Abstract

CARS spectral profiles are functionally described by the variation of the square of the total third-order, nonlinear susceptibility with the anti-Stokes frequency shift. This inherent, squared susceptibility signal dependence, when weighted by an experiment dependent convolution, produces a CARS spectral profile which is a problem specific to the experiment design.

Fourier transform spectral interferometric coherent anti-Stokes Raman scattering (FTSI-CARS) spectroscopy

Sang-Hyun Lim, Allison G. Caster, and Stephen R. Leone
Opt. Lett. 32(10) 1332-1334 (2007)

Simultaneous rotational coherent anti-Stokes Raman spectroscopy and coherent Stokes Raman spectroscopy with arbitrary pump–Stokes spectral separation

Alan C. Eckbreth and Torger J. Anderson
Opt. Lett. 11(8) 496-498 (1986)

Comparison of gas temperatures measured by coherent anti-Stokes Raman spectroscopy (CARS) of O₂ and N₂

Thomas A. Reichardt, Paul E. Schrader, and Roger L. Farrow
Appl. Opt. 40(6) 741-747 (2001)

Thermometry for turbulent flames by coherent anti-Stokes Raman spectroscopy with simultaneous referencing to the modeless excitation profile

Eric H. van Veen and Dirk Roekaerts
Appl. Opt. 44(32) 6995-7004 (2005)

Heterodyne coherent anti-Stokes Raman scattering (CARS) imaging

Eric O. Potma, Conor L. Evans, and X. Sunney Xie
Opt. Lett. 31(2) 241-243 (2006)