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Re: AW: Cochlear nonlinearity & TTS
Navid, Richard and the listees,
I have heard a lot of speculation about the cochlear amplifier for many
years. One of the questions that I have wondered about
as a signal processing engineer for many years, is with all the
sophisticated nonlinearities, delays, amplifiers, filters
etc that are present in the auditory periphery, how does it "represent"
an acoustic signal in the neural spike patterns
that emanate from the auditory periphery? (I guess everyone wonders
about it.)
Is it possible to reconstruct the acoustic signal if you were able to
measure/monitor the
spike patterns that are put out by all the auditory nerve fibers? What
is the reconstruction 'algorithm"?
(I know about Egbert deBoer's reconstruction method for a single
nerve fiber.) Is'n't the information about the signal
distributed across many, many nerve fibers? Should'nt the
reconstruction take information from
all nerve fibers and fuse them to reconstruct the signal? Just wondering
aloud. RK
Richard F. Lyon wrote:
At 9:17 AM -0800 1/16/07, Navid Shahnaz wrote:
Thank you Reinhart for your clarification. Does the cochlear
amplifier works on both sides of the excitation pattern peak on the
BM? or the amplifier operates wore efficiently at a place that is
just above or toward the apex from the point of disturbance created
by travelling wave? Operationally this point may be an ideal point as
it is less likely saturates the amplifier due to sharp slope of the
travelling wave on the apical side.
Cheers
Navid
Navid,
Both Monita and Reinhart have given good explanations, but let me add
a bit.
The way I think of it, the active amplification is active everywhere,
but it competes with the passive loss mechanisms, and is only
significant at low enough levels. The active loss mechanism (damping)
increases rapidly apically when a sine wave travels past a
characteristic place. Because of the active gain, the response to a
sine wave can travel further before it damps out; from the "passive
peak" that Reinhart mentions, the peak response location can be
further apical, up to about a half octave worth of place further, when
the active amplification is significant, to the "active peak". The
"net" amplification is positive (in dB per mm or whatever) before the
response peak, and negative after the response peak, pretty much by
definition of peak. That net includes the active gain, which
saturates, and the passive loss, which doesn't, so it's level dependent.
In addition to the saturation that reduces the active gain at high
level, there is also efferent control that turns down the gain in
response to afferent response level and possibly other central control
signals. This effect of efferent control of mechanical gain has been
directly demonstrated, but I don't recall exactly who/when/where to
cite right now.
Dick
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