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Wavelet basis functions in biomedical signal processing

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J. Rafiee et al. / Expert Systems with Applications xxx (2010) xxx–xxx 3<br />

Power Spectral Density [V 2 /Hz]<br />

2000<br />

1800<br />

1600<br />

1400<br />

1200<br />

1000<br />

800<br />

600<br />

400<br />

200<br />

differences and cognitive-affective state, the underly<strong>in</strong>g constant<br />

shape of EEG <strong>signal</strong>s was of primary importance <strong>in</strong> this study<br />

and is not expected to vary between subjects.<br />

2.3. VPA <strong>signal</strong>s<br />

2000<br />

1500<br />

1000<br />

500<br />

0<br />

1 2 3 4 5<br />

0<br />

0 10 20 30 40 50<br />

Frequency (Hz)<br />

Fig. 3. Power spectrum density (V 2 /Hz) of EEG <strong>signal</strong>s recorded from one of the<br />

three channels of the data acquisition system.<br />

VPA is one of the most common measure for female sexuality<br />

and the application of VPA studies is <strong>in</strong> a broad variety of gynecology,<br />

such as female sexual arousal (Laan, Everaerd, & Evers, 1995),<br />

sexual function (Rosen et al., 2000), sexual dysfunction (Basson et<br />

al., 2004). The vag<strong>in</strong>al photoplethysmograph monitors the changes<br />

<strong>in</strong> backscattered light <strong>in</strong> the vag<strong>in</strong>al canal to reflect sexual arousal<br />

(Prause et al., 2005). An embedded light source, usually <strong>in</strong>frared,<br />

generates a light <strong>signal</strong> that is reflected back to a receiv<strong>in</strong>g photocell.<br />

The received <strong>signal</strong> is <strong>in</strong>terpreted as an <strong>in</strong>dex of vasocongestion,<br />

although it is likely to reflect several poorly-characterized<br />

physiological processes <strong>in</strong> the vag<strong>in</strong>a (Prause & Janssen, 2005).<br />

The <strong>signal</strong> pulses with heartbeats, which typically are around 60<br />

BPM <strong>in</strong> the laboratory, and slow waves concordant with breath<strong>in</strong>g<br />

rate are evident <strong>in</strong> many participants, which may be <strong>in</strong>fluenced by<br />

vag<strong>in</strong>al canal length.<br />

Two <strong>signal</strong>s are typically extracted: The first is the DC <strong>signal</strong>,<br />

which provides an <strong>in</strong>dex of the total amount of blood. The second<br />

is the AC <strong>signal</strong>, abbreviated as VPA, which reflects phasic changes<br />

<strong>in</strong> the vascular walls that result from pressure changes with<strong>in</strong> the<br />

vessels. Both <strong>signal</strong>s have been found to be sensitive to responses<br />

to erotic stimulation (Geer, Morokoff, & Greenwood, 1974). However,<br />

the construct validity of VPA is better established (Laan et<br />

al., 1995) and is used <strong>in</strong> this study. VPA was collected us<strong>in</strong>g the<br />

Biopac (Model MP100) data acquisition system. The <strong>signal</strong> is first<br />

band-pass filtered between 0.5 and 30 Hz. The sampl<strong>in</strong>g rate was<br />

fixed at 80 Hz.<br />

Us<strong>in</strong>g PSD, the frequency content of VPA <strong>signal</strong>s are depicted <strong>in</strong><br />

Fig. 5 for one specific subject. Low-frequency VPA from 20 subjects<br />

was recorded <strong>in</strong> six conditions. Each subject was tested watch<strong>in</strong>g a<br />

neutral movie followed by an erotic movie with normal blood alcohol<br />

levels (BAL), 0.025 BAL, and 0.08 BAL.<br />

3. Mother wavelet selection<br />

<strong>Wavelet</strong> (Daubechies, 1991) is a capable transform with a flexible<br />

resolution <strong>in</strong> both time- and frequency-doma<strong>in</strong>s, which can<br />

ma<strong>in</strong>ly be divided <strong>in</strong>to discrete and cont<strong>in</strong>uous forms; the former<br />

is faster because of low computational time, but the cont<strong>in</strong>uous<br />

type is more efficient and reliable because it ma<strong>in</strong>ta<strong>in</strong>s all <strong>in</strong>formation<br />

without down-sampl<strong>in</strong>g. Cont<strong>in</strong>uous wavelet transform of a<br />

<strong>signal</strong> sðtÞ 2L 2 ðRÞ can be def<strong>in</strong>ed as<br />

1=2 Z þ1<br />

<br />

CWTðt; xÞ ¼ x x 0<br />

¼hsðtÞ; wðtÞi<br />

1<br />

sðt 0 Þw <br />

x<br />

x 0<br />

<br />

ðt 0 tÞdt 0<br />

where himeans the <strong>in</strong>ner product of the <strong>signal</strong> and w 2 L 2 ðRÞnf0g<br />

which is usually termed the mother wavelet function. The mother<br />

wavelet function must satisfy the admissibility condition:<br />

0 c w ¼ 2p<br />

Z þ1<br />

1<br />

j^wðnÞj 2 dn<br />

jnj þ1<br />

and the ratio of x/x 0 is the scale factor. The mother wavelet is assumed<br />

to be centered at time zero and to oscillate at frequency x 0 .<br />

Essentially, Eq. (1) can be <strong>in</strong>terpreted as a decomposition of the <strong>signal</strong><br />

s(t 0 ) <strong>in</strong>to a family of shifted and dilated wavelets w[(x/<br />

x 0 )(t 0 t)]. The wavelet <strong>basis</strong> function w[(x/x 0 )(t 0 t)] has variable<br />

width with consideration to x at each time t, and is wide for<br />

small x and narrow for large x. By shift<strong>in</strong>g x(t 0 ) at fixed parameter<br />

x, the (x/x 0 )-scale mechanisms <strong>in</strong> the time response s(t 0 ) can be<br />

extracted and localized. Alternatively, by dilat<strong>in</strong>g x(t 0 ) at a fixed t,<br />

all of the multiscale events of s(t 0 )att can be analyzed accord<strong>in</strong>g<br />

to the scale parameter (x/x 0 ).<br />

In terms of frequency, low frequencies (high scales) correspond<br />

to global <strong>in</strong>formation of a <strong>signal</strong> (that usually spans the entire <strong>signal</strong>),<br />

whereas high frequencies (low scales) correspond to detailed<br />

<strong>in</strong>formation. In small scales, a temporally localized analysis is<br />

done; as the scale <strong>in</strong>creases, the breadth of the wavelet function <strong>in</strong>creases,<br />

result<strong>in</strong>g <strong>in</strong> analysis with less time resolution but greater<br />

frequency resolution. The wavelet <strong>functions</strong> are band-pass <strong>in</strong> nature,<br />

thus partition<strong>in</strong>g the frequency axis. In fact, a fundamental<br />

property of wavelet <strong>functions</strong> is that c = Df/f where Df is a measure<br />

of the bandwidth, f is the center frequency of the pass-band, and c<br />

is a constant. The wavelet <strong>functions</strong> may therefore be viewed as a<br />

bank of analysis filters with a constant relative pass-band.<br />

ð1Þ<br />

ð2Þ<br />

Fig. 4. Channel locations <strong>in</strong> EEG <strong>signal</strong>s.<br />

Please cite this article <strong>in</strong> press as: Rafiee, J., et al. <strong>Wavelet</strong> <strong>basis</strong> <strong>functions</strong> <strong>in</strong> <strong>biomedical</strong> <strong>signal</strong> process<strong>in</strong>g. Expert Systems with Applications (2010),<br />

doi:10.1016/j.eswa.2010.11.050

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