Polarization properties, high-order Raman spectra, and frequency asymmetrybetween Stokes and anti-Stokes scattering of Raman modes in a graphite whisker - art. no. 214301

The Raman spectra of a new type of graphite whiskers have been measured in the range of 150-7800 cm(-1). The intensity of the over-tone (2D) located a t similar to 2700 cm(-1) is found to be about 10 times stronger than that o f the C-C stretching mode (G) at 1582 cm(-1). Because of the peculiar enhan cement of the 2D mode, high-order Raman bands up to fifth order at similar to 7500 cm(-1) have been observed. Polarized micro-Raman spectroscopy has b een per-formed on an individual graphite whisker, and angular-dependent int ensity measurements of all Raman modes in the VV and HV geometries are in a greement with the theoretical calculated results. Laser-energy-dependent di spersion effects and the frequency discrepancy of Raman modes between their Stokes and anti-Stokes lines in graphite whiskers are also carefully inves tigated. The energy dispersion of the D mode and G mode is very similar to that of highly oriented pyrolytic graphite (HOPG). In contrast to the Raman spectra of HOPG and other graphite materials, two laser-energy-dependent R aman lines are revealed in the low-frequency region of the Raman spectra of graphite whiskers. which are believed to be the resonantly enhanced phonon s in the transverse-acoustic and longitudinal-acoustic phonon branches. Mor eover, the obvious energy dispersion of the D' mode at similar to 1620 cm(- 1) is observed in graphite whiskers. The results clearly reveal how strongl y the peak parameters of Raman modes of graphite materials are dependent on their structural geometry. The Stokes and anti-Stokes scattering experimen ts show that the frequency discrepancy between the Stokes and anti-Stokes s ides of a Raman mode in graphite materials is equal to the frequency value covered by the one-phonon energy of this Raman mode in its frequency versus laser energy curve, which is the product of the one-phonon energy of this mode (E omega (s)) and the value of its laser-energy dispersions (partial d erivativeE omega (s)/partial derivative epsilon (L)).