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1 ollectively encode the wide range of audible sound pressures.
2 i generated by head movements and changes in sound pressure are detected by hair cells with amazing s
3                                              Sound pressure attenuated with distance from the reef at
4 n the acoustic environment: the variation in sound pressure in each frequency band, relative to the m
5 e basilar membrane and at the stapes, and as sound pressure in the ear canal.
6 elocity toward scala tympani but at 80-90 dB sound pressure level (in decibels relative to 20 microPa
7 including the measurement of peak equivalent sound pressure level (peSPL) and peak sound pressure lev
8 valent sound pressure level (peSPL) and peak sound pressure level (pSPL).
9  suppresses its spiking response to a 100-dB sound pressure level (SPL) acoustic stimulus and maintai
10 ontractions were studied as functions of the sound pressure level (SPL) and duration of 2-kHz tone bu
11 osition of the spider of approximately 65 dB sound pressure level (SPL).
12  nymphs have auditory thresholds of 70-80 dB sound pressure level (SPL).
13 eater than the acoustic input power at 10 dB sound pressure level (SPL).
14 acebo for both clicks (dexamethasone: 6.7-dB sound pressure level [SPL] vs. placebo: 33.4-dB SPL, P=.
15 V and hearing thresholds were elevated 50 dB sound pressure level across the frequency spectrum.
16 al of two acoustic indices, i.e. the average sound pressure level and the acoustic complexity index b
17 ich presented a significantly higher ambient sound pressure level and were more acoustically complex
18                                 Increases in sound pressure level appeared to be largely driven by la
19    These cells never fired to tones at 50 dB sound pressure level but fired to frequency-modulated sw
20 d identically (8-16 kHz noise band at 100 dB sound pressure level for 2 h) but at different ages (4-1
21  the device's performance and applicability, sound pressure level is characterized in both space and
22 ect operates by continuously integrating the sound pressure level of background noise through tempora
23  neurons are typically above 100-120 dB SPL (sound pressure level re 20 microPa).
24 lative to 20 microPascals) and at 100-110 dB sound pressure level responses undergo two large phase s
25 rnible auditory brainstem responses (ABR) to sound pressure level stimuli up to 100 dB, indicating a
26 y noise bursts; prepulses for PPI were 70 dB sound pressure level tones of 4, 12, and 20 kHz.
27                                              Sound pressure level was modulated trapezoidally at the
28 d areas of Moorea Island (French Polynesia), sound pressure level was positively correlated with the
29 er exposure to a traumatic unilateral 80 dB (sound pressure level) 4 kHz tone.
30 percentile was associated with a 1.6-dB SPL (sound pressure level) decrease in DPOAE amplitude (95% C
31 0-10000 Hz) and input levels (e.g., 50-75 dB sound pressure level).
32  of NH listeners when compared at equal SPL (sound pressure level).
33 the unit over a wide dynamic range (10-90 dB sound pressure level).
34 e youngest embryos (maximum intensity 107 dB sound pressure level).
35 ber auditory nerve responses at 70 and 50 dB sound pressure level, have been quantified, based on KL
36                     At an intensity of 60 dB sound pressure level, the bats' hearing extended from 2.
37 sed during passive listening to brief, 95-dB sound pressure level, white noise bursts presented inter
38 e effects depend nonlinearly on the stimulus sound pressure level.
39 lliculus (IC) change their firing rates with sound pressure level.
40 tic stimulus (a hiss) of approximately equal sound pressure level.
41  with no requirement of knowing the incident sound pressure level.
42 ar growth rate of the response to increasing sound pressure level; and the amount of distortion to be
43 ng from 113 Hz to 49 kHz at a level of 60 dB sound-pressure level or less, with their best sensitivit
44  elevation and, correspondingly, on the high sound pressure levels (>100 dB SPL) necessary to produce
45 es in response to white noise stimuli at low sound pressure levels (</=84 dB SPL), revealing a previo
46 uditory system operates over a vast range of sound pressure levels (100-120 dB) with nearly constant
47  masker-probe delays, over a range of masker sound pressure levels (SPLs) and frequencies.
48                             Both the ambient sound pressure levels and the estimated effective vocali
49 les thermoacoustic emissions at loud audible sound pressure levels of 90.1 dB, which are inaccessible
50 tion paralleling the loudness function up to sound pressure levels of at least 120 dB.
51 ound-evoked vibrations over a range of input sound pressure levels spanning six orders of magnitude.
52 eocilia in vivo deflect <100 nm even at high sound pressure levels, often it takes >500 nm of stereoc
53 al frequency distribution at low to moderate sound pressure levels: one peak occurred around the prep
54 4, representing lowest to highest A-weighted sound pressure measurements in decibels.
55 l measurements indicate a minimum detectable sound pressure of approximately 20 muPa at 16 kHz.
56 chanically gated ion channel that transduces sound, pressure, or movement into changes in excitabilit
57                                       Ramped sound pressure waves (150-250 Hz) evoked electrotonic po

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