{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2024,8,4]],"date-time":"2024-08-04T15:13:00Z","timestamp":1722784380108},"reference-count":0,"publisher":"Wiley","issue":"1","license":[{"start":{"date-parts":[[1983,2,1]],"date-time":"1983-02-01T00:00:00Z","timestamp":412905600000},"content-version":"vor","delay-in-days":0,"URL":"http:\/\/onlinelibrary.wiley.com\/termsAndConditions#vor"}],"content-domain":{"domain":[],"crossmark-restriction":false},"short-container-title":["The Journal of Physiology"],"published-print":{"date-parts":[[1983,2]]},"abstract":"<jats:p>Receptor potentials of single hair cells in the free\u2010standing region of the basilar papilla of the anaesthetized alligator lizard were measured intracellularly with micropipettes. Stimuli were primarily acoustic pulses (clicks) delivered to the tympanic membrane. The receptor potential was independent of click repetition rate for the range 10\u2010150 clicks\/s. This property is presumed to be the basis of the rate independence of the extracellular cochlear microphonic potential. The receptor potential wave\u2010form consisted of a fast oscillatory component (or oscillation) superimposed on a usually positive (depolarizing) slow component. Reversal of the stimulus polarity resulted in a reversal of the polarity of the oscillations; the polarity of the slow component remained unchanged. The relative magnitudes of the two components depended on click level. At the higher click levels the magnitudes of the slow and oscillatory components were comparable. The relation of the receptor potential to the stimulus was non\u2010linear; the peak\u2010to\u2010peak magnitude of the receptor potential increased less than proportionately with increasing sound\u2010pressure level, and reversal of the stimulus polarity did not result in a reversal of the receptor potential. The receptor\u2010potential magnitude for high\u2010level clicks ranged from 1\u201013 mV peak\u2010to\u2010peak with an average value of 3.5 mV. At the lower click levels the magnitude of the slow component was much smaller than that of the oscillatory component. The relation of the receptor potential to the acoustic stimulus approached that of a linear system, the magnitude of the receptor potential became approximately proportional to the sound\u2010pressure level, and reversal of the stimulus polarity resulted in approximate reversal of the receptor potential. For low\u2010level stimuli the frequency of the oscillations of the receptor potential in response to clicks was approximately equal to the frequency of maximal a.c. response to tones. Apparently, both phenomena reflect the frequency selectivity of the processes generating the receptor potential. The frequency of oscillations in the click response varied from one cell to another (range of 1.0\u20102.2 kHz in this study). The results are qualitatively consistent with a model (Weiss, Mulroy &amp; Altmann, 1974) that contains a linear, band\u2010pass filter followed by a rectifier followed by a low\u2010pass filter.<\/jats:p>","DOI":"10.1113\/jphysiol.1983.sp014559","type":"journal-article","created":{"date-parts":[[2014,12,19]],"date-time":"2014-12-19T07:00:10Z","timestamp":1418972410000},"page":"699-721","source":"Crossref","is-referenced-by-count":19,"title":["Receptor potentials of lizard hair cells with free\u2010standing stereocilia: responses to acoustic clicks."],"prefix":"10.1113","volume":"335","author":[{"given":"K","family":"Baden\u2010Kristensen","sequence":"first","affiliation":[],"role":[{"role":"author","vocabulary":"crossref"}]},{"given":"T F","family":"Weiss","sequence":"additional","affiliation":[],"role":[{"role":"author","vocabulary":"crossref"}]}],"member":"311","published-online":{"date-parts":[[1983,2]]},"container-title":["The Journal of Physiology"],"original-title":[],"language":"en","link":[{"URL":"https:\/\/api.wiley.com\/onlinelibrary\/tdm\/v1\/articles\/10.1113%2Fjphysiol.1983.sp014559","content-type":"unspecified","content-version":"vor","intended-application":"text-mining"},{"URL":"https:\/\/physoc.onlinelibrary.wiley.com\/doi\/pdf\/10.1113\/jphysiol.1983.sp014559","content-type":"unspecified","content-version":"vor","intended-application":"similarity-checking"}],"deposited":{"date-parts":[[2023,10,19]],"date-time":"2023-10-19T08:56:13Z","timestamp":1697705773000},"score":1,"resource":{"primary":{"URL":"https:\/\/physoc.onlinelibrary.wiley.com\/doi\/10.1113\/jphysiol.1983.sp014559"}},"subtitle":[],"short-title":[],"issued":{"date-parts":[[1983,2]]},"references-count":0,"journal-issue":{"issue":"1","published-print":{"date-parts":[[1983,2]]}},"alternative-id":["10.1113\/jphysiol.1983.sp014559"],"URL":"https:\/\/doi.org\/10.1113\/jphysiol.1983.sp014559","archive":["Portico"],"relation":{},"ISSN":["0022-3751","1469-7793"],"issn-type":[{"value":"0022-3751","type":"print"},{"value":"1469-7793","type":"electronic"}],"subject":[],"published":{"date-parts":[[1983,2]]}}}