Psychoacoustics of Dynamic ‘Center-of-Gravity’ Signals

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Psychoacoustics of Dynamic ‘Center-of- Gravity’ Signals Larry Feth Ashok Krishnamurthy Ohio State University

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Psychoacoustics of Dynamic ‘Center-of-Gravity’ Signals. Larry Feth Ashok Krishnamurthy Ohio State University. Spectral Center-of-Gravity. Chistovitch and Lublinskaja (1976,1979) Perceptual Formant at ‘Center-of-Gravity’ Two-formant synthetic vowel - PowerPoint PPT Presentation

Transcript of Psychoacoustics of Dynamic ‘Center-of-Gravity’ Signals

Page 1: Psychoacoustics of Dynamic ‘Center-of-Gravity’ Signals

Psychoacoustics of Dynamic ‘Center-of-Gravity’ Signals

Larry FethAshok KrishnamurthyOhio State University

Page 2: Psychoacoustics of Dynamic ‘Center-of-Gravity’ Signals

Spectral Center-of-Gravity Chistovitch and Lublinskaja

(1976,1979)

Perceptual Formant at ‘Center-of-Gravity’

Two-formant synthetic vowel Matched by adjustable single-formant signal Center frequency of match depends on

relative amplitudes of the two formants

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Experimental Paradigm

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Chistovitch and Lublinskaja Results

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Voelcker Two-tone Signals

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Voelcker Two-tone Signals

Initially, led to the EWAIF model Envelope-Weighted Average of

Instantaneous Frequency (time domain) Point by point multiply E x F values Sum over N periods Divide by sum of weights

Indicates pitch change in periodic signals

Helmholtz (1954, 2nd English edition) Jeffress (1964)

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EWAIF Model

Signal ( ) with envelope ( )

instantaneous frequency ( ).

EWAIF (Envelope weighted

average of instantaneous frequency)

( ) ( )EWAIF[ ( )]

( )

x t e t

i t

e t i t dtx t

e t dt

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IWAIF Model Predictions

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Two-tone resolution task Feth and O’Malley (1977)

Two-tone resolution I = 1 dB; f independent variable ‘Voelcker-tone pair’ pitch discrimination inverted “u-shaped” psychometric

functions Components resolved beyond –75% point ~3.5 Bark separation = jnnd

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Voelcker Signal: Discrimination Task

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Discrimination Results

Jnnd – ‘Just not noticeable difference’

Filled circles Breakpoint estimates

Open circles CR – critical ratio CBW CB – ‘empirical’ CBW Solid line TW envelope

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IWAIF Model

Intensity Weighted Average of Instantaneous Frequency = Centroid of signal’s positive power spectrum (Anantharaman, et al., 1993)

2

2

20

20

( ) ( )IWAIF[ ( )]( )

| ( )|

| ( )|

e t i t dtx te t dt

f X f df

X f df

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Dynamic Center-of-Gravity Effect

Lublinskaja (1996) Three-formant synthetic Russian vowels Listeners identified vowels with:

‘conventional’ formant transitions co-modulated formant pairs that exhibit the same

dynamic spectral center-of-gravity ID functions were very similar with formant

pairs separated by 4.3 Bark or less

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Psychophysics

Anantharaman (1998) Two-tone signals with dynamic c-o-g

effect We called them ‘Virtual Frequency’

Glides Listeners matched transition rates in

VF glides to those in FM glides IWAIF model predicts results for

transitions from 2 to ~5 ERB

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Dynamic Center-of-Gravity Signals

Waveform

Long-term Spectrum

Spectrogram

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Rate-matching results

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Model Results

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Short-term running IWAIF Model

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IWAIF Model Results

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Application of ST-IWAIF Model

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More Psychophysics

Research Question(s) What is being ‘integrated’ in spectral

integration?OR

Where in the auditory system is the processing located?

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Psychophysics Iyer, et al., (2001)

Temporal acuity for FM and VF glides Step vs. linear ramp discrimination Similar T values may mean common

process

Masking patterns for FM and VF glides Peripheral process i.e., ‘Energy Masking’ Different results – VF not peripheral process

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Temporal Acuity Paradigm

Step (red) versus Glide (blue) transitions for FM tone (left panel) and Virtual Frequency (right panel)

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Temporal Acuity Results

Just discriminable step duration for FM (solid lines; filled symbols) and VF (dashed lines; unfilled symbols) signals. Frequency separations are 2, 5 and 8 ERBu. The results for 1000 Hz are represented by circles and those for 4000 Hz by triangles. Average for 4 listeners.

Frequency separation (ERBu)

2 ERBu 5 ERBu 8 ERBu

Step

Dur

ation

(mse

c)

0

2

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Dynamic Center-of-Gravity Maskers

Masking of brief probe by FM glide (left panel) and by VF glide (right panel). Probe is in the spectro-temporal center of each masker. Five auditory filter bands are illustrated.

Time

Fl

Fc

Fh

Time

Fl

Fc

Fh

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Masking Results

Masking of a 20 ms probe by FM (light blue) and VF (darker blue) maskers. The probe is placed at the beginning, middle, and end of the masker. Significant differences are seen at 5 and 8 ERB for the middle position and the initial position at 8 ERB. Average for 4 listeners.

Probe in initial position

0.00

5.00

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30.00

35.00

2 ERBu 5 ERBu 8 ERBu

Frequency separation

Am

ou

nt

of

Ma

sk

ing

(d

B S

PL

)

FM Masker

VF Masker

Probe in medial position

0.00

5.00

10.00

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35.00

2 ERBu 5 ERBu 8 ERBu

Frequency separation

Am

ount

of M

aski

ng (d

B SP

L)

FM Masker

VF Masker

Probe in final position

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35.00

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Frequency separation

Am

ount

of M

aski

ng (d

B S

PL)

FM Masker

VF Masker

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Glide Direction Asymmetry Gordon and Poeppel

3 Frequency ranges: (for F1,F2 & F3) ~ 30 unpracticed listeners 20 trials / signal One interval Direction Identification: Up vs. Dn

Best results at high frequency (F3) range 10- through 160 ms ‘Up’ is easier to ID than ‘Dn’ Less clear-cut results at low or mid-freq. ranges

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Glide Direction Asymmetry

Gordon and Poeppel – ARLO (2002)Identification of FM Sweep direction is easier for rising than for

falling tones.

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Glide Direction Asymmetry Dawson, (2002)

Tested only high frequency range (F3) Practiced listeners; ~ 100% all

conditions! Modified procedure

Rove each frequency sweep over 1 octave

Practice to ~ asymptote

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Glide ID Results Average for 4

listeners One-interval ID task 250 trials / datum

point Well-practiced Subj’s Starting frequency

roved over 1-octave range

Summary FM ‘easier’ than VF Up ‘easier’ than Down

Duration (ms)

5 10 20 30 40 50 80 160

Perc

ent C

orre

ct Id

entif

icat

ion

50

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FM Up

FM Down

VF Up

VF Down

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CV Identification Experiment

[da] – [ga] continuum: varying F3 transition Duration: 50 ms transition into 200 ms base F3 onset: 2018 to 2658 Hz in 80 Hz steps F3 base: 2527 Hz (constant)

Formant transition ‘type’: Klatt synthesizer Frequency Modulated tone glide Virtual Frequency glide

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CV Identification: Stimuli

Spectrogram 1. Step 1 of Klatt Monaural Continuum—/ga/ endpoint

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CV Identification: Stimuli

Spectrogram 2. Step 1 of FM Monaural Continuum—/ga/ endpoint

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CV Identification: Stimuli

Spectrogram 3. Step 1 of VF Monaural Continuum—/ga/ endpoint

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CV Identification: Stimuli

Spectrogram 4. Step 1 of Dichotic FM Continuum—/ga/ endpoint

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CV Identification: Stimuli

Spectrogram 5. Step 1 of Dichotic VF Continuum—/ga/ endpoint

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CV Identification Experiment

Listeners: 8 adults with normal hearing

Procedure: One interval, 2-AFC 3 transition types: Klatt, FM or VF 6 of 8 tokens tested 20 repetitions / token

Results are averaged for the 8 listeners

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CV Identification: Results

Fig. 4. Mean Responses for FM Tone and Virtual Glide Conditions

Formant 3 Onset Frequency (in Hz)

1900 2000 2100 2200 2300 2400 2500 2600 2700

% /

da

/ R

esp

on

ses

0

20

40

60

80

100FM

Virtual Glide

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CV Identification: ResultsFig. 7. Mean Responses for Dichotic Condition

F3 Onset Frequency (Hz)

1900 2000 2100 2200 2300 2400 2500 2600 2700

% /d

a/ R

espo

nses

10

20

30

40

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Klatt

FM

Virtual Glide

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Psychoacoustics of Dynamic ‘Center-of-Gravity’ Signals

Conclusions ‘Excitation’ is integrated not signal

energy The processing is central not peripheral

Masking Patterns are very different Temporal Acuity results are similar for FM & VF

glides Direction ID Asymmetry is similar for FM & VF

glides

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Psychoacoustics of Dynamic ‘Center-of-Gravity’ Signals

Conclusions CV identification functions are similar for:

Klatt synthesized sounds FM formant sounds VF formant sounds

Thus, it doesn’t matter how ‘excitation’ is moved from A to B, the brain will interpret it as the same sound.

The effect is evident under dichotic listening; further support for central processing.

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Collaborators

Rob FoxNandini Iyer

Jayanth Anantharaman

Ewa Jacewicz Robin Dawson

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Psychoacoustics of Dynamic ‘Center-of-Gravity’ Signals

Thank You

Questions?

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Up vs. Down FM Glide

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Up vs. Down FM Glide

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Up vs. Down VF Glide

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Up vs. Down VF Glide

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Effect of Masker Direction

Masking produced by VF (above) and FM (below) maskers with F = 5 ERB. Purple bars are “up” glides; yellow bars are “down” glides. Centered probe.

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Effect of Masker Position

Masking produced by VF (above) and FM (below) maskers with F = 5 ERB. Purple bars are “up” glides; yellow bars are “down” glides.

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Klatt & FM Parameters

Fig. 1. Formant 3 Transitions for Klatt and FM Tokens

Time (ms)

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Fre

qu

ency

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2700

Step 1 (/ga/ endpoint)Step 2 Step 3 Step 4 Step 7 Step 8 (/da/ endpoint)

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Virtual Frequency Parameters

Fig. 2. Tone Amplitude Changes in Step 1 (/ga/) of VG Continuum (2018 Hz virtual onset)

Time (ms)

0 10 20 30 40 50 60

Rel

ativ

e A

mpl

itud

e

0.0

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1.0 Tone 1 (2018 Hz)Tone 2 (2658 Hz)

Fig. 3. Tone Amplitude Changes in Step 8 (/da/) ofVG Continuum (2578 Hz virtual onset)

Time (ms)

0 10 20 30 40 50 60

Rel

ativ

e A

mpl

itud

e

0.0

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Tone 1 (2018 Hz) Tone 2 (2658 Hz)