“…For isotropic transparent material, a single acoustic phonon at frequency ω (=2π f ) is probed at a given wave vector, ± q = k i – k s selected by the scattering geometry, where ± q is for Stokes and anti-Stokes components, k i and k s are wavevectors of the incident and scattered light. Using energy and momentum conservation laws, a doublet with frequency, ω = ± cq , relative to the central Rayleigh line (ω = 0) appears in the spectrum of the scattered light analyzed by a six-pass tandem-Fabry–Perot interferometer. , Here, c denotes the sound velocity (longitudinal or transverse) in the medium, and the momentum magnitude q depends on the scattering geometry. In the so-called transmission geometry, q trans = (4π/λ)sin α, where α = θ/2, with θ being the scattering angle between k i and k s and λ (=532 nm) is the laser wavelength in vacuum.…”