2000
DOI: 10.1063/1.1309200
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Nonlinear propagation of phase-conjugate focused sound beams in water

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Cited by 3 publications
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“…Figure 8 displays rms pressures in the time-reversed field ͑a͒ along the axis and ͑b͒ in the focal plane for absorption A f ϭ0.04, focusing gain Gϭ19, and mirror located at m ϭ3.5 with m ϭϱ. These parameters correspond to those of the experiments reported by Brysev et al, 10 who used a source of radius aϭ7.5 mm and focal length dϭ39 mm radiating in water at frequency f ϭ6.23 MHz, with the mirror at distance z m ϭ131 mm. Values of the nonlinearity parameter are varied from N f ϭ0 ͑lin-ear͒ to N f ϭ1 ͑substantial shock formation͒.…”
Section: B Focused Incident Beamsmentioning
confidence: 88%
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“…Figure 8 displays rms pressures in the time-reversed field ͑a͒ along the axis and ͑b͒ in the focal plane for absorption A f ϭ0.04, focusing gain Gϭ19, and mirror located at m ϭ3.5 with m ϭϱ. These parameters correspond to those of the experiments reported by Brysev et al, 10 who used a source of radius aϭ7.5 mm and focal length dϭ39 mm radiating in water at frequency f ϭ6.23 MHz, with the mirror at distance z m ϭ131 mm. Values of the nonlinearity parameter are varied from N f ϭ0 ͑lin-ear͒ to N f ϭ1 ͑substantial shock formation͒.…”
Section: B Focused Incident Beamsmentioning
confidence: 88%
“…9, 10 We henceforth concentrate on mirrors of infinite radius ( m ϭϱ) in order to emphasize nonlinear effects in the time-reversed field.…”
Section: A Unfocused Incident Beamsmentioning
confidence: 99%