
0.15<br />
0.14<br />
0.13<br />
0.12<br />
0.11<br />
RESOLUTION (nm)<br />
Example:<br />
If <strong>the</strong> starting<br />
wavelength is 600 nm,<br />
<strong>the</strong>n <strong>the</strong> range is<br />
~188 nm, providing<br />
a 600-788 nm<br />
wavelength range and<br />
0.137 nm resolution.<br />
SPECTRAL RANGE (nm)<br />
220<br />
210<br />
200<br />
190<br />
180<br />
170<br />
160<br />
150<br />
1200 mm -1 Grating and 5 µm Slit<br />
0.120<br />
0.115<br />
0.110<br />
0.105<br />
0.100<br />
0.095<br />
0.090<br />
0.085<br />
0.080<br />
RESOLUTION (nm)<br />
Example:<br />
If <strong>the</strong> starting<br />
wavelength is 300 nm,<br />
<strong>the</strong>n <strong>the</strong> range is<br />
~215 nm, providing<br />
a 300-515 nm<br />
wavelength range and<br />
0.117 nm resolution.<br />
140<br />
0.10<br />
200 400 600 800 1000<br />
STARTING WAVELENGTH (nm)<br />
140<br />
0.075<br />
200 400 600 800 1000<br />
STARTING WAVELENGTH (nm)<br />
SPECTRAL RANGE (nm)<br />
150<br />
140<br />
130<br />
120<br />
110<br />
100<br />
90<br />
80<br />
1800 mm -1 Grating and 5 µm Slit<br />
0.10<br />
0.09<br />
0.08<br />
0.07<br />
0.06<br />
RESOLUTION (nm)<br />
Example:<br />
If <strong>the</strong> starting<br />
wavelength is 700 nm,<br />
<strong>the</strong>n <strong>the</strong> range is<br />
~90 nm, providing<br />
a 700-790 nm<br />
wavelength range and<br />
0.065 nm resolution.<br />
SPECTRAL RANGE (nm)<br />
150<br />
140<br />
130<br />
120<br />
110<br />
100<br />
90<br />
80<br />
1800 mm -1 Grating and 5 µm Slit<br />
0.080<br />
0.070<br />
0.060<br />
0.050<br />
RESOLUTION (nm)<br />
Example:<br />
If <strong>the</strong> starting<br />
wavelength is 700 nm,<br />
<strong>the</strong>n <strong>the</strong> range is<br />
~90 nm, providing<br />
a 700-790 nm<br />
wavelength range and<br />
0.05 nm resolution.<br />
70<br />
0.05<br />
200 400 600 800 1000<br />
STARTING WAVELENGTH (nm)<br />
70<br />
0.040<br />
200 400 600 800 1000<br />
STARTING WAVELENGTH (nm)<br />
SPECTRAL RANGE (nm)<br />
110<br />
100<br />
90<br />
80<br />
70<br />
60<br />
50<br />
40<br />
2400 mm -1 Grating and 5 µm Slit<br />
0.07<br />
0.06<br />
0.05<br />
0.04<br />
0.03<br />
RESOLUTION (nm)<br />
Example:<br />
If <strong>the</strong> starting<br />
wavelength is 600 nm,<br />
<strong>the</strong>n <strong>the</strong> range is<br />
~56 nm, providing<br />
a 600-656 nm<br />
wavelength range and<br />
0.039 nm resolution.<br />
SPECTRAL RANGE (nm)<br />
110<br />
100<br />
90<br />
80<br />
70<br />
60<br />
50<br />
40<br />
2400 mm -1 Grating and 5 µm Slit<br />
0.055<br />
0.045<br />
0.035<br />
0.025<br />
RESOLUTION (nm)<br />
Example:<br />
If <strong>the</strong> starting<br />
wavelength is 600 nm,<br />
<strong>the</strong>n <strong>the</strong> range is<br />
~56 nm, providing<br />
a 600-656 nm<br />
wavelength range and<br />
0.029 nm resolution.<br />
30<br />
0.02<br />
200 400 600 800 1000<br />
STARTING WAVELENGTH (nm)<br />
30<br />
0.015<br />
200 400 600 800 1000<br />
STARTING WAVELENGTH (nm)<br />
www.oceanoptics.com Tel: +1 727-733-2447 37
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
HR Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Accessories for Ultimate Control<br />
Accessories for our HR Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> give you incredible ve<strong>rs</strong>atility, help make your measurements easier and add access to a host <strong>of</strong> o<strong>the</strong>r<br />
functions.<br />
Breakout Box<br />
For easier access to a variety <strong>of</strong> functions in <strong>the</strong> HR Series, <strong>the</strong><br />
HR4-BREAKOUT is a passive module that separates signals<br />
from <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r’s 30-pin accessory port to an array <strong>of</strong><br />
standard connecto<strong>rs</strong> and heade<strong>rs</strong>.<br />
Use it for external triggering, RS-232 interface, light source coupling,<br />
analog input/output and more. This box is powered by<br />
<strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r and interfaces directly to it via its serial port.<br />
Item Code: HR4-BREAKOUT<br />
HR4, USB4, HR2+, QE adapter for external connections<br />
Item Code: HR4-CBL-DB15<br />
Accessory cable<br />
Remora Wireless Access Point<br />
Add <strong>the</strong> Remora to your HR configuration to communicate over E<strong>the</strong>rnet<br />
or Wi-Fi. When used with SpectraSuite S<strong>of</strong>tware, Remora turns your device<br />
into a network accessible spe<strong>ctro</strong>m<strong>ete</strong>r. Remotely capture spectral data<br />
from anywhere via E<strong>the</strong>rnet or wireless network (ra<strong>the</strong>r than traditional<br />
USB). This allows you to change param<strong>ete</strong><strong>rs</strong> and enjoy all <strong>of</strong> <strong>the</strong> functionality<br />
<strong>of</strong> your spe<strong>ctro</strong>m<strong>ete</strong>r as if it were connected directly to your computer.<br />
Item Code: REMORA-HR-FCC<br />
E<strong>the</strong>rnet/wireless adapter for HR2000, HR2000+ and HR4000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong>; Americas<br />
ve<strong>rs</strong>ion<br />
Item Code: REMORA-HR-CE<br />
E<strong>the</strong>rnet/wireless adapter for HR2000, HR2000+ and HR4000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong>; non-Americas<br />
ve<strong>rs</strong>ion<br />
38 www.oceanoptics.com Tel: +1 727-733-2447<br />
Technical Tip<br />
HR4000/USB4000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> use <strong>the</strong> Toshiba TCD1304 d<strong>ete</strong>ctor and can be operated in External Hardware Trigger<br />
mode. There are some subtle differences between spectra acquired in this mode and spectra acquired in Normal (freerunning)<br />
mode. This is due to differences in timing signals between <strong>the</strong> two operating modes. In External Hardware<br />
Trigger mode, <strong>the</strong> Toshiba TCD1304 d<strong>ete</strong>ctor operates in Shutter mode. This is done to continuously clear <strong>the</strong> d<strong>ete</strong>ctor<br />
while waiting for <strong>the</strong> trigger signal. With this approach, key system performance param<strong>ete</strong><strong>rs</strong> such as signal to noise ratio,<br />
RMS noise and so on are maintained.<br />
Still, <strong>the</strong>re are limitations associated with Shutter mode operation. For example, d<strong>ete</strong>ctor sensitivity can change. This is not an ele<strong>ctro</strong>nic anomaly<br />
but an inherent characteristic <strong>of</strong> <strong>the</strong> CCD. The consequence is that you need to make all your measurements, including dark and reference measurements,<br />
in <strong>the</strong> same trigger mode as your sample. This makes certain applications difficult to achieve with an HR4000 or USB4000. For those<br />
applications -- including time normalized analysis and absolute irradiance and color measurements, all below 3.8 ms – we <strong>of</strong>fer <strong>the</strong> HR2000+ and<br />
USB2000+. For information on o<strong>the</strong>r trade-<strong>of</strong>fs associated with Shutter mode operation, visit <strong>the</strong> Technical Resources section <strong>of</strong> our website at<br />
www.oceanoptics.com/technical.asp.
Application Notes<br />
Using <strong>the</strong> HR2000+CG for Reflection Testing<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
The HR2000+CG Spe<strong>ctro</strong>m<strong>ete</strong>r is a ve<strong>rs</strong>atile, high-performance option for a range <strong>of</strong> applications. In this experiment, we conducted a feasibility<br />
study for a customer measuring reflectance <strong>of</strong> ceramic discs.<br />
Figure 1.<br />
Background<br />
The customer supplied us with five composite ceramic disc<br />
samples. Each sample comprised both grey and white portions<br />
and was labeled accordingly. Special care was taken to isolate<br />
similar disc samples from each o<strong>the</strong>r. The purpose <strong>of</strong> this study<br />
was to measure <strong>the</strong> percent reflection <strong>of</strong> <strong>the</strong> grey portion <strong>of</strong><br />
<strong>the</strong> discs.<br />
Experimental Procedure<br />
The samples were analyzed using <strong>the</strong> HR2000+CG Spe<strong>ctro</strong>m<strong>ete</strong>r<br />
(200-1050 nm); an HL-2000-HP-FHSA, which has 20 W output<br />
power; an R400-7-VIS-NIR Reflection Probe with <strong>the</strong> RPH-1<br />
Probe Holder; and SpectraSuite spe<strong>ctro</strong>scopy s<strong>of</strong>tware. Multiple<br />
measurements <strong>of</strong> each sample (on both sides) were acquired to<br />
demonstrate <strong>the</strong> repeatability <strong>of</strong> <strong>the</strong> prescribed setup (see photo<br />
above). This setup occupies a small footprint.<br />
Results<br />
The multiple measurements <strong>of</strong> <strong>the</strong> grey samples demonstrated<br />
superior reflection spectrum repeatability over <strong>the</strong> region <strong>of</strong><br />
400-1000 nm (Figure 1). Ano<strong>the</strong>r grey sample exhibited good<br />
repeatability over <strong>the</strong> same spectral range with deviation from<br />
<strong>the</strong> mean reflectivity within ±13%. However, <strong>the</strong> next set <strong>of</strong><br />
samples displayed a wide variation in reflection spectra over<br />
400-1000 nm with a deviation from <strong>the</strong> mean on <strong>the</strong> order <strong>of</strong><br />
±30% (Figure 2).<br />
Figure 2.<br />
Despite <strong>the</strong> superior repeatability <strong>of</strong> <strong>the</strong> fi<strong>rs</strong>t set <strong>of</strong> samples, differentiation<br />
between <strong>the</strong> two samples would be difficult given <strong>the</strong> flat spectral nature<br />
and roughly <strong>the</strong> same mean reflectivity. The second set <strong>of</strong> samples can be<br />
differentiated from <strong>the</strong> previous two in spite <strong>of</strong> a higher deviation from its<br />
mean reflectivity.<br />
Unfortunately, <strong>the</strong> ±30% spread in reflection spectra for <strong>the</strong> initial samples<br />
rende<strong>rs</strong> it difficult to differentiate one from <strong>the</strong> o<strong>the</strong>r and from <strong>the</strong> o<strong>the</strong>r<br />
grey disc samples.<br />
This conclusion reinforced <strong>the</strong> customer’s hypo<strong>the</strong>sis that specular<br />
reflection alone would not be sufficient for discriminating <strong>the</strong> variations in<br />
<strong>the</strong> ceramic disc samples.<br />
www.oceanoptics.com Tel: +1 727-733-2447 39
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
QE65000 and Maya2000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Scientific-Grade Spe<strong>ctro</strong>scopy in a Small Footprint<br />
<strong>Ocean</strong> <strong>Optics</strong> <strong>of</strong>fe<strong>rs</strong> highly sensitive spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> specifically suited for low<br />
light-level applications such as fluorescence, DNA sequencing and Raman<br />
spe<strong>ctro</strong>scopy. The QE65000 achieves up to 90% quantum efficiency with<br />
high signal-to-noise and excellent signal processing speed. Although <strong>the</strong><br />
QE65000 features a back-illuminated d<strong>ete</strong>ctor that has a great response<br />
in <strong>the</strong> UV, <strong>the</strong> Maya Series (Maya2000 and Maya2000 Pro) are even better<br />
choices for deep-UV response (
QE65000 and Maya2000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Optimizing QE65000 and Maya2000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> for Your Application<br />
Our high-sensitivity back-thinned 2D FFT-CCD spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> for low light-level, UV-sensitivity and o<strong>the</strong>r scientific applications are available in three<br />
ve<strong>rs</strong>atile options: an improved ve<strong>rs</strong>ion <strong>of</strong> our <strong>the</strong>rmoelectrically cooled QE65000 Spe<strong>ctro</strong>m<strong>ete</strong>r, distinguished by improved stray light and low noise<br />
characteristics; and <strong>the</strong> uncooled Maya2000 and Maya2000 Pro, which <strong>of</strong>fer greater than 75% (90% Maya, 75% Maya Pro) quantum efficiency, high<br />
dynamic range and excellent UV response.<br />
QE65000 and Maya series optical bench options are described below. Although <strong>the</strong> bench diagram is specific to <strong>the</strong> QE65000, <strong>the</strong> optical design is<br />
nearly identical to <strong>the</strong> Maya2000 and Maya2000 Pro. The primary differences are <strong>the</strong> d<strong>ete</strong>ctor and <strong>the</strong>rmoelectric cooler.<br />
7<br />
8<br />
4<br />
4<br />
Collimating Mirror: specify standard<br />
or SAG+<br />
The collimating mirror is matched to <strong>the</strong> 0.22 numerical<br />
aperture <strong>of</strong> our optical fiber. Light reflects from this<br />
mirror, as a collimated beam, toward <strong>the</strong> grating. Opt to<br />
install a standard mirror or a SAG+UPG-HR mirror.<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
1<br />
1<br />
3<br />
5 6<br />
2<br />
SMA 905 Connector<br />
Light from a fiber ente<strong>rs</strong> <strong>the</strong> optical bench through <strong>the</strong> SMA 905<br />
Connector. The SMA 905 bulkhead provides a precise locus for <strong>the</strong> end <strong>of</strong><br />
<strong>the</strong> optical fiber, fixed slit, absorbance filter and fiber clad mode aperture.<br />
5<br />
6<br />
Grating: specify grating<br />
We install <strong>the</strong> grating on a platform that we <strong>the</strong>n rotate<br />
to select <strong>the</strong> starting wavelength you’ve specified. Then<br />
we permanently fix <strong>the</strong> grating in place to eliminate<br />
mechanical shifts or drift.<br />
Focusing Mirror: specify standard<br />
or SAG+<br />
This mirror focuses fi<strong>rs</strong>t-order spectra on <strong>the</strong> d<strong>ete</strong>ctor<br />
plane and sends higher orde<strong>rs</strong> to light traps built into<br />
<strong>the</strong> optical bench. Both <strong>the</strong> collimating and focusing<br />
mirro<strong>rs</strong> are made in-house to guarantee <strong>the</strong> highest<br />
reflectance and <strong>the</strong> lowest stray light possible. Opt for a<br />
standard mirror or a UV-absorbing SAG+UPG-HR mirror.<br />
2<br />
3<br />
Fixed Entrance Slit: specify slit size<br />
Light passes through <strong>the</strong> installed slit, which acts as <strong>the</strong> entrance aperture.<br />
Slits are available in widths from 5 µm to 200 µm. Each is permanently<br />
fixed to <strong>the</strong> SMA 905 bulkhead. (Without a slit, a fiber acts as <strong>the</strong> entrance<br />
aperture.)<br />
Longpass Absorbing Filter: optional<br />
If selected, an OF-1 absorbing filter is installed between <strong>the</strong> slit and <strong>the</strong><br />
clad mode aperture in <strong>the</strong> SMA 905 bulkhead. The filter is used to limit<br />
bandwidth <strong>of</strong> light entering <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r.<br />
7<br />
8<br />
D<strong>ete</strong>ctor with TE cooling<br />
The TE-cooled, back-thinned, “2D” d<strong>ete</strong>ctor provides<br />
great signal processing speed, improved signal-to-noise<br />
ratio and great native response in <strong>the</strong> UV. It generates<br />
virtually no dark noise, allowing for long integration<br />
times.<br />
OFLV Filte<strong>rs</strong>: optional<br />
Our proprietary filte<strong>rs</strong> precisely block second- and thirdorder<br />
light from reaching specific d<strong>ete</strong>ctor elements.<br />
Technical Tip<br />
In a typical symmetrical crossed Czerny-Turner optical design, <strong>the</strong>re are two mirro<strong>rs</strong> that help move light around <strong>the</strong><br />
optical bench on its way to <strong>the</strong> d<strong>ete</strong>ctor: <strong>the</strong> collimating mirror (fi<strong>rs</strong>t mirror), which makes parallel <strong>the</strong> light entering <strong>the</strong><br />
bench and <strong>the</strong>n reflects that light onto <strong>the</strong> grating; and <strong>the</strong> focusing (second) mirror, which focuses <strong>the</strong> light onto <strong>the</strong><br />
d<strong>ete</strong>ctor plane.<br />
The SAG+ mirro<strong>rs</strong> we use were developed by our sister company <strong>Ocean</strong> Thin Films. These silver-coated mirro<strong>rs</strong> have<br />
very high reflection values -- >97% across visible and near infrared wavelengths. What’s more, <strong>the</strong>y absorb nearly all UV<br />
light, a characteristic that reduces <strong>the</strong> effects <strong>of</strong> excitation scattering in fluorescence measurements.<br />
www.oceanoptics.com Tel: +1 727-733-2447 41
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
QE65000 Spe<strong>ctro</strong>m<strong>ete</strong>r<br />
Scientific-Grade Spe<strong>ctro</strong>scopy in a Small Footprint<br />
QE65000<br />
The QE65000 Spe<strong>ctro</strong>m<strong>ete</strong>r is <strong>the</strong> most sensitive spe<strong>ctro</strong>m<strong>ete</strong>r<br />
we’ve developed. Its Hamamatsu FFT-CCD d<strong>ete</strong>ctor provides 90%<br />
quantum efficiency as well as superior signal-to-noise ratio and<br />
signal processing speed.<br />
QE65000’s onboard programmable microcontroller puts you in<br />
command <strong>of</strong> <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r and its accessories and provides 10<br />
user-programmable digital inputs/outputs as well as a pulse<br />
generator for triggering o<strong>the</strong>r devices.<br />
The QE65000’s great quantum efficiency is not its only distinguishing<br />
feature. Its 2D area d<strong>ete</strong>ctor lets us bin (or sum) a vertical row<br />
<strong>of</strong> pixels. That <strong>of</strong>fe<strong>rs</strong> significant improvement in <strong>the</strong> signal-to-noise<br />
ratio (>1000:1) performance and signal processing speed <strong>of</strong> <strong>the</strong> d<strong>ete</strong>ctor<br />
compared with a linear CCD, where signals are digitally added<br />
by an external circuit.<br />
Because <strong>the</strong> QE65000’s d<strong>ete</strong>ctor is back-thinned, it has outstanding<br />
native response in <strong>the</strong> UV. It’s an excellent option for low light-level<br />
applications such as fluorescence, Raman spe<strong>ctro</strong>scopy, DNA<br />
sequencing, astronomy and thin-film reflectivity. Its TE-cooled<br />
d<strong>ete</strong>ctor feature low noise and low dark signal, enabling low lightlevel<br />
d<strong>ete</strong>ction and long integration times from 8 ms to 15 minutes.<br />
Features<br />
- Onboard programming<br />
- Multiple interface and bench options<br />
- Quantum efficiency <strong>of</strong> 90%<br />
- Ideal for low light level applications<br />
Physical<br />
Dimensions:<br />
182 mm x 110 mm x 47 mm<br />
Weight:<br />
1.18 kg (without power supply)<br />
D<strong>ete</strong>ctor<br />
D<strong>ete</strong>ctor: Hamamatsu S7031-1006<br />
D<strong>ete</strong>ctor range: 200-1100 nm<br />
Pixels:<br />
1024 x 58 (1044 x 64 total pixels)<br />
Pixel size: 24 μm 2<br />
Pixel well depth: 300,000 ele<strong>ctro</strong>ns/well, 1.5 m elec/column<br />
Sensitivity:<br />
22 ele<strong>ctro</strong>ns/count all λ; 26 photons/count @ 250 nm<br />
Quantum efficiency: 90% peak; 65% at 250 nm<br />
Optical Bench<br />
Design:<br />
f/4, Symmetrical crossed Czerny-Turner<br />
Focal length:<br />
101.6 mm input and output<br />
Entrance aperture: 5, 10, 25, 50, 100 or 200 µm wide slits or fiber (no slit)<br />
Grating options: 14 different grating options, UV through Shortwave NIR<br />
HC1grating:<br />
Provides 200-1050 nm range (best efficiency)<br />
OFLV filter options: OFLV-QE (200-950 nm); OFLV-QE-250 (250-1000 nm);<br />
OFLV-QE-300 (300-1050 nm); OFLV-QE-350<br />
(350-1100 nm); OFLV-QE-400 (400-1150 nm)<br />
O<strong>the</strong>r filter options: Longpass OF-1 filte<strong>rs</strong><br />
Fiber optic connector: SMA 905 to 0.22 NA single-strand optical fiber<br />
Spe<strong>ctro</strong>scopic<br />
Wavelength range: Grating dependent<br />
Optical resolution: ~0.14-7.7 nm FWHM<br />
Signal-to-noise ratio: 1000:1 (at full signal)<br />
A/D resolution: 16 bit<br />
Dark noise:<br />
3 RMS counts<br />
Dynamic range: 7.5 x 10 9 (system), 25000:1 for a single acquisition<br />
Integration time: 8 ms-15 minutes<br />
Stray light:<br />
99.8%<br />
Ele<strong>ctro</strong>nics<br />
Power consumption: 500 mA @ 5 VDC (no TE cooling); 3.5 A @ 5 VDC (with<br />
TE cooling)<br />
Data transfer speed: Full scans to memory every 8 ms with USB 2.0 port,<br />
18 ms with USB1.1 port, 300 ms with serial port<br />
Inputs/Outputs: 10 onboard digital user-programmable GPIOs (general<br />
purpose inputs/outputs)<br />
Breakout box:<br />
Yes, HR4-BREAKOUT<br />
Trigger modes: 4 modes<br />
Gated delay feature: Yes<br />
Connector:<br />
30-pin connector<br />
Power-up time:
Maya2000 and Maya2000Pro<br />
Our Maya2000® and Maya2000 Pro Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> <strong>of</strong>fer you <strong>the</strong><br />
perfect solution for applications that demand low light-level,<br />
UV-sensitive operation.<br />
This back-thinned, 2D FFT-CCD, uncooled instrument <strong>of</strong>fe<strong>rs</strong> greater<br />
than 90% quantum efficiency, high dynamic range and UV response<br />
to 190 nm and lower. The Maya2000 Series can deliver accurate<br />
analysis down to 185 nm with high dynamic range and good<br />
signal-to-noise ratio.<br />
The Hamamatsu FFT-CCD d<strong>ete</strong>cto<strong>rs</strong> used in <strong>the</strong> Maya2000 and<br />
Maya2000 Pro have excellent performance characteristics. Because<br />
<strong>of</strong> <strong>the</strong>ir UV response, FFT-CCD d<strong>ete</strong>cto<strong>rs</strong> do not require UV-sensitive<br />
coatings and provide performance advantages such as low dark<br />
current and good signal processing.<br />
Features<br />
- USB 2.0 interface<br />
- Low-noise ele<strong>ctro</strong>nics<br />
- Optical resolution to ~0.035 nm (FWHM); resolution depends on<br />
groove density <strong>of</strong> grating and size <strong>of</strong> entrance aperture (slit)<br />
- 14 grating options including HC-1 composite grating for coverage<br />
from 175-1100 nm (additional charge)<br />
- Slits available in widths <strong>of</strong> 5, 10, 25, 50, 100 and 200 µm<br />
- Optional order-sorting filte<strong>rs</strong> to eliminate second- and third-order<br />
effects<br />
- Fully controllable strobe signals (single or continuous)<br />
- 10 onboard digital user- programmable GPIOs<br />
Maya2000 Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
High Sensitivity and Deep UV Measurement<br />
Maya2000<br />
Maya2000 Pro<br />
D<strong>ete</strong>ctor: Hamamatsu S9840 Hamamatsu S10420<br />
Architecture: Back-thinned, 2D Back-thinned, 2D<br />
Thermoelectric<br />
cooling:<br />
No<br />
No<br />
Pixels: All: 2080 x 20<br />
Active: 2048 x 14<br />
All: 2068 x 70<br />
Active: 2048 x 64<br />
Pixel size: 14 µm square 14 µm square<br />
Column height: 196 µm 896 µm<br />
Pixel depth: 130,000 e- 200,000 e-<br />
Peak QE: >90% 75%<br />
QE @ 250 nm: 40% 65%<br />
CCD effective number <strong>of</strong> ~12 bit ~14 bit<br />
bits:<br />
Integration time: 6 ms - 10 seconds 6 ms – 5 seconds<br />
A/D converter: 16 bit, 500 kHz 16 bit, 250 kHz<br />
Dynamic range: 5000:1 (typical: ~8000:1) 10000:1 (typical:<br />
~12000:1)<br />
Signal-to-noise ratio: 350:1 450:1<br />
Non-linearity (uncorrected):<br />
~4.0% ~10.0%<br />
Linearity (corrected): 12000:1<br />
Signal-to-Noise: 350:1 450:1<br />
2D imaging properties: No Yes<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
www.oceanoptics.com Tel: +1 727-733-2447 43
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
QE65000 and Maya Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Bench Accessories for Your High-sensitivity Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
SMA 905 Connector<br />
A precision SMA 905 Connector aligns to <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r’s entrance slit and ensures concentricity<br />
<strong>of</strong> <strong>the</strong> fiber. For an upgrade fee that includes <strong>the</strong> cost <strong>of</strong> ano<strong>the</strong>r connector and labor, we will<br />
replace <strong>the</strong> standard SMA 905 Connector with a different connector <strong>of</strong> your choice.<br />
Fixed Entrance Slits<br />
One option available with <strong>the</strong> user-configured spe<strong>ctro</strong>m<strong>ete</strong>r is <strong>the</strong> size <strong>of</strong> <strong>the</strong> entrance aperture,<br />
with <strong>the</strong> width d<strong>ete</strong>rmining <strong>the</strong> amount <strong>of</strong> light entering <strong>the</strong> bench. A slit is fixed in place; it only<br />
can be changed by our technicians.<br />
Slit Description QE Pixel Resolution Maya Pixel Resolution<br />
SLIT-5 5-µm wide x 1-mm high ~2.0 pixels ~2.0 pixels<br />
SLIT-10 10-µm wide x 1-mm high ~2.2 pixels ~2.2 pixels<br />
SLIT-25 25-µm wide x 1-mm high ~2.6 pixels ~2.6 pixels<br />
SLIT-50 50-µm wide x 1-mm high ~3.3 pixels ~3.3 pixels<br />
SLIT-100 100-µm wide x 1-mm high ~4.7 pixels ~4.7 pixels<br />
SLIT-200 200-µm wide x 1-mm high ~8.9 pixels ~8.9 pixels<br />
Longpass Absorbing Filter<br />
We <strong>of</strong>fer longpass absorbing or blocking filte<strong>rs</strong>; each filter has a transmission band and a blocking<br />
band to restrict radiation to a certain wavelength region for eliminating second- and third-order<br />
effects. These filte<strong>rs</strong> are installed permanently between <strong>the</strong> slit and <strong>the</strong> clad mode aperture in <strong>the</strong><br />
bulkhead <strong>of</strong> <strong>the</strong> SMA 905 Connector.<br />
OF1-WG305<br />
OF1-GG375<br />
OF1-GG395<br />
OF1-GG475<br />
OF1-OG515<br />
OF1-OG550<br />
OF1-OG590<br />
Item<br />
Description<br />
Longpass filter; transmits light >305 nm<br />
Longpass filter; transmits light >375 nm<br />
Longpass filter; transmits light >395 nm<br />
Longpass filter; transmits light >475 nm<br />
Longpass filter; transmits light >515 nm<br />
Longpass filter; transmits light >550 nm<br />
Longpass filter; transmits light >590 nm<br />
Collimating and Focusing Mirro<strong>rs</strong><br />
You can replace <strong>the</strong> standard aluminum-coated reflective mirro<strong>rs</strong> with our proprietary, UV-absorbing<br />
SAG+ Mirro<strong>rs</strong>, which increase reflectance in <strong>the</strong> VIS-NIR and, in turn, increase <strong>the</strong> sensitivity<br />
<strong>of</strong> <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r. SAG+ Mirro<strong>rs</strong> are <strong>of</strong>ten specified for fluorescence. These mirro<strong>rs</strong> also absorb<br />
nearly all UV light, which reduces <strong>the</strong> effects <strong>of</strong> excitation scattering in fluorescence measurements.<br />
Unlike most silver-coated mirro<strong>rs</strong>, <strong>the</strong> SAG+ mirro<strong>rs</strong> won’t oxidize<br />
Item Code: SAG+UPG-HR<br />
Grating and Wavelength Range<br />
With a choice <strong>of</strong> 14 gratings, you can easily customize <strong>the</strong> spectral range and most efficient region<br />
<strong>of</strong> your QE65000 or Maya2000 Series Spe<strong>ctro</strong>m<strong>ete</strong>r. Our gratings are permanently fixed in place at<br />
<strong>the</strong> time <strong>of</strong> manufacture and are available in both ruled and holographic ve<strong>rs</strong>ions. See page 47 for<br />
grating options and efficiency curves and consult an <strong>Ocean</strong> <strong>Optics</strong> Applications Scientist for details.<br />
44 www.oceanoptics.com Tel: +1 727-733-2447
QE65000 and Maya Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
D<strong>ete</strong>cto<strong>rs</strong> and Accessories for Your High-sensitivity Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Back-thinned Area D<strong>ete</strong>cto<strong>rs</strong><br />
The Hamamatsu FFT-CCD d<strong>ete</strong>cto<strong>rs</strong> used in <strong>the</strong> QE65000, Maya2000 and Maya2000 Pro have great<br />
UV response and provide up to 90% quantum efficiency (defined as how efficiently a photon is<br />
converted to a photo-ele<strong>ctro</strong>n). The QE65000 uses <strong>the</strong> S7031-1006 2D array d<strong>ete</strong>ctor, <strong>the</strong> Maya2000<br />
uses <strong>the</strong> S9840 d<strong>ete</strong>ctor and <strong>the</strong> Maya2000 Pro uses <strong>the</strong> S10420 d<strong>ete</strong>ctor. All three d<strong>ete</strong>cto<strong>rs</strong> are<br />
responsive from 200-1100 nm.<br />
D<strong>ete</strong>cto<strong>rs</strong> with OFLV Filte<strong>rs</strong><br />
OFLV Variable Longpass Order-sorting Filte<strong>rs</strong> are applied to <strong>the</strong> d<strong>ete</strong>ctor’s window to eliminate second- and third-order effects. We use a patented<br />
coating technology to apply <strong>the</strong> filter to <strong>the</strong> substrate.<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
QE65000 D<strong>ete</strong>ctor Options<br />
Item<br />
DET-QE<br />
DET-QE-OFLV-200<br />
DET-QE-OFLV-250<br />
DET-QE-OFLV-300<br />
DET-QE-OFLV-350<br />
DET-QE-OFLV-400<br />
DET-QE-WINDOWLESS<br />
Description<br />
Hamamatsu S7031 d<strong>ete</strong>ctor, installed, w/no variable longpass filter<br />
Hamamatsu S7031 d<strong>ete</strong>ctor, installed, w/OFLV-QE-200 variable longpass filter<br />
Hamamatsu S7031 d<strong>ete</strong>ctor, installed, w/OFLV-QE-250 variable longpass filter<br />
Hamamatsu S7031 d<strong>ete</strong>ctor, installed, w/OFLV-QE-300 variable longpass filter<br />
Hamamatsu S7031 d<strong>ete</strong>ctor, installed, w/OFLV-QE-350 variable longpass filter<br />
Hamamatsu S7031 d<strong>ete</strong>ctor, installed, w/OFLV-QE-400 variable longpass filter<br />
Hamamatsu S7031 d<strong>ete</strong>ctor, installed, with no window options; required for VUV applications<br />
Maya2000 and Maya2000 Pro D<strong>ete</strong>ctor Options<br />
Item Description Spe<strong>ctro</strong>m<strong>ete</strong>r<br />
DET-MAYA Hamamatsu S9840 d<strong>ete</strong>ctor, installed, w/no variable longpass filter Maya2000<br />
DET-MAYA-OFLV-200 Hamamatsu S9840 d<strong>ete</strong>ctor, installed, w/OFLV-200 variable longpass filter Maya2000<br />
DET-MAYA-UV Hamamatsu S9840 d<strong>ete</strong>ctor, installed, w/UV window Maya2000<br />
DET-MAYA-VIS Hamamatsu S9840 d<strong>ete</strong>ctor, installed, w/VIS window Maya2000<br />
DET-MAYA-WINDOWLESS Hamamatsu S9840 d<strong>ete</strong>ctor, installed, w/no window options; required for VUV applications Maya2000<br />
DET-MAYAPRO Hamamatsu S10420 d<strong>ete</strong>ctor, installed, w/no variable longpass filter Maya2000 Pro<br />
DET-MAYAPRO-OFLV-200 Hamamatsu S10420 d<strong>ete</strong>ctor, installed, w/OFLV-200 variable longpass filter Maya2000 Pro<br />
DET-MAYAPRO-UV Hamamatsu S10420 d<strong>ete</strong>ctor, installed, w/UV window Maya2000 Pro<br />
DET-MAYAPRO-VIS Hamamatsu S10420 d<strong>ete</strong>ctor, installed, w/VIS window Maya2000 Pro<br />
DET-MAYAPRO-WINDOWLESS Hamamatsu S10420 d<strong>ete</strong>ctor, installed, with no window options; required for VUV applications Maya2000 Pro<br />
Technical Tip<br />
Just as flexibility is built into your spe<strong>ctro</strong>m<strong>ete</strong>r options, so, too, is flexibility built in to your experiment param<strong>ete</strong><strong>rs</strong>. We<br />
use <strong>the</strong> term Scope Mode in s<strong>of</strong>tware to indicate “raw signal” coming from <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r. The Scope Mode spectrum<br />
is <strong>the</strong> digital signal created from <strong>the</strong> d<strong>ete</strong>ctor’s analog signal, which is generated as <strong>the</strong> result <strong>of</strong> photons being<br />
converted into ele<strong>ctro</strong>ns. The arbitrary units <strong>of</strong> <strong>the</strong> Scope mode spectrum are called “counts.”<br />
By changing <strong>the</strong> integration time, adjusting signal averaging and so on you can condition <strong>the</strong> raw signal to maximize<br />
intensity or reduce noise, for example. Once you have optimized your base signal you are ready to enter a Processed Mode. Processed data<br />
involves taking a dark, taking a reference and <strong>the</strong>n going into a specific mode such as absorbance, transmission, reflection, relative irradiance,<br />
absolute irradiance, color and so on. In a Processed Mode <strong>the</strong> y-axis units are no longer arbitrary and <strong>the</strong>refore can be used to make qualitative,<br />
and is some cases quantitative, comparisons.<br />
www.oceanoptics.com Tel: +1 727-733-2447 45
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
QE and Maya Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Choosing <strong>the</strong> Right Grating<br />
Groove Density<br />
The Groove density (lines/mm -1 ) <strong>of</strong> a grating d<strong>ete</strong>rmines its dispe<strong>rs</strong>ion, while <strong>the</strong><br />
angle <strong>of</strong> <strong>the</strong> groove d<strong>ete</strong>rmines <strong>the</strong> most efficient region <strong>of</strong> <strong>the</strong> spectrum. The<br />
greater <strong>the</strong> groove density, <strong>the</strong> better <strong>the</strong> optical resolution possible, but <strong>the</strong><br />
more truncated <strong>the</strong> spectral range.<br />
Spectral Range<br />
The dispe<strong>rs</strong>ion <strong>of</strong> <strong>the</strong> grating across <strong>the</strong> linear array is also expressed as <strong>the</strong> “size”<br />
<strong>of</strong> <strong>the</strong> spectra on <strong>the</strong> array. The spectral range (bandwidth) is a function <strong>of</strong> <strong>the</strong><br />
groove density and does not change. When you choose a starting wavelength<br />
for a spe<strong>ctro</strong>m<strong>ete</strong>r, you add its spectral range to <strong>the</strong> starting wavelength to<br />
d<strong>ete</strong>rmine <strong>the</strong> wavelength range. For several gratings, <strong>the</strong> spectral range <strong>of</strong> a<br />
grating varies according to <strong>the</strong> starting wavelength range. The rule <strong>of</strong> thumb is<br />
this: The higher <strong>the</strong> starting wavelength, <strong>the</strong> more truncated <strong>the</strong> spectral range.<br />
Blaze Wavelength<br />
For ruled gratings, <strong>the</strong> blaze wavelength is <strong>the</strong> peak wavelength in an efficiency<br />
curve. For holographic gratings, it is <strong>the</strong> most efficient wavelength region.<br />
Best Efficiency ( >30%)<br />
All ruled or holographically etched gratings optimize fi<strong>rs</strong>t-order spectra at certain<br />
wavelength regions; <strong>the</strong> “best” or “most efficient” region is <strong>the</strong> range where<br />
efficiency is >30%. In some cases, gratings have a greater spectral range than is<br />
efficiently diffracted. For example, Grating 1 has about a 650 nm spectral range,<br />
but is most efficient from 200-575 nm. In this case, wavelengths >575 nm will<br />
have lower intensity due to <strong>the</strong> grating’s reduced efficiency.<br />
Grating and Wavelength Range<br />
With a choice <strong>of</strong> 14 gratings, you can easily customize your QE65000 or Maya2000 Series Spe<strong>ctro</strong>m<strong>ete</strong>r through its groove density, spectral range and<br />
blaze wavelength. Our gratings are permanently fixed in place at <strong>the</strong> time <strong>of</strong> manufacture and we <strong>of</strong>fer both ruled and holographic ve<strong>rs</strong>ions. Questions<br />
about which one is best for you? Contact an <strong>Ocean</strong> <strong>Optics</strong> Applications Scientist for details.<br />
Grating<br />
Number<br />
Intended<br />
Use<br />
Groove<br />
Density<br />
46 www.oceanoptics.com Tel: +1 727-733-2447<br />
Spectral<br />
Range<br />
Blaze<br />
Wavelength<br />
HC-1 w/QE65000 UV-NIR 300/600 (variable) 750 nm Variable 200-950 nm<br />
HC-1 w/Maya2000s UV-NIR 300/600 (variable) 900 nm Variable 200-1100 nm<br />
H1 UV 600 425-445 nm 300 nm 200-575 nm<br />
H2 UV-VIS 600 415-445 nm 400 nm 250-800 nm<br />
H3 VIS-Color 600 410-440 nm 500 nm 350-850 nm<br />
H4 NIR 600 410-430 nm 750 nm 530-1100 nm<br />
H5 UV-VIS 1200 205-220 nm Holographic UV 200-400 nm<br />
H6 NIR 1200 140-195 nm 750 nm 500-1100 nm<br />
H7 UV-VIS 2400 72-102 nm Holographic UV 200-500 nm<br />
H9 VIS-NIR 1200 165-205 nm Holographic VIS 400-800 nm<br />
H10 UV-VIS 1800 95-140 nm Holographic UV 200-635 nm<br />
H11 UV-VIS 1800 75-135 nm Holographic VIS 320-720 nm<br />
H12 UV-VIS 2400 60-100 nm Holographic VIS 260-780 nm<br />
H13 UV-NIR 300 800-900 nm 500 nm 300-1100 nm<br />
H14 NIR 600 410-420 nm 1000 nm 650-1100 nm<br />
Best<br />
Efficiency (>30%)
QE65000 and Maya Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Gratings for QE65000/Maya2000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
The graphs below are grating efficiency curves for gratings with groove densities <strong>of</strong> 600, 1200, 1800 and 2400 mm -1 . Additional information is available<br />
at www.oceanoptics.com/Products/bench_grating_hr.asp.<br />
Groove Density <strong>of</strong> 600 mm -1 Groove Density <strong>of</strong> 1200 mm -1<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Relative Efficiency<br />
Relative Efficiency<br />
Grating #1 Grating #2 Grating #3 Grating #4 Grating #14<br />
Grating #5 Grating #6 Grating #9<br />
Groove Density <strong>of</strong> 1800 mm -1<br />
Groove Density <strong>of</strong> 2400 mm -1<br />
Relative Efficiency<br />
Relative Efficiency<br />
Grating #10 Grating #11<br />
Grating #7 Grating #12<br />
Grating Selection Tips:<br />
Variable Groove Density <strong>of</strong> 600 mm -1 /300 mm -1<br />
- These efficiency curves relate only to <strong>the</strong> grating. System response<br />
is affected by a number <strong>of</strong> variables, including d<strong>ete</strong>ctor response.<br />
- Grating selection <strong>of</strong>ten involves trade-<strong>of</strong>fs. For example, gratings<br />
with very high groove density (mm -1 ) allow greater optical resolution<br />
but at <strong>the</strong> expense <strong>of</strong> a truncated spectral range. If <strong>the</strong> user is<br />
characterizing two or three closely aligned laser wavelengths, such<br />
a trade-<strong>of</strong>f <strong>of</strong> resolution for range might be acceptable. For o<strong>the</strong>r<br />
applications, a wider range with good resolution would make better<br />
sense.<br />
Absolute Efficiency (%)<br />
- The HC-1 grating is a good option for broad spectral coverage<br />
(200-950 nm in <strong>the</strong> QE65000) without sacrificing optical resolution.<br />
HC-1<br />
www.oceanoptics.com Tel: +1 727-733-2447 47
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
QE65000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Predicted Ranges & Resolution<br />
SPECTRAL RANGE (nm)<br />
600 mm -1 Grating and 5 µm Slit<br />
450<br />
0.245<br />
445<br />
440<br />
0.240<br />
435<br />
430<br />
0.235<br />
425<br />
420<br />
0.230<br />
415<br />
410<br />
0.225<br />
405<br />
400<br />
0.220<br />
200 400 600 800 1000<br />
STARTING WAVELENGTH (nm)<br />
RESOLUTION (nm)<br />
Example:<br />
If <strong>the</strong> starting<br />
wavelength is 400 nm,<br />
<strong>the</strong>n <strong>the</strong> range is<br />
~437 nm, providing<br />
a 400-837 nm<br />
wavelength range and<br />
0.239 nm resolution.<br />
SPECTRAL RANGE (nm)<br />
150<br />
140<br />
130<br />
120<br />
110<br />
100<br />
90<br />
80<br />
1800 mm -1 Grating and 5 µm Slit<br />
0.080<br />
0.070<br />
0.060<br />
0.050<br />
70<br />
0.040<br />
200 400 600 800 1000<br />
STARTING WAVELENGTH (nm)<br />
RESOLUTION (nm)<br />
Example:<br />
If <strong>the</strong> starting<br />
wavelength is 700 nm,<br />
<strong>the</strong>n <strong>the</strong> range is<br />
~90 nm, providing<br />
a 700-790 nm<br />
wavelength range and<br />
0.05 nm resolution.<br />
SPECTRAL RANGE (nm)<br />
220<br />
210<br />
200<br />
190<br />
180<br />
170<br />
160<br />
1200 mm -1 Grating and 5 µm Slit<br />
0.120<br />
0.115<br />
0.110<br />
0.105<br />
0.100<br />
0.095<br />
0.090<br />
0.085<br />
RESOLUTION (nm)<br />
Example:<br />
If <strong>the</strong> starting<br />
wavelength is 300 nm,<br />
<strong>the</strong>n <strong>the</strong> range is<br />
~215 nm, providing<br />
a 300-515 nm<br />
wavelength range and<br />
0.117 nm resolution.<br />
SPECTRAL RANGE (nm)<br />
110<br />
100<br />
90<br />
80<br />
70<br />
60<br />
50<br />
2400 mm -1 Grating and 5 µm Slit<br />
0.055<br />
0.045<br />
0.035<br />
0.025<br />
RESOLUTION (nm)<br />
Example:<br />
If <strong>the</strong> starting<br />
wavelength is 600 nm,<br />
<strong>the</strong>n <strong>the</strong> range is<br />
~56 nm, providing<br />
a 600-656 nm<br />
wavelength range and<br />
0.029 nm resolution.<br />
150<br />
0.080<br />
40<br />
140<br />
0.075<br />
200 400 600 800 1000<br />
STARTING WAVELENGTH (nm)<br />
30<br />
0.015<br />
200 400 600 800 1000<br />
STARTING WAVELENGTH (nm)<br />
Note: These predicted range and resolution figures apply only to QE65000 Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Network Adapter for QE65000 and Maya2000<br />
Remora Turns Your QE65000 or Maya2000 into a Networked Spe<strong>ctro</strong>m<strong>ete</strong>r<br />
Add a Remora Network Adapter to your QE65000<br />
or Maya2000 Series Spe<strong>ctro</strong>m<strong>ete</strong>r to communicate<br />
over E<strong>the</strong>rnet or Wi-Fi. Use Remora with SpectraSuite<br />
S<strong>of</strong>tware to turn your device into a network-accessible<br />
spe<strong>ctro</strong>m<strong>ete</strong>r. Remotely capture spectral data from<br />
anywhere.<br />
Plus, Remora allows multiple use<strong>rs</strong> to<br />
access data and experiment settings without <strong>the</strong> need<br />
for additional equipment. Remora’s web interface<br />
works with all popular web browse<strong>rs</strong> and allows<br />
you to monitor data from a PDA, iPhone, and most<br />
Internet-ready devices.<br />
Item codes: REMORA-QE-FCC (FCC-compliant ve<strong>rs</strong>ion)<br />
REMORA-QE-CE (CE-compliant ve<strong>rs</strong>ion)<br />
48 www.oceanoptics.com Tel: +1 727-733-2447
Application Notes<br />
Maya2000 Pro Spectral Measurements Extend to 153 nm<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Our Maya2000 Pro Spe<strong>ctro</strong>m<strong>ete</strong>r delive<strong>rs</strong> high quantum efficiency and high dynamic range and is responsive in <strong>the</strong> deep UV (~185-300 nm). The<br />
Extra-Deep UV option extends spectral measurements to 153 nm.<br />
Introduction<br />
Spectral measurements to 153 nm can be achieved easily and<br />
economically with <strong>the</strong> high-sensitivity Maya2000 Pro with <strong>the</strong><br />
Extra-Deep UV option. A variety <strong>of</strong> materials have spectral<br />
signatures in <strong>the</strong> vacuum ultraviolet (VUV) spectral region (from<br />
10 nm-200 nm); VUV spe<strong>ctro</strong>scopy is useful for applications<br />
ranging from biomedicine to semiconductor testing.<br />
Because <strong>the</strong> spectral<br />
response <strong>of</strong><br />
standard silicon<br />
chargecoupled<br />
device (CCD)<br />
d<strong>ete</strong>cto<strong>rs</strong><br />
drops <strong>of</strong>f rapidly<br />
at wavelengths as<br />
long as 400 nm, and<br />
because oxygen and water<br />
absorb in <strong>the</strong> VUV spectral<br />
band, maintaining sufficient signal<br />
outside a vacuum is not possible. Nitrogen<br />
purging <strong>of</strong> <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r helps to mitigate water and<br />
oxygen absorption in <strong>the</strong> VUV. Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> with a vacuum<br />
purging feature require custom configuration and are <strong>of</strong>ten too<br />
expensive and unwieldy for many common applications.<br />
The Maya2000 Pro with <strong>the</strong> Extra-Deep UV option’s clever design<br />
changes all that. The spe<strong>ctro</strong>m<strong>ete</strong>r features a 101.6-mm focal<br />
length optical bench with a compact crossed Czerny-Turner<br />
design and a back-thinned CCD d<strong>ete</strong>ctor that <strong>of</strong>fe<strong>rs</strong> superior UV<br />
and VUV performance. To minimize signal attenuation inside <strong>the</strong><br />
optical path, <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r bench is purged with nitrogen,<br />
achieving a robust signal for VUV experiments at wavelengths as<br />
low as 153 nm.<br />
Experimental Conditions<br />
To test performance, we started with a Maya2000 Pro configured<br />
with a high resolution, UV-enhanced 2400 g/mm holographic<br />
diffraction grating and a 5 µm slit. The back-thinned d<strong>ete</strong>ctor<br />
(Hamamatsu S10420-1106) features a peak quantum efficiency<br />
<strong>of</strong> 75%, with UV quantum efficiencies as high as 50%. A custom<br />
magnesium fluoride (MgF2) glass window is placed over <strong>the</strong><br />
d<strong>ete</strong>ctor for improved transmission over VUV wavelengths.<br />
Maya2000 Pro Emission Spectrum <strong>of</strong> VUV Source<br />
The sharply defined spectral peaks at wavelengths as low are 153 nm are measured using <strong>the</strong><br />
Maya2000 Pro.<br />
The test sample for <strong>the</strong> experiment was a VUV deuterium lamp with a<br />
VUV-grade optical window, coupled directly to <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r. We enclosed<br />
<strong>the</strong> source and spe<strong>ctro</strong>m<strong>ete</strong>r and purged <strong>the</strong> region with standard<br />
laboratory-grade nitrogen.<br />
Results<br />
Integration time for <strong>the</strong> measurement was 50 ms. The resultant emission<br />
spectrum shows sharply defined spectral peaks at wavelengths as low<br />
as 153 nm, with a strong central peak around 161 nm (see spectra). The<br />
system operated with a spectral resolution <strong>of</strong> 0.1 nm and a signal-to-noise<br />
ratio <strong>of</strong> 450:1.<br />
We have also used <strong>the</strong> system to measure a solution containing carbon,<br />
hydrogen/deuterium, nitrogen, oxygen, sulfur, chlorine, bromine, silicon<br />
and fluorine chromatographically separated into a column and placed in<br />
a vacuum chamber with a helium plasma mixture. VUV spectral features<br />
were clearly apparent in <strong>the</strong> spectrum, suggesting a wide variety <strong>of</strong> shortwavelength<br />
applications is achievable.<br />
Conclusions<br />
The results demonstrate that <strong>the</strong> reliable and economical Maya2000 Pro<br />
can be easily extended to VUV applications. If you have spe<strong>ctro</strong>scopy<br />
experiments or applications in <strong>the</strong> VUV, look no fur<strong>the</strong>r than <strong>the</strong> Maya2000<br />
Pro as your short-wavelength, affordable, robust solution.<br />
www.oceanoptics.com Tel: +1 727-733-2447 49
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
NIRQuest and SIR Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Full Range <strong>of</strong> Options for NIR and Mid-IR Applications<br />
We <strong>of</strong>fer two great technologies for your NIR (900-2500 nm) and Mid-IR<br />
(900-6500 nm) application needs:<br />
- NIRQuest Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Feature a fixed optical bench, fiber input and an InGaAs array <strong>of</strong><br />
d<strong>ete</strong>ctor elements. Array-based systems are a must for capturing<br />
transient phenomena and are recommended for high speed acquisition<br />
in general. All units work with low OH optical fibe<strong>rs</strong> with SMA 905 input<br />
and use SpectraSuite operating s<strong>of</strong>tware.<br />
- SIR Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Are rotating grating (scanning) spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> that use a stepper motor<br />
with optical encoder to rotate a grating through 45,000 steps. The<br />
d<strong>ete</strong>ctor is fixed in placed and, because <strong>of</strong> its large area, has exceptional<br />
optical resolution and signal to noise. SIRs can be used with optical<br />
fibe<strong>rs</strong> or in free-beam mode using direct-attach lenses. They are wellsuited<br />
for characterizing lase<strong>rs</strong>. Also, if you don’t require a spe<strong>ctro</strong>m<strong>ete</strong>r,<br />
you can choose one <strong>of</strong> our high-sensitivity Single Point D<strong>ete</strong>cto<strong>rs</strong>.<br />
One o<strong>the</strong>r NIR option is <strong>the</strong> ANIR Series <strong>of</strong> Fourier Transform Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
(FTS). These FTS systems typically have greater sensitivity and require<br />
shorter sampling times than o<strong>the</strong>r spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> and are well suited for<br />
transmission measurements <strong>of</strong> gases and liquids. Options are available for<br />
applications from 900-4500 nm.<br />
NIR and Mid-IR Spe<strong>ctro</strong>m<strong>ete</strong>r Models at a Glance<br />
With NIRQuest and SIR Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong>, you can opt for <strong>the</strong> standard, default configuration or mix and match gratings, slits and o<strong>the</strong>r accessories for a<br />
custom setup. ANIR systems come in standard configurations.<br />
Type Wavelength Range Models<br />
Array-based 900-1700 nm NIRQuest512<br />
Fourier Transform 900-1700 nm ANIR-900-1700<br />
Array-based 900-2050 nm NIRQuest256-2.1<br />
Array-based 900-2200 nm NIRQuest512-2.2<br />
Array-based 900-2500 nm NIRQuest512-2.5<br />
Array-based 900-2500 nm NIRQuest256-2.5<br />
Scanning 900-2600 nm SIR-2600<br />
Fourier Transform 900-2600 nm ANIR-900-2600<br />
Scanning 1300-3400 nm SIR-3400<br />
Fourier Transform 2000-4500 nm ANIR-2000-4500<br />
Scanning 2000-5000 nm SIR-5000<br />
Scanning 3000-6500 nm SIR-6500<br />
Why NIRQuest?<br />
NIRQuest represents <strong>the</strong> culmination <strong>of</strong> a decade’s worth <strong>of</strong> experience with compact NIR spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> and advances<br />
in InGaAs array d<strong>ete</strong>cto<strong>rs</strong> that have improved overall system performance dramatically. With NIRQuest, you’ll<br />
experience more grating options, better throughput and higher optical resolution than in our earlier generation <strong>of</strong><br />
NIR spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong>. There’s all that – plus external triggering.<br />
50 www.oceanoptics.com Tel: +1 727-733-2447
NIRQuest Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Near-Infrared Measurements for Nearly Anything<br />
NIRQuest<br />
No matter what your work demands, NIRQuest® has you covered. The<br />
NIRQuest Series <strong>of</strong> Near-Infrared Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> deliver excellent performance,<br />
accuracy and reliability.<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
These small-footprint spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> cover various ranges (depending on your<br />
configuration) from 900-2500 nm and are ideal for demanding applications<br />
ranging from moisture d<strong>ete</strong>ction and chemical analysis to high-resolution laser<br />
and optical fiber characterization.<br />
Features<br />
- 512-element InGaAs array d<strong>ete</strong>ctor options covering 900-1700 nm,<br />
900-2200 nm and 900-2100 nm<br />
- 256-element options covering 900-2050 nm and 900-2500 nm<br />
- Wide range <strong>of</strong> grating and optical bench options to optimize your setup<br />
- External hardware triggering function for capturing data when an external<br />
event occu<strong>rs</strong> or to trigger an event after data acquisition<br />
Each NIRQuest spe<strong>ctro</strong>m<strong>ete</strong>r model is preset with optical bench and grating options appropriate for many NIR applications. However, we also <strong>of</strong>fer a<br />
full range <strong>of</strong> slit, filter and grating options to optimize your setup for higher resolution needs or o<strong>the</strong>r similar performance requirements.<br />
NIRQuest Options at a Glance<br />
Model Description Best for These Application Needs<br />
NIRQuest256-2.1 NIR Spe<strong>ctro</strong>m<strong>ete</strong>r, 900-2050 nm, 256-element InGaAs array; includes Good response at higher wavelengths (peak d<strong>ete</strong>ctor response<br />
grating NIR2 (900-2050 nm), order-sorting filter and 25 µm slit<br />
~1900 nm) and optical resolution
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
NIRQuest Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Specifications Comparison Table<br />
Physical NIRQuest512 NIRQuest512-2.2 NIRQuest512-2.5 NIRQuest256-2.1 NIRQuest256-2.5<br />
Dimensions (mm): 182 x 110 x 47 182 x 110 x 47 182 x 110 x 47 182 x 110 x 47 182 x 110 x 47<br />
Weight: 1.18 kg (2.6 lb.) 1.18 kg (2.6 lb.) 1.18 kg (2.6 lb.) 1.18 kg (2.6 lb.) 1.18 kg (2.6 lb.)<br />
D<strong>ete</strong>ctor<br />
Useable range: 900-1700 nm 900-2200 nm 900-2550 nm 900-2050 nm 900-2500 nm<br />
Pixels/Pixel size: 512/ 25 µm x 500 µm 512/ 25 µm x 250 µm 512/ 25 µm x 250 µm 256/ 50 µm x 500 µm 256/ 50 µm x 500 µm<br />
Optical Bench<br />
Slit (standard): 25 µm 25 µm 25 µm 25 µm 25 µm<br />
Entrance aperture (custom<br />
options):<br />
Grating options (standard):<br />
Grating options (custom):<br />
10 µm, 50 µm, 100 µm<br />
and 200 µm (or no slit)<br />
Grating NIR3, 150 l/mm,<br />
900-1700 nm<br />
NIR10, NIR11, NIR12,<br />
NIR13 and NIR14<br />
10 µm, 50 µm, 100 µm<br />
and 200 µm (or no slit)<br />
Grating NIR2, 100 l/mm,<br />
900-2050 nm<br />
NIR2, NIR3, NIR10,<br />
NIR11, NIR12 and NIR13<br />
10 µm, 50 µm, 100 µm<br />
and 200 µm (or no slit)<br />
Grating NIR1, 75 l/mm,<br />
1075-2500 nm<br />
NIR2, NIR3, NIR10,<br />
NIR11, NIR12 and NIR13<br />
10 µm, 50 µm, 100 µm<br />
and 200 µm (or no slit)<br />
Grating NIR2, 100 l/mm,<br />
900-2050 nm<br />
NIR2, NIR3, NIR10,<br />
NIR11, NIR12 and NIR13<br />
10 µm, 50 µm, 100 µm<br />
and 200 µm (or no slit)<br />
Grating NIR1, 75 l/mm,<br />
1075-2500 nm<br />
NIR2, NIR3, NIR10,<br />
NIR11, NIR12 and NIR13<br />
Order-sorting (standard): NA Yes Yes Yes Yes<br />
Longpass filter:<br />
OF1-RG830 longpass OF1-RG830 longpass OF1-RG830 longpass OF1-RG830 longpass OF1-RG830 longpass<br />
NIR filter (optional) NIR filter (optional) NIR filter (optional) NIR filter (optional) NIR filter (optional)<br />
Fiber optic connector:<br />
SMA 905 to 0.22 NA<br />
optical fiber<br />
SMA 905 to 0.22 NA<br />
optical fiber<br />
SMA 905 to 0.22 NA<br />
optical fiber<br />
SMA 905 to 0.22 NA<br />
optical fiber<br />
SMA 905 to 0.22 NA<br />
optical fiber<br />
Spe<strong>ctro</strong>scopic<br />
Wavelength range: 900-1700 nm w/NIR3 900-2200 nm w/NIR2 900-2500 nm w/NIR1 900-2050 nm w/NIR2 900-2500 nm w/NIR1<br />
Optical resolution<br />
(FWHM):<br />
~3.1 nm w/25 µm slit ~5.0 nm w/25 µm slit ~6.3 nm w/25 µm slit ~7.6 nm w/25 µm slit ~ 9.5 nm w/25 µm slit<br />
Signal-to-noise ratio at<br />
full signal:<br />
>15000:1 @ 100 ms<br />
integration; >13000:1 @<br />
1000 ms integration<br />
10000:1 @ 100 ms<br />
integration<br />
10000:1 @ 100 ms<br />
integration<br />
10000:1 @ 100 ms<br />
integration<br />
7500:1 @ 10 ms integration<br />
A/D resolution 16-bit 16-bit 16-bit 16-bit 16-bit<br />
Dark noise: 6 RMS counts @ 100 ms 6 RMS counts @ 100 ms 4 RMS counts @ 10 ms 6 RMS counts @ 100 ms 8 RMS counts @ 10 ms<br />
12 RMS counts @<br />
1000 ms<br />
12 RMS counts @<br />
250 ms<br />
16 RMS counts @<br />
250 ms<br />
12 RMS counts @<br />
250 ms<br />
12 RMS counts @ 30 ms<br />
Dynamic range:<br />
15 x 10 6 (system);<br />
15000:1 for a single<br />
acquisition<br />
15 x 10 6 (system);<br />
10000:1 for a single<br />
acquisition<br />
15 x 10 6 (system);<br />
10000:1 for a single<br />
acquisition<br />
15 x 10 6 (system);<br />
10000:1 for a single<br />
acquisition<br />
15 x 10 6 (system);<br />
7500:1 for a single<br />
acquisition<br />
Integration time: 1 ms-120 seconds 1 ms-2000 ms 1 ms – 400 ms 1 ms-2000 ms 1 ms-60 ms<br />
Ele<strong>ctro</strong>nics<br />
Data transfer speed: Full scan to memory<br />
every 5 ms with USB<br />
Full scan to memory<br />
every 5 ms with USB<br />
Full scan to memory<br />
every 5 ms with USB<br />
Full scan to memory<br />
every 5 ms with USB<br />
Full scan to memory<br />
every 5 ms with USB<br />
Trigger modes: 2 modes 2 modes 2 modes 2 modes 2 modes<br />
Strobe functions: Yes Yes Yes Yes Yes<br />
Temperature & Thermoelectric Cooling<br />
Temperature limits<br />
(environmental):<br />
TEC setpoint (s<strong>of</strong>tware<br />
controlled):<br />
Computer<br />
Operating systems<br />
10-35 ºC (0-90% noncondensing)<br />
Control at -5 ºC (up to<br />
30 ºC below ambient)<br />
Windows 2000/XP and<br />
Vista (32-bit only); Mac<br />
OS X and Linux w/USB<br />
port; any 32-bit Windows<br />
OS with serial port<br />
10-35 ºC (0-90% noncondensing)<br />
Control at -20 ºC (up to<br />
45 ºC below ambient)<br />
Windows 2000/XP and<br />
Vista (32-bit only); Mac<br />
OS X and Linux w/USB<br />
port; any 32-bit Windows<br />
OS with serial port<br />
10-35 ºC (0-90% noncondensing)<br />
Control at -20 ºC (up to<br />
45 ºC below ambient)<br />
Windows 2000/XP and<br />
Vista (32-bit only); Mac<br />
OS X and Linux w/USB<br />
port; any 32-bit Windows<br />
OS with serial port<br />
10-35 ºC (0-90% noncondensing)<br />
Control at -20 ºC (up to<br />
45 ºC below ambient)<br />
Windows 2000/XP and<br />
Vista (32-bit only); Mac<br />
OS X and Linux w/USB<br />
port; any 32-bit Windows<br />
OS with serial port<br />
10-35 ºC (0-90% noncondensing)<br />
Control at -20 ºC (up to<br />
45 ºC below ambient)<br />
Windows 2000/XP and<br />
Vista (32-bit only); Mac<br />
OS X and Linux w/USB<br />
port; any 32-bit Windows<br />
OS with serial port<br />
52 www.oceanoptics.com Tel: +1 727-733-2447
NIRQuest Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Optical Bench Options for Your Custom NIRQuest Spe<strong>ctro</strong>m<strong>ete</strong>r<br />
Each NIRQuest model is available as a standard configuration comprising some combination <strong>of</strong> InGaAs array d<strong>ete</strong>ctor, grating, order-sorting filter and<br />
25 µm slit. In addition, you can customize your NIRQuest by mixing and matching optical bench accessories with <strong>the</strong> assistance <strong>of</strong> an <strong>Ocean</strong> <strong>Optics</strong><br />
Applications Scientist. Here are your options:<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
D<strong>ete</strong>cto<strong>rs</strong><br />
Each NIRQuest Spe<strong>ctro</strong>m<strong>ete</strong>r uses a different Hamamatsu InGaAs-array d<strong>ete</strong>ctor and comes with a<br />
preconfigured combination <strong>of</strong> that d<strong>ete</strong>ctor and optical bench components. If you wish to<br />
customize your setup – for example, change <strong>the</strong> slit size – you’ll need to itemize <strong>the</strong> components,<br />
beginning with <strong>the</strong>se d<strong>ete</strong>ctor options:<br />
Item<br />
Description<br />
NQ256-2.1<br />
NIR Spe<strong>ctro</strong>m<strong>ete</strong>r, 900-2100 nm, 256-element InGaAs array<br />
NQ256-2.5<br />
NIR Spe<strong>ctro</strong>m<strong>ete</strong>r, 900-2500 nm, 256-element InGaAs array<br />
NQ512<br />
NIR Spe<strong>ctro</strong>m<strong>ete</strong>r, 900-1700 nm, 512-element InGaAs array<br />
NQ512-2.2<br />
NIR Spe<strong>ctro</strong>m<strong>ete</strong>r, 900-2200 nm, 512-element InGaAs array<br />
NQ512-2.5<br />
NIR Spe<strong>ctro</strong>m<strong>ete</strong>r, 900-2500 nm, 512-element InGaAs array<br />
Fixed Entrance Slits<br />
Our entrance slits are rectangular apertures that are 1 mm tall and come in various widths. The<br />
standard NIRQuest configuration has a 25 µm slit. Here are your o<strong>the</strong>r options:<br />
Slit Description Pixel Resolution (approximate), by Model<br />
NIRQuest512 NIR-<br />
Quest512-2.2<br />
NIR-<br />
Quest512-2.5<br />
NIR-<br />
Quest256-2.1<br />
NIR-<br />
Quest256-2.5<br />
SLIT-10 10 µm width 2.0 pixels 2.0 pixels 2.0 pixels 6.7 pixels 8.3 pixels<br />
x 1 mm<br />
height<br />
SLIT-25 25 µm width 3.1 pixels 3.1 pixels 3.1 pixels 7.6 pixels 9.5 pixels<br />
x 1 mm<br />
height<br />
SLIT-50 50 µm width 3.6 pixels 3.6 pixels 3.6 pixels 8.9 pixels 11.1 pixels<br />
x 1 mm<br />
height<br />
SLIT-100 100 µm 6.6 pixels 6.6 pixels 6.6 pixels 11.2 pixels 13.9 pixels<br />
width x 1 mm<br />
height<br />
SLIT-200 200 µm<br />
width x 1 mm<br />
height<br />
12.3 pixels 12.3 pixels 12.3 pixels 17.9 pixels 22.2 pixels<br />
Order-sorting and Longpass Filte<strong>rs</strong><br />
Order-sorting filte<strong>rs</strong> and longpass filte<strong>rs</strong> are installed in <strong>the</strong> optical bench. Order-sorting filte<strong>rs</strong> are<br />
standard with all NIRQuest models except <strong>the</strong> NIRQuest512. For custom NIRQuest orde<strong>rs</strong>, you’ll<br />
need to call out <strong>the</strong> appropriate OSF filter (see table). The OF1-RG830 is a longpass filter<br />
recommended for custom configurations with Grating NIR1 or Grating NIR2.<br />
Item<br />
OSF-NIRQUEST256-2.1<br />
OSF-NIRQUEST256-2.5<br />
OSF-NIRQUEST512-xx<br />
OF1-RG830<br />
Description<br />
Order-sorting filter, installed, for custom NIRQUEST256-2.1 configurations<br />
Order-sorting filter, installed, for custom NIRQUEST256-2.5 configurations<br />
Order-sorting filter, installed, for custom NIRQUEST512 configurations; contact<br />
an Applications Scientist for details<br />
Longpass filter, installed, transmits >830 nm; recommended for custom NIR-<br />
Quest configurations with Grating NIR1 or Grating NIR2<br />
www.oceanoptics.com Tel: +1 727-733-2447 53
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
NIRQuest Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Choosing <strong>the</strong> Right Grating<br />
Grating Options<br />
Customized NIRQuest Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> are available with a choice <strong>of</strong> up to eight gratings. With each<br />
grating, you consider its groove density (which helps d<strong>ete</strong>rmine <strong>the</strong> resolution), its spectral range<br />
(which helps d<strong>ete</strong>rmine <strong>the</strong> wavelength range) and its blaze wavelength (which helps d<strong>ete</strong>rmine<br />
<strong>the</strong> most efficient range).<br />
Grating Intended Use Groove Density Spectral Range Blaze Wavelength Best Efficiency (>30%)<br />
(lines/mm)<br />
NIR1 NIRQuest256-2.5, NIRQuest512-2.5 75 1600 nm 1700 nm 1075-2500 nm<br />
NIR2<br />
NIRQuest256-2.1, NIRQuest256-2.5,<br />
100 1200 nm 1600 nm 900-2050 nm<br />
NIRQuest512-2.2, NIRQuest512-2.5<br />
NIR3<br />
NIRQuest256-2.1, NIRQuest256-2.5,<br />
150 ~800 nm 1100 nm 900-1700 nm<br />
NIRQuest512, NIRQuest512-2.2, NIRQuest512-2.5<br />
NIR10 NIRQuest256-2.1, NIRQuest256-2.5,<br />
300 350-380 nm 1200 nm 750-2200 nm<br />
NIRQuest512, NIRQuest512-2.2, NIRQuest512-2.5<br />
NIR11 NIRQuest256-2.1, NIRQuest256-2.5,<br />
400 240-290 nm 1600 nm 980-2500 nm<br />
NIRQuest512, NIRQuest512-2.2, NIRQuest512-2.5<br />
NIR12 NIRQuest256-2.1, NIRQuest256-2.5,<br />
500 160-220 nm 1370 nm 900-2500 nm<br />
NIRQuest512, NIRQuest512-2.2, NIRQuest512-2.5<br />
NIR13 NIRQuest256-2.1, NIRQuest256-2.5,<br />
600 100-180 nm 1200 nm 800-2500 nm<br />
NIRQuest512, NIRQuest512-2.2, NIRQuest512-2.5<br />
NIR14 NIRQuest512 1000 50-90 nm 1310 nm 900-1700 nm<br />
Additional grating options, adjustments to starting and ending wavelengths and similar customization may be available. Also, spectral range can vary<br />
by starting wavelength. For optimum performance, starting wavelengths should be set at >/= 900 nm. Please contact an Applications Scientist for<br />
details.<br />
Grating NIR1, 75 l/mm, 1075-2500 nm<br />
Grating NIR2, 100 l/mm, 900-2500 nm<br />
For more grating curves, see page 55.<br />
Technical Tip<br />
Gratings and slits are fixed in place and can only be replaced at our manufacturing facility. That’s why it’s important to<br />
consider all <strong>the</strong> variables involved in system performance, including d<strong>ete</strong>ctor and grating response, slit size and o<strong>the</strong>r<br />
bench accessories. Our Application Scientists have configured thousands <strong>of</strong> spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> for all sorts <strong>of</strong> applications<br />
and can <strong>of</strong>fer invaluable consultation as you consider your application.<br />
54 www.oceanoptics.com Tel: +1 727-733-2447
Grating NIR3, 150 l/mm, 900-1700 nm<br />
NIRQuest Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
NIRQuest Grating Efficiency Curves<br />
Grating NIR10, 300 l/mm, 750-2200 nm<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Grating NIR11, 400 l/mm, 980-2500 nm<br />
Grating NIR12, 500 l/mm, 900-2500 nm<br />
Grating NIR13, 600 l/mm, 800-2500 nm<br />
Grating NIR14, 1000 l/mm, 900-1700 nm<br />
www.oceanoptics.com Tel: +1 727-733-2447 55
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Application Notes<br />
High-resolution NIR Analysis<br />
New d<strong>ete</strong>ctor and optical bench options make it possible to configure near-infrared spe<strong>ctro</strong>m<strong>ete</strong>r setups for high-resolution applications such<br />
as laser and optical fiber characterization. Our NIRQuest-series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> cover various segments <strong>of</strong> <strong>the</strong> 900-2500 nm region and serve a<br />
variety <strong>of</strong> application needs.<br />
Introduction<br />
Near-infrared spe<strong>ctro</strong>scopy is a common analytical technique<br />
for chemistry and process control, where typical applications<br />
include identification <strong>of</strong> species and d<strong>ete</strong>rmination <strong>of</strong> water<br />
and fat content. In applications like those, absorbance peaks<br />
are <strong>of</strong>ten broad and optical resolution requirements <strong>of</strong> lesser<br />
concern than performance param<strong>ete</strong><strong>rs</strong> such as low noise and<br />
high sensitivity.<br />
Yet <strong>the</strong>re also are number <strong>of</strong> NIR applications where optical<br />
resolution <strong>of</strong>
SIR Series<br />
Our SIR Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> are fiber-based systems that use a unique design<br />
that allows rapid spectral scans over its entire spectral range.<br />
They can also provide real-time data from several discr<strong>ete</strong> wavelengths. Its<br />
compact design allows you to integrate <strong>the</strong> SIR easily into OEM applications and<br />
online process environments. SIRs are especially useful for laser-based<br />
applications.<br />
SIR Series Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Scanning Infrared Spe<strong>ctro</strong>scopy<br />
Spe<strong>ctro</strong>m<strong>ete</strong>r<br />
SIR spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> use single-point d<strong>ete</strong>cto<strong>rs</strong> and high angular resolutiontunable<br />
grating systems. The zero-backlash mechanical design provides superior<br />
accuracy and repeatability.<br />
This combination, along with an innovative 24-bit A/D converter, provides high spectral resolution and very high<br />
signal-to-noise data.<br />
NEW<br />
FOR 2011<br />
Features<br />
- USB 2.0 compliant - Rugged aluminum housing<br />
- Fast data transfer - Extended IR range<br />
Specifications<br />
SIR-2600 SIR-3400 SIR-5000 SIR-6500<br />
Range: 0.9-2.6 µm 1-3.4 µm 2-5 µm 3.0-6.5 µm<br />
D<strong>ete</strong>ctor: Extended range InGaAs with 2<br />
stage cooler<br />
InAs with 3 stage cooler<br />
MCT Photovoltaic with 3 stage<br />
cooler<br />
Diffraction grating: 600 lines 300 lines 300 lines 150 lines<br />
Optical design: -- Czerny-Turner F3 --<br />
Slits available: -- 10 µm, 50 µm, 100 µm, 200 µm, 500 µm --<br />
Optical input: -- SMA-905/906 with optional lensed input --<br />
Analog resolution: -- 24-bit, 16,777,216 counts --<br />
Triggering options: -- Internal and external synchronizational --<br />
MCT Photovoltaic with 3 stage<br />
cooler<br />
Technical Tip<br />
IR Light Sources<br />
Because SIR Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> cover NIR and mid-IR<br />
wavelengths, you’ll need to consider light sources<br />
with response in those regions. Our HL-2000 Tungsten<br />
Halogen Source has response to about 2000 nm, so<br />
you’ll need something different for most SIR models.<br />
We recommend our Cool Red Light Source, a high-power silicon nitride emitter<br />
with output from ~600-6500 nm. Additional information on <strong>the</strong> Cool Red is<br />
available in <strong>the</strong> Light Sources section. Also, you’ll need optical fiber and sampling<br />
accessories that will transmit at <strong>the</strong> longer mid-IR wavelengths. Some <strong>of</strong> your options<br />
are described in <strong>the</strong> table on <strong>the</strong> next page.<br />
SIR Bench Accessories<br />
SIR-DARK-SHUTTER SIR Dark Reference Shutter<br />
SIR-FILTER-SHUTTER<br />
SIR-SLIT-5<br />
SIR-SLIT-10<br />
SIR-SLIT-50<br />
SIR-SLIT-100<br />
SIR-SLIT-200<br />
SIR-SLIT-500<br />
SIR High-Pass Filter Shutter (2 options)<br />
5 µm Slit for SIR Series<br />
(recommended for SIR-2600 only)<br />
10 µm Slit for SIR Series<br />
50 µm Slit for SIR Series<br />
100 µm Slit for SIR Series<br />
200 µm Slit for SIR Series<br />
500 µm Slit for SIR Series<br />
www.oceanoptics.com Tel: +1 727-733-2447 57
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Single Point D<strong>ete</strong>cto<strong>rs</strong><br />
Measurements from Deep UV to Far IR<br />
Specifications<br />
Bandwidth:<br />
Trigger modes supported:<br />
Digital I/O:<br />
Digital resolution:<br />
Sample speed:<br />
TE cooler controller:<br />
100 kHz<br />
Internal and external with phase delay<br />
4 TTL level I/Os<br />
24 bits to 17 bits (depending on sampling speed)<br />
7 Hz to 3 kHz<br />
Up to 3 stage cooler with 0.1 °C stability<br />
Model D<strong>ete</strong>ctor Wavelength<br />
SPD-PYRO<br />
Pyro-electric<br />
8 µm - 14 µm<br />
Packaged with ele<strong>ctro</strong>nics<br />
SPD-SIR-2600<br />
Extended InAs<br />
900 nm - 2600 nm<br />
with 3 stage cooler<br />
SPD-SIR-3400 InAs with 3 stage cooler 1 µm - 3.4 µm<br />
SPD-SIR-6500<br />
MCT Photovoltaic 3 µm - 6.5 µm<br />
with 3 stage cooler<br />
SPD-VIS Hybrid Si-InGaAs 200 nm - 1100 nm<br />
Our Single Point D<strong>ete</strong>cto<strong>rs</strong> are <strong>the</strong> ideal tool for high signal-to-noise,<br />
single point fiber optic and free-beam measurements.<br />
At <strong>the</strong> heart <strong>of</strong> <strong>the</strong> Single Point D<strong>ete</strong>ctor Series is a low-noise reamplifier<br />
circuit with a 24-bit A/D digital converter. The Single Point<br />
D<strong>ete</strong>ctor can be customized with a range <strong>of</strong> d<strong>ete</strong>cto<strong>rs</strong> from Deep UV<br />
to <strong>the</strong> Far IR (200 nm - 14 um).<br />
These d<strong>ete</strong>cto<strong>rs</strong> can support cooled d<strong>ete</strong>cto<strong>rs</strong> as well as synchronization<br />
with external events. Single Point D<strong>ete</strong>cto<strong>rs</strong> can receive a trigger<br />
from external sources and also be triggered. The s<strong>of</strong>tware controls<br />
also support user-programmed digital I/O.<br />
The <strong>Ocean</strong> <strong>Optics</strong> Single Point D<strong>ete</strong>cto<strong>rs</strong> include s<strong>of</strong>tware and a s<strong>of</strong>tware<br />
development kit for use<strong>rs</strong> who write <strong>the</strong>ir own applications.<br />
Features<br />
- Included s<strong>of</strong>tware and s<strong>of</strong>tware development kit<br />
- Several triggering modes supported<br />
- Integrated temperature control for TE cooled d<strong>ete</strong>cto<strong>rs</strong><br />
- Low noise amplifier and 24 bit A/D converter<br />
- Integrated dark level <strong>of</strong>fset to increase dynamic range for high-background<br />
measurements<br />
Technical Tip<br />
Accessories for Your Mid-IR Systems<br />
Most <strong>Ocean</strong> <strong>Optics</strong> light sources, optical fibe<strong>rs</strong> and sampling accessories transmit light from <strong>the</strong> UV to <strong>the</strong> Shortwave<br />
NIR – from about 200-2000 nm. For measurements at longer wavelengths, you’ll need accessories constructed with IRresponsive<br />
materials such as sapphire, fluoride, chalcogenide and zinc selenide. Some <strong>of</strong> your options are listed in <strong>the</strong><br />
table below. For additional information, consult an <strong>Ocean</strong> <strong>Optics</strong> Applications Scientist.<br />
Item<br />
74-SAPPHIRE-25<br />
74-SAPPHIRE-5<br />
74-ZNSE-25<br />
P450-0.5-FLUORIDE<br />
P450-1-FLUORIDE<br />
P450-1.5-Fluoride<br />
P500-0.5-CHAL<br />
P500-1-CHAL<br />
Description<br />
25.4 mm/1-inch Sapphire Lens Collimator for direct attachment <strong>of</strong> fiber coupling<br />
5 mm/0.20-inch Sapphire Lens Collimator for direct attachment <strong>of</strong> fiber coupling<br />
25.4mm/1-inch ZnSe AR-coated Mid-IR Collimator for direct attachment <strong>of</strong> fiber coupling<br />
Fluoride Fibe<strong>rs</strong> for mid-IR transmission, 450 µm core, 0.5 m<strong>ete</strong><strong>rs</strong>, SMA 905 terminated, PVDF Jacket<br />
Fluoride Fibe<strong>rs</strong> for Mid-IR transmission, 450 µm core, 1.0 m<strong>ete</strong><strong>rs</strong>, SMA 905 terminated, PVDF Jacket<br />
Fluoride Fibe<strong>rs</strong> for Mid-IR transmission, 450 µm core, 1.5 m<strong>ete</strong><strong>rs</strong>, SMA 905 terminated, PVDF Jacket<br />
Chalcogenide Fibe<strong>rs</strong> for Mid-IR transmission, 500/550 µm core, 0.5 m<strong>ete</strong><strong>rs</strong>, SMA 905 terminated, PVDF Jacket<br />
Chalcogenide Fibe<strong>rs</strong> for Mid-IR transmission, 500/550 µm core, 1.0 m<strong>ete</strong><strong>rs</strong>, SMA 905 terminated, PVDF Jacket<br />
58 www.oceanoptics.com Tel: +1 727-733-2447
ANIR Se<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
The ANIR series <strong>of</strong> scanning Fourier Transform Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> (FTS)<br />
uses an exclusive micro-actuated lamellar grating and operates with<br />
a single photodiode d<strong>ete</strong>ctor. The actuation <strong>of</strong> <strong>the</strong> interferom<strong>ete</strong>r<br />
system is actively controlled by a laser enabling a precise and reliable<br />
operation. The single photodiode d<strong>ete</strong>ction ensures highest<br />
dynamic range and signal quality at very attractive pricing.<br />
ANIR Spe<strong>ctro</strong>m<strong>ete</strong>r Series<br />
Portable Fourier Transform Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
ANIR-0.9-1.7 ANIR-0.9-2.6 ANIR-2.0-4.5<br />
Spectral range: 900 – 1700 nm 900 – 2600 nm 2000 – 4500 nm<br />
D<strong>ete</strong>ctor type: InGaAs InGaAs MCT<br />
Resolution in wave<br />
number:<br />
At 1000 nm:<br />
At 1700 nm:<br />
At 2600 nm:<br />
At 4500 nm:<br />
8 cm -1<br />
1.4 nm<br />
4.2 nm<br />
8 cm -1<br />
1.4 nm<br />
4.2 nm<br />
9.7 nm<br />
8 cm -1<br />
9.7 nm<br />
29.2 nm<br />
Wavelength < 0.5 nm < 0.5 nm < 0.5 nm<br />
accuracy:<br />
Signal-to-noise > 1000:1 > 1000:1 300:1<br />
ratio:<br />
A/D converter: 16 bit 16 bit 16 bit<br />
Minimum scan time: 1 s 1 s 1 s<br />
Effective measurement<br />
5 s 5 s 5 s<br />
time:<br />
Optical Bench<br />
Optical fiber<br />
entrance:<br />
Fiber optic connector:<br />
Physical<br />
Dimensions:<br />
650 μm (fiber core<br />
diam<strong>ete</strong>r)<br />
650 μm (fiber core<br />
diam<strong>ete</strong>r)<br />
650 μm (fiber core<br />
diam<strong>ete</strong>r)<br />
SMA 905 SMA 905 SMA 905<br />
210 mm x 100 mm<br />
x 70 mm<br />
210 mm x 100 mm<br />
x 70 mm<br />
Weight: 850 g 850 g 850 g<br />
210 mm x 100 mm<br />
x 70 mm<br />
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
ANIR Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> are fiber-based, USB-powered and portable.<br />
The modular <strong>concept</strong> <strong>of</strong> <strong>the</strong> ANIR allows use<strong>rs</strong> to adapt it for specific<br />
applications, as <strong>the</strong> wavelength range is solely dependent on <strong>the</strong><br />
d<strong>ete</strong>ctor choice.<br />
Features<br />
- Extensive wavelength range (three models covering<br />
900-4500 nm)<br />
- High resolution <strong>of</strong> 8 cm -1<br />
- Optional param<strong>ete</strong><strong>rs</strong> available such as variable gain, resolution<br />
and scan speed<br />
- High throughput and signal to noise ratio<br />
- Low power consumption and reliable operation<br />
Sample Applications<br />
- Food analysis<br />
- Gas d<strong>ete</strong>ction<br />
- Environmental monitoring<br />
- Material identification<br />
- Process control<br />
- Laser characterization<br />
About Fourier Transform Spe<strong>ctro</strong>scopy (FTS)<br />
A Fourier Transform spe<strong>ctro</strong>m<strong>ete</strong>r is <strong>the</strong> instrument <strong>of</strong> choice for high-resolution<br />
atomic and molecular spe<strong>ctro</strong>scopy. A Fourier Transform is a ma<strong>the</strong>matical<br />
operation that transforms (or<br />
decomposes) a signal into a<br />
set <strong>of</strong> trigonomic functions.<br />
In <strong>the</strong> case <strong>of</strong> a spe<strong>ctro</strong>m<strong>ete</strong>r,<br />
Fourier Transform<br />
converts raw data into a<br />
spectrum via a technique<br />
<strong>of</strong> collecting spectra<br />
based on measurements<br />
<strong>of</strong> <strong>the</strong> coherence <strong>of</strong> a<br />
radiative source, using timeor<br />
space-domain measurements <strong>of</strong><br />
radiation. This technique uses <strong>the</strong> Wiener-Khinchin<br />
<strong>the</strong>orem, a <strong>the</strong>orem useful for analyzing <strong>the</strong> response <strong>of</strong><br />
Linear Time Invariant (LTI) systems to an arbitrary input signal.<br />
As a result, an FTS spe<strong>ctro</strong>m<strong>ete</strong>r is more sensitive and requires a much shorter<br />
sampling time than <strong>the</strong> standard types <strong>of</strong> spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong> used today. An FTS<br />
spe<strong>ctro</strong>m<strong>ete</strong>r such as <strong>the</strong> ARCoptix ANIR spe<strong>ctro</strong>m<strong>ete</strong>r has an interferometric<br />
module with scanner for laser-assisted positioning control (pictured) and is perfectly<br />
suited for high accuracy transmission measurements <strong>of</strong> gases and liquids.<br />
www.oceanoptics.com Tel: +1 727-733-2447 59
Spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong><br />
Spe<strong>ctro</strong>m<strong>ete</strong>r Accessories<br />
Additional Options Add Value to Your Spe<strong>ctro</strong>m<strong>ete</strong>r<br />
The SteadiQ provides an environmentally controlled atmosphere for your<br />
<strong>Ocean</strong> <strong>Optics</strong> spe<strong>ctro</strong>m<strong>ete</strong>r, helping to stabilize temperature effects and<br />
eliminate temperature drift in inclement conditions or extreme temperatures.<br />
The rugged, portable device ensures more accurate, reliable results in field<br />
applications including solar irradiance, volcanic observation, greenhouse<br />
monitoring and industrial environments such as cold food storage.<br />
Available in both UV and VIS ve<strong>rs</strong>ions, <strong>the</strong> SteadiQ interfaces directly with our<br />
USB, HR, Maya, QE65000 and NIRQuest Series spe<strong>ctro</strong>m<strong>ete</strong><strong>rs</strong>. In extreme hot<br />
or extreme cold conditions, SteadiQ operates independently from outside<br />
temperatures. It connects easily to <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r with preconfigured<br />
plug-ins and communicates via <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r’s USB port.<br />
Features<br />
- Interfaces directly with your <strong>Ocean</strong> <strong>Optics</strong> spe<strong>ctro</strong>m<strong>ete</strong>r<br />
- Operates independently from outside temperatures<br />
- Perfect for extreme hot or cold conditions<br />
- Available in UV-NIR (200-1100 nm) and VIS-NIR (400-2500 nm) ve<strong>rs</strong>ions<br />
- Externally controlled dark measurement<br />
Spe<strong>ctro</strong>m<strong>ete</strong>r Models Supported<br />
- USB2000+<br />
- USB4000<br />
- HR2000+<br />
- HR4000<br />
- QE65000<br />
- Maya2000<br />
- Maya2000 Pro<br />
- NIRQuest512<br />
- NIRQuest256-2.1<br />
- NIRQuest256-2.5<br />
Physical<br />
Dimensions:<br />
465 mm x 300 mm x 414 mm<br />
Weight (SteadiQ only):<br />
12 kg<br />
Spe<strong>ctro</strong>scopic<br />
Wavelength range SteadiQ-UV:<br />
200-1100 nm (practical range depends on <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r configuration)<br />
Wavelength range SteadiQ-VIS:<br />
400-2500 nm depending on spe<strong>ctro</strong>m<strong>ete</strong>r configuration<br />
Temperature Stability<br />
Inside temperature: 23 °C ± 1 °C between +5 °C to +40 °C<br />
23 °C ± 2 °C between -20 °C and +60 °C<br />
Ele<strong>ctro</strong>nics & Communication<br />
Operating voltage:<br />
Including 110/220 VAC > 24 VDC; 7 A<br />
Communication interface:<br />
Via USB connection on <strong>the</strong> spe<strong>ctro</strong>m<strong>ete</strong>r<br />
60 www.oceanoptics.com Tel: +1 727-733-2447<br />
Technical Tip<br />
Turn your NIRQuest into a network-accessible spe<strong>ctro</strong>m<strong>ete</strong>r with <strong>the</strong> Remora Network Adapter. Use Remora to communicate<br />
with your <strong>Ocean</strong> <strong>Optics</strong> spe<strong>ctro</strong>m<strong>ete</strong>r over E<strong>the</strong>rnet or Wi-Fi. Remotely capture spectral data from anywhere<br />
via E<strong>the</strong>rnet or wireless network (ra<strong>the</strong>r than traditional USB). This allows you to change param<strong>ete</strong><strong>rs</strong> and enjoy all <strong>of</strong> <strong>the</strong><br />
functionality <strong>of</strong> your spe<strong>ctro</strong>m<strong>ete</strong>r as if it were connected directly to your computer.<br />
Remora’s web interface is accessible from your PC, mobile phone, PDA, iPhone and most Internet-ready devices. Use<br />
your favorite web browser to view live data in Scope Mode and maintain <strong>the</strong> ability to change experiment param<strong>ete</strong><strong>rs</strong> on <strong>the</strong> fly. Adding Remora<br />
to your spe<strong>ctro</strong>m<strong>ete</strong>r is as quick and simple as configuring any wireless router. Plug in <strong>the</strong> Remora, browse to its web interface to configure it for<br />
your network, and <strong>of</strong>f you go. Use your favorite web browser to view live data directly on your web-capable device without installing any s<strong>of</strong>tware.