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. 2019 Feb 19;10(3):1329–1338. doi: 10.1364/BOE.10.001329

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Published by The Optical Society under the terms of the Creative Commons Attribution 4.0 License. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI.

Published by The Optical Society under the terms of the Creative Commons Attribution 4.0 License. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI.

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Fig. 6 — Fit results for (left) Stokes and (right) anti-Stokes parts of the Brillouin spectrum of methanol and water. Lorentzian and Gaussian functions were used resulting in R² = 0.996 and 0.982 (methanol), 0.994 and 0.989 (water), respectively. Note that negative frequency shifts have been converted to positive shifts.