21.03.2015 Views

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

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

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

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!