Multipass spectroscopic absorption cells

Multiple-pass or long path absorption cells are commonly used in spectroscopy to measure low-concentration components or to observe weak spectra in gases or liquids. Several important advances were made in this area beginning in the 1930s, and research into a wide range of applications continues to the present day.

Pfund Cell - An early multipass absorption cell

Functional Overview

Generally the goal of this type of sample cell is to improve detection sensitivity by increasing the total optical path length that travels through a small, constant sample volume. In principle, a longer path length results in greater detection sensitivity. Focusing mirrors must be used to redirect the beam at each reflection point, resulting in the beam being restricted to a predefined space along a controlled path until it exits the optical cavity. The output of the cell is the input of an optical detector (a specialized type of transducer), which senses specific changes in the properties of the beam that occur during interaction with the test sample. For instance, the sample may absorb energy from the beam, resulting in an attenuation of the output that is detectable by the transducer. Two conventional multipass cells are called the White cell and Herriott cell. ^[1]

Pfund Cell

In the late 1930s August Pfund used a triple-pass cell like the one shown above for atmospheric study. The cell, which became known as the Pfund cell, is constructed using two identical spherical mirrors, each having a hole carefully machined into its center. The separation distance between the mirrors is equal to the mirror focal length. A source enters from a hole in either mirror, is redirected twice at two reflection points, and then exits the cell through the other mirror on the third pass. The Pfund cell was one of the earliest examples of this type of spectroscopic technique and is noted for having used multiple passes. ^[2]

White cell

 

White cell animation - Count 8 reflective passes

The White cell was first described in 1942 by John U. White in his paper Long Optical Paths of Large Aperture,^[3] and was a significant improvement over previous long path spectroscopic measurement techniques. A White cell is constructed using three spherical, concave mirrors having the same radius of curvature. The mirrors are separated by a distance equal to their radii of curvature. The animation on the right shows a White Cell in which a beam makes eight reflective passes or traversals. The number of traversals can be changed quite easily by making slight rotational adjustments to either M2 or M3; however, the total number of traversals must always occur in multiples of four. The entering and exiting beams do not change position as traversals are added or removed, while the total number of traversals can be increased many times without changing the volume of the cell, and therefore the total optical path length can be made large compared to the volume of the sample under test. The spots from various passes can overlap on mirrors M2 and M3 but must be distinct on mirror M1. If the input beam is focused in the plane of M1, then each round trip will also be focused in this plane. The tighter the focus, the more nonoverlapping spots there can be on M1 and thus the higher the maximum pathlength.

At present the White cell is still the most commonly used multipass cell and provides many advantages.^[4] For example,

• The number of traversals is easily controlled
• It allows for high numerical aperture
• It is reasonably stable (but not as stable as the Herriott cell)

White cells are available with path lengths ranging from less than a meter to many hundreds of meters.^[5]

Herriott cell

 

Herriott cell - Adjust D to change the number of passes

The Herriott cell first appeared in 1965 when Donald R. Herriott and Harry J. Schulte published Folded Optical Delay Lines while at Bell Laboratories.^[6] The Herriott cell is made up of two opposing spherical mirrors. A hole is machined into one of the mirrors to allow the input and output beams to enter and exit the cavity. Alternatively, the beam may exit through a hole in the opposite mirror. In this fashion the Herriott cell can support multiple light sources by providing multiple entrance and exit holes in either of the mirrors. Unlike the White cell, the number of traversals is controlled by adjusting the separation distance D between the two mirrors. This cell is also commonly used and has some advantages^[4] over the White cell:

• It is simpler than the White cell with only two mirrors that are easier to position and less susceptible to mechanical disturbance of the cell
• Can be more stable than the White cell

However, the Herriot cell does not accept high numerical aperture beams. In addition, larger sized mirrors must be used when longer path lengths are needed.

Circular Multipass Cells

 

Circular Multipass Cell - The beam propagates on a star pattern. The path length can be adjusted by changing the incidence angle Φ.

Another category of multipass cells is generally referred to as circular multipass reflection cells. They were first introduced by Thoma and co-workers in 1994.^[7] Such cells rely on a circular arrangement of mirrors. The beam enters the cell under an angle and propagates on a star-shaped pattern (see picture on the right). The path length in circular multipass cells can be varied by adjusting the incidence angle of the beam. An advantage lies in their robustness towards mechanical stress such as vibrations or temperature changes. Furthermore, circular multipass cells stand out because of the small detection volumes they provide.^[8] A stable beam propagation is achieved by shaping individual reflection points to form a non-concentric mirror-arrangement.^[9][10]

In a special case, a circular mirror is used, allowing continuous adjustment of the angle of incidence. A drawback of this circular cell configuration is the inherent concentric mirror arrangement which leads to imperfect imaging after a large number of reflections.

See also

• Laser absorption spectrometry
• Tunable diode laser absorption spectroscopy
• Optical system
• Absorption spectroscopy
• Infrared spectroscopy
• Absorption (optics)
• Optical density
• Optical depth
• Reflectivity

References

1. White; Tittel (2002). "Tunable infrared laser spectroscopy". Annual Reports on the Progress of Chemistry, Section C. 98. RSCPublishing: 219–272. doi:10.1039/B111194A.
2. "LONG PATH GAS CELLS".
3. White, John (1942). "Long Optical Paths of Large Aperture". Journal of the Optical Society of America. 32 (5): 285. Bibcode:1942JOSA...32..285W. doi:10.1364/josa.32.000285.
4. Robert, Claude (2007). "Simple, stable, and compact multiple-reflection optical cell for very long optical paths". Applied Optics. 46 (22): 5408–5418. Bibcode:2007ApOpt..46.5408R. doi:10.1364/AO.46.005408. PMID 17676157.
5. John M. Chalmers (1999). "Chapter 4: Mid-infrared spectroscopy". Spectroscopy in process analysis. CRC Press LLC. p. 117. ISBN 1-84127-040-7.
6. Herriott, Donald; Schulte, Harry (1965). "Folded Optical Delay Lines". Applied Optics. 4 (8): 883–891. Bibcode:1965ApOpt...4..883H. doi:10.1364/AO.4.000883.
7. Thoma (1994). "A multiple-reflection cell suited for absorption measurements in shock tubes". Shock Waves. 4 (1): 51. Bibcode:1994ShWav...4...51T. doi:10.1007/bf01414633. S2CID 122233071.
8. Tuzson, Bela (2013). "Compact multipass optical cell for laser spectroscopy". Optics Letters. 38 (3): 257–9. Bibcode:2013OptL...38..257T. doi:10.1364/ol.38.000257. PMID 23381403.
9. Graf, Manuel (2018). "Compact, circular, and optically stable multipass cell for mobile laser absorption spectroscopy". Optics Letters. 43 (11): 2434–2437. Bibcode:2018OptL...43.2434G. doi:10.1364/OL.43.002434. PMID 29856397.
10. "IRcell-S – multipass cell without absorption mask". Fast, broadband and high-resolution dual-comb spectrometers – IRsweep. 2019-12-10. Retrieved 2020-10-05.