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Highmultiple spontaneous otoacoustic emissions confirm theory of local tuned oscillators
SpringerPlus volumeÂ 2, ArticleÂ number:Â 135 (2013)
Abstract
Understanding the origin of spontaneous otoacoustic emissions (SOAEs) in mammals has been a challenge for more than three decades. Right from the beginning two mutually exclusive concepts were explored. After 30 years this has now resulted in two well established but incompatible theories, the global standingwave theory and the local oscillator theory. The outcome of this controversy will be important for our understanding of inner ear functions, because local tuned oscillators in the cochlea would indicate the possibility of frequency analysis via local resonance also in mammals. A previously unexploited opportunity to gain further information on this matter lies in the occasional cases of highmultiple SOAEs in human ears, which present a large number of adjacent small frequency intervals. Here, eight healthy ears of four subjects (12 to 32 SOAEs per ear) are compared with individually simulated ears where frequency spacing was randomgenerated by two different techniques. Further, a group of 1000 ears was simulated presenting a mean of 21.3 SOAEs per ear. The simulations indicate that the typical frequency spacing of human SOAEs may be due to random distribution of emitters along the cochlea plus a graded probability of mutual closerange suppression between adjacent emitters. It was found that the distribution of frequency intervals of SOAEs shows no abovechance probability of multiples of the preferred minimum distance (PMD) between SOAEs and that the size of PMD is related to SOAE density. The variation in size between adjacent small intervals is not significantly different in randomgenerated than in measured data. These three results are not in agreement with the global standingwave theory but are in line with the local oscillator theory. In conclusion, the results are consistent with intrinsic tuning of cochlear outer hair cells.
Background
The global standingwave theory (GST) and the local oscillator theory (LOT) of SOAE generation have been extensively described and discussed (recently in: Wit and van Dijk 2012). Here the two concepts are only outlined very briefly. The GST, based on concepts of Kemp (1979), Zweig and Shera (1995), and Shera (2003), proposes coherent reflections of basilar membrane (BM) traveling waves between the stapes and points of slight functional irregularities along the cochlear duct, in analogy with the coherent wave reflections in the optical cavity of a laser. Part of the energy of the BM standing wave vibrates the stapes, and via backward middle ear transmission sound is emitted into the ear canal. The standing wave is sustained by energy input from elements of the cochlear amplifier, in particular the outer hair cells (OHC). The LOT, based on concepts of Johannesma (1980), Bialek and Wit (1984), and van Hengel et al. (1996), proposes that the same elements of the cochlear amplifier behave as local oscillators without being coupled to a standing wave. They transmit part of their vibrational energy directly through cochlea and middle ear to the ear canal.
Of the many qualities of SOAEs that the two theories have to account for, perhaps the most complex and demanding one is the observed spacing order of multiple SOAEs in one ear. Schloth (1983) and Dallmayr (1985, 1986) reported a preferred minimum distance (PMD) between spectrally neighboring SOAEs, which appears as outstanding mode in interval histograms. Later studies replicated this result, and Braun (1997) determined on the basis of a pool of 5245 intervals of human SOAEs that the mean PMD amounts to almost exactly 1 semitone (ST) = 1/12 of an octave (recently reviewed in: Wit and van Dijk, 2012).
According to the GST, â€śthe characteristic SOAE spacing can be traced to the value of the wavelength of the traveling waveâ€ť (Shera 2003, p. 259). In other words, the GST assumes a general standing wave system that selfstabilizes as the best fit to multiple sites of irregularities. By doing so, it amplifies multiple frequencies simultaneously, leading to multiple SOAEs with a characteristic, wavelength dependent, frequency spacing.
Concerning the LOT, van Hengel et al. (1996) used a mathematical cochlear model to test the effect of frequency distance on mutual interaction of SOAEs. They concluded that â€śthe resulting suppression profile leads to natural minimal distances of effective emissions, without any necessity of additional assumptions about the mechanics of the cochleaâ€ť (p. 3570).
Thus, for the LOT the PMD is a shortrange effect of mutual interaction of oscillators, whereas for the GST it is a longrange effect of the wavelength of the BM traveling wave. This conflict has the advantage that it can be resolved by experimental data. The simple empirical question is, can the predicted shortrange and/or longrange effects be observed in measured SOAE data?
Highmultiple SOAEs (>10) in each ear of normal hearing human subjects are occasionally found in large screenings. Indications that SOAE mechanisms might vary according to emission numbers per ear have not been found, and there are no known reasons to expect such a variation. Therefore highmultiple SOAEs can reasonably be regarded as representative for all human SOAEs. Because of their large number of adjacent small SOAE intervals, ears with highmultiple SOAEs provide a unique and previously unexploited opportunity to examine the question of SOAE spacing order, and thus also the question of SOAE generation.
Three groups of results are reported that are not in agreement with the global standingwave theory but are in line with the local oscillator theory of SOAE generation.
Results
Real and simulated data of eight single ears
The histogram of frequency intervals between adjacent SOAEs in eight ears (Figureâ€‰1A) replicates the wellknown mode at 100 Cent = 1 ST. The corresponding histograms of the data from two simulations (Figureâ€‰1B, 1C) also each show a single outstanding mode on the small interval side. For the first simulation (Figureâ€‰1B) the mode is at 75 Cent = 0.75 ST, for the second simulation (Figureâ€‰1C) the mode is at 120 Cent = 1.2 ST.
Considering the single 0.1 ST bins across the three histograms, a conspicuous difference between real and simulated data appears. The real data show a narrow 1bin mode, whereas the simulations show wider modes of 4 and 3 bins. Comparison of the smoothed data (Figureâ€‰1D) shows that the height of the single mode is equally outstanding for the two simulations as for the real data.
Besides the mode at 1 ST there is no further peak in Figureâ€‰1A. In particular, it is important to note that at the multiples of 1 ST, i.e. at 2 ST and 3 ST, distribution density is flat. Further, as shown in Figureâ€‰1D, at 2 ST and above distribution density both for the real and the simulated data generally is almost flat.
The lower half of Figureâ€‰2 shows the spectral SOAE distribution in the two ears of subject BD. The exact size of all small intervals in the 0.5 to 1.5 ST range is marked by triangles above the respective interval. This technique shows that not only the large intervals (>1.5 ST), but also the small ones, vary considerably from one interval to the next.
Five of the eight ears had five or more cases of pairs of adjacent small intervals in the 0.5 to 1.5 ST range, thus enabling the calculation of an informative mean difference (see first five ears in lines 5 & 6 of Tableâ€‰1). In each of the five ears the mean difference was close to 0.25 ST. Across all eight ears, based on all individual pairs of adjacent intervals, it was 0.26 ST (SD = 0.19 ST; range 0.00 ST to 0.84 ST). Because PMD ~ 1 ST, it follows that the mean variation between adjacent small intervals was 0.26 of the PMD.
The upper half of Figureâ€‰2 shows the simulated SOAE distribution for subject BD from the second simulation (Sim2). Both real and simulated data show sections of strongly or moderately fluctuating interval size. The statistics of interval variation is shown in Tableâ€‰1. Statistical tests (lines 8A and 8B of Tableâ€‰1) show that the difference between real and simulated data never reaches the level of significance (P > 0.1 in each test).
Real and simulated data of groups of ears
The interval distribution of 1000 simulated ears with highmultiple SOAEs in Figureâ€‰3A and 3B provides the following information. The distribution is unimodal and heavytailed on the right. Due to the large number of simulations, the curve is smooth, and the type of its shape can easily be discerned. The slope left of the peak, which is formed by the linear decrease in existence probability of intervals, shows the shape of a half parabola. The slope right of the peak, which is only formed by random distribution of SOAEs, shows the shape of an exponential decay.
The real data of both ear groups in Figureâ€‰3A and 3B show a tendency towards a half parabola left of the peak. Right of the peak, the group data in Figureâ€‰3A show a tendency towards an exponential decay, whereas those in Figureâ€‰3B show a nearly linear downward slope from 100 to 180 Cent. This difference between the groups of 8 and 18 ears apparently reflects the difference in SOAE density per ear. In the 8ear group the mean number of emissions per ear was 21, in the 18ear group it was 19.2. The lower emitter density caused a higher probability of intervals > PMD, as seen in Figureâ€‰3B.
The comparison of real data from highmultiple SOAEs with those from low and mediummultiple SOAEs in Figureâ€‰4 shows a conspicuous difference of the location of the peak on the xaxis. Low and mediummultiple SOAEs show a smaller PMD than highmultiple SOAEs. In the interval range between 50 and 170 Cent the former group has a mean interval of 101.7 Cent (SD = 25.8 Cent), and the latter group has a mean interval of 108.3 Cent (SD = 28.5 Cent). For a test on significance of this difference all intervals in the two data pools had to be considered as independent sample points, because due to the wellknown large variation of intervals even within one ear (as in Figureâ€‰2 and Tableâ€‰1) earspecific or subjectspecific clustering of interval size could never be observed. A goodnessoffit KolmogorovSmirnov test (KStest) of the distribution in 10Cent bins (Figureâ€‰4) showed that neither of the two data sets differed significantly from a normal distribution. An Ftest showed that the variances of the two data sets did not differ significantly. Therefore the difference of the mean of the two data sets could be tested by the ttest. The result showed that the difference is significant (P < 0.02). Additionally, the two distributions were compared by a nonparametric test, the KStest. Again the difference was found to be significant (P < 0.02).
Discussion
Random distribution and closerange suppression
The statistical results in Tableâ€‰1 show that the simulated spectral distributions of SOAEs in human ears lead to a variation between small adjacent intervals that does not differ significantly from that in the measured data. This result indicates that two factors may be sufficient to cause the observed phenomena: a stochastic occurrence of emission generators along the cochlea plus a graded probability of closerange suppression of an emitter by an adjacent stronger one. The largescale group simulations (Figureâ€‰3) further show that a simple linear increase of suppression probability for intervals from 95 to 55 Cent would be consistent with the measured data from highmultiple SOAEs. The physical basis of graded closerange suppression may lie in the tissue between OHC, such as the reticular lamina and the tectorial membrane. If the amount of tissue between two vibrating OHC decreases, the probability increases that the oscillator with the higher amplitude suppresses its neighbor.
Both the group of 18 ears with highmultiple and the group of 134 ears with low and mediummultiple SOAEs show the absence of multiples of PMD at 200 and 300 Cent (Figureâ€‰4). A periodicity of increased SOAE probability based on the PMD does not appear. Also this observation indicates that the spectrum of emission generators along the cochlea may primarily be stochastic and may secondarily be shaped by closerange mutual suppression.
The size of the PMD is related to the density of SOAEs in an ear (Figureâ€‰4). For highmultiple SOAEs it amounts to ca 100 Cent, and for low and mediummultiple SOAEs it amounts to ca 90 Cent, a difference that is statistically significant (Results, part 2). The physical basis of this difference may lie in the fact that in an ear with high emitter density there is a relevant probability that an emitter has closerange neighbors on both sides, as shown in Figureâ€‰2. The summation of destructive vibrational interference from two sides is likely to extend the range of effective suppression. In an ear with many emitters, a single emitter would, on average, need more space to survive suppression from neighbors. This variation of the PMD is therefore consistent with the general indication, derived from the group simulations (Figureâ€‰3), that the PMD phenomenon is an effect of graded probability of closerange suppression.
Consequences for global standingwave theory (GST)
A central prediction of the GST is that multiple SOAEs in one ear are spaced in relation to the wavelength of a BM standing wave (see Background section). Because multiple SOAEs in one ear usually do not show long chains with similar frequency spacing, an assumption of the GST has been that many SOAEs have â€śdropped outâ€ť from the chain (Shera, 2003). If the â€śdropoutâ€ť hypothesis is correct, spacing statistics should not only show an increased probability of the PMD interval but also of its multiples, such as 2PMD and 3PMD. Talmadge et al. (1993, their Figure Eight) indicated on the basis of data from subject BD that multiples of PMD possibly might have an abovechance probability. Mathematical simulations of the GST showed that distribution modes at multiples of the PMD are an essential and necessary consequence of the GST. If such simulations do not contain a mandatory algorithm for the â€śdropoutâ€ť of SOAEs, effects at PMD multiples can of course not appear (Ku et al. 2008, their Figure TenId and TenIId). If such a â€śdropoutâ€ť algorithm is applied, e.g., by setting a reasonable threshold of sound level for the detection of SOAEs, effects of PMD multiples become quite conspicuous (Ku et al. 2009, their Figure Thirteen a and Thirteen b). Here, in one GST simulated ear, two cases of 2PMD, three cases of 3PMD, and one case of 6PMD appear.
In an investigation of several other questions, Braun (1997) reported the size distribution of 5245 monaural intervals in the 0â€“800 Cent range. He observed that multiples of PMD had no abovechance probability and pointed out the consequences for concepts that postulated the opposite. Shera (2003, section VIIE, third paragraph) focused on the fact that the observations of Braun (1997) were based on all possible intervals per ear (allorder intervals), not only on intervals between adjacent SOAEs (firstorder intervals). He then argued that summations of small intervals to larger ones would lead to broad peaks in the distribution histogram at the locations of PMD multiples, which therefore possibly would disappear in the noise floor. In other words, he asserted that multiples of PMD would have existed, but were disguised by the technique of analyzing allorder intervals (Shera 2003, section VIIE, last sentence of third paragraph). Thus, Shera was fully aware of the fact that the GST, by definition, predicted a multimodal distribution of SOAE intervals. The present results (Figureâ€‰4), which are exclusively based on intervals between adjacent SOAEs (firstorder intervals), again show the absence of the predicted multimodal distribution and therefore disprove a central component of the GST.
The finding that the mean variation between adjacent small intervals (0.5 to 1.5 ST) was not significantly different between real and random generated SOAE data (Tableâ€‰1) also indicates that the spectral spacing of emissions may be stochastic and unrelated to the wavelength of cochlear waves. Clearly, if the regular spacing of the excursion peaks of a BM standing wave influenced the spectral distribution of SOAEs in one ear, SOAE spacing necessarily would show some degree of regularity in the variation between adjacent small intervals. The consistency of the measured variation with that in the random generated simulations indicates the absence of such regularity and thus the absence of a relation between SOAE spacing and BM standing waves.
The relation between size of PMD and number of emissions per ear (Figureâ€‰4) has not been reported before. Also this finding is inconsistent with the GST. The â€śdropoutâ€ť hypothesis of the GST (see above) can explain that the number of emissions per ear varies according to the number of â€śdropoutsâ€ť from the quasiperiodic chain of emissions that is determined by the wavelength of a BM standing wave. The number of â€śdropoutsâ€ť, however, cannot have a significant causal relation to the wavelength of the standing wave, and thus to the size of the PMD. The wavelength of BM traveling waves is determined by macromechanical parameters of the BM and the cochlea, and the existence or absence of SOAEs cannot significantly be related to these parameters, which is confirmed by the common observation that many healthy and functionally completely normal human ears show no SOAEs at all.
Consequences for local oscillator theory (LOT)
Early observations that SOAEs interact with each other (Burns et al. 1984) indicated that emission generators, i.e., local oscillators, mutually interact within the cochlea (e.g., van Hengel et al. 1996; Wit and van Dijk 2012). Of particular interest were neighboring oscillators, because the amplitude of radiated waves usually decreases with distance. Because two SOAEs in one ear extremely rarely have an interval below 0.5 ST, it has often been assumed that this fact is due to mutual suppression.
Here, for single ears two types of closerange suppression were simulated, a total suppression beyond a simple lowside limit (Sim1), and a progressive suppression over a lowside range (Sim2). The two simulations have shown that both types of suppression lead to a strong distribution peak slightly above the limitation (Figureâ€‰1). The group simulation of 1000 ears showed that a linear increase of suppression probability with decreasing interemitter distance almost perfectly mirrored the real data (Figureâ€‰3). All simulations taken together indicate that stochastic spacing of emitters plus closerang suppression alone can explain the PMD phenomenon.
The observation that the PMD slightly varies with SOAE frequency (Methods, part 5) would be compatible both with the GST and the LOT. The anatomy of the cochlear partition varies along the cochlea, which has an effect on the wavelength of traveling waves (relevant for GST) as well as on interemitter tissue and thus interemitter suppression (relevant for LOT). The relation between emission number per ear and size of PMD (Figureâ€‰4), however, is in conflict with the GST (Discussion, part 2), whereas it can be explained by the LOT (Discussion, part 1).
Relation to other data and to cochlear mechanics
SOAE frequencies are mirrored by frequencies of peaks in any spectrum of evoked OAEs, and also by frequencies of best sensitivity in the microspectrum of hearing threshold (Zwicker and Schloth 1984; Talmadge et al. 1998). However, the reverse is not true. Many peaks in the spectra of evoked OAEs and hearing sensitivity are not mirrored by SOAEs. It is still unknown if this discrepancy is due to measurement limitations in recording lowlevel SOAEs or due to an additional mechanism that is related to evoked OAEs and threshold microstructure but not to SOAEs.
Numerous empirical studies reported evidence that OAE related intracochlear backward transmission toward the stapes occurs via fast compressional sound waves, and not via slow backward traveling waves (Ren 2004; Ren et al. 2006; Ruggero 2004; Siegel et al. 2005, He et al. 2008; He et al. 2010). These results are consistent with the LOT, because the LOT does not require a backward traveling wave, and local oscillatorgenerated emissions can reach the stapes through the cochlear fluids. However, the intracochlear reflection at the stapes cannot result in standing waves of the basilar membrane, if there is no reverse traveling wave. Therefore, the above referenced data do not support the GST.
Several other statistical properties of human SOAEs are not compatible with the determination of SOAE frequencies by cochlear macromechanics, as suggested by the GST. Abovechance binaural mirroring (Braun 1998), abovechance binaural (but not monaural) frequency ratios that presumably play a role in pitch extraction in the auditory midbrain (Braun 2000), and the bimodal frequency distribution around the two peaks at 1.5 kHz and 3 kHz (Braun 2006), each, and independently, indicate efferent neural influence on the probability of local cochlear oscillations, because alternative mechanisms could neither be found nor be suggested.
Zheng et al. (2011) reported a frequency specific ringing of the BM that indicates local tuning within the organ of Corti. These findings, in combination with the present ones, suggest intrinsic tuning of cochlear outer hair cells (Canlon et al. 1988; Brundin et al. 1989a and Brundin et al. 1989b; Brundin and Russell, 1994). Additionally, because the barn owl presents SOAEs as high in the frequency range as humans (Taschenberger and Manley, 1997) without motility of hair cell bodies, intrinsic tuning of hair bundle motility (Nam and Fettiplace, 2008) should be considered as a candidate for the origin of SOAEs also in mammals.
Medical applications
Three decades after their discovery, otoacoustic emissions (OAEs) are today widely used in medical diagnosis. However, uncertainty as to their physiological causes severely impedes further applications. Currently, the main medical application of OAEs is checking the status of hearing. One can expect, however, a much larger potential of OAEs in the context of highly complex disorders, such as tinnitus (Geven et al. 2012) or MĂ©niĂ¨reâ€™s disease (Avan et al. 2011). For example, diagnostic tests on tinnitus or MĂ©niĂ¨reâ€™s disease that use OAEs in combination with macromechanical manipulations of the cochlea (Nubel et al. 1995), such as lowfrequency biasing of BM position (Scholz et al. 1999), are likely to benefit from knowledge of OAE physiology.
Conclusions
The distribution of frequency intervals of human spontaneous otoacoustic emissions (SOAEs) shows no abovechance probability of multiples of the preferred minimum distance (PMD) between SOAEs. The size of PMD is related to SOAE density. The variation in size between adjacent small intervals is not significantly different in randomgenerated than in measured data. Each of these three results is contrary to the predictions of the global standingwave theory (GST) but in agreement with the local oscillator theory (LOT) of SOAE generation. Overall, the results are consistent with intrinsic tuning of cochlear outer hair cells (OHC) as a key functional element in the frequency analysis of the inner ear.
Methods
Primary data set
There are two preconditions for the collection of a relevant number of highmultiple SOAEs: the screening of many subjects (>100), and the best possible techniques for recording and signal analysis. Several survey studies were carried out in the early 1990s, when the principal aim was to establish prevalence conditions of SOAEs in humans. The ones that collected the largest numbers of SOAEs were those of Russell (1992) and Talmadge et al. (1993). These authors applied similar advanced techniques, which is reflected by the similar statistical results that they reported. In both studies the best available methods of acoustic recording and data extraction, which have not further developed since then, were applied. The raw data from these two surveys were reused in many later investigations (for a recent example: Wit and van Dijk 2012, Figure Ten ad and acknowledgments). Here, from each of these two studies the data from the two subjects presenting the highest numbers of SOAEs were investigated by newly developed techniques. The four subjects, BD, JK, DZF7A, and MZF13A were all adult females, healthy, and normal hearing. At their ages of 34, 20, 21, and 21 they presented 57, 44, 35, and 32 SOAEs, respectively.
For each of the eight ears, all frequency intervals between adjacent SOAEs were calculated into values of the logarithmic Cent scale [100 Cent = 1 semitone (ST); 12 ST = 1 octave]. Then the intervals of the 168 SOAEs of the eight ears were pooled and their size distribution was calculated for bins of 10 Cent = 0.1 ST and displayed in a histogram.
First simulation of eight single ears
The possible effects of mutual suppression of adjacent SOAEs on spacing order were investigated by using two different simulations. The first simulation applied a simple lowside limit of interval size for each ear, i.e., intervals that were smaller than a given value were excluded. The second simulation applied a progressive range of existence probability on the lowend side of interval size, i.e., the probability of small intervals decreased progressively toward the given smallest interval. Both simulations had in common that each of the eight real SOAE distributions per ear was mirrored by an individually simulated, randomgenerated distribution.
For the simulations the RANDBETWEEN function of the software package Microsoft Excel (version 9.0.3821 SR1 from 2000) was used. This function generates, for each round of application, one random selected integer from within a given range between two integers, such that each integer within the range occurs with equal probability. The randomness is algorithm based and its quality is generally considered as fully sufficient for medium size simulations as the present ones. Indications to the contrary have not become known over the period of twelve years that this software package has been in use worldwide (internet scans). Here, the function was used to generate simulated SOAE frequencies, randomly with equal occurrence probability, from within the SOAE frequency range of the real ear. For example, for the simulation of the right ear of subject BD, 32 SOAE frequencies were generated from within the range of 629 Hz to 6140 Hz.
In the first simulation, the empirically observed general lowside limit of ~ 0.5 ST for intervals between adjacent SOAEs (Braun 1997) was simulated as follows. First, the smallest interval in the real ear was determined, e.g., 0.67 ST in the right ear of subject BD. Second, from this value a lowside limit for the simulated intervals of this ear was derived by using the nearest lowside multiple of 0.10 ST, such as 0.50 ST, 0.60 ST, 0.70 ST, etc., as the exclusion criterion. Thus for this ear the lowside limit was 0.60 ST, leading to a rejection of intervals < 0.61 ST. Third, after random generation, the higher SOAE frequency of all pairs whose interval fell into the rejection zone, i.e. was too small, was deleted and replaced by a new randomgenerated SOAE frequency. Fourth, the replacement procedure was repeated until the lowside criterion was satisfied for all intervals of this ear, e.g., no interval was < 0.61 ST.
For ears BDR, JKL, DZF7AR, and MZF13AR the exclusion criterion was < 0.61 ST. For the other four ears it was < 0.51 ST. When determining the exclusion criteria, the extremely small interval of 0.11 ST in MZF13AR was neglected as an extreme outlier and the equally untypical interval of 0.36 ST in DZF7AL was taken to justify the lower of the two typical limits, i.e. < 0.51 ST. Separately for the two rounds of simulations, the interval distribution of the 168 simulated SOAEs of the eight simulated ears was analyzed in the same way as for real SOAEs.
Second simulation of eight single ears
In the second simulation, the results from the first simulation were reprocessed in order to take into account the gradual decrease of intervals between 0.9 ST and 0.5 ST in the real data. The progressive decrease of intervals towards the smallest one was simulated by using several limits at steps of 0.1 ST, with each limit mirroring the real data. For example, in the right ear of subject BD the four 0.1 ST bins between 0.5 ST and 0.9 ST show 0, 4, 0, and 5 cases, respectively. These numbers were taken as maximum in the corresponding bins in the second simulation, and the same deletion and replacement procedure as in the first simulation was applied until all maximumperbin conditions were satisfied. It should be noted that the number of simulated intervals could in the end be below the given maximum of some bins, because each deletion and replacement of a randomgenerated SOAE frequency leads to a reordering of the complete chain of SOAE frequencies per ear. Further, it was not possible to add an interval to a bin, because random generation does not permit this. Therefore, the data of the second simulation unavoidably showed slightly less small intervals below 0.9 ST than the real data.
Possible longrange effects in SOAE spacing order were investigated by computing the size variation between adjacent small intervals. Because PMD amounts to almost exactly 1 ST with a range from ~ 0.5 ST to ~ 1.5 ST at the base of the distribution mode (Braun 1993 and Braun 1997), all intervals between 0.5 and 1.5 ST entered into the analysis. The interval size variation was analyzed statistically, separately per ear and also for the total of all eight ears, by comparing real and simulated data. Goodnessoffit KolmogorovSmirnov tests (KStest) showed that the data sets are consistent with a normal distribution and Ftests showed that the variances do not differ significantly. Therefore application of the ttest was appropriate. Additionally, the data set of the total of the eight ears was compared with each the two data sets of the total of the eight simulated ears by a nonparametric test, the KStest.
Simulation of a group of 1000 ears
Additionally to the simulation of single ears, the effect of decreasing existence probability of small intervals with decreasing interval size was also simulated for highmultiple SOAEs in general. Van Hengel and Maat (1993, their Figure Four) showed in a simple mechanical model that the probability of an emission being suppressed by an adjacent stronger one increases with decrease of interval size. Here, 1000 ears with a possible maximum of 32 SOAEs each, in the frequency range of the right ear of subject BD (629 Hz to 6140 Hz), were simulated by random generation (as described above) and a simple linear decrease of existence probability of intervals from 100 to 50 Cent.
The existence probability decreased in five steps of 20%. Above 95 Cent intervals had an existence probability of 100%, for the range of 95 to 86 Cent it was 80%, for 85 to 76 Cent 60%, for 75 to 66 Cent 40%, for 65 to 56 Cent 20%, and below 56 Cent 0%. The 1000 ears were simulated in five blocks of 200. In the first block no intervals < 96 Cent were permitted, in the second no < 86, in the third no < 76, in the fourth no < 66, and in the fifth no < 56 Cent. For each SOAE of each ear a separate random generation was carried out. First, 32 SOAEs in the given range, 629 Hz to 6140 Hz, were generated. Second, the lowest number of the 32 was selected as the first SOAE, and all other numbers were discarded. Third, 31 SOAEs in an adapted new range, between the first SOAE plus permitted minimum distance (in Hz) and 6140 Hz, were generated. Fourth, the lowest number of the 31 was selected as second SOAE, and again all other numbers were discarded. Fifth and following, adaptation of range, random generation, and selection of lowest number was repeated until the adapted range was smaller than the permitted minimum distance, such that no further random generation was possible.
Due to the random character of the procedure, the resulting number of SOAEs per ear always was below 32. Across the 1000 simulated ears the mean number of SOAEs per ear was 21.310 and the total number of SOAEs was 21310. Therefore the simulation provided no optimum representation of the right ear of subject BD. But it provided an adequate representation of the group of eight ears with highmultiple SOAEs, as analyzed above, because the mean number of SOAEs per ear in this group was 21. The simulated ears presented 20310 intervals between adjacent SOAEs, which were plotted in a distribution diagram in contrast to the group data of the eight real ears as analyzed above. In a further diagram they were also plotted in contrast to the group data of the 18 ears from the two surveys of Russell (1992) and Talmadge et al. (1993) that presented â‰Ą15 SOAEs per ear with a group mean of 19.2 SOAEs per ear.
Empirical data of highmultiple vs. low and mediummultiple SOAEs
For a comparison of the data from highmultiple SOAEs with those from low and mediummultiple SOAEs, all ears from the two surveys of Russell (1992) and Talmadge et al. (1993) that presented <10 SOAEs per ear were considered. Because van Hengel et al. (1996, their Figure Four) and Shera (2003, his Figure Three), by using data from Talmadge et al. (1993), had shown that the PMD, as an octave fraction, slightly decreased with the increase of the mean frequency of SOAE pairs, it was necessary to compare data sets with a similar overall mean of SOAE frequency. For the abovedescribed group with â‰Ą15 SOAEs per ear the overall mean was 2144 Hz. For the above described group with <10 SOAEs per ear it was 2320 Hz. The latter group therefore was reduced in order to obtain two groups with matching overall mean SOAE frequency. For this purpose the mean SOAE frequency for each single ear in the latter group was determined. Then the ear with the highest mean was iteratively deleted from the group until the groupâ€™s overall mean was within Â± 0.005 of the mean of the other group. After completion of the procedure the overall mean of the reduced group with <10 SOAEs per ear was 2151 Hz, and the reduced groupâ€™s 134 ears presented 648 SOAEs, the mean being 4.8 SOAEs per ear.
Abbreviations
 BM:

Basilar membrane
 GST:

Global standingwave theory
 LOT:

Local oscillator theory
 OAE:

Otoacoustic emission
 OHC:

Outer hair cell
 PMD:

Preferred minimum distance
 SOAE:

Spontaneous otoacoustic emission
 ST:

Semitone.
References
Avan P, Giraudet F, Chauveau B, Gilain L, Mom T: Unstable distortionproduct otoacoustic emission phase in MeniĂ¨re's disease. Hear Res 2011, 277: 8895. 10.1016/j.heares.2011.03.006
Bialek W, Wit HP: Quantum limits to oscillator stability: theory and experiments on acoustic emissions from the human ear. Phys Lett 1984, 104A: 173178.
Braun M: Comment on: Talmadge CL, Tubis A, On modeling the connection between spontaneous and evoked otoacoustic emissions. In Biophysics of Hair Cell Sensory Systems. Edited by: Duifhuis H, Horst JW, van Dijk P, van Netten SM. World Scientific, Singapore; 1993:3132.
Braun M: Frequency spacing of multiple spontaneous otoacoustic emissions shows relation to critical bands: a largescale cumulative study. Hear Res 1997, 114: 197203. 10.1016/S03785955(97)001603
Braun M: Accurate binaural mirroring of spontaneous otoacoustic emissions suggests influence of timelocking in medial efferents. Hear Res 1998, 118: 129138. 10.1016/S03785955(98)000288
Braun M: Inferior colliculus as candidate for pitch extraction: multiple support from statistics of bilateral spontaneous otoacoustic emissions. Hear Res 2000, 145: 130140. 10.1016/S03785955(00)000836
Braun M: A retrospective study of the spectral probability of spontaneous otoacoustic emissions: rise of octave shifted second mode after infancy. Hear Res 2006, 215: 3946. 10.1016/j.heares.2006.03.008
Brundin L, Flock A, Canlon B: Tuned motile responses of isolated cochlear outer hair cells. Acta Otolaryngol Suppl 1989, 467: 229234.
Brundin L, Flock A, Canlon B: Soundinduced motility of isolated cochlear outer hair cells is frequencyspecific. Nature 1989, 342: 814816. 10.1038/342814a0
Brundin L, Russell I: Tuned phasic and tonic motile responses of isolated outer hair cells to direct mechanical stimulation of the cell body. Hear Res 1994, 73: 3545. 10.1016/03785955(94)902801
Burns EM, Strickland EA, Tubis A, Jones K: Interactions among spontaneous otoacoustic emissions. I. Distortion products and linked emissions. Hear Res 1984, 16: 271278. 10.1016/03785955(84)901163
Canlon B, Brundin L, Flock A: Acoustic stimulation causes tonotopic alterations in the length of isolated outer hair cells from guinea pig hearing organ. Proc Natl Acad Sci USA 1988, 85: 70337035. 10.1073/pnas.85.18.7033
Dallmayr C: Spontane otoakustische Emissionen: Statistik und Reaktion auf akustische StĂ¶rtĂ¶ne. Acustica 1985, 59: 6775.
Dallmayr C: StationĂ¤re und dynamische Eigenschaften spontaner und simultan evozierter otoakustischer Emissionen. Technische UniversitĂ¤t MĂĽnchen, Dissertation; 1986.
Geven LI, Wit HP, de Kleine E, van Dijk P: Wavelet analysis demonstrates no abnormality in contralateral suppression of otoacoustic emissions in tinnitus patients. Hear Res 2012, 286: 3040. 10.1016/j.heares.2012.02.008
He W, Fridberger A, Porsov E, Grosh K, Ren T: Reverse wave propagation in the cochlea. Proc Natl Acad Sci USA 2008, 105: 27292733. 10.1073/pnas.0708103105
He W, Fridberger A, Porsov E, Ren T: Fast reverse propagation of sound in the living cochlea. Biophys J 2010, 98: 24972505. 10.1016/j.bpj.2010.03.003
Johannesma PIM: Narrow band filters and active resonators. Comments on papers by DT Kemp and RA Chum, and HP Wit and RJ Ritsma. In Psychophysical, Physiological, and Behavioural Studies in Hearing. Edited by: van den Brink G, Bilsen FA. Delft University Press, Delft; 1980:6263.
Kemp DT: The evoked cochlear mechanical response and the auditory microstructure  evidence for a new element in cochlear mechanics. Scand Audiol Suppl 1979, 9: 3547.
Ku EM, Elliott SJ, Lineton B: Statistics of instabilities in a state space model of the human cochlea. J Acoust Soc Am 2008, 124: 10681079. 10.1121/1.2939133
Ku EM, Elliott SJ, Lineton B: Limit cycle oscillations in a nonlinear state space model of the human cochlea. J Acoust Soc Am 2009, 126: 739750. 10.1121/1.3158861
Nam JH, Fettiplace R: Theoretical conditions for highfrequency hair bundle oscillations in auditory hair cells. Biophys J 2008, 95: 49484962. 10.1529/biophysj.108.138560
Nubel K, Kabudwand E, Scholz G, Mrowinski D: Diagnosis of endolymphatic hydrops with low tone masked otoacoustic emissions. Laryngorhinootologie 1995, 74: 651656. 10.1055/s2007997819
Ren T: Reverse propagation of sound in the gerbil cochlea. Nat Neurosci 2004, 7: 333334. 10.1038/nn1216
Ren T, He W, Scott M, Nuttall AL: Group delay of acoustic emissions in the ear. J Neurophysiol 2006, 96: 27852791. 10.1152/jn.00374.2006
Ruggero MA: Comparison of group delays of 2f1â€“f2 distortion product otoacoustic emissions and cochlear travel times. Acoust Res Lett Online 2004, 5: 143147. 10.1121/1.1771711
Russell AF: Heritability of Spontaneous Otoacoustic Emissions. Dissertation, University of Illinois, UrbanaChampaign, IL, University Microfilms International, Ann Arbor, MI; 1992.
Schloth E: Relation between spectral composition of spontaneous otoacoustic emissions and finestructure of threshold in quiet. Acustica 1983, 53: 250256.
Scholz G, Hirschfelder A, Marquardt T, Hensel J, Mrowinski D: Lowfrequency modulation of the 2f1f2 distortion product otoacoustic emissions in the human ear. Hear Res 1999, 130: 189196. 10.1016/S03785955(99)000106
Shera CA: Mammalian spontaneous otoacoustic emissions are amplitudestabilized cochlear standing waves. J Acoust Soc Am 2003, 114: 244262. 10.1121/1.1575750
Siegel JH, Cerka AJ, RecioSpinoso A, Temchin AN, van Dijk P, Ruggero MA: Delays of stimulusfrequency otoacoustic emissions and cochlear vibrations contradict the theory of coherent reflection filtering. J Acoust Soc Am 2005, 118: 24342443. 10.1121/1.2005867
Talmadge CL, Long GR, Murphy WJ, Tubis A: New offline method for detecting spontaneous otoacoustic emissions in human subjects. Hear Res 1993, 71: 170182. 10.1016/03785955(93)90032V
Talmadge CL, Tubis A, Long GR, Piskorski P: Modeling otoacoustic emission and hearing threshold fine structures. J Acoust Soc Am 1998, 104: 15171543. 10.1121/1.424364
Taschenberger G, Manley GA: Spontaneous otoacoustic emissions in the barn owl. Hear Res 1997, 110: 6176. 10.1016/S03785955(97)000701
Van Hengel PWJ, Maat A: Periodicity in frequency spectra of click evoked and spontaneous OAEs: theory meets experiment. In Biophysics of Hair Cell Sensory Systems. Edited by: Duifhuis H, Horst JW, van Dijk P, van Netten SM. World Scientific, Singapore; 1993:4753.
Van Hengel PWJ, Duifhuis H, van den Raadt MPMG: Spatial periodicity in the cochlea: the result of interaction of spontaneous emissions? J Acoust Soc Am 1996, 99: 35663571. 10.1121/1.414955
Wit HP, van Dijk P: Are human spontaneous otoacoustic emissions generated by a chain of coupled nonlinear oscillators? J Acoust Soc Am 2012, 132: 918926. 10.1121/1.4730886
Zheng J, Ramamoorthy S, Ren T, He W, Zha D, Chen F, Magnusson A, Nuttall AL, Fridberger A: Persistence of past stimulations: storing sounds within the inner ear. Biophys J 2011, 100: 16271634. 10.1016/j.bpj.2011.02.025
Zweig G, Shera CA: The origin of periodicity in the spectrum of evoked otoacoustic emissions. J Acoust Soc Am 1995, 98: 20182047. 10.1121/1.413320
Zwicker E, Schloth E: Interrelation of different otoacoustic emissions. J Acoust Soc Am 1984, 75: 11481154. 10.1121/1.390763
Acknowledgments
I thank Carrick L. Talmadge for making available the SOAE raw data of his research group.
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Braun, M. Highmultiple spontaneous otoacoustic emissions confirm theory of local tuned oscillators. SpringerPlus 2, 135 (2013). https://doi.org/10.1186/219318012135
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DOI: https://doi.org/10.1186/219318012135
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