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Contents - Max-Planck-Institut für Physik komplexer Systeme

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2.8 Coupling Virtual and Real Hair Bundles in a Hybrid Experiment<br />

KAI DIERKES, FRANK JÜLICHER, BENJAMIN LINDNER<br />

Active amplification in hearing. Humans possess an<br />

extraordinary ability to detect complex sound stimuli<br />

and to analyze their spectral and temporal fine structure.<br />

It has been recognized that the human sense of<br />

hearing relies on an active nonlinear process boosting<br />

vibrations within the cochlea [1], i.e. the inner ear organ<br />

responsible for the coding of auditory signals into patterns<br />

of neural activity. Spontaneous otoacoustic emissions,<br />

i.e. sounds emanating from the ear canal even<br />

in the absence of any external auditory stimulus, constitute<br />

a striking manifestation of this active amplifier.<br />

As of today, its exact biophysical implementation, however,<br />

remains elusive.<br />

Two processes on a cellular scale have been suggested<br />

to play the key role in auditory amplification [2]. On<br />

the one hand, there is the ability of outer hair cells to<br />

undergo length changes in response to modulations of<br />

their transmembrane potential (electromotility). On the<br />

other hand, hair bundles, which also constitute the universal<br />

mechano-transducers in the inner ear, can generate<br />

active forces and even perform spontaneous oscillations<br />

(hair-bundle motility).<br />

The hair-bundle amplifier. The hair bundle is a tuft<br />

of a few tens to a few hundreds stiff finger-like protrusions,<br />

termed stereocilia, emanating from the surface<br />

of specialized sensory hair cells. Upon deflection,<br />

minute geometric rearrangements within the hair<br />

bundle lead to the opening and closing of mechanically<br />

gated ion channels. In this way, the hair bundle<br />

transduces mechanical stimuli (deflections) into electrical<br />

signals (ionic currents).<br />

Next to operating as mere transducers, hair bundles<br />

from the bullfrog’s sacculus have been shown to exhibit<br />

many features reminiscent of the auditory amplifier.<br />

Even in the absence of external stimulation,<br />

hair bundles can perform noisy spontaneous oscillations<br />

[3]. The forces necessary for these oscillations<br />

to occur are produced by calcium-regulated molecular<br />

motors, which operate on the inside of stereocilia. Most<br />

importantly, hair bundles can amplify weak periodic<br />

stimuli in a frequency-dependent manner [4]. In particular,<br />

for intermediate driving amplitudes, a nonlinear<br />

decay of sensitivity is observed, similar to the one<br />

characteristic for cochlear responses [4].<br />

However, noise limits the extent of amplification a single<br />

hair bundle can achieve [5]. Noise stems from<br />

thermal interactions with the bathing fluid, stochastic<br />

opening of the mechanically gated ion channels, and a<br />

fluctuating component of force production by molecular<br />

motors. The operation of a single hair bundle therefore<br />

does not suffice to quantitatively account for the<br />

operation of the whole cochlea.<br />

Coupled hair bundles. Hair bundles in vivo are often<br />

found to be attached to overlying elastic structures,<br />

such as tectorial or otolithic membranes. This suggests<br />

the possibility that coupling of hair bundles plays a role<br />

to enhance the properties of hair-bundle mediated amplification.<br />

A<br />

X 1<br />

F<br />

EXT<br />

-F<br />

1<br />

K K<br />

X X 2<br />

F<br />

EXT<br />

F<br />

K<br />

-F 2<br />

F EXT<br />

X<br />

∆<br />

Real-time<br />

simulation<br />

Figure 1: Coupling a hair bundle to two cyber clones by dynamic<br />

force clamp. (A) Schematic representation of a system of three coupled<br />

hair bundles. A hair bundle (blue) is connected to one neighbor<br />

on each side (orange and red) by identical springs. Relative movements<br />

of the hair bundles induce coupling forces. (B) Experimental<br />

realization. A single hair bundle is monitored. Two cyber clones,<br />

substituting the two flanking hair bundles in (A), are simulated on<br />

the computer. In real-time coupling forces and possibly also external<br />

periodic forces are computed and exerted by means of a glass fiber<br />

that was attached to the hair bundle’s tip. We adjusted cyber-clone<br />

parameters such that our stochastic simulation would mimic the dynamics<br />

of the hair bundle used during the experiment, i.e. in particular<br />

its frequency, amplitude and quality of oscillation. Adopted<br />

from [9].<br />

Contributions of our group. In earlier studies, we approached<br />

this hypothesis from a theoretical point of<br />

view. On the basis of an existing biophysical description<br />

of stochastic hair-bundle dynamics [5], we investigated<br />

the effect of elastic coupling [6]. In our simulations,<br />

we found that elastic coupling could induce synchronization<br />

among hair bundles and lead to an effective<br />

noise reduction. The latter manifested itself in an<br />

increased phase coherence of spontaneous oscillations<br />

and an enhancement of nonlinear amplification. In particular,<br />

we observed a sharpend frequency tuning and<br />

a pronounced increase in sensitivity to weak amplitude<br />

stimulation. An analysis of the response characteristics<br />

of a generic noisy oscillator helped to further understand<br />

the detrimental effect of noise in this particular<br />

context [7, 8].<br />

56 Selection of Research Results<br />

B

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