Jennifer Lentz — Psychoacoustics- Perception of Normal and Impaired Hearing with Audiology Applications

Yield

569 of 2208 paragraphs kept (25.8%). Target for mining: 30%–50% — ⚠️ BELOW target.

Pre-Assessment

Jennifer Lentz is a Professor of Speech, Language, and Hearing Sciences at Indiana University (Purdue School of Health and Human Sciences), a psychoacoustician who has published extensively on normal and impaired auditory perception, including work on loudness, cochlear implants, and temporal processing. The book title frames it as a survey text explicitly pairing psychoacoustic perception with audiology applications, which is a good sign for your stated purpose.

Given your mining stance and desire for “lists of concepts and theories and models,” this book should yield a high density of established facts (experimental findings on loudness, pitch, masking, temporal/spatial resolution) and structured conceptual frameworks/theories (such as auditory filter models, loudness models like the Moore/Glasberg model, and peripheral vs. central processing distinctions). It will likely be more textbook-concepts than inspiration/speculation — Lentz writes as a researcher-textbook author, so you should expect explanatory models presented with supporting evidence rather than provocative new theories. If you plan to mine it, expect a meaty but conceptually dense read that will reward a structured note-taking approach.

Reading Goal

Prioritizing: Factual Claims (Reader wants to understand actual perception differences, needs concrete facts), Definitional Content (Asks for concepts, theories, and models — definitions are core to this), Causal Relationships (Understanding perception requires cause-effect mechanisms behind hearing), Connection Points (Links between normal/impaired perception and related models are useful), Contrarian or Surprising Claims (Surprising contrasts between normal and impaired hearing are informative) De-prioritizing: Inspiration and Speculation (Reader wants systematic understanding, not speculative ideas)

Thesis

Psychoacoustics explains perception through physiological mechanisms · ch. 0

Argument

  1. Auditory perception depends on understanding ear capabilities and hearing loss effects — ch. 0
  2. Physiological tests measure sound representation, never the perception itself — ch. 0
  3. Successful communication requires multiple distinct auditory perception abilities beyond simple detection. — ch. 0
  4. Standard audiological tests miss most of the perceptual abilities humans need to communicate — ch. 0
  5. Hearing-impaired perception studies illuminate the mechanisms behind normal hearing — ch. 0
  6. The audiogram is a behavioral test rooted in a century of psychoacoustics — ch. 0
  7. Topic-based organization beats sequential background chapters for teaching audiology — ch. 0
  8. The audiogram measures only detection and conceals varied sensorineural perceptual deficits. — ch. 0
  9. Reliable perception measurement emerged only in the early 1800s — ch. 1
  10. Psychoacoustics originated in early 1700s experimental psychology — ch. 1
  11. Early psychoacoustics lacked tools to control sound intensity independently of frequency — ch. 2
  12. The decibel unit enabled standardized hearing characterization — ch. 2
  13. Corporate and technical goals, notably telephony, shaped which auditory abilities researchers studied — ch. 2
  14. Sensorineural hearing loss compresses the full loudness range into fewer decibels — ch. 2
  15. Harvey Fletcher pioneered threshold measurement, loudness relations, and the masking model. — ch. 2
  16. Bell Labs research priorities were shaped by telephone engineering needs — ch. 2
  17. Early 20th-century hearing research was steered by telephone engineering needs. — ch. 2
  18. Modern audiology rests on the premise that perception connects to physics — ch. 2
  19. Helmholtz made the first psychoacoustic observations in hearing — ch. 2
  20. The 1935 Beasley survey first established US normal-hearing thresholds — ch. 2
  21. Fletcher originated threshold measurement, loudness relations, and masking models — ch. 2
  22. Hearing loss was first quantified as a percentage of remaining dynamic range — ch. 2
  23. Early commercial audiometers cost about $25,000 in modern currency, driving a portable redesign. — ch. 2
  24. Audibility thresholds can be expressed on physical or perceptual decibel scales — ch. 2
  25. The telephone industry drove development of technologies for measuring hearing. — ch. 2
  26. The audiogram’s form was contested because no standard existed for its axes. — ch. 2
  27. Harvey Fletcher shaped modern psychoacoustics and audiology at Bell Labs — ch. 2
  28. Fechner made conscious perception measurable and founded experimental psychology — ch. 2
  29. Earliest hearing-loss tests measured duration and distance of audibility — ch. 2
  30. Pitch perception involves both spectral and temporal representations of sound — ch. 2
  31. The dynamic range of hearing is largest between 500 and 6000 Hz — ch. 2
  32. Psychoacoustics measures detection, discrimination, magnitude, and recognition of sounds — ch. 2
  33. The audiogram only captures detection thresholds and fails to predict real-world speech perception — ch. 2
  34. Early psychoacoustics neglected loudness because sound intensity could not yet be controlled. — ch. 2
  35. Threshold measurement method, not listener differences, caused the 10 dB gap — ch. 2
  36. Wundt built drop-based devices isolating intensity from frequency for controlled study. — ch. 2
  37. Wundt founded experimental psychology as separate from biology and philosophy — ch. 2
  38. Speech intelligibility indexes average signal-to-noise ratio across critical bands — ch. 2
  39. Early hearing-loss assessment relied on tuning-fork duration and distance thresholds. — ch. 2
  40. A widely used audiometric standard was calibrated roughly 10 dB off — ch. 2
  41. Weber’s law states JND is a constant fraction of stimulus magnitude — ch. 2
  42. Early audiogram standardization debates concerned level units and axes, not frequency scaling. — ch. 2
  43. Bell Labs pursued only hearing questions relevant to telephone engineering. — ch. 2
  44. Binaural sound localization depends on ear-level temporal and intensity encoding efficiency — ch. 2
  45. The audiogram measures only detection thresholds, so it misses everyday speech-in-noise ability. — ch. 2
  46. Pure tones are used for audiometry because they are frequency-specific — ch. 3
  47. Absolute threshold is the minimum detectable sound level without external noise — ch. 3
  48. Audiograms test pure-tone detection because pure tones are maximally frequency-specific — ch. 3
  49. Auditory perception is a four-level hierarchy from detection to comprehension. — ch. 3
  50. Lower-level auditory deficits cascade upward but not all higher-level deficits trace downward. — ch. 3
  51. Audiometry pure-tone durations are set by perception, not acoustic independence — ch. 4
  52. A 1 Pa peak-amplitude tone produces 91 dB SPL — ch. 4
  53. Short sound durations necessarily produce broad frequency bandwidths. — ch. 4
  54. A pure tone’s peak amplitude is the maximum pressure it achieves per cycle. — ch. 4
  55. Shorter sounds necessarily have broader spectral bandwidths — ch. 4
  56. Outer and middle ear structures provide frequency-specific amplification of incoming sound — ch. 4
  57. ASHA prescribes 1-2 second steady and 200-ms pulsed tones for audiometry — ch. 4
  58. Short tones smear extra frequencies into their spectra, a cost called spectral splatter. — ch. 4
  59. Combined outer and middle ear amplification spans roughly 600 to 4000 Hz — ch. 4
  60. Longer pure-tone durations produce narrower spectral peaks with less splatter — ch. 4
  61. Middle ear stiffness reduces low-frequency gain while added mass reduces high-frequency gain — ch. 4
  62. The ear analyzes frequencies by location along the basilar membrane. — ch. 4
  63. Time and frequency representations are linked so short durations broaden bandwidth — ch. 4
  64. Peak amplitude misrepresents complex sounds with varying amplitude — ch. 4
  65. The mid-frequency hearing advantage explains why alarms and speech amplification target 1000-6000 Hz. — ch. 5
  66. Hearing thresholds were first systematically mapped in the 1930s using two distinct measurement paradigms — ch. 5
  67. 95 percent of auditory nerve fibers carry coded signals from inner hair cells upward — ch. 5
  68. High spontaneous-rate fibers have low thresholds while low SR fibers have high thresholds. — ch. 5
  69. Two-ear listening improves sound-field thresholds by 10 to 15 dB — ch. 5
  70. Hearing depends on sequential physiological stages, each with distinct perceptual consequences when damaged. — ch. 5
  71. Outer hair cell loss reduces hearing sensitivity by up to 60 dB — ch. 5
  72. Outer hair cells respond better than inner hair cells to low-frequency sound — ch. 5
  73. Auditory nerve fibers divide into three types by spontaneous firing rate. — ch. 5
  74. Live cochleas are much more sharply tuned than cadaver measurements suggested — ch. 5
  75. Auditory nerve fibers’ thresholds correlate inversely with their spontaneous firing rates. — ch. 5
  76. Individual auditory nerve fibers cannot code the full hearing dynamic range — ch. 5
  77. Forced-choice paradigms present one signal amid two or more observation intervals. — ch. 6
  78. A full clinical audiogram can be collected in about fifteen minutes. — ch. 6
  79. Adaptive procedures converge on thresholds without explicit psychometric functions — ch. 6
  80. Signal detection theory models signals and noise as two probability distributions — ch. 6
  81. In signal detection theory, threshold responses depend on an internal response criterion reflecting bias. — ch. 6
  82. An unusually low false positive rate signals a patient exaggerating hearing loss — ch. 6
  83. Free-field hearing thresholds can exceed headphone thresholds by over 15 dB — ch. 6
  84. Self-adjustment threshold methods are fast but lack a standardized response criterion across listeners. — ch. 6
  85. Constant-stimuli threshold measurement is time consuming because many trials are needed per level. — ch. 6
  86. Clinical threshold changes are measured relative to normative curves, not in absolute dB SPL — ch. 6
  87. Forced-choice testing cancels listener response criterion effects in threshold estimation — ch. 6
  88. Response bias distorts threshold measurements in hearing experiments. — ch. 6
  89. Noise can damage high-threshold auditory fibers while audiograms still look normal — ch. 6
  90. Hearing loss does not change the psychometric function’s 12-dB detection range — ch. 6
  91. Response bias can contaminate any psychophysical threshold estimate — ch. 6
  92. Thresholds are statistical detection probabilities, not absolute cutoffs — ch. 6
  93. Hearing-loss severity categories lead patients to underestimate their communication difficulties — ch. 6
  94. Threshold from up-down staircases is the averaged level at response reversals. — ch. 6
  95. Damage location in the ear maps onto specific frequency regions of hearing loss. — ch. 6
  96. Exaggerated hearing loss appears as an overly conservative response bias during audiometry — ch. 6
  97. The outer and middle ear, not the cochlea, shape the absolute threshold curve. — ch. 6
  98. Damage to high-threshold auditory nerve fibers can escape threshold detection yet impair speech-in-noise perception. — ch. 6
  99. Adaptive staircases track a listener’s responses to set signal level — ch. 6
  100. Undefined observation intervals prevent patients from anticipating signals and biasing thresholds low — ch. 6
  101. Research staircase methods require start level, step, and stop criteria — ch. 6
  102. The method of limits estimates thresholds by averaging ascending and descending detection levels — ch. 6
  103. The shape of the audiogram reflects outer and middle ear transfer, not cochlear transmission — ch. 6
  104. Staircase rules specify how many correct trials precede a level decrease — ch. 6
  105. The method of constant stimuli needs prior knowledge of testable levels — ch. 6
  106. Patient false positives signal a reasonable response criterion, not poor performance — ch. 6
  107. Smaller step sizes in audiometry detect feigned hearing loss — ch. 6
  108. The audiogram’s inverted axis breaks standard scientific plotting convention — ch. 6
  109. Clinical threshold testing uses undefined observation intervals to prevent anticipation from lowering thresholds. — ch. 6
  110. Early otosclerosis adds stiffness and thus selectively reduces low-frequency hearing — ch. 6
  111. Middle-ear stiffness increases cause low-frequency hearing loss — ch. 6
  112. Standard clinical threshold testing estimates the 85-95% detection point — ch. 6
  113. Both conductive and sensorineural damage drastically alters absolute threshold curves. — ch. 6
  114. Some false positives during threshold testing indicate healthy response bias — ch. 6
  115. Threshold estimates reflect both ear sensitivity and listener response bias — ch. 6
  116. Ossicular mass increases from otosclerosis cause high-frequency hearing loss — ch. 6
  117. Psychometric functions map continuous stimulus scales onto probabilistic detection judgements — ch. 6
  118. Masking occurs when one sound interferes with perceiving another — ch. 7
  119. Energetic and informational masking operate through distinct peripheral and central mechanisms — ch. 7
  120. White noise amplitude is described by total power or spectrum level (LPC). — ch. 7
  121. Noise is defined relationally against the signal rather than acoustically — ch. 7
  122. Filter cutoff frequency is conventionally the 3-dB-down point. — ch. 7
  123. Healthy ears exploit gaps in fluctuating maskers better than steady ones — ch. 7
  124. White noise carries constant power per hertz across the human hearing range — ch. 7
  125. A filter’s transfer function describes gain in dB independent of sound level. — ch. 7
  126. Narrowband noise needs bandwidth and center frequency descriptors — ch. 7
  127. Masking depends on acoustic relationships between masker and signal, not on subjective noise. — ch. 7
  128. Hearing loss acts like a filter attenuating specific frequencies — ch. 7
  129. White noise has flat power across the 20 to 20,000 Hz hearing range — ch. 7
  130. Two noises with equal LPC differ in total power by their bandwidth — ch. 7
  131. Masking experiments revealed the auditory filter underlying frequency selectivity — ch. 7
  132. The excitation pattern is the internal representation of a stimulus spectrum — ch. 7
  133. A masker’s intensity, frequency content, and temporal pattern determine its masking capability. — ch. 8
  134. Frequency selectivity is the auditory system’s ability to represent one frequency independently of another. — ch. 8
  135. Three acoustic properties determine whether a sound masks another. — ch. 8
  136. Masking experiments infer auditory representation from masker effects on signals. — ch. 8
  137. Early cochlear measurements were distorted by post-mortem damage — ch. 8
  138. Broadband maskers at low levels mask mid frequencies more than extremes. — ch. 8
  139. Hawkins and Stevens measured broadband-noise masking of pure tones across eight masker levels. — ch. 8
  140. Conductive hearing loss can be modeled as a filter, but sensorineural loss cannot — ch. 8
  141. Masking is quantified as the threshold shift between unmasked and masked conditions. — ch. 8
  142. A masker masks most when its frequency matches the signal frequency — ch. 8
  143. Masking patterns reveal the ear’s internal psychological representation of a sound. — ch. 8
  144. Band-pass filters are specified by either two cutoffs or center frequency plus bandwidth — ch. 8
  145. Beyond threshold, masker and signal levels rise one-for-one in decibels — ch. 8
  146. Masking effectiveness depends on masker-signal power, frequency, and timing relationships — ch. 8
  147. Tuning curves map the lowest level that evokes neural or basilar response — ch. 8
  148. Similar frequencies mask each other by competing for the same cochlear location. — ch. 8
  149. Amount of masking is expressed as a decibel difference, not an absolute SPL level — ch. 8
  150. Basilar membrane tuning is sharper in living than dead cochleae — ch. 8
  151. The notched-noise method directly measures auditory filter shape. — ch. 9
  152. Low-frequency maskers mask high-frequency signals more than the reverse, and this worsens with intensity. — ch. 9
  153. The excitation pattern plots auditory-filter output power against filter center frequency — ch. 9
  154. Excitation patterns smooth the spectrum, blurring harmonic and formant detail the acoustic signal carries — ch. 9
  155. There is a critical bandwidth beyond which adding noise power no longer increases masking — ch. 9
  156. The basilar membrane’s logarithmic spacing justifies plotting auditory representations on log frequency axes — ch. 9
  157. The ear’s frequency selectivity is imperfect and worsens at higher frequencies — ch. 9
  158. A narrow noise band can mask signals multiple octaves away at high stimulus levels. — ch. 9
  159. The ear’s frequency selectivity worsens as frequency rises above 500 Hz. — ch. 9
  160. The band-widening paradigm measures signal threshold while varying masker bandwidth — ch. 9
  161. Masking effectiveness depends only on masker power inside the critical band. — ch. 9
  162. ERB is the standard metric for auditory filter bandwidth — ch. 9
  163. Only low-numbered harmonics are resolved, higher ones blur together in the internal representation — ch. 9
  164. Only masker power within the critical band around a signal affects its threshold — ch. 9
  165. The ear’s frequency resolution worsens progressively at higher frequencies. — ch. 10
  166. Identifying a vowel requires at least two of its formants — ch. 11
  167. Wider auditory filters admit excess noise that fully obscures high-frequency formants — ch. 11
  168. Simultaneous-masked PTCs are broader than forward-masked PTCs, with similar overall shape — ch. 11
  169. Simultaneous masking yields broader tuning curves than forward masking. — ch. 11
  170. Listeners use distributed spectral information but not all of it — ch. 11
  171. Widening modulated-noise bandwidth can paradoxically lower detection thresholds. — ch. 11
  172. Impaired frequency selectivity, suppression, and fluctuation use jointly degrade hearing — ch. 11
  173. Normal-hearing listeners exploit temporal dips in fluctuating maskers to detect signals. — ch. 11
  174. Clinical maskers must be wider than the critical band to work — ch. 11
  175. Impaired frequency selectivity and lost suppression increase masking and reduce spectral contrasts — ch. 11
  176. Forward masking reveals an effect that only appears when sounds co-occur. — ch. 11
  177. Fluctuating maskers produce masking release that Fletcher’s power spectrum model cannot explain. — ch. 11
  178. Simultaneous-masking filters may understate the ear’s true spectral resolution — ch. 11
  179. Psychophysical tuning curves measure frequency selectivity via tone-on-tone masking. — ch. 11
  180. A masker only shifts thresholds that already lie below its EML. — ch. 11
  181. Listeners benefit from spectral profiles bandwidth-wide yet do not use all available spectral information — ch. 11
  182. Two-tone suppression makes simultaneous masking appear broader than forward masking — ch. 11
  183. Reduced frequency selectivity hurts speech perception less than reduced audibility does — ch. 11
  184. Cross-hearing via bone conduction can contaminate thresholds, requiring masking in audiometry. — ch. 11
  185. Masking by bandlimited noise depends only on masker energy within the critical band. — ch. 11
  186. Spectral valleys contribute little to vowel identification compared with formants — ch. 11
  187. Masking release from modulated noise also improves speech perception. — ch. 11
  188. Loss of cochlear suppression explains similar PTCs across masking conditions. — ch. 11
  189. Cochlear damage increases susceptibility to masking, hurting speech in noise. — ch. 11
  190. Hearing loss impairs frequency selectivity beyond what stimulus level differences explain. — ch. 11
  191. Sensorineural hearing loss worsens masking beyond mere threshold elevation — ch. 11
  192. A worked dB EML example shows masking calculations in practice. — ch. 11
  193. Absence of recruitment in sensorineural loss signals retrocochlear pathology. — ch. 12
  194. Loudness coding requires pooled responses across many auditory nerve fibers — ch. 12
  195. A tone and wideband noise of very different levels can equally sound loud — ch. 12
  196. A sound’s softness is only meaningful relative to who can hear it — ch. 12
  197. Fletcher and Munson’s 1933 loudness data remain essentially accurate today. — ch. 12
  198. The full loudness range squeezes into a smaller dynamic range for impaired listeners. — ch. 12
  199. A-weighted decibels better predict hearing damage than unweighted sound pressure level. — ch. 12
  200. Hyperacusis is a separate pathology from sensorineural hearing loss — ch. 12
  201. Gustav Fechner mathematically formulated the law named after his mentor Weber. — ch. 12
  202. Loudness cannot be explained by single auditory nerve fiber firing alone — ch. 12
  203. Stevens defined one sone as a 40 dB SPL 1000-Hz tone — ch. 12
  204. Wider bandwidth increases perceived loudness at equal sound pressure — ch. 12
  205. Humans discriminate level differences of under half a decibel across a 100 dB range — ch. 12
  206. Categorical loudness scaling measures uncomfortable and comfortable loudness levels using verbal categories — ch. 12
  207. Sound pressure and intensity are distinct quantities interconvertible by a known relationship — ch. 12
  208. Weber’s law holds for noise intensity discrimination above about 20 dB SL — ch. 12
  209. The auditory system’s ~120 dB dynamic range exceeds any single nerve fiber’s coding capacity — ch. 12
  210. A sound’s bandwidth independently affects how loud it sounds. — ch. 12
  211. Pure-tone Weber functions slope downward across all tested frequencies — ch. 12
  212. Reaction time measures loudness across the full hearing range — ch. 12
  213. Fiber-type-specific damage produces distinct loudness perception abnormalities. — ch. 12
  214. Loudness grows faster at low levels than Stevens’ power law predicts — ch. 12
  215. Reaction time spans the full hearing range where psychometric functions cover only 10-15 dB — ch. 12
  216. Outer and middle ear damage changes the loudness frequency balance — ch. 12
  217. Hearing-impaired listeners show faster loudness growth but similar discomfort thresholds — ch. 12
  218. Sound level meters measure pressure, from which intensity is derived — ch. 12
  219. Intensity is directly quantifiable acoustically while loudness requires human listeners — ch. 12
  220. Categorical loudness scaling uses labeled bars from Not Heard to Too Loud — ch. 12
  221. Sensorineural hearing loss causes abnormal rapid loudness growth called recruitment — ch. 12
  222. Wide bandwidth noise sounds as loud as a narrower tone despite lower level — ch. 12
  223. Severe hearing loss from inner hair cell loss reduces maximum loudness — ch. 12
  224. Near-threshold sounds may sound louder to impaired than to normal ears — ch. 12
  225. Excitation pattern differences grow with filter frequency, favoring the high-frequency edge — ch. 12
  226. Recruitment can explain why loudness summation is absent in noise-induced hearing loss — ch. 12
  227. Reaction time measures loudness in animals and language-disabled people — ch. 12
  228. Noise intensity discrimination improves by pooling multiple frequency regions — ch. 12
  229. Graph scaling choices shape the inferred form of loudness functions. — ch. 12
  230. The phon scale defines loudness relative to equal-loudness matches at 1 kHz — ch. 12
  231. Larger baseline weights require proportionally larger differences to be noticed — ch. 12
  232. Loudness grows as a power law of intensity, not linearly. — ch. 12
  233. Loudness models estimate total neural activity since it cannot be measured directly — ch. 12
  234. Intensity discrimination measures the smallest detectable change in loudness — ch. 12
  235. Outer hair cell damage steepens the basilar membrane’s growth function — ch. 12
  236. Miller’s 1947 study tested Weber’s law with noise stimuli — ch. 12
  237. Higher-frequency auditory filters carry more intensity-difference information than the signal-centered filter — ch. 12
  238. No single standard metric describes auditory intensity discrimination — ch. 12
  239. A 10 dB increase always doubles perceived loudness above 40 dB — ch. 12
  240. The loudness-intensity relationship is named Stevens’ power law. — ch. 12
  241. Loudness discomfort levels are measured to fit hearing aids and assess hyperacusis — ch. 12
  242. Weber fractions in audition are computed from intensity, not decibels — ch. 12
  243. Magnitude estimation lets listeners assign numbers proportional to perceived loudness. — ch. 12
  244. Just noticeable differences are proportional to baseline stimulus size — ch. 12
  245. Loudness balancing measures loudness by matching a test sound’s level to a reference — ch. 12
  246. The term UCL fits the measurement better than LDL, yet US practice favors LDL — ch. 12
  247. Clinical LDL testing uses categorized loudness scaling with ascending stepped levels — ch. 12
  248. Loudness is not reducible to sound pressure level or signal power — ch. 12
  249. Loudness is a psychological percept measurable only through human report — ch. 12
  250. Outer hair cell loss is the primary driver of loudness recruitment — ch. 12
  251. Different auditory nerve fiber types have distinct response thresholds. — ch. 12
  252. Mild-moderate losses show recruitment while severe-profound losses show underrecruitment — ch. 12
  253. Stevens had to invent both the tools and the unit for measuring loudness — ch. 12
  254. Loudness models can guide hearing aid programming and alarm design — ch. 12
  255. Stevens anchored the sone unit to a 1000-Hz tone at 40 dB SPL. — ch. 12
  256. Loudness as perception can never be directly measured physiologically — ch. 12
  257. Loudness is measured either by rating magnitude or by matching equal loudness — ch. 12
  258. The near miss to Weber’s law results from the ear using spread-of-excitation across frequency — ch. 12
  259. Near miss to Weber’s law occurs for tones but not noise — ch. 12
  260. Central auditory processing across frequencies produces the near miss — ch. 12
  261. Weber fraction for tones is level but not frequency dependent — ch. 12
  262. ‘Sound level’ is a deliberately vague unit-free term for sound size — ch. 12
  263. Basilar membrane vibration can be measured in vivo by tracking a bead’s movement — ch. 12
  264. Magnitude estimation of loudness yields only relative, not absolute, values. — ch. 12
  265. Intensity discrimination improves with level for tones, violating Weber’s law — ch. 12
  266. Sounds are time-varying when their intensity changes over time — ch. 13
  267. Brief quiet gaps in sounds can introduce spectral cues that contaminate gap detection results — ch. 13
  268. Temporal fine structure is vital yet not perceived as a temporal event — ch. 13
  269. Gap detection measures the smallest audible silent gap — ch. 13
  270. White noise is not a valid stimulus to assess gap perception. — ch. 13
  271. Temporal processing deficits undermine speech understanding and music appreciation — ch. 13
  272. A sound must decay enough before a following sound stops fusing with it — ch. 13
  273. Gap detection thresholds improve with increasing stimulus bandwidth but not frequency region — ch. 13
  274. Temporal processing is essential for hearing speech and music — ch. 13
  275. Gap added to a tone creates audible spectral splatter or side lobes. — ch. 13
  276. Inserting a temporal gap into a stimulus produces spectral splatter at the gap edges — ch. 13
  277. Auditory stimuli separate into fine structure and slower envelope — ch. 13
  278. Gap detection acuity improves with presentation level up to about 30 dB SL. — ch. 14
  279. Elevated gap detection thresholds in hearing loss stem from threshold elevation, not temporal pathology — ch. 14
  280. The ear integrates energy over time to lower detection thresholds for longer sounds — ch. 16
  281. Modulation depth m ranges from unmodulated to fully modulated sounds — ch. 16
  282. Narrowband noises contain fewer frequencies and show greater amplitude fluctuations than broadband noise. — ch. 16
  283. Amplitude-modulated sounds split into slow-varying envelope and fast-varying fine structure — ch. 16
  284. Slow release from forward masking impairs comprehension of rapid speech. — ch. 16
  285. Gap detection offers quick but shallow measures of temporal acuity — ch. 16
  286. Forward masking reveals how the ear’s perceptual representation of sound decays over time — ch. 16
  287. Wide bandwidth improves temporal perception while low-pass filtering limits it — ch. 16
  288. Narrowband noise’s natural waveform fluctuations mask the presence of inserted gaps — ch. 16
  289. Wider stimulus bandwidth improves the ear’s temporal acuity — ch. 16
  290. Narrower noise bandwidths produce slower amplitude fluctuation rates — ch. 16
  291. Temporal order thresholds exceed gap detection because listeners must hold sound identities in memory — ch. 16
  292. Temporal modulation detection is independent of hearing threshold — ch. 16
  293. The auditory system represents modulations below 55 Hz well and worse above — ch. 16
  294. Gap detection measures only on-off sensitivity, not coding of fluctuation rates. — ch. 16
  295. Soft sounds give the ear inadequate access to rapid amplitude changes in speech — ch. 16
  296. Gap detection tasks measure how the ear follows temporal changes relevant to communication — ch. 16
  297. Hearing loss reduces audibility and restricts usable bandwidth for temporal processing — ch. 16
  298. Intense forward maskers produce both more masking and more release — ch. 16
  299. Narrowband noises fluctuate more than wideband stimuli, making them useful for studying fluctuation coding — ch. 16
  300. Narrow-band devices like telephones degrade temporal cue coding and raise listening effort — ch. 16
  301. Amplitude modulation below about 60 Hz is well represented in hearing — ch. 16
  302. Temporal modulation transfer functions trade completeness against measuring time — ch. 16
  303. Gap detection experiments vary in whether listeners report a gap or count of sounds — ch. 16
  304. Forward masking requires maskers with similar frequency components and high intensity — ch. 16
  305. Stimulus fluctuations hurt gap detection but aid speech perception elsewhere — ch. 16
  306. Gap detection improves with bandwidth because the ear listens across more auditory filters — ch. 16
  307. High modulation detection thresholds signal poor temporal representation of those rates. — ch. 16
  308. The auditory system can discard uninformative temporal information during detection — ch. 17
  309. Sensorineural hearing loss disrupts some temporal abilities but not others, with wide individual variability — ch. 17
  310. Listeners with hearing loss form a heterogeneous perceptual group, not a single category — ch. 17
  311. Hearing-impaired ears can outperform normal ears at amplitude modulation detection — ch. 17
  312. Outer hair cell damage removes cochlear compressive nonlinearity — ch. 17
  313. Similar critical durations do not imply normal temporal integration — ch. 17
  314. Presenting speech at the same loudness minimizes forward-masking differences — ch. 17
  315. Two separated tone pulses aid detection more than one, unaffected by intervening noise level — ch. 17
  316. Temporal integration models divide on time constant assumptions of hundreds versus single-digit milliseconds. — ch. 17
  317. The energy detector model fails because it accumulates interfering noise along with signal energy. — ch. 17
  318. The audiogram cannot predict which hearing-impaired listeners have temporal processing deficits — ch. 17
  319. Hearing-impaired listeners gain half or less benefit from longer stimulus durations — ch. 17
  320. Forward masking decay slows markedly after masker offset in hearing loss — ch. 17
  321. Sensorineural hearing loss reduces temporal integration benefit by half or more — ch. 17
  322. Prolonged forward masking makes vowels mask consonants in impaired ears — ch. 17
  323. Auditory integration over time may involve intelligent selection of informative samples — ch. 17
  324. Comparing hearing-impaired and normal listeners requires controlling for both sensation level and absolute level — ch. 17
  325. Gap detection and amplitude modulation are usually intact after sensorineural loss — ch. 17
  326. Sensory neural hearing loss preserves temporal resolution when audibility is compensated — ch. 18
  327. Temporal processing of sound has three distinct measurable categories. — ch. 18
  328. Hearing loss extends internal masker persistence and shrinks duration benefits — ch. 18
  329. Pitch lacks a magnitude dimension, complicating its subjective measurement — ch. 19
  330. Period histograms visualize neural firing synchrony by spike phase — ch. 19
  331. Helmholtz’s place theory says pitch derives from the basilar membrane’s location of maximum excitation. — ch. 19
  332. Pitch arises from where along the cochlea a sound maximally stimulates — ch. 19
  333. Fundamental frequency is coded dually via harmonics and envelope rate — ch. 19
  334. Removing low harmonics from a complex tone leaves its pitch unchanged. — ch. 19
  335. Place coding poorly carries pitch when harmonics go unresolved. — ch. 19
  336. Physiological coding of frequency does not by itself explain perceived pitch. — ch. 19
  337. Pitch is formally defined as where sounds fall on a musical scale — ch. 19
  338. Helmholtz’s place theory failed to explain all pitch phenomena, prompting more complex models. — ch. 19
  339. The auditory system can extract pitch from resolved low-frequency harmonics using place patterns — ch. 19
  340. Pooled neural firing encodes stimulus period as spike intervals. — ch. 19
  341. Not all sounds have a pitch even though all have frequency content — ch. 19
  342. Auditory frequency is encoded by both place and temporal codes. — ch. 19
  343. Pure-tone temporal coding is low-frequency only, but complex tones use both fiber types. — ch. 19
  344. Harmonic amplitudes shape timbre and loudness but not pitch. — ch. 19
  345. Pitch can be derived from harmonic spacing even without the fundamental present. — ch. 19
  346. Harmonic tones are integer multiples of a fundamental frequency — ch. 19
  347. Sounds missing many harmonics still evoke a weak pitch sensation — ch. 20
  348. Fundamental frequency differences between voices improve speech intelligibility — ch. 20
  349. Resolved harmonics use place pitch coding while unresolved harmonics use temporal coding — ch. 20
  350. Increasing intensity improves frequency discrimination, much more at low frequencies — ch. 20
  351. At 1000 Hz humans detect frequency changes of about 0.2 percent — ch. 20
  352. Level-dependent frequency discrimination contradicts a purely temporal pitch code — ch. 20
  353. The mel scale defines pitch by assigning 1000 mels to a 1000-Hz tone — ch. 20
  354. Removing harmonics degrades f0 discrimination but it stays precise without them — ch. 20
  355. Voice differences include formant and temporal cues beyond fundamental frequency — ch. 20
  356. Sensorineural hearing loss worsens diplacusis, which even normal hearers have mildly — ch. 20
  357. Place and temporal codes each offer distinct neural mechanisms for extracting pitch — ch. 20
  358. FDL findings compromise a purely temporal account of low-frequency pitch. — ch. 20
  359. Random intensity variation disrupts place but not temporal pitch coding — ch. 20
  360. Modern pitch research relies on discrimination tasks because subjective pitch ratings are problematic — ch. 20
  361. Resolved low-numbered harmonics are required to encode pitch by place — ch. 20
  362. Same-sex background voices mask speech for listeners of either sex. — ch. 20
  363. The residue pitch refuted Helmholtz’s place theory of pitch percept. — ch. 20
  364. Pitch is coded by different mechanisms above and below roughly 3 kHz — ch. 20
  365. Physiological measures alone cannot prove how pitch perception works — ch. 20
  366. Listeners identify melodies perfectly using only temporal information because amplitude-modulated noise can encode pitch — ch. 20
  367. Stevens measured pitch shifts of up to 15-20% with changing intensity. — ch. 20
  368. Hearing impairment disrupts both place and temporal pitch codes — ch. 20
  369. Pitch cannot be measured absolutely, only relative to another tone — ch. 20
  370. Pitch may be jointly coded by temporal patterns and their cochlear location — ch. 20
  371. Hearing-impaired frequency discrimination does not correlate with audiogram or frequency selectivity — ch. 20
  372. The Weber fraction for frequency declines below 1500 Hz then rises above 2000 Hz — ch. 20
  373. Both place and temporal codes could underlie pitch, confounding identification of the main code — ch. 20
  374. Pitch strength is a distinct perceptual dimension absent from loudness — ch. 20
  375. The frequency-pitch mapping was established before models of pitch existed — ch. 20
  376. Sensorineural hearing loss damages pitch, harming speech-in-noise communication — ch. 20
  377. Hearing-impaired listeners usually hear the correct pitch but with more variability — ch. 20
  378. The existence region supports a place-based harmonic template model of pitch — ch. 20
  379. Temporal codes yield weak pitches compared to place codes — ch. 20
  380. Individual hearing-impaired listeners compensate by relying on whichever pitch code remains intact — ch. 20
  381. Audiograms and frequency selectivity fail to predict pitch perception deficits — ch. 20
  382. Reported pitch-with-intensity shifts vary widely with method — ch. 20
  383. Absolute frequency discrimination worsens as reference frequency increases — ch. 20
  384. Pitch has no magnitude like loudness, so magnitude scaling misapplies to it. — ch. 20
  385. Simultaneous synthetic vowels can be separated by their fundamental frequencies alone. — ch. 20
  386. Across-filter neural synchrony provides a robust pitch code — ch. 20
  387. Pitch of harmonic sounds is determined by the fundamental frequency. — ch. 20
  388. Pitch shifts with intensity but individual listener variability is large. — ch. 20
  389. Melodic interval identification degrades once about 9-10 harmonics are removed — ch. 20
  390. Place code governs pitch perception of pure tones above about 4 to 5 kHz — ch. 20
  391. Hearing loss disrupts pitch via place, temporal, and interaural mechanisms. — ch. 20
  392. Auditory nerve phase locking can encode slow waveform fluctuations across filters — ch. 20
  393. Raising intensity lowers pitch at low frequencies but raises it at high frequencies. — ch. 20
  394. Missing fundamental pitch survives even when cochlear distortion is masked out — ch. 20
  395. Pitch enables voice identification and the cocktail party listening effect — ch. 20
  396. Hearing loss disrupts pitch perception through multiple independent coding failures — ch. 20
  397. Experiments isolating two-ear advantages must present stimuli over headphones — ch. 21
  398. Ear separation on one axis makes horizontal binaural cues strongest — ch. 21
  399. High-frequency tones produce ambiguous azimuthal localization due to phase wrapping. — ch. 21
  400. Head shadow attenuates sound arriving at the far ear unless the source is centered — ch. 21
  401. The lateral superior olive compares ear intensities via excitation and inhibition — ch. 21
  402. Small detection-threshold gains amplify into much larger identification-level changes — ch. 21
  403. Two ears give small but consistent gains across all auditory tasks — ch. 21
  404. Interaural phase difference varies with frequency while interaural time difference does not — ch. 21
  405. Interaural level differences grow with frequency and side placement — ch. 21
  406. High-frequency tones yield multiple possible source locations from a single phase difference — ch. 21
  407. High-frequency sounds reflect off the head while low-frequency sounds diffract around it — ch. 21
  408. All sound locations sharing one ITD form an infinite cone of confusion — ch. 21
  409. Sound’s wavelength determines whether it reflects off the head or diffracts around it — ch. 21
  410. ITDs are frequency-independent physically yet frequency-dependent perceptually. — ch. 21
  411. Interaural level differences grow with frequency and reach up to 20 dB. — ch. 21
  412. Headphone experiments measure binaural summation by stimulating each ear independently — ch. 21
  413. Sound location is mapped with azimuth and elevation coordinates — ch. 21
  414. Binaural summation gives a consistent two-ears vs one-ear benefit — ch. 21
  415. The cone of confusion prevents up-down and front-back sound discrimination — ch. 21
  416. Rayleigh first proposed ILDs code high frequencies and ITDs code low frequencies — ch. 21
  417. Head movements and pinna shape resolve ambiguous sound localization — ch. 21
  418. Frontal minimum audible angle is about one degree for low frequencies — ch. 22
  419. Sound localization is most accurate when facing the sound source — ch. 22
  420. The just-detectable speaker shift defines the minimum audible angle. — ch. 22
  421. Antiphasic speech improves word identification by 20 percentage points at low SNRs. — ch. 24
  422. The auditory system lacks robust access to interaural phase above 1000 Hz — ch. 24
  423. Pinna cues drive the need for individualized HRTFs in vertical localization — ch. 24
  424. Horizontal-plane localization needs no listener-specific HRTF, but vertical does — ch. 24
  425. Head-related transfer functions encode all body-induced spectral and temporal sound changes — ch. 24
  426. Separating signal from masker locations improves detection through two binaural effects — ch. 24
  427. The first arriving sound wave dominates perceived localization regardless of level — ch. 24
  428. An 8 dB better-ear advantage can raise word identification by 56 percentage points — ch. 24
  429. Headphones allow separating interaural phase from interaural time delay — ch. 24
  430. Adding correlated noise across ears can improve rather than worsen monaural detection — ch. 24
  431. Pinnae shape the sound spectrum to encode elevation and front-back position — ch. 24
  432. Complex sounds allow envelope time-difference coding at high frequencies — ch. 24
  433. The better-ear advantage alone yields an 8 dB SRT benefit worth 56 percentage points — ch. 24
  434. Inverting signal phase at one ear vastly releases speech from masking. — ch. 24
  435. Interaural phase discrimination is finest at midline and low frequencies — ch. 24
  436. Headphone experiments reveal auditory abilities that free-field studies cannot expose. — ch. 24
  437. Head shadow gives one ear a better signal-to-noise ratio in typical listening — ch. 24
  438. Headphone studies reveal ILD perception abilities hidden by natural field acoustics — ch. 24
  439. Speech understanding benefits when the signal is phase-inverted at one ear. — ch. 24
  440. Interaural noise correlation inversely drives the magnitude of binaural release from masking. — ch. 24
  441. Separating a signal from a competing noise location aids detection beyond diotic summation — ch. 24
  442. A 5-dB hearing asymmetry doubles the perceived interaural level difference — ch. 25
  443. Three distinct perceptual phenomena define the precedence effect. — ch. 25
  444. Hearing-impaired listeners gain far less binaural-squelch advantage than normal hearers — ch. 25
  445. Cochlear damage disrupts temporal fine structure needed by the MSO — ch. 25
  446. Sensorineural hearing loss causes wide variability in sound localization ability — ch. 25
  447. Low sensation level impairs ITD and ILD discrimination even in normal listeners — ch. 25
  448. Asymmetrical-hearing-loss listeners must physically reposition to exploit their better ear — ch. 25
  449. Two ears yield summation, localization, and echo suppression jointly — ch. 25
  450. Even small hearing asymmetries across ears disrupt binaural hearing. — ch. 25
  451. Two ears improve detection, localization, and masking resistance over one. — ch. 25
  452. Hearing loss correlates weakly with precedence-effect echo thresholds. — ch. 25
  453. Echo-fusion thresholds vary widely among hearing-impaired listeners regardless of audiometric thresholds. — ch. 25
  454. Hearing-impaired listeners benefit roughly two-thirds less from binaural squelch than normal-hearing listeners. — ch. 25
  455. Hearing aids cannot restore sound localization because coding damage, not audibility, is the cause — ch. 25
  456. Degraded interaural timing coding, not audiometric asymmetry, explains reduced MLD in hearing loss. — ch. 25
  457. Restoring audibility does not restore sound localization in hearing loss — ch. 25
  458. Amplification cannot restore sound localization impaired by binaural encoding loss. — ch. 25
  459. The precedence effect reduces masking from reflections in rooms — ch. 25
  460. Head shadow makes high-frequency binaural cues inaudible in sloping hearing loss — ch. 25
  461. Binaural summation largely survives sensorineural hearing loss when sounds stay audible — ch. 25
  462. Whether loudness recruitment degrades speech perception remains unsettled — ch. 26
  463. Amplification only compensates for elevated thresholds, not other perceptual deficits from hearing loss. — ch. 26
  464. Frequency selectivity in normal-hearing listeners worsens at high sound levels — ch. 26
  465. The choice of hearing aid prescriptive rule barely affects speech intelligibility. — ch. 26
  466. Speech intelligibility depends on which frequency bands matter for specific materials. — ch. 26
  467. Tinnitus is the top service-connected military disability yet lacks any diagnostic test. — ch. 26
  468. Tinnitus pitch spans the entire region of hearing loss, not a single frequency — ch. 26
  469. ABLB laddergram rung divergence reveals whether loudness grows faster in an impaired ear — ch. 26
  470. Independent compression in each ear distorts binaural localization cues — ch. 26
  471. Nonlinear hearing aid amplification partially restores distorted loudness perception. — ch. 26
  472. Tinnitus loudness matches do not predict tinnitus annoyance or diagnostic value — ch. 26
  473. Loudness recruitment makes raised speech feel too loud even without abnormal sound perception — ch. 26
  474. Deficits at lower perceptual levels propagate upward through Erber’s hearing hierarchy — ch. 26
  475. Pitch perception deficits from hearing loss impair speech segregation from noise. — ch. 26
  476. Hearing aid algorithms distort auditory cues yet still improve speech understanding — ch. 26
  477. Directional hearing-aid microphones improve speech-in-noise SNR by over 7 dB. — ch. 26
  478. Tinnitus has no objective diagnostic test and is diagnosed by self-report alone — ch. 26
  479. Binaural sound lateralizes to the ear receiving the louder signal — ch. 26
  480. Hearing loss reduces the effect of inherent noise fluctuations on speech masking. — ch. 26
  481. Tinnitus loudness matches fall 5 to 15 dB above audiometric threshold — ch. 26
  482. WDRC processing distorts the temporal cues hearing-impaired listeners rely on for stop consonants — ch. 26
  483. Signal Detection Theory principles help audiologists extract true thresholds from feigning patients — ch. 26
  484. Behavioral psychoacoustics tests detect retrocochlear pathology poorly but rule out healthy ears well — ch. 26
  485. Hearing aids address three deficits but leave frequency, temporal, and pitch processing unaddressed. — ch. 26
  486. Audibility deficits must be corrected before supra-threshold factors can be studied. — ch. 26
  487. Re-instructing suspected feigners shifts their decision criterion toward true thresholds — ch. 26
  488. Pitch cues convey identity, intonation, and emotion beyond mere speech content — ch. 26
  489. Alternate binaural loudness balancing plots recruitment as non-parallel laddergram rungs — ch. 26
  490. Compression hearing aids distort spectral temporal and binaural cues in poorly understood ways — ch. 26
  491. Zero false positives during threshold testing signals feigned hearing loss — ch. 26
  492. Low-level auditory deficits cascade upward to impair speech comprehension — ch. 26
  493. Even slight hearing losses of 16-25 dB HL may benefit from hearing aids. — ch. 26
  494. Processing spectral peaks and valleys in separate compression channels erases their level difference — ch. 26
  495. Rollover signs make loud amplification harmful to retrocochlear patients — ch. 26
  496. Elevated hearing thresholds degrade speech perception by rendering key cues inaudible — ch. 26
  497. Hearing-impaired listeners show intact gap detection but prolonged forward masking that hides consonants — ch. 26
  498. Auditory processing disorder is a contested diagnosis lacking a single-locus definition — ch. 26
  499. Raising speech level reduces the advantage from masker fluctuation absence — ch. 26
  500. Hearing loss is a sensory-representation deficit, not merely an acoustic one. — ch. 26
  501. Directional hearing aid microphones can degrade sound localization by attenuating lateral sounds — ch. 26
  502. Audiology is rooted in psychoacoustics and remains founded on it — ch. 26
  503. More hearing aid compression channels measurably degrade vowel perception in hearing-impaired listeners. — ch. 26
  504. Precision medicine may soon tailor treatment to individual perceptual disorder profiles — ch. 26
  505. Contralateral interference reveals true thresholds about 15-20 dB below the interference level — ch. 26
  506. Word recognition that declines with louder speech signals retrocochlear pathology. — ch. 26
  507. A 1 dB SNR improvement boosts intelligibility by 7 to 19 percent — ch. 26
  508. A 1 dB SNR improvement raises speech intelligibility by 7 to 19 percent. — ch. 26
  509. Small amounts of hearing loss disproportionately impair speech-in-noise perception — ch. 26
  510. Tinnitus character signals underlying medical conditions — ch. 26
  511. Reduced dynamic range makes linear hearing aid amplification unsafe — ch. 26
  512. A missing audiometric shadow curve reveals feigned (non-organic) hearing loss. — ch. 26
  513. Speech reception thresholds closely duplicate averaged audiometric thresholds — ch. 26
  514. Central auditory processing diagnosis requires exclusionary peripheral and cognitive tests — ch. 26
  515. The audiogram fails as a robust indicator of perceptual deafness deficits — ch. 26
  516. Hearing aids often worsen rather than improve sound localization. — ch. 26

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