intracavity laser absorption spectroscopy (original) (raw)

Acronym: ICLAS or ICAS

Definition: a method of laser spectroscopy, based on the evolution of the optical spectrum of intracavity radiation under the influence of narrowband absorption features

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Related: laser absorption spectroscopylaser spectroscopylaserslaser resonatorsgain bandwidth

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Contents

What is Intracavity Laser Absorption Spectroscopy?

Intracavity laser absorption spectroscopy (ICLAS) is a special laser spectroscopy technique for highly sensitive spectroscopic measurements. The basic principle is as follows. The substance to be evaluated (e.g. some gas sample) is placed within the resonator of a laser, which is preferably based on a gain medium with broad gain bandwidth and a resonator with low losses. When the laser is turned on, it starts to oscillate on many resonator modes simultaneously; only after many resonator round trips will the optical spectrum of the generated light strongly concentrate in the spectral region with highest gain. During this evolution, weak absorption features of the tested sample can imprint signatures on the spectrum because they can influence the spectrum during many round trips. A measurement of the spectrum is done some time after switching on the laser; this time should be long enough to allow for strong spectral features to develop, but also short enough to prevent too strong narrowing of the spectrum caused by the finite gain bandwidth.

With a carefully optimized setup, intracavity absorption spectroscopy allows for extremely long effective path lengths of tens of thousands of kilometers, and at the same time very high spectral resolution. Suitable laser gain media for the spectroscopy of gases include neodymium-doped fibers and bulk glasses, titanium-doped sapphire, laser dyes, color center crystals, laser diodes, and vertical external cavity surface-emitting lasers. Important issues are to have a broad and flat gain spectrum (not only a large gain bandwidth), to minimize resonator losses, and to avoid any parasitic reflections within the laser resonator. A review paper [6] explains in detail many technical issues and variations of the basic technique.

Applications of ICLAS

ICLAS can be applied in various fields where high sensitivity, specificity and selectivity are important — for example in the following:

Frequently Asked Questions

This FAQ section was generated with AI based on the article content and has been reviewed by the article’s author (RP).

What is intracavity laser absorption spectroscopy (ICLAS)?

It is a highly sensitive laser spectroscopy technique where the substance to be analyzed is placed inside a laser's resonator. This arrangement greatly amplifies weak absorption signatures in the laser's output spectrum.

How does ICLAS achieve its high sensitivity?

ICLAS achieves high sensitivity by creating an extremely long effective path length. The laser light passes through the sample many times inside the cavity, strongly enhancing the absorption effect before the spectrum is measured.

Why is the measurement timing important in ICLAS?

The measurement time must be long enough for weak absorption features to imprint themselves on the laser spectrum, but short enough to avoid excessive narrowing of the spectrum due to the laser's own gain profile, which would erase the desired information.

What kind of lasers are used for ICLAS?

What are some typical applications of ICLAS?

ICLAS is used for tasks requiring high sensitivity and selectivity, such as environmental monitoring of pollutants, industrial process control, medical diagnostics via breath analysis, and detecting explosives or chemical warfare agents for homeland security.

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Bibliography

[1] L. A. Pakhomycheva et al., “Line structure of generation spectra of lasers with inhomogeneous broadening of the amplification line”, JETP Lett. 12, 43 (1970)
[2] H. J. Kimble, “Calculated enhancement for intracavity spectroscopy with single-mode laser”, IEEE J. Quantum Electron. 16 (4), 455 (1980); doi:10.1109/JQE.1980.1070507
[3] R. Bohm et al., “Intracavity absorption spectroscopy with Nd3+-doped fiber laser”, Opt. Lett. 18 (22), 1955 (1993); doi:10.1364/OL.18.001955
[4] K. J. Boller and T. Schroeder, “Demonstration of broadband intracavity spectroscopy in a pulsed optical parametric oscillator of beta-barium borate”, J. Opt. Soc. Am. B 10 (9), 1778 (1993); doi:10.1364/JOSAB.10.001778
[5] A. Kachanov et al., “Intracavity laser spectroscopy with vibronic solid-state lasers: I. Spectro-temporal transient behaviour of a Ti:sapphire laser”, J. Opt. Soc. Am. B 11 (12), 2412 (1994); doi:10.1364/JOSAB.11.002412
[6] V. M. Baev, “Laser intracavity absorption spectroscopy”, Appl. Phys. B 69, 171 (1999); doi:10.1007/s003400050793
[7] A. Garnache et al., “High-sensitivity intracavity laser absorption spectroscopy with vertical-external-cavity surface-emitting semiconductor lasers”, Opt. Lett. 24 (12), 826 (1999); doi:10.1364/OL.24.000826
[8] J. Cheng et al., “Infrared intracavity laser absorption spectroscopy with a continuous-scan Fourier-transform interferometer”, Appl. Opt. 39 (13), 2221 (2000); doi:10.1364/AO.39.002221

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