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The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM...

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The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms the BM upward. (This is a closed system, so these pressure pulses are resolved by inward and outward movements at the round window, which is covered by the internal tympanic membrane .)
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Page 1: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms the BM upward. (This is a closed system, so these pressure pulses are resolved by inward and outward movements at the round window, which is covered by the internal tympanic membrane.)

Page 2: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

Durrant & Lovrinic (1995)

Page 3: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.
Page 4: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.
Page 5: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.
Page 6: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

Note that differences in frequency can be seen in two ways: (1) by differences in the place along the BM with the greatest motion amplitude (this will become the basis of place theory/the place principle/tonotopic theory); (2) by differences in the rate at which the BM vibrates (this will become the basis of synchrony theory).

f = 3,000 Hz

f = 1,000 Hz

f = 300 Hz

Page 7: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.
Page 8: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

Suppose we were to mix two sinusoids together – one low frequency (e.g., 200 Hz) and the other of much higher frequency (e.g., 3000 Hz).

What kind of traveling wave envelope pattern would we expect to see on the basilar membrane?

0 500 1000 1500 2000 2500 3000 3500 40000

10

20

30

40

50

60

70

80

90

100

Frequency (Hz)

Am

plitu

de

200 Hz, 3000 Hz

200 Hz + 3000 Hz

Page 9: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

Figure 4-15. The basilar membrane varies continuously in stiffness from base to apex. The greater stiffness of the membrane at the base makes the basal end respond better to high frequencies than low frequencies, while the opposite is true of the apical end. After von Bekesy (1960), Rhode (1973), and Durrant & Lovrinic (1995).

3000 Hz 200 Hz

Page 10: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

Input: Complex optical signal with many frequencies mixed together.

Output: Individual frequency components have been “unmixed” – low frequencies directed to one spatial location, high frequencies directed to a different spatial location, mid-frequencies directed to the appropriate place in the middle.

Page 11: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.
Page 12: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

What should be happening at the 8th N for two signals that differ in frequency?

Page 13: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

FRCs for 8th N fibers at two different locations along the basilar membrane. These two nerve fibers are said to have two different “characteristic frequencies” (CFs; sometimes “best frequencies” – BFs).

One fiber responds best (has the highest firing rate) at 900 Hz, the other at 1700 Hz.

This has nothing to do with the fiber itself – the differ-ences in CF occur because the 900 Hz fiber is connected to a hair cell that is closer to the apex than the 1700 Hz fiber. The differences in CF are due to the basilar membrane, not the fiber.

CF=Characteristic Frequency(also Best Frequency)

(Note: normalized firing rate means that the spontaneous discharge rate of the fiber has been subtracted out.)

Page 14: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

Figure 4-29. Neural tuning curves for auditory nerve fibers with three different characteristic frequencies (CFs). The threshold of the fiber is the lowest (i.e., sensitivity is greatest) at the characteristic frequency of the fiber. Data from Kiang and Moxon (1974).

Another way to measure cochlear frequency analysis: 8th N tuning curves. The threshold for the nerve fiber is measured for pure tones at different frequencies. Thresholds are lowest at the fiber’s CF.

(2060: Skip)

Page 15: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

What controls the CF of a fiber? Consider this thought experiment:

Question: Suppose an afferent 8th N with a CF of 125 Hz were to be disconnected from the apical end of the BM and reconnected at the basal end. Now we re-measure the CF of the fiber. What will happen?

a. The CF remains 125 Hz. Why should it matter where it’s located? If the CF is 125 at the apical end, and it’s really the same fiber (which it is), the CF will remain 125 Hz.

b. The CF has to change to something much higher because now because the hair cells that stimulate the nerve to fire are connected to a section of the BM that is much stiffer than before (when it was connected at the apex) and therefore will respond best to high frequency vibration. It’s not the fiber that controls CF, it’s the stiffness of the section of the BM that it’s attached to.

c. Not enough information. We need to know the sound level as well as the frequency.

Page 16: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

Moral of the Story

Although we refer to the CF of the fiber, CF is not determined by the fiber at all.

CF is controlled by the stiffness of that section of the BM that is closest to the IHC that stimulates the 8thN fiber.

•An 8thN fiber that innervates an IHC connected near the base of the cochlea will have a high CF.

•An 8thN fiber that innervates an IHC connected near the apex of the cochlea will have a low CF.

That’s all there is to the story: CF is controlled by the BM, not the fiber. The fibers are more-or-less interchangeable.

Page 17: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

These are the FRCs we saw earlier. They present the view of the cochlear as a bank of BP filters. For place theory to work, the filters must be numerous (closely spaced), and (b) narrow. We only see two in this figure, but there are ~3,000 of them, so we’re ok there.

Are the filters narrow enough? They look ok here, but notice that the presentation level of the input sinusoids for the data shown here is 45 dBSPL, which is quite low. Will these BP filters remain narrow as the presentation level is increased? The great Jerzy Rose and his buddies at Wisconsin addressed this question as well.

Page 18: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

The previous figure showed FR curves for two fibers with different CFs, but for a very soft signal – 45 dBSPL. What happens to the shapes of FR curves at higher sound levels? Shown here are FR curves – measured at the 8th N – for a single fiber (CF=1700 Hz) at 8 different signal intensities from 25-95 dBSPL.

Frequency response curves for a single auditory nerve fiber (CF=1700 Hz) at eight different signal intensities. Note that the frequency response curves are relatively narrow at low presentation levels but become very broad at higher intensities. Data and figure from Rose et al. (1971).

How do the shapes of these bandpass filters change with increases in sound level?

Rose et al. (1971)

This is the FRC we saw earlier – at 45 dBSPL.

Page 19: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

Synchrony coding (simplified version): The period of the 8th N pulse train matches the period of the original signal; e.g., if the signal has a freq of 100 Hz, the most common interspike interval on the 8th N will be 10 ms. High frequency = short interspike interval, low frequency = long interspike interval. What could be more straightforward?

Page 20: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

So: (a) if the signal period is 10 ms (100 Hz), the most common interspike interval will be 10 ms; (b) if the signal period is 5 ms (200 Hz), the most common interspike interval will be 5 ms; (c) if the signal period is 1 ms (1000 Hz), the most common interspike interval will be 1 ms; (d) if the signal period is 0.5 ms (2000 Hz), the most common interspike interval will be 0.5 ms. Right?

What’s wrong with this? Can the interspike interval be 0.5 ms?

Page 21: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

Volley Theory (an elaboration of synchrony coding)

Basic idea is pretty straightforward: Because of refractory intervals, no individual fiber can fire with a period equal to that of the input signal for a 2 kHz signal. Individual fibers catch a cycle, miss one or more, catch another one, miss a few, etc. The period of the input signal is not preserved on any individual fiber, but it is reflected in the most common interspike interval of a population of fibers.

Page 22: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

The Bus Analogy (from Peter Dallos, I think).

Page 23: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

8th N voltage

Input signal

Post-stimulus Time (PST) Histogram for sinusoids at 599 and 217 Hz.

f = 217 Hz, t = ~4.6 ms

Aside: Note the differences in amplitude, which might seem contrary to the all-or-none principle. They don’t contradict all-or-none. The amp differences are real enough, but they have no information value.

Page 24: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

8th N voltage

Input signal

Post-stimulus Time (PST) Histogram for sinusoids at 599 and 217 Hz.

f = 217 Hz, t = ~4.6 ms

Aside (cont’d): All of the information in neural pulse trains is conveyed by: (a) the rate of occurrence, (spikes per second) and (b) the time of occurrence. Neural pulses are treated by the CNS like switches that are either on of off.

Page 25: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

Another View of the Volley Principle Both of these pictures of volley

theory are oversimplified since they show the neuron always firing at the time when the signal amplitude reaches a peak. This is not the case since the entire hair cell-nerve fiber relationship is probabilistic rather than deterministic. The point of maximum amplitude is the time when the probability of a pulse is greatest (though not guaranteed).

However, if the fiber is most likely to fire at the amplitude peak, the most common interspike interval (of a population of fibers) will equal the period of the input signal.

Page 26: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

Best Picture Yet of the Volley Principle

Note that this figure accurately shows that the 8th N pulses do not all occur a the waveform peak; they are just more likely there. Because of this, the most frequent inter-spike interval will correspond to the period of the input signal.

Page 27: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

Again with the Volley Principle

This figure shows the output of just 4 nerve fibers. There are ~30,000 8N fibers in humans. So, even though there is a random element to 8N firing, you can do a lot of ensemble averaging to find the most common inter-spike interval. The behavior of any individual fiber cannot be predicted, but the behavior of a large population of fibers IS predictable.

Page 28: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

Another Thought Experiment

Cochlea is unrolled and the auditory nerve is exposed. Patient is awake and able to tell us what he hears.

We have a stimulating electrode and can deliver any pattern of electrical current at any rate to any of these nerve fibers – alone or in combination.

According to place theory, how would we artificially induce a sensation of high pitch; i.e., fool the listener into thinking he’d heard a high frequency sound?

How about low pitch?

According to synchrony theory, how would we artificially induce a sensation of high pitch; i.e., fool the listener into thinking he’d heard a high frequency sound?

How about low pitch?

cochlear branch of 8th N: ~30,000 fibers

to brainstem

Page 29: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

Place Theory & Synchrony Theory

So, we have a place or tonotopic code: Frequency is coded by the place along the BM where 8th N electrical activity is greatest .

We also have a synchrony code (with the volley principle tacked on to make it work even above the limits imposed by refractory intervals) based on the timing of 8th N pulses: Frequency is coded by the interspike interval of a population of fibers (short interspike interval=high freq; long interspike interval=low freq).

Is one of these theories right and the other one wrong? Probably not.

Commonly Held View

~15 to ~400 Hz: Mainly synchrony ~400 to ~4000-5000: Both place & synchrony Above ~4000-5000: Only place

Page 30: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

Pulse Coding on the Auditory Nerve

Rose et al. (1971)

Page 31: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

Pulse Coding on the Auditory Nerve

Rose et al. (1971)

FIG. 11. Period histograms for a fiber responding to a complex periodic sound when the sound pressure level of both primaries is successively raised in lo-dB steps. Tones are locked in a ratio of 3:4. Period of complex sound = 4,998 psec. Each bin = 100 psec. Phase angle and amplitude of each primary used in construction of the fitted waveform are specified for each graph. Ra = amplitude ratio. Each histogram based on two stimulus presentations. Stimulus duration: 10 sec.

Page 32: The causality here is pretty straightforward: Compression at the stapes footplate deforms the BM downward, rarefaction at the stapes footplate deforms.

http://www.youtube.com/watch?v=PeTriGTENoc

Youtube video

(Clicking on the link should work. If not: (a) copy/paste link into your browser, or (b) search Youtube for “auditory transduction”)


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