Rr. Fay et Pl. Eddswalton, DIVERSITY IN FREQUENCY-RESPONSE PROPERTIES OF SACCULAR AFFERENTS OF THE TOADFISH, OPSANUS-TAU, Hearing research, 113(1-2), 1997, pp. 235-246
The frequency response of primary saccular afferents of toadfish (Opsa
nus tau) was studied in the time and frequency domains using the rever
se correlation (revcor) method, Stimuli were noise bands with flat acc
eleration spectra delivered as whole-body motion. The recorded acceler
ation waveform was averaged over epochs preceding and following each s
pike. This average, termed the revcor, is an estimate of the response
of an equivalent linear filter intervening between body motion and spi
ke initiation. The spectrum of the revcor estimates the shape of the e
quivalent linear filter. Revcor responses were brief, damped oscillati
ons indicative of relatively broadly tuned filters. Filter shapes were
generally band-pass and differed in bandwidth, band edge slope, and c
haracteristic frequency (74 Hz to 140 Hz). Filter shapes tend to be in
dependent of stimulus level. Afferents can be placed into two groups w
ith respect to characteristic frequency (74-88 Hz and 140 Hz). Some hi
gh-frequency afferents share a secondary peak at the characteristic fr
equency of low-frequency afferents, suggesting that an afferent may re
ceive differently tuned peripheral inputs. For some afferents having s
imilar filter shapes, revcor responses often differ only in polarity,
probably reflecting inputs from hair cells oriented in opposite direct
ions. The origin of frequency selectivity and its diversity among sacc
ular afferents may arise from a combination of hair cell resonance and
micromechanical processes. The resulting frequency analysis is the si
mplest yet observed among vertebrate animals. During courtship, male t
oadfish produce the 'boatwhistle' call, a periodic vocalization having
several harmonics of a 130 Hz fundamental frequency. The saccule enco
des the waveform of acoustic particle acceleration between < 50 and ab
out 250 Hz. Thus, the fundamental frequency component of the boatwhist
le is well encoded, but the successive higher harmonics are filtered o
ut. The boatwhistle is thus encoded as a time-domain representation of
its fundamental frequency or pulse repetition rate.