Figure 7.
Perturbations to the frequency and half-width of (0,8) mode as a function of frequency, with argon in the resonator at 100 kPa. The frequency was swept by changing the temperature of the resonator, which changes the speed of sound.
Perturbations to the frequency and half-width of (0,8) mode as a function of frequency, with argon in the resonator at 100 kPa. The frequency was swept by changing the temperature of the resonator, which changes the speed of sound.