4pPA3. Thermal phonon resonance in a cylindrical cavity.

Session: Thursday Afternoon, December 5

Time: 2:30


Author: Koichiro Hattori
Location: Inst. of Indust. Sci., Univ. of Tokyo, 7-22-1, Roppongi, Minato-ku, Tokyo, 106 Japan
Author: Keiji Sakai
Location: Inst. of Indust. Sci., Univ. of Tokyo, 7-22-1, Roppongi, Minato-ku, Tokyo, 106 Japan
Author: Kenshiro Takagi
Location: Inst. of Indust. Sci., Univ. of Tokyo, 7-22-1, Roppongi, Minato-ku, Tokyo, 106 Japan

Abstract:

Resonance phenomena were observed of a thermally excited phonon confined in a very small space. The power spectrum changes due to the boundary condition of the cavity shape. A cylindrical cavity which has a 1450-(mu)m inner diameter containing water was prepared as a sample. The resonance frequency in the cylindrical cavity is given by a solution of Bessel's function. An optical beating system is used which has a hyperfrequency resolution to detect this fine structure of the resonance spectrum. The spatial decay of phonons is very large in the liquid sample. The low-frequency measurement is required to observe the resonance phenomena, because the phonon can reflect many times in the cavity. Generally though, a broadening of the wave vector due to angular divergence of the laser light is very large in a small-angle light-scattering measurement, since the wave vectors of the resonance peaks are determined only by a boundary of the cavity. Several resonance peaks can be observed around the 8 MHz measurement and a typical peak width is 50 kHz. The strong peaks are observed at every 500 kHz. These peaks are the symmetric and lowest asymmetric tangential modes.


ASA 132nd meeting - Hawaii, December 1996