Abstract
The phonon-phonon volume interaction due to the nonlinear elastic properties of solids has been investigated together with nonlinearities in the end-surface generation of microwave phonons. The experimental method consisted of generating a microwave-ultrasonic fundamental at one end of a rod and detecting the second harmonic at the opposite end by means of the piezoelectric effect. For Z-cut quartz and sapphire, where the phonon-phonon interaction dominates, experimental observations prove that the original flow of energy from the fundamental to the second harmonic is completely reversed after longitudinal waves are reflected from a stress-free surface or from a half-wavelength-thick transducer. Thus, the second harmonic in an almost lossless medium vanishes upon arrival at the generating transducer because the reflection reverses the phase angle 2φ1 relative to φ2, where φ1 and φ2 are the phase angles, respectively, of the fundamental and the second harmonic. When the thickness of the CdS transducers was made less than one-half wavelength, the smaller phase shift produced a correspondingly smaller energy reversal. For transverse waves in AC-cut quartz, the original increase of the second harmonic due to volume nonlinearities was unaffected by the presence of the stress-free boundary, thereby confirming that there is no phase shift for transverse waves. These phase-shift phenomena, together with the frequency and rod-length dependence of the harmonic generation, were used to separate surface from volume nonlinearities. By measuring the coupling constants of the phonon-phonon interaction at 4.2°K, the following third-order elastic coefficients (in units of 1011 N/m2) were obtained: c111=2.6±0.5 for X-cut natural quartz, and -38±3 for 0.01% Cr-doped a-oriented sapphire grown by the Verneuil process; c333=14±4 for Z-cut quartz, and -21±1 for both undoped and 0.01% Cr-doped c-oriented sapphire.

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