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Adaptive AM–FM Signal Decomposition With Application to ... - ICS

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292 IEEE TRANSACTIONS ON AUDIO, SPEECH, AND LANGUAGE PROCESSING, VOL. 19, NO. 2, FEBRUARY 2011<br />

etc., and , where is the conjugate opera<strong>to</strong>r.<br />

This model is an extension <strong>to</strong> the classic harmonic model<br />

in which the term is omitted [27]. As a result, it follows<br />

that the signal in (1) is projected on<strong>to</strong> the complex exponential<br />

functions, as in the simple harmonic case, and <strong>to</strong> functions of<br />

type . It is worth noting that the model in (1) can also<br />

be written for nonharmonically related frequency components.<br />

Therefore, a more general model can be expressed as<br />

(2)<br />

where will be referred <strong>to</strong> as initial estimates of the frequencies<br />

that will be considered <strong>to</strong> be known. Initial frequencies<br />

(or ) are considered <strong>to</strong> be known but not necessary optimal<br />

in representing the input signal in the mean squared error sense.<br />

For speech as well as for music signals, this is quite often the<br />

case.<br />

Assuming that the speech signal is defined on ,<br />

the estimation of the model parameters<br />

is<br />

performed in<strong>to</strong> two steps. At first, the fundamental frequency,<br />

and the number of harmonic components, , are estimated<br />

using spectral and au<strong>to</strong>correlation information as described in<br />

[27]. Then, the computation of is performed<br />

by minimizing a mean squared error which leads <strong>to</strong> a simple<br />

least squares solution [27]. The same procedure is applied if<br />

the initial estimates of frequencies are not restricted <strong>to</strong> be<br />

multiples of a fundamental frequency. In this case, frequencies<br />

may be obtained by peak picking the magnitude spectrum of<br />

the Fourier transform of the input signal as suggested in [24].<br />

In the following, we will not restrict the analysis <strong>to</strong> ,<br />

unless otherwise mentioned.<br />

From (2), it is easily seen that the instantaneous amplitude of<br />

each component is a time-varying function given by<br />

where and denote the real and the imaginary parts of ,<br />

respectively.<br />

Since both the amplitudes and the slopes are complex<br />

variables, the instantaneous frequency of each component is not<br />

a constant function over time but varies according <strong>to</strong><br />

while the instantaneous phase is given by<br />

A feature of the model worth noting is that the second term of<br />

the instantaneous frequency in (4) depends on the instantaneous<br />

(3)<br />

(4)<br />

(5)<br />

Fig. 1. Projection of b<br />

component.<br />

in<strong>to</strong> one parallel and one perpendicular <strong>to</strong> a<br />

amplitude. In other words, the accuracy of the frequency estimation<br />

(or, the estimation of phase function) depends on the amplitude<br />

information [28].<br />

B. Frequency-Domain Properties of QHM<br />

To understand the important features of QHM, we suggest<br />

discussing its frequency domain properties. To this end, let us<br />

consider the Fourier transform of in (2)<br />

where is the Fourier transform of the analysis window,<br />

, and is the derivative of over . For simplicity,<br />

we will only consider the th component of<br />

To reveal the main properties of QHM, we suggest the projection<br />

of on<strong>to</strong> as illustrated in Fig. 1. Accordingly,<br />

where denotes the perpendicular (vec<strong>to</strong>r) <strong>to</strong> , while<br />

and are computed as<br />

and<br />

Thus, the th component of can be written as<br />

Considering the Taylor series expansion of<br />

we obtain<br />

(6)<br />

(7)<br />

(8)<br />

(9)<br />

(10)<br />

(11)<br />

(12)

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