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Evaluation method for Raman depolarization measurements including geometrical effects and polarization aberrations

Evaluation method for Raman depolarization measurements including geometrical effects and polarization aberrations
Evaluation method for Raman depolarization measurements including geometrical effects and polarization aberrations
In this article, we address the notoriously difficult problem to quantitatively link measured Raman depolarization values to theoretical polarizability tensor quantities, since quantum calculations do not incorporate experimental parameters. For this, we introduce a numerical model to calculate, for realistic experimental configurations, effective Raman line strength functions, phi, which find their way into depolarization ratios, ρ. The model is based on interlinked integrations over the angles in the light collection path and a finite Raman source volume along the excitation laser beam. The model deals also with the conditional aperture parameters, associated with more than one optical component in the light collection path. Finally, we also can take into account polarization aberrations introduced by the sample cell windows. The procedure was fully tested for Raman depolarization spectra of selected hydrogen isotopologues. Distinct aspects affecting Raman depolarization data were validated, namely: (1) excitation polarization impurities; (2) extended Raman excitation volumes; (3) Raman light collection over finite solid angles; and (4) polarization aberrations introduced by optics in the light collection path. The correction of the experimental measurement data for the aforementioned effects resulted in depolarization ratios for the Q1(J") Raman lines of H2 and T2, which mostly differed by less than 5% from those obtained by quantum-calculations.
0377-0486
453-462
Schlösser, M.
0a5a00ea-42b2-4450-83b6-31e798d77858
James, T.M.
5b0ac1dc-de2d-420f-b715-db5019aa8b66
Fischer, S.
85fe26ec-1561-4f9a-abaa-006d49d65582
Lewis, R.J.
fa4ab7fa-230c-4cf2-8c79-4ee1ae1fb8a0
Bornschein, B.
0bfad77e-1c0e-4495-8c66-68c0eb564ce7
Telle, H.H.
94ef8f4e-d4f0-41ce-9231-d5a6682b42f8
Schlösser, M.
0a5a00ea-42b2-4450-83b6-31e798d77858
James, T.M.
5b0ac1dc-de2d-420f-b715-db5019aa8b66
Fischer, S.
85fe26ec-1561-4f9a-abaa-006d49d65582
Lewis, R.J.
fa4ab7fa-230c-4cf2-8c79-4ee1ae1fb8a0
Bornschein, B.
0bfad77e-1c0e-4495-8c66-68c0eb564ce7
Telle, H.H.
94ef8f4e-d4f0-41ce-9231-d5a6682b42f8

Schlösser, M., James, T.M., Fischer, S., Lewis, R.J., Bornschein, B. and Telle, H.H. (2013) Evaluation method for Raman depolarization measurements including geometrical effects and polarization aberrations. Journal of Raman Spectroscopy, 44 (3), 453-462. (doi:10.1002/jrs.4201).

Record type: Article

Abstract

In this article, we address the notoriously difficult problem to quantitatively link measured Raman depolarization values to theoretical polarizability tensor quantities, since quantum calculations do not incorporate experimental parameters. For this, we introduce a numerical model to calculate, for realistic experimental configurations, effective Raman line strength functions, phi, which find their way into depolarization ratios, ρ. The model is based on interlinked integrations over the angles in the light collection path and a finite Raman source volume along the excitation laser beam. The model deals also with the conditional aperture parameters, associated with more than one optical component in the light collection path. Finally, we also can take into account polarization aberrations introduced by the sample cell windows. The procedure was fully tested for Raman depolarization spectra of selected hydrogen isotopologues. Distinct aspects affecting Raman depolarization data were validated, namely: (1) excitation polarization impurities; (2) extended Raman excitation volumes; (3) Raman light collection over finite solid angles; and (4) polarization aberrations introduced by optics in the light collection path. The correction of the experimental measurement data for the aforementioned effects resulted in depolarization ratios for the Q1(J") Raman lines of H2 and T2, which mostly differed by less than 5% from those obtained by quantum-calculations.

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More information

Published date: March 2013
Organisations: Optoelectronics Research Centre

Identifiers

Local EPrints ID: 356334
URI: http://eprints.soton.ac.uk/id/eprint/356334
ISSN: 0377-0486
PURE UUID: 18354b79-fddb-45ab-a0c8-1f543c5864ca

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Date deposited: 13 Sep 2013 10:41
Last modified: 14 Mar 2024 14:47

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Contributors

Author: M. Schlösser
Author: T.M. James
Author: S. Fischer
Author: R.J. Lewis
Author: B. Bornschein
Author: H.H. Telle

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