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JARO: Journal of the Association for Research in Otolaryngology logoLink to JARO: Journal of the Association for Research in Otolaryngology
. 2018 Jun 4;19(5):571–587. doi: 10.1007/s10162-018-0678-4

Psychophysical Tuning Curves as a Correlate of Electrode Position in Cochlear Implant Listeners

Lindsay DeVries 1,, Julie G Arenberg 1
PMCID: PMC6226415  PMID: 29869047

Abstract

Speech understanding abilities vary widely among cochlear implant (CI) listeners. A potential source of this variability is the electrode-neuron interface (ENI), which includes peripheral factors such as electrode position and integrity of remaining spiral ganglion neurons. Suboptimal positioning of the electrode array has been associated with poorer speech outcomes; however, postoperative computerized tomography (CT) scans are often not available to clinicians. CT-estimated electrode-to-modiolus distance (distance from the inner wall of the cochlea) has been shown to account for some variability in behavioral thresholds. However, psychophysical tuning curves (PTCs) may provide additional insight into site-specific variation in channel interaction. Thirteen unilaterally implanted adults with the Advanced Bionics HiRes90K device participated. Behavioral thresholds and PTCs were collected for all available electrodes with steered quadrupolar (sQP) configuration, using a modified threshold sweep procedure, used in Bierer et al. (Trends Hear 19:1–12, 2015). PTC bandwidths were quantified to characterize channel interaction across the electrode array, and tip shifts were assessed to identify possible contributions of neural dead regions. Broader PTC bandwidths were correlated with electrodes farther from the modiolus, but not correlated with sQP threshold, though a trend was observed. Both measures were affected by scalar location, and PTC tip shifts were observed for electrodes farther from the modiolus. sQP threshold was the only variable correlated with word recognition. These results suggest PTCs may be used as a site-specific measure of channel interaction that correlates with electrode position in some CI listeners.

Keywords: psychophysical tuning curves, cochlear implants, electrode position, imaging, psychophysics

INTRODUCTION

Cochlear implants (CIs) are neural prostheses that provide auditory input to people with severe-to-profound hearing loss. Outcomes are highly variable across listeners; performance on word and sentence tests ranges from 0 to 100 % (Koch et al. 2004; Won et al. 2007; Holden et al. 2013). A potential source of this high variability is the electrode-neuron interface (ENI), which includes peripheral components such as electrode position, bone and tissue growth, and the integrity of remaining spiral ganglion neurons (Bierer 2010; Pfingst et al. 2011; Long et al. 2014). Computational modeling, CT imaging, electrophysiological, and behavioral studies have demonstrated that behavioral thresholds are higher and spatial spread of excitation is broader for electrodes distant from target spiral ganglion neurons, or those that may be near degenerated neurons (Goldwyn et al. 2010; Long et al. 2014; Kalkman et al. 2014; DeVries et al. 2016). Broader spread of excitation increases channel interaction, or overlapping areas of neural activation, which may lead to poorer spectral resolution and decreased word understanding (e.g., Abbas et al. 2004; Hughes and Stille 2008; Jones et al. 2013).

Animal studies have demonstrated that long-term deafness results in smaller evoked potential responses and fewer surviving spiral ganglion neurons (Smith and Simmons 1983; Hall 1990; Shepherd and Javel 1997; Ramekers et al. 2014). Human temporal bone studies have directly measured spiral ganglion survival rates in both non-CI and CI listeners, with rates ranging from 4 to 100 % survival (e.g., Hinojosa and Lindsay 1980; Linthicum et al. 1991; Khan et al. 2005). Others have studied potential indirect measures of neural health in CI listeners, such as behavioral thresholds (Long et al. 2014; Zhou and Pfingst 2016). Despite this, it is not currently possible to directly assess neural health in vivo in CI listeners.

Using CT imaging techniques, one can directly estimate a different component of the ENI—electrode position. CT imaging provides information including, but not limited to electrode-to-modiolus distance, scalar location, insertion angle, and wrapping factor (Verbist et al. 2005; Skinner et al. 2002; Teymouri et al. 2011; Holden et al. 2013). By quantifying this aspect of the ENI, deductive inferences may be made about neural status local to each electrode. Thus, disambiguating different aspects of the ENI may provide important information about the functional capacity of a given implant channel, which may have a direct effect on success with the device.

While CT imaging may offer insight into the ENI, this technique has notable disadvantages, such as high costs, exposing patients to radiation, no direct information about neural status, and limited availability. Therefore, an alternative method to measure electrode position is needed. A recent study in our laboratory compared aspects of electrode position to the electrically evoked compound action potential (ECAP); however, in that study, many participants did not have measureable ECAPs, or responses were noisy due to large stimulus artifact (DeVries et al. 2016). Therefore, evaluating a more reliable measure of channel interaction, such as the psychophysical tuning curve (PTC), is warranted.

Bierer and Faulkner (2010) demonstrated that broad PTCs were correlated with higher behavioral thresholds using focused stimulation, such that channels with higher thresholds had broader spatial tuning; these findings echoed those of Nelson et al. (2008) with bipolar stimulation. These studies suggest that focused PTCs may capture site-specific variations in spatial tuning. However, the use of PTCs has not been explored to estimate electrode-to-modiolus distance in CI listeners. Furthermore, PTCs have not been fully characterized across the electrode array, as most studies have examined a small subset of electrodes due to the lengthy testing time required with traditional psychophysical methods (e.g., Nelson et al. 2008, 2011). The present study used a faster method for obtaining focused PTCs based on a Békésy-like sweep procedure recently used for measuring focused thresholds in CI listeners (Bierer et al. 2015).

In broad terms, this study aims to assess (1) the viability of using PTCs as a site-specific measure of channel interaction, (2) if measures of electrode position allow for inferences about neural status, and (3) insight into the identification and assessment of poor ENIs.

Specifically, we quantify the relationship between PTC bandwidths, focused behavioral thresholds, and electrode-to-modiolus distances. We predict that channels with broader PTC bandwidths will have (1) larger electrode-to-modiolus distances, (2) scalar locations outside of scala tympani, and (3) higher focused thresholds. Other comparisons between focused behavioral thresholds, electrode-to-modiolus distance, scalar location, PTC tip location, and word recognition were made.

These findings may help advance understanding of the complexities of the ENI and how site-specific measures of channel interaction relate to word recognition.

METHODS

Subjects

Thirteen adult subjects who were unilaterally implanted after 2001 with Advanced Bionics HiRes90k devices participated (Table 1). Subjects were at least 21 years of age (M = 62.8, SD = 15.3), and eight were males. Two subjects were pre-lingually deafened (diagnosed with severe to profound hearing loss before the age of 4), one was peri-lingually deafened (diagnosed with severe to profound hearing loss at age 4), and the remaining ten were post-lingually deafened. Two subjects were deafened in childhood (S54, age 7, and S46, age 14), but are still considered with the post-lingually deafened subjects as they learned language before they were diagnosed with a severe-to-profound hearing loss. All subjects were fluent English speakers. Each participant provided written consent, and the experiments were conducted in accordance with guidelines set by the University of Washington Human Subjects Division.

TABLE 1.

The demographic information for all 13 subjects including ear implanted, chronological age, age diagnosed with a profound hearing loss, age at implantation, duration of deafness, etiology (if known), electrode array type and electrode spacing, and clinical CNC word score

ID Ear Age Age at profound HL Age implanted Duration of deafness (years) Etiology Electrode array/spacing (mm) CNC word score (%)
S22 R 77 55 66 11 Suspected genetic 1-J Helix/0.85 50
S29 L 86 47 77 30 Noise HiFocus 1 J/1.1 76
S40 L 55 4 50 46 EVA HiFocus 1 J/1.1 20
S42 R 67 50 50 0 Idiopathic HiFocus 1 J Pos./0.9 93
S43 R 71 50 67 17 Noise Mid-Scala/0.85 78
S46 R 66 14 62 48 Unknown HiFocus 1 J/1.1 30
S47 R 68 28 37 9 Unknown Mid-Scala/0.85 83
S49 R 44 1.5 43 41.5 Suspected genetic Mid-Scala/0.85 30
S53 R 54 1 44 43 Meningitis 1-J Helix/0.85 84
S54 L 26 7 23 16 Suspected EVA Mid-Scala/0.85 72
S55 R 63 41 49 8 Suspected genetic HiFocus 1 J/1.1 92
S56 L 72 30 58 28 Idiopathic HiFocus 1 J Pos./0.9 76
S57 R 67 63 65 2 Idiopathic Mid-Scala/0.85 62

CT Imaging

CT scans were performed at the University of Washington Medical Center within the last 3 years. CT scans were analyzed at Washington University in St. Louis, MO. Briefly, ANALYZE software was used to create 3-dimensional image volumes by combining information from each subject’s postoperative scan and a single body donor cochlea (Fig. 1; for details, see Skinner et al. 2002; for verification of the method, see Teymouri et al. 2011). Preoperative CT scans were not available for the subjects participating in the present study; therefore, a scan of the non-implanted ear was used to identify structural anatomy, and this image was co-registered with the image of the implanted ear. Micro CT and orthogonal-plane fluorescence optical sectioning (OPFOS) images from a donor cochlea were used to locate and visualize the non-bony structures. The two CT-estimated metrics used in this study were electrode-to-modiolus distance and scalar location. Electrode-to-modiolus distance refers to the lateral distance (mm) of an electrode from the medial wall of the cochlea. Scalar location denotes the positioning of an electrode in the fluid-filled cochlear compartments: scala tympani (ST), intermediate, and scala vestibuli (SV). Intermediate refers to those electrodes that could not be clearly determined to be in ST or SV.

FIG. 1.

FIG. 1

a Example of one forward (blue) and one reverse (red) sweep for S53, probe 4. The x-axis is masker electrode (apical to basal), and the y-axis is stimulus level (dB rel. to 1 μA). The black triangles represent the mean masker level for each of the cardinal electrodes. b Example PTC for S53, probe 4. The x-axis is masker electrode (apical to basal), and the y-axis is masker level (percent dynamic range). The PTC ERBDR is labeled (black rectangle), and the PTC ERBDR value is marked inside the plot. The PTC tip (filled green circle) and probe electrode (blue arrow) are also labeled

Electrical Stimulation

All stimuli were presented using the Bionic Ear Data Collection System version 1.18.315 (Advanced Bionics, Valencia, CA). For behavioral testing, a custom Matlab (Mathworks, Inc. Natick, MA) script controlled the BEDCS software. Two types of electrode configurations were used in this study: monopolar (MP) and steered quadrupolar (sQP). MP stimulation consists of an active intracochlear electrode and a return extracochlear electrode; the large distance between the source/sink yields a broad electrical field. sQP stimulation was used in the present study as it has been found to be equivalent to partial tripolar in another study, in which many of the same subjects participated (Bierer et al. 2015). sQP stimulation consists of four intracochlear electrodes: the two middle electrodes serve as active electrodes, and the two outer electrodes serve as return electrodes for a fraction of the active current (an extra cochlear electrode carries the remainder of the return current). Current is steered between the two middle electrodes according to the fraction, α with a value of one steers’ current to the basal electrode and 0 to the apical electrode. By convention, channel number is defined as the basal active electrode when α = 1. In the present study, this convention was maintained for electrodes 3 to 15. For electrode 2, however, it was necessary to use the same set of electrodes as channel 3 (the most apical channel possible with the 4-electrode sQP configuration) in conjunction with an α value of 0 to center the current on electrode 2. This arrangement is referred to as “channel 2,” even though electrode 2 is the apical active electrode. For current focusing, the outer two electrodes in the sQP configuration receive a fraction of the return current according to σ (Landsberger and Srinivasan 2009; Srinivasan et al. 2010; Bierer et al. 2015). As with the commonly used partial tripolar configuration, higher σ results in a narrower electrical field than MP stimulation (Litvak et al. 2007). A value of σ = 0.5 was used in the present study for masker stimulation to retain sufficiently focused stimulation while avoiding unreasonably high current limits and side-lobe activation. For the shorter duration probe stimulation, an σ value of 0 (monopolar) was used to ensure the probe stimulus was salient to the listener. MP stimulation was used for probe stimuli, rather than sQP stimulation, because the high current requirements to achieve most comfortable level (MCL) for a very brief pulse train were often unobtainable within the compliance limits of the device with sQP; further, some subjects could not perceive the probe stimulus using the more focused sQP stimulation. A fixed probe level measured in percent dynamic range was used to facilitate direct comparisons of PTCs across electrodes and subjects (McKay 2012).

Most Comfortable Listening Levels

MCLs were measured for use in the PTC procedure, described below. MCLs for masker and probe stimuli were determined using the Advanced Bionics clinical loudness scale (Advanced Bionics, Valencia, CA). To determine MCL, current level was increased manually until subjects reported a loudness rating of “6,” or “most comfortable.” The level was changed in 2 dB steps until a loudness rating of 4 was reached; thereafter the level was changed in 0.5 or 0.1 dB steps, depending on subject response. Device compliance limits were not reached for any subject. MCLs served as the maximum stimulus level for all psychophysical procedures.

Single-Channel Behavioral Thresholds

Single-channel thresholds were measured for electrodes 2–15 using the sweep threshold procedure (Bierer et al. 2015). Stimuli were biphasic, cathodic-leading pulses trains (102 μs/ph, 0-μs interphase gap, 200.4 ms duration, 997.9 pulses per second) using sQP stimulation with σ = 0.9; highly focused thresholds were measured to capture local variability for later comparison with PTC measures. Pulse trains were presented starting at 6 dB below the MCL, with α-value increasing from 0 to 1 in 0.1 steps from electrode 2–15 for a forward sweep (apical to basal), and from 15 to 2 (basal to apical), for a backward sweep (based on Sęk et al. 2005; for details, see Bierer et al. 2015). A forward and backward sweeps were run for each set of stimuli and averaged to estimate thresholds. Device compliance limits were not reached for any subject during threshold measurement. Sweep thresholds served as the minimum stimulus levels for all psychophysical procedures.

Sweep Psychophysical Tuning Curves

Single-channel behavioral thresholds were measured for masker and probe stimuli using sQP stimulation and the threshold sweep procedure (Bierer et al. 2015). Stimuli were biphasic, cathodic-leading pulse trains (102 μs/ph, 0-μs interphase gap, 997.9 pulses per second), presented to electrodes 2–15 (apical to basal), for both masker (200.4 ms duration) and probe (20 ms duration) stimuli. Masker stimuli were presented with sQP stimulation using an σ = 0.5; probe stimuli used σ = 0. These thresholds determined the lower limit of stimulation, and the MCLs determined the upper limit.

PTCs were obtained for all available electrodes within a forward-masking paradigm using a modified threshold sweep procedure (Fig. 1a; Bierer et al. 2015). This procedure is similar to the sweep threshold procedure (see single-channel behavioral thresholds section), though in this case the masker was swept across the electrode array, varying in level, while the probe remained fixed in level and location. Each PTC sweep took approximately 6 min, with a total of 24 min per electrode for a complete PTC. Probe stimuli were presented at 30 % probe dynamic range when possible; for some subjects, the level was increased to 40–50 % dynamic range due to some subject’s inability to do the task with the probe at a softer level. Probe levels were set as a percentage of the probe dynamic range to ensure that the stimuli were consistently soft and equally loud across all probe electrodes (McKay 2012). Masker levels were normalized to the percentage of the masker dynamic range, which reduces variability and allows for ease of comparison across all probe electrodes and subjects.

The listener was presented with a box on the computer screen and instructed to hold down the space bar when they heard the target sound (probe) and release the space bar when they no longer heard it. This procedure was repeated until all available electrodes served as probes. Two subjects, S40 and S49 had difficulty with the sweep PTC procedure; they were unable to hear the probe in the presence of the masker, even at higher levels and at longer masker-probe intervals. In those cases, a two-interval, two-alternative, forced choice (2IFC) procedure, identical to that used by Bierer and Faulkner (2010) was used for all electrodes to explore the central hypothesis. A recent study by Bierer et al. (2015) did not find any systematic differences between 2IFC thresholds and the threshold sweep procedure, which allows for significantly faster collection of psychophysical data.

PTC Quantification

PTCs were characterized as a function of masker level, normalized to the masker-alone dynamic range. The equivalent rectangular bandwidth (ERBDR) was used to quantify the spatial extent of masker-probe interaction by equating the PTC to a rectangular function of equivalent minimum masker level (Fig. 1b). It was calculated by dividing the area above the PTC by the minimum masker level (PTC tip). This is a commonly used method in psychoacoustics, which avoids selection of a fixed masker level from which a PTC bandwidth is often derived. PTCs with probes near the end of the electrode array (typically electrodes 2 and 15) were not fully characterized on one side due to the lack of electrodes to use as maskers. Partial tuning curves were defined as those for which the tip of the PTC was determined to be at the end of the electrode array. Under the assumption that neural excitation would extend to neurons beyond the array, partial tuning curves were completed by mirroring the masker levels from the measured data on the side with a full complement of masker electrodes.

PTC tip shifts were quantified to examine the relationship between suspected areas of poor neural health and electrode position. For each subject, two runs of PTC sweeps were collected. One run consists of forward and backward sweeps. The difference between PTC sets was calculated and averaged to assess within-subject variability between sweep sets. This resulted in an individual criterion cut-off for what was considered a tip shift. For example, if there was a 15 % mean difference between PTC sets, a greater than 15 % difference between the masker level at the probe and the tip (the minimum masker level) was considered to be a tip shift. Table 2 shows the tip shift criterion used, standard deviation between PTC sets, and number of tip shifts for each subject. There were 39 tip shifts out of the 182 PTCs. There were eight PTCs with tips shifted by more than one electrode. There were 19 apical and 20 basal tip shifts in this dataset. The tip shifts were collapsed across electrodes and are reported as “tip shift” or “no tip shift” and analyzed as a binary variable.

TABLE 2.

Individual mean difference (percent masker dynamic range) and standard deviation between two sets of PTC sweeps

ID Mean Diff. (%DR) SD (±) No. of tip shifts
S22 12.3 0.09 5
S29 12.5 0.12 4
S40 11.5 .08 4
S42 19.5 0.25 4
S43 18.1 0.15 3
S46 17.9 0.16 4
S47 12.6 0.09 1
S49 11.9 .08 4
S53 14.8 0.18 2
S54 13.7 0.11 2
S55 8.9 0.08 4
S56 9.3 0.08 1
S57 13.5 0.11 1

For S40 and S49, the values were calculated by comparing each run from the 2IFC procedure. The mean differences are used as criterion for whether a PTC tip shift occurred

Word Recognition

Scores on a word recognition task were obtained to evaluate clinical performance in the context of sQP threshold, electrode-to-modiolus distance, and PTC ERBDR. Performance on the consonant-nucleus-consonant (CNC) words was obtained from each subject’s clinical audiologist. Per audiologist report, the CNC words were presented at 60 dB-SPL in the sound field using the subject’s everyday speech processor program. For subjects S46 and S49, the only scores available from the audiologist were in the bimodal condition; therefore, they were tested in the laboratory in the CI-only condition at 60 dB-SPL in the sound field using the subject’s everyday speech processor program. All scores were from within the last 2 years and are reported in Table 1.

Statistical Analysis

SPSS statistical software was used to perform linear mixed effect analyses for between-subjects comparisons (IBM Corp. Released 2015. IBM SPSS Statistics for Windows). The first analysis assessed whether PTC ERBDRs measured with the 2IFC procedure (used for S40 and S49) significantly differed from those subjects who used the modified threshold sweep procedure. This analysis showed no significant effect of psychophysical task on PTC ERBDRs (F(20.3) = .18, P = .68); therefore PTC ERBDRs from both tasks were compiled in all following statistical models.

The first model included sQP threshold as the dependent variable, electrode-to-modiolus distance as the independent variable of interest, and duration of deafness as a covariate. The second analysis included PTC ERBDR as the dependent variable, with sQP threshold, and electrode-to-modiolus distance as fixed factors, and duration of deafness as a covariate. Duration of deafness was added as a continuous covariate in these models due to the presence of two pre- (S49, S53) and one peri-lingually (S40) deafened subject in this dataset; these three subjects have similar durations of deafness (41.5, 43, and 46 years, respectively). Additional linear mixed effect analyses were conducted to evaluate the effects of scalar location (dependent ordinal variable) on sQP threshold, electrode-to-modiolus distance, and PTC ERBDR. For all mixed effects models, electrode was added as the repeated factor, and subjects were entered as a random factor, so that each subject had their own intercept for the effects of interest (Baayen et al. 2008). A Bonferroni correction was applied to all multiple comparisons and is noted where appropriate; all p-values reported from this procedure are adjusted for a significance level of α = .05.

A generalized estimating equation (GEE) procedure was performed to evaluate the presence of a tip shift (dependent binary variable) on sQP threshold, electrode-to-modiolus distance, and PTC ERBDR (independent continuous variables). The GEE procedure extends the generalized linear model to allow for a repeated measures analysis on a binary dependent variable (IBM Corp. Released 2015. IBM SPSS Statistics for Windows); reported results are from a Wald’s test.

A multiple linear regression analysis was performed to evaluate the relationship between clinical CNC scores and mean electrode-to-modiolus distance, mean sQP threshold, and mean PTC ERBDR.

RESULTS

Electrode-to-Modiolus Distance Using CT Imaging

Figure 2 highlights the variability in electrode array positioning observed in 3D cochlear reconstructions for all subjects, arranged by electrode array type. In general, the electrode trajectories in Fig. 2 are consistent with the designs of the four types of arrays, which partially determine how far the electrodes are from the modiolus, and thus how close they are to target auditory neurons. The 1 J electrode array (S29, S40, S46, and S55) has a lateral design, whereas the 1-J Helix (S22, S53) is pre-curved to achieve a more medial position. The 1 J with positioner (S42, S56), by design, pushes the electrode array even more medially. The Mid-Scala array (S43, S49, S47, S54, S57) is pre-curved and designed for mid-scalar placement to protect cochlear structures.

FIG. 2.

FIG. 2

CT view of cochlea and electrode array along the midmodiolar axis (red and yellow dashed lines), for all subjects, organized by electrode array type. The evenly spaced red dots represent electrodes; the outermost dot represents the insertion depth marker. The white line represents the 0 ° reference point from which insertion depth is measured, extending from the midmodiolar axis. Row 1: 1 J; row 2: 1-J Helix and 1 J with positioner; row 2: Mid-Scala electrode array

Focused Behavioral Thresholds and Electrode-to-Modiolus Distance

Figure 3a shows electrode-to-modiolus distance (left ordinate) and sQP threshold (right ordinate) profiles for each subject. Scalar location is indicated by symbol (see legend). sQP thresholds ranged from 28.8–55.7 dB rel. to 1 μA (M = 45.67 dB rel. to 1 μA, SD = 6.12) across all subjects and electrodes (Table 3). Electrode-to-modiolus distance, or the lateral distance in millimeters from the modiolus, ranged from 0.18 to 2.2 mm (M = 1.06 mm, SD = .52; see Table 3). Figure 3b illustrates the relationship between sQP threshold and electrode-to-modiolus distance, with individual subject data distinguished by color and shape; the line of best fit for all subjects is plotted (solid black). Figure 4c shows the line of best fit for individual subjects, as well as the group line of best fit (solid black). Consistent with previous studies (Long et al. 2014; Cohen et al. 2003), a strong association between sQP thresholds and electrode-to-modiolus distance was observed. Results from the linear mixed effect analysis show a significant relationship between electrode-to-modiolus distance and sQP threshold (F(1,170.5) = 57.33 P < .001); in other words, across subjects, electrodes with higher behavioral thresholds tended to be farther from the modiolus. It is worth noting that for the six subjects where this relationship was observed (S42, S43, S47, S49, S53, S57), four have the Mid-Scala electrode array; the other two subjects have 1 J with positioner and a 1-J Helix array. For subjects with the 1-J array (S29, S40, S46, S55), which tends to sit laterally to the modiolus, electrode-to-modiolus distance did not correlate with sQP threshold, likely due to low variability in electrode position in this data set. Due to the small sample size for each electrode array, statistical differences between array types cannot be further examined.

FIG. 3.

FIG. 3

a sQP threshold in dB rel. to 1 μA (green line) and electrode-to-modiolus distance in mm (blue line) for all subjects, organized by electrode array type. Scalar information is represented by symbols along the electrode-to-modiolus distance line: ST (circles), Intermediate (diamonds), and SV (triangles). b Scatter plot comparing electrode-to-modiolus distance with sQP threshold for individual subjects (distinguished by color) and the line of best fit for all subjects (solid black line). c The line of best fit for individual subjects for the data in panel B (lines distinguished by color), and for all subjects (solid black line)

TABLE 3.

Means and standard deviations for electrode-to-modiolus distance, sQP threshold, and tuning equivalent rectangular bandwidth (ERBDR); data shown are for electrodes 2–15

ID EMD (mm)
mean (SD)
Focused thres. (dB)
mean (SD)
Tuning ERBDR (mm)
mean (SD)
Threshold-distance
RMS error
%DR for PTCs
S22 1.12 (.37) 42.72 (6.92) 2.14 (1.14) 6.22 30
S29 1.52 (.23) 47.15 (3.32) 3.70 (1.37) 3.31 40
S40 1.79 (.22) 54.27 (1.30) 5.40 (2.40) 1.32 50 (2IFC)
S42 .64 (.33) 36.96 (4.80) 3.07 (1.73) 2.3 30
S43 .84 (.44) 44.69 (3.95) 3.09 (1.48) 1.9 40
S46 1.80 (.34) 50.67 (1.58) 5.51 (2.23) 1.59 30
S47 .87 (.46) 38.39 (5.91) 2.61 (.76) 2.08 30
S49 .94 (.47) 50.70 (2.15) 2.85 (1.02) 1.49 40 (2IFC)
S53 .66 (.17) 45.41 (3.01) 2.30 (.96) 2.09 30
S54 .89 (.46) 47.14 (5.77) 3.16 (1.43) 5.27 50
S55 1.06 (.26) 44.88 (1.47) 5.81 (1.74) 1.48 40
S56 .62 (.33) 46.26 (1.53) 4.51 (2.62) 1.53 30
S57 .90 (.39) 43.39 (4.32) 2.89 (1.27) 4.58 30
Summary 1.06 (.52) 45.68 (6.13) 3.62 (2.01) N/A N/A

Threshold-distance RMS error, number of tip shifts, and %DR used for PTCs are also listed. The summary line indicates means and standard deviations across subjects

FIG. 4.

FIG. 4

PTCs across the electrode array for three example subjects (S56, S53, and S57). The x-axis denotes the masker electrode (apical to basal). The y-axis represents the masker level in percent dynamic range. The numbered lines inside the plot are probe electrodes, labeled at the tip of the PTC. The mean PTC ERBDR in mm is marked inside each plot

While duration of deafness significantly contributed to this relationship (F(11.6) = 15.4 P < .001), duration of deafness did not dictate whether a correlation between sQP threshold and electrode-to-modiolus distance existed. Those subjects with longer durations of deafness tended to have higher thresholds overall, but this did not preclude a significant, positive correlation with electrode distance; the line of best fit was simply shifted up the y-axis for these subjects.

Psychophysical Tuning Curve Characteristics

There was wide variability observed in the PTCs within and across subjects. Across subjects, PTC ERBDRs ranged from 0.70 to 10.40 mm, with a mean of 3.62 mm (SD = 2.01; Table 3). There was a total of 39 tip shifts out of 182 PTCs; S22 had the greatest number of tip shifts at five (see Table 2). There was no apparent effect of apical or basal-ward tip shifts in the data.

Figure 4 shows all 14 PTCs across the electrode array for three example subjects S56 (a), S57 (b), and S53(c). PTCs are plotted as masker level (% dynamic range) as a function of masker electrode (apical to basal). The mean ERBDR for these subjects is marked on each panel. There was a high degree of overlap, or presumed channel interaction, between PTCs within a given subject. This is particularly evident for S56 (Fig. 4a), where most PTCs are overlapping, and some PTC tips (such as electrode 3) are shifted quite far basally, and some apically (electrode 5). S57 (Fig. 4b) had quite deep PTCs, with few tip shifts; however, a high degree of PTC overlap is observed across the electrode array. S53 (Fig. 4c) had shallower PTCs apically, and deeper PTCs basally; there are more easily observable PTC tips and less channel interaction overall. Interestingly, though the PTC characteristics of these example subjects differ, their clinical performance is very similar (Table 1).

Comparisons between Focused Thresholds, Electrode-to-Modiolus Distances, and Tuning Curve Bandwidths

Scatterplots of PTC ERBDRs and electrode-to-modiolus distance (Fig. 5a), and sQP thresholds (Fig. 5c) are shown for all subjects, with individual data distinguished by color and shape. Figure 5b, d show the lines of best fit for individual subjects and the group (solid black line). Table 4 shows results for within-subject correlations for these comparisons. Results from the linear mixed effect analysis show PTC ERBDRs are correlated with electrode-to-modiolus distance (F(1,163.87) = 9.30, P = .003). Although there was a trend toward higher sQP thresholds for broader PTC ERBDRs, there was no statistically significant effect (F(1,177.83) = 3.14 P = .08). There was no effect of duration of deafness (F(1,13.96) = .02, P = .89). These results indicate that PTC ERBDRs are broader for electrodes farther from the modiolus, but that PTC ERBDRs were not a reliable correlate of focused behavioral thresholds in these subjects.

FIG. 5.

FIG. 5

Comparisons between sQP threshold, electrode position, and PTC ERBDRs for individual subjects. a Electrode-to-modiolus distance and PTC ERBDR individual data and group best fit line. b Electrode-to-modiolus distance and PTC individual and group best-fit lines c sQP threshold and PTC ERBDR individual data and group best fit line. D: sQP threshold and PTC ERBDR individual and group best-fit lines

TABLE 4.

Individual Pearson’s r and p values (* indicates statistical significance) for the correlations between: PTC ERBDRs and sQP thresholds (dB rel. to 1 μA), in the left two columns, labeled threshold-ERBDR, and between PTC ERBDRs and electrode-to-modiolus distance (EMD; mm) in the right two columns, labeled as EMD-ERBDR

ID r (threshold-ERBDR) p (threshold-ERBDR) r (EMD-ERBDR) p (EMD-ERBDR)
S22 − .06 .83 .53 .05*
S29 − .45 .11 .81 .0004*
S40 − .18 .53 .47 .09
S42 .62 .02* .70 .006*
S43 .53 .053 .66 .01*
S46 .20 .48 .17 .56
S47 .49 .08 .55 .04*
S49 .26 .36 .18 .55
S53 .51 .06 .19 .51
S54 .70 .006* .21 .48
S55 .05 .87 .28 .34
S56 .26 .36 − .27 .35
S57 .69 .006* .60 .02*

Scalar Location

CT-estimated scalar location was assessed for all subjects and electrodes. Of 182 electrodes, 54.4 % were in ST, the target scalar location during surgical implantation. Most of the other electrodes were estimated to be in the intermediate position (28 %), with the remaining electrodes in the SV (17.6 %). Figure 6 presents box plots of the distribution of scalar location for sQP threshold (a), electrode-to-modiolus distance (b), and PTC ERBDR (c). Results from the linear mixed effect analysis show a main effect of scalar location for sQP threshold (F(1.174.7) = 7.59, P = .001), electrode-to-modiolus distance (F(1.177.31) = 18.93, P < .0001), and PTC ERBDR (F(1,170.09) = 7.0, P < .01).

FIG. 6.

FIG. 6

Box-and-whisker plots for the distribution of scalar location relative to a sQP threshold (dB rel. to 1 μA), b electrode position (mm), and c PTC ERBDR (mm). Scalar location is labeled as scala tympani (ST), intermediate, and scala vestibuli (SV)

After Bonferroni adjustment, results show that sQP thresholds were higher for electrodes in SV as compared to ST (P < .0001) and as compared to electrodes in the intermediate position (P = .05). There were no significant differences in sQP threshold between intermediate electrodes and those in ST (P = .11). As expected, electrodes located in either SV (P = .003) or the intermediate position (P < .001) had greater electrode-to-modiolus distances as compared to ST; there were no significant differences between electrodes in SV and the intermediate position (P = .58). As sQP threshold and electrode-to-modiolus distance was shown to be correlated in this study and others (Long et al. 2014; DeVries et al. 2016), these results indicate that for electrodes in SV, high sQP thresholds may be primarily driven by electrode position. PTC ERBDRs were significantly broader for electrodes in SV (P < .01) as compared to ST but did not reach statistical significance when compared to electrodes in the intermediate position (P = .06). There were no significant differences in PTC ERBDRs between intermediate electrodes and those in ST (P = .19).

It is important to interpret these analyses with caution. While the linear mixed effect analysis accounts for uneven sample sizes, the boxplots show that the distributions of the variables of interest tend to overlap substantially in many cases (particularly with sQP threshold). This may signify that the statistically significant effects observed are small in magnitude.

Effect of PTC Tip Shifts

Results from the GEE procedure (see “Statistical Analysis”) show no effect of tip shift for sQP threshold (χ2 = 2.33, P = .13; Fig. 7a) or PTC ERBDR (χ2 = .50, P = .48; Fig. 7a). Interestingly, there was a significant effect of tip shift for electrode-to-modiolus distance (χ2 = 7.35, P = .007; Fig. 7b), wherein electrodes with PTC tip shifts were likely to be positioned more lateral to the modiolus.

FIG. 7.

FIG. 7

Box-and-whisker plots for the distribution of PTC tip shifts relative to a sQP threshold (dB rel. to 1 μA), b electrode position (mm), and c PTC ERBDR (mm). Tip shifts are coded either absent (“no”) or present (“yes”) or for all 182 PTCs in this data set

Further analyses were conducted to ascertain whether the number of within-subject tip shifts were correlated with high sQP thresholds not predicted by electrode-to-modiolus distance (quantified as greater than + 1 SD above the mean). In other words, we examined whether high sQP thresholds not accounted for by electrode position were correlated with more tip shifts, and thus possibly indicative of poor neural health. However, a linear regression showed that tip shifts were not correlated with sQP thresholds + 1 SD from the best-fit line (F(1,11) = 1.68, P = .22).

Word Recognition

Figure 8 shows mean performance on the CNC word test (% correct) in relation to mean sQP threshold (a), mean electrode-to-modiolus distance (b), and mean PTC ERBDR (c). This set of predictors accounted for a significant amount of variance in CNC word scores (R2 = .72, F(3,9) = 7.56, P = .008, R2adjusted = .62). The model shows no significant effect of mean PTC ERBDR (T19 = 1.65, R = − .26, P = .13) or mean electrode-to-modiolus distance (T19 = − 1.76, R = − .66, P = .11). sQP thresholds had a unique positive effect on CNC word scores (T19 = − 2.86, R = − .76, P = .02), wherein subjects with higher mean sQP thresholds across the array tended to have lower CNC word scores.

FIG. 8.

FIG. 8

Correlations between the variables of interest and clinical CNC word scores (% correct). a Mean sQP threshold (dB rel. to 1 μA). b Electrode-to-modiolus distance (mm). c Mean PTC ERBDR (mm). The pre−/peri-lingually deafened subjects (S40, S49, and S53) are represented by filled in symbols, for ease of viewing

DISCUSSION

The present study assessed the relationship between PTC ERBDRs, sQP behavioral thresholds and CT-estimated electrode position. Results support the hypothesis that electrodes farther from the modiolus tend to have higher behavioral thresholds, broader PTC ERBDRs, are translocated to SV, and a higher number of PTC tip shifts across the electrode array. There was no relationship observed between sQP thresholds and PTC ERBDRs or tip shifts. Mean sQP thresholds were correlated with word recognition, whereas mean PTC ERBDRs and mean electrode-to-modiolus distances were not, indicating that sQP thresholds may capture an additional aspect of the electrode-neuron interface important for speech perception.

Focused Single-Channel Behavioral Thresholds and Electrode-to-Modiolus Distance

Consistent with other studies, sQP thresholds were correlated with electrode-to-modiolus distance, such that electrodes with higher thresholds had larger electrode-to-modiolus distances (Cohen et al. 2001; Cohen 2009; Long et al. 2014; DeVries et al. 2016). As duration of deafness increased, sQP thresholds tended to be higher, but this did not preclude a significant relationship with electrode-to-modiolus distance in some subjects. These findings are supported by histological data (Kawano et al. 1998), computational modeling (Briaire and Frijns 2006; Frijns et al. 1995, 1996; Goldwyn et al. 2010), and EABR thresholds in animals (Shepherd et al. 1993).

Figure 3b, c demonstrates that electrode-to-modiolus distance does not account for all the variability in sQP thresholds. It may be presumed that sQP thresholds not predicted by electrode-to-modiolus distance reflect areas with poor neural survival, though bone and tissue growth and tissue impedance may affect this relationship as well.

PTC Bandwidths, Electrode-to-Modiolus Distance, and Focused Single-Channel Behavioral Thresholds

Electrodes with broader PTC ERBDRs were correlated with electrodes located farther from the modiolus, consistent with previous studies that used electrophysiological (Brown et al. 1990; Cohen et al. 2003; Hughes and Abbas 2006; DeVries et al. 2016) and modeling techniques (Briaire and Frijns 2006). PTC ERBDRs were not correlated with sQP thresholds, though results trended toward significance in the expected direction. This result is consistent with a recent study in our laboratory that used the electrically evoked compound action potential (DeVries et al. 2016).

sQP thresholds likely capture the effects of electrode-to-modiolus distance and other factors such as neural status, which may explain the lack of relationship between sQP thresholds and PTC ERBDRs. It is also possible that ERBDRs are unable to capture this relationship. Other studies have used slopes or fixed widths to quantify PTCs (e.g., Nelson et al. 2008); comparisons between these methods will be made in a future study. We also used a monopolar probe and pTP masker, resulting in a lower degree of current focusing compared to another study that found a strong correlation between highly focused PTCs and behavioral thresholds (Bierer and Faulkner 2010). Finally, the use of %DR to set probe levels does not guarantee that the probes were equally loud for the listener, though PTC widths have been shown to be insensitive to probe level (Nelson et al. 2008, 2011). It may be this methodological “noise” in the PTC measure weakened the correlations between PTC ERBDRs, sQP thresholds, and electrode-to-modiolus distance for some subjects.

Effects of Scalar Location

Electrodes translocated from ST to SV had higher sQP thresholds, greater electrode-to-modiolus distances, and broader PTC ERBDRs (Fig. 6), consistent with a recent study (DeVries et al. 2016). These results are reflective of the physical distance between electrodes located in ST and those in SV (Teymouri et al. 2011), which likely leads to increased current requirements and broader spread of excitation.

Shepherd et al. (1993) evaluated EABR thresholds in implanted adult cats at different scalar locations within ST. EABR thresholds were reduced when moving from lateral electrode placements to peripheral dendrite and spiral ganglion cell body positions. Frijns et al. (1995, 1996) extended this work using a computational model examining the same ST positions as the Shepherd study, with comparable results. These findings have also been observed in a guinea pig model (Snyder et al. 2004).

Some studies have found that a greater number of electrodes located in SV correlates with poorer CNC word recognition (Finley et al. 2008; Holden et al. 2013); however, we were unable to replicate that finding with these data. (T12 = 1.07, P = .31).

These results support the contention that ST is the ideal scalar location for electrode array insertion, although behavioral and electrophysiological variability is noted even within ST. Given previously observed relationships between scalar location and word recognition (Holden et al. 2013), this underlines the importance of surgical technique and electrode array design to optimize implant insertions.

PTC Tip Shifts and Electrode-to-Modiolus Distances

There were 39 tip shifts out of a possible 182 PTCs, with no evidence of a predominance of apical or basalward shifts, as seen by others (Nelson et al. 2008). PTC tip shifts were analyzed across subjects and electrodes in relation to sQP threshold, electrode-to-modiolus distance, and PTC ERBDR (Fig. 7).

There was no significant relationship between PTC tip shifts and sQP threshold or PTC ERBDRs. This is inconsistent with other studies that have found electrodes with tip shifts tend to have broader PTCs (Nelson et al. 2008; Bierer and Faulkner 2010). It is possible we did not replicate this result due to the very small number of tip shifts larger than one electrode contact observed in this study; it may be that more dramatic tip shifts are needed to observe these relationships.

Electrodes farther from the modiolus tended to have more tip shifts; this is perhaps unexpected, as tip shifts are traditionally viewed as indicative of neural status. Bierer et al. (2010) measured forward-masked PTCs in the inferior colliculus of guinea pigs, and found PTC tips shifted toward the apex where the guinea pig cochlea tapers, causing the apical electrodes to be much closer to the modiolus. In the present study, it is possible that asymmetrical current spread occurred for electrodes farther from the modiolus, due to the increase in current required to reach auditory neurons. This spread may have caused a small shift in the tip of the PTC, which was the predominant type of tip shift observed in this data set.

Word Recognition

We observed a significant, negative correlation between mean sQP threshold and CNC word recognition in these subjects (Fig. 8a), but no correlation with mean electrode-to-modiolus distance (Fig. 8b) or mean PTC ERBDR (Fig. 8c).

Poorer word recognition in subjects with higher mean focused thresholds is consistent with a recent study in our laboratory (DeVries et al. 2016). However, this result has not been observed by others using bipolar (Pfingst et al. 2004) and phased array stimulation (Long et al. 2014). In the Long study, high within-subject variance for focused thresholds was negatively correlated with the logit-transformed CNC word scores, similar to the findings of Pfingst et al. 2004. We were unable to replicate these results using the within-subject variance of sQP thresholds and raw (T12 = .70, P = .50) and logit-transformed (T12 = .55, P = .59) CNC scores. Long also found that higher RMS error from the threshold-distance correlation was predictive of poorer logit-transformed CNC word recognition scores; subjects with thresholds well predicted by electrode-to-modiolus distance tended to perform better with their implant. The present study did not replicate these results for either raw (T12 = .13, P = .90) or logit-transformed (T12 = − .07, P = .95) CNC word scores, similar to a recent study in our laboratory (DeVries et al. 2016).

Bierer (2007) used the standard deviation of the absolute value of the difference between focused thresholds of adjacent channels, finding a relationship between higher threshold variability and lower CNC word scores. Pfingst et al. (2004) found the same result using the mean of the difference between thresholds. We were unable to replicate the results using the unsigned difference of the standard deviation (T12 = .86, P = .41) or the mean of the difference between thresholds (T12 = − 1.34, P = .21).

Zhou et al. (2018) found that steeper multipulse integration (MPI) functions measured with bipolar stimulation were correlated with lower speech reception thresholds. MPI measures have been shown to predict spiral ganglion neural density in implanted guinea pigs (Zhou et al. 2015), thus pointing to a possible relationship between behavioral threshold-related measurements and neural survival.

Given that the present study was unable to replicate results from some of the above studies, it is likely due to a limitation within this dataset, possibly due to insufficient variability in CNC word scores.

The finding that there is no relationship between mean electrode-to-modiolus distance and word recognition is consistent with recent studies (Long et al. 2014; Holden et al. 2013; van der Marel et al. 2015; DeVries et al. 2016), though Aschendorff et al. (2007) did observe that perimodiolar insertions tended to result in better speech outcomes. van der Marel et al. (2015) examined six electrode position-related factors and did not find any correlations with word recognition, but did find that duration of deafness and preoperative word scores correlated with speech outcomes, as others have found (Blamey et al. 2013).

There was no correlation between PTC ERBDR and word recognition, consistent with other studies (Cohen et al. 2003; Anderson et al. 2011; Nelson et al. 2011), though the Anderson study did find a positive correlation between the inverse of the PTC bandwidth and sentence recognition. This is also consistent with previous studies that used the ECAP (Brown et al. 1990; Cohen et al. 2003; Hughes and Abbas 2006), and one that measured ECAP ERBDRs in all available electrodes (DeVries et al. 2016). Constraints introduced by the speech processor may make it difficult to compare spatial spread measured via direct stimulation to speech recognition, as suggested by others (Nelson et al. 2008, 2011; Anderson et al. 2011).

Duration of deafness was negatively correlated with CNC word scores (T12 = − 2.68, P = .02). It is possible that pooling the pre/peri- and post-lingually deafened subjects weakened the correlations between the variables of interest and CNC word scores. However, one pre-lingually deafened subject (S53) scored 84 % on CNC words, and a post-lingually deafened subject (S46) is a much poorer performer (Fig. 8). Central mechanisms and plasticity resulting from deprivation during auditory development are not well understood in humans. It has been suggested that variability in central plasticity may contribute to a variability in performance into adulthood (Lazard et al. 2012).

While PTC ERBDRs were correlated with electrode-to-modiolus distance, they were not correlated with word recognition. The fact that position-related factors did not correlate with word recognition, but duration of deafness and mean focused thresholds did, suggests that additional factors at the ENI are stronger contributors to word recognition.

CONCLUSIONS

The widely documented variability in CI listener outcomes is likely due, in part, to the status of the electrode-neuron interface. Quantifying and disambiguating factors that contribute to poor electrode-neuron interfaces that may be useful for optimization of programming techniques for these listeners. The ability to evaluate the electrode-neuron interface in the clinical environment is limited due to resources, time, and costs. Therefore, identifying measurements that may help to bypass these limitations is of the utmost importance.

This study demonstrated that a measure of spatial spread of excitation, or channel interaction, was correlated with electrode-to-modiolus distance, but not with behavioral thresholds. Scalar location appears to influence behavioral thresholds, degree of channel interaction, and electrode-to-modiolus distance, indicating that proper placement of the electrode array may have an influence on psychophysical and objective measurements.

Behavioral thresholds were the only variable correlated with word recognition. This may indicate that while spatial measures of channel interaction reflect an important aspect of the electrode-neuron interface, and may prove useful for device programming, performance with the implant is not fully captured by electrode position or degree of channel interaction.

Finally, these results suggest that electrode array placement influences spatial spread of excitation and that PTCs may be a useful behavioral measure to disambiguate electrode-neuron interface factors for some CI listeners. Future studies will use PTCs and electrode position to create experimental programs that account for electrodes with high degrees of channel interaction and determine if performance can be meaningfully improved when incorporating this information.

Acknowledgements

The authors would like to acknowledge Kelly Jahn for assisting with data collection, Timothy Holden for analyzing the CT scans, and our subjects for their time and dedication.

Funding Information

This study received funding from RO1 DC012142 (JGA) and T32 DC 000033 (University of Washington Speech and Hearing Sciences: LAD).

Compliance with Ethical Standards

Conflict of Interest

The authors declare that they have no conflict of interest.

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