Spontaneous otoacoustic emissions (SOAEs) are a signature of cochlear amplification, a process associated with outer hair cell (OHC) function and required for the sensitivity and frequency selectivity of cochlear responses. Although normal mice rarely exhibit these signals, those with mutations that influence the structure of the tectorial membrane (TM) show a greater incidence of these phenomena. In this report, we study mouse models with mutations affecting the striated-sheet matrix that forms the body of this accessory structure. In addition to CEACAM16, the matrix is composed of both α- and β-tectorin (TECTA and TECTB respectively) and these latter two noncollagenous proteins are the focus of this study. Of all the mutants tested to date, mice heterozygous (het) for a missense mutation (c.5609A>G, p.Tyr1870Cys) in Tecta (TectaY1870C/+ mice) are prolific emitters with an average of ∼7 SOAEs per cochlea, which is higher than in the very few normal mice with SOAEs where the average is 2-3 per cochlea. A small number of homozygous Tectb−/- mice lacking TECTB are also emitters, but they produce only one SOAE in any given ear. Although both mouse mutants have hearing loss, SOAE frequencies coincide with frequency regions where some degree of amplification is retained. The larger number of SOAEs in TectaY1870C/+ mice appears to correlate with an increase in porosity (1), which controls the spread of excitation of tectorial membrane traveling waves. Sellon and colleagues reported that this change in the material properties of the TM was associated with the larger size of nanoscale pores linked to the Y1870C missense mutation in TECTA. In mice lacking Tectb, where porosity is wild-type like, the number of SOAEs per cochlea is small and only a few of these animals present with this phenomenon. Characterization of traveling-wave properties in other emitting TM mutants will be required to know if the correlation between increased porosity and increased numbers of SOAEs reliably causes the change in phenotype.

1.
Sellon
J
,
Ghaffari
R
,
Farrahi
S
,
Richardson
G
, &
Freeman
D
(
2014
)
Porosity controls spread of excitation in tectorial membrane traveling waves
.
Biophysical J.
106
:
1406
1413
.
2.
Dallos
P
&
Fakler
B
(
2002
)
Prestin, a new type of motor protein
.
Nat Rev Mol Cell Biol
3
(
2
):
104
111
.
3.
Hudspeth
AJ
(
2014
)
Integrating the active process of hair cells with cochlear function
.
Nat Rev Neurosci
15
(
9
):
600
614
.
4.
Legan
PK
, et al. (
2014
)
Three deaf mice: mouse models for TECTA-based human hereditary deafness reveal domain-specific structural phenotypes in the tectorial membrane
.
Hum Mol Genet
23
(
10
):
2551
2568
.
5.
Cheatham
MA
, et al. (
2014
)
Loss of the tectorial membrane protein CEACAM16 enhances spontaneous, stimulus-frequency, and transiently evoked otoacoustic emissions
.
J Neurosci
34
(
31
):
10325
10338
.
6.
Rau
A
,
Legan
PK
, &
Richardson
GP
(
1999
)
Tectorin mRNA expression is spatially and temporally restricted during mouse inner ear development
.
J Comp Neurol
405
(
2
):
271
280
.
7.
Hildebrand
MS
, et al. (
2011
)
DFNA8/12 caused by TECTA mutations is the most identified subtype of nonsyndromic autosomal dominant hearing loss
.
Hum Mutat
32
(
7
):
825
834
.
8.
Russell
IJ
, et al. (
2007
)
Sharpened cochlear tuning in a mouse with a genetically modified tectorial membrane
.
Nat Neurosci
10
(
2
):
215
223
.
9.
Legan
PK
, et al. (
2000
)
A targeted deletion in alpha-tectorin reveals that the tectorial membrane is required for the gain and timing of cochlear feedback
.
Neuron
28
(
1
):
273
285
.
10.
Legan
PK
, et al. (
2005
)
A deafness mutation isolates a second role for the tectorial membrane in hearing
.
Nat Neurosci
8
(
8
):
1035
1042
.
11.
Masaki
K
, et al. (
2010
)
Tectorial membrane material properties in Tecta(Y)(1870C/+) heterozygous mice
.
Biophys J
99
(
10
):
3274
3281
.
12.
Nobili
R
,
Vetesnik
A
,
Turicchia
L
, &
Mammano
F
(
2003
)
Otoacoustic emissions from residual oscillations of the cochlear basilar membrane in a human ear model
.
J Assoc Res Otolaryngol
4
(
4
):
478
494
.
13.
Meaud
J
&
Bowling
T
(
2016
)
Effect of tectorial membrane longitudinal viscoelasticity on cochlear stability
.
Abs Assoc Res Otolaryngol
: p.
433
.
14.
Hubbard
A
(
1993
)
A traveling-wave amplifier model of the cochlea
.
Science
259
:
68
71
.
15.
Békésy
Gv
(
1960
)
Experiments in Hearing
(
McGraw-Hill
,
New York
).
16.
Cheatham
MA
, et al. (
2016
)
Increased Spontaneous Otoacoustic Emissions in Mice with a Detached Tectorial Membrane
.
J Assoc Res Otolaryngol
17
(
2
):
81
88
.
17.
Liberman
MC
,
Zuo
J
, &
Guinan
JJ
, Jr.
(
2004
)
Otoacoustic emissions without somatic motility: can stereocilia mechanics drive the mammalian cochlea?
J. Acoust. Soc. Am.
116
(
3
):
1649
1655
.
18.
Jones
GP
,
Elliott
SJ
,
Russell
IJ
, &
Lukashkin
AN
(
2015
)
Modified protein expression in the tectorial membrane of the cochlea reveals roles for the striated sheet matrix
.
Biophys J
108
(
1
):
203
210
.
19.
Jones
GP
,
Lukashkina
VA
,
Russell
IJ
,
Elliott
SJ
, &
Lukashkin
AN
(
2013
)
Frequency-dependent properties of the tectorial membrane facilitate energy transmission and amplification in the cochlea
.
Biophys J
104
(
6
):
1357
1366
.
This content is only available via PDF.