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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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