The thermoelastic mechanism for laser generation of acoustic waves in liquids is presented first of all. The
amplitude of the acoustic waves excited by this mechanism is so small that most of time it can not satisfy application
requirements. In our research, a Helmholtz resonance photoacoustic cell is employed to resolve the problem. It consists
of a sample cell and a Helmholtz resonator. When the modulating frequency of a laser beam is equal to the acoustical
resonance frequency of a Helmholtz resonator, the photoacoustic cell corresponds to an acoustic amplifier in the
photoacoustic system. And then the amplifying performance of a Helmholtz resonance photoacoustic cell under liquids is
investigated. The theoretical analysis indicates that both the resonance frequency and the magnitude of enlargement are
dependent on the parameters of the Helmholtz resonator and the medium characteristics in and around the cell. After that,
for a given laser source, a photoacoustic cell is designed to amplify the acoustic waves excited by the laser beam. The
resonance frequency, the peak magnitude of enlargement, and the transfer function are analyzed theoretically. At last, an
experimental system is set up. The photoacoustic signal is simulated by a single-frequency acoustic signal. The acoustic
waves both inside and outside the photoacoustic cell are picked up using broadband piezoelectric hydrophones
synchronously. The transfer function curve of the resonance photoacoustic cell is obtained experimentally. The results
derived from theoretic analysis and those obtained from experiments agree with each other well.
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