Target response in a focused, modulated sound field: Modeling and experiment

2018 ◽  
Vol 143 (3) ◽  
pp. 1739-1739
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Timothy D. Daniel ◽  
Philip L. Marston ◽  
Ahmad T. Abawi ◽  
Ivars P. Kirsteins
1999 ◽  
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L. Simon ◽  
J. Hardy

1988 ◽  
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T. Hidaka ◽  
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S. Masuda

2004 ◽  
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Thierry Le Pollès ◽  
Judicaël Picaut ◽  
Michel Bérengier ◽  
Claude Bardos

Wave Motion ◽  
2020 ◽  
Vol 94 ◽  
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Yanfang Zheng ◽  
Xinyu Zhao ◽  
Sung-Jin Song ◽  
Jianhai Zhang

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Judicaël Picaut ◽  
Stéphane Colle ◽  
Michel Bérengier

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Judical Picaut

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Thierry Le Pollès ◽  
Judicaël Picaut ◽  
Stéphane Colle ◽  
Michel Bérengier ◽  
Claude Bardos

1999 ◽  
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Judicaël Picaut ◽  
Laurent Simon

1973 ◽  
Vol 16 (2) ◽  
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Author(s):  
John H. Mills ◽  
Seija A. Talo ◽  
Gloria S. Gordon

Groups of monaural chinchillas trained in behavioral audiometry were exposed in a diffuse sound field to an octave-band noise centered at 4.0 k Hz. The growth of temporary threshold shift (TTS) at 5.7 k Hz from zero to an asymptote (TTS ∞ ) required about 24 hours, and the growth of TTS at 5.7 k Hz from an asymptote to a higher asymptote, about 12–24 hours. TTS ∞ can be described by the equation TTS ∞ = 1.6(SPL-A) where A = 47. These results are consistent with those previously reported in this journal by Carder and Miller and Mills and Talo. Whereas the decay of TTS ∞ to zero required about three days, the decay of TTS ∞ to a lower TTS ∞ required about three to seven days. The decay of TTS ∞ in noise, therefore, appears to require slightly more time than the decay of TTS ∞ in the quiet. However, for a given level of noise, the magnitude of TTS ∞ is the same regardless of whether the TTS asymptote is approached from zero, from a lower asymptote, or from a higher asymptote.


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