Generalized Optical Design of the Double-Row Circular Multi-Pass Cell

A new design of circular multi-pass cells (CMPC) with two rows of reflection spots on mirrors is presented. The effective optical path length (OPL) of this novel CMPC is double that of traditional CMPC with the same diameter and interval of spots. This OPL can be readily adjusted to have regular intervals by rough rotation adjustment. We achieved a spatial separation of pre- and post-transfer optical systems that was adequately large even in the cases with a large number of passes. Analytical chief ray tracing analysis and a generalized method for parameter determination for designing the cell are presented in detail. The stable condition of the double-row CMPC (DR-CMPC) is also derived by the ABCD matrix method. Designs with maximum effective OPL of 74.72 m, 48.67 m and 24.57 m are demonstrated and verified by ray tracing simulations within a 25 cm diameter DR-CMPC. An adjustment of the regular intervals to 1 m can be achieved in both designs. The overall astigmatism of the design with an effective OPL of 74.72 m is only 9.30 × 10−6 mm, which is four orders of magnitude smaller than that of the traditional CMPC with similar geometric parameters.

[1]  Herwig Kogelnik,et al.  Off-Axis Paths in Spherical Mirror Interferometers , 1964 .

[2]  Liqun Sun,et al.  Generalized design of a zero-geometric-loss, astigmatism-free, modified four-objective multipass matrix system. , 2016, Applied optics.

[3]  J B McManus,et al.  Astigmatic mirror multipass absorption cells for long-path-length spectroscopy. , 1995, Applied optics.

[4]  Kopin Liu,et al.  A simple yet effective multipass reflector for vibrational excitation in molecular beams. , 2008, The Review of scientific instruments.

[5]  David R Glowacki,et al.  Design and performance of a throughput-matched, zero-geometric-loss, modified three objective multipass matrix system for FTIR spectrometry. , 2007, Applied optics.

[6]  Yargo Bonetti,et al.  Versatile multipass cell for laser spectroscopic trace gas analysis , 2012 .

[7]  Albert Manninen,et al.  Compact multipass optical cell for laser spectroscopy. , 2013, Optics letters.

[8]  Semen M. Chernin,et al.  Development of optical multipass matrix systems , 2001 .

[9]  Herbert L. Strauss,et al.  A new white type multiple pass absorption cell. , 1970, Applied optics.

[10]  S. Chernin,et al.  Promising version of the three-objective multipass matrix system. , 2002, Optics express.

[11]  Semen M. Chernin Multipass systems of new generation in high-resolution spectroscopy for fundamental and applied atmosphere investigations , 1995, Other Conferences.

[12]  Donald R. Herriott,et al.  Folded Optical Delay Lines , 1965 .

[13]  John U. White Long Optical Paths of Large Aperture , 1942 .

[14]  L. Casperson,et al.  Principles of lasers , 1983, IEEE Journal of Quantum Electronics.

[15]  Manuel Graf,et al.  Beam folding analysis and optimization of mask-enhanced toroidal multipass cells. , 2017, Optics letters.

[16]  Guofan Jin,et al.  Generalized method for calculating astigmatism of the unit-magnification multipass system. , 2010, Applied optics.

[17]  Cornelius Zetzsch,et al.  Circular multireflection cell for optical spectroscopy. , 2010, Applied optics.

[18]  Yu-Chi Chang,et al.  Mid-infrared spectroscopy for gases and liquids based on quantum cascade technologies. , 2014, The Analyst.

[19]  S. Chernin,et al.  Optical multipass matrix systems. , 1991, Applied optics.

[20]  Lukas Emmenegger,et al.  Circular paraboloid reflection cell for laser spectroscopic trace gas analysis. , 2016, Journal of the Optical Society of America. A, Optics, image science, and vision.

[21]  Semen M. Chernin NEW GENERATION OF MULTIPASS SYSTEMS IN HIGH RESOLUTION SPECTROSCOPY , 1996 .

[22]  H. J. Bernstein,et al.  Rotation‐Vibration Spectra of Diatomic and Simple Polyatomic Molecules with Long Absorbing Paths. I. The Spectrum of Fluoroform (CHF3) from 2.4μ to 0.7μ , 1948 .