“…The effects of the finite laser pulse duration (hence spectrum) are eliminated by the deconvolution operation of computing the complex quotient where ± refers to the sense of the local oscillator through ±t in eqs 2 and 3, C is the detector constant, $' is the index part of xg>, and all time and frequency dependencies have been suppressed. The in-phase local oscillator probes the imaginary, or loss, part (x$") that is related to the Raman cross section of the sample,10 ^L, -phase = =F 2 [X^7pump/probe]) (6) while the complex local oscillator probes the complex x$.…”