- Research
- Open Access

# Basis approach to estimate the instantaneous frequencies in multicomponent AM-FM signals

- Mohammadali Sebghati
^{1}, - Hamidreza Amindavar
^{1}Email author and - James A Ritcey
^{2}

**2014**:8

https://doi.org/10.1186/1687-4722-2014-8

© Sebghati et al.; licensee Springer. 2014

**Received: **22 October 2013

**Accepted: **20 February 2014

**Published: **5 March 2014

## Abstract

In this paper, an analytical approach to estimate the instantaneous frequencies of a multicomponent signal is presented. A non-stationary signal composed of oscillation modes or resonances is described by a multicomponent AM-FM model. The proposed method has two main stages. At first, the signal is decomposed into its oscillation components. Afterwards, the instantaneous frequency of each component is estimated. The decomposition stage is performed through the basis expansion exploiting orthogonal rational functions in the complex plane. Orthogonal rational bases are generalized to expand linear time-varying systems. To decompose the non-stationary signal, its equivalent time-varying system is sought. The time-varying poles of this system are required to construct appropriate basis functions. An adaptive data segmentation algorithm is provided for this purpose. The effect of noise is scrutinized analytically and evaluated experimentally to verify the robustness of the new method. The performance of this method in extraction of embedded instantaneous frequencies is asserted by simulations on both synthetic data and real-world audio signal.

## Keywords

## 1 Introduction

Non-stationary signals which are a compound of constituents with time-varying amplitudes and frequencies can be characterized by amplitude-modulated frequency-modulated (AM-FM) models. This modeling is attended to express genuine signals in communications [1, 2], acoustic and speech processing [3–6], biomedical signal processing [7], and image processing [8]. To estimate instantaneous amplitudes (IAs) and instantaneous frequencies (IFs) embedded in a multicomponent signal [9], the first step is decomposing it into oscillation components. This procedure is termed ‘demodulation’, ‘separation’ or ‘decomposition’ in the literature. Each component should represent a valid oscillation for which the definition of instantaneous frequency is physically meaningful [10].

All methods of multicomponent AM-FM signal decomposition and parameter estimation can be categorized into non-parametric and parametric methods. One class of non-parametric approaches is based on the joint time-frequency processing. Widespread time-frequency distributions (TFDs) such as short-time Fourier transform (STFT), Wigner-Ville distribution, and Choi-Williams distribution are employed [11]. These methods are limited by the well-known compromise between time and frequency resolution. Moreover, the cross-terms appear troublesome. The energy separation algorithm (ESA) which uses a non-linear differential operator, called Teager-Kaiser energy operator (TKEO), is another method [12]. The energy separation algorithm which tracks the energy of the source producing the signal is originally applicable for monocomponent AM-FM signals. Nevertheless, they are modified for application in multicomponent cases by designing a bank of filters. Multiband-ESA (MESA) that consists of bandpass filtering followed by monocomponent energy separation is introduced based on this concept [13]. The separation performed by bandpass filtering is proper when components are spectrally far enough.

Huang et al. [14] proposed an iterative technique known as the empirical mode decomposition (EMD). This technique is an algorithmic way to extract oscillation modes embedded in the signal, named intrinsic mode functions (IMFs). Each IMF gives a valid IF which is estimated by applying the Hilbert transform (HT) [14]. The proposed algorithm for the implementation of EMD called the sifting process showed several drawbacks such as sensitivity to perturbation and mode mixing problem [15]. To overcome these difficulties, the original EMD is modified, and a new algorithm is developed which is named ensemble empirical mode decomposition (EEMD) [15]. This method is indeed the iteration of EMD for noise-added signals. In each iteration, controlled white noise is added to the data, and EMD is applied. Each individual trial may generate noisy results, but the noise is canceled out by taking the average of the results. Thus, true solution is the ensemble mean of enough trials. Although each trial produces a set of IMFs, the sum of IMFs is not necessarily an IMF. An empirical solution for this issue is suggested in [15]. EMD and EEMD methods suffer from the lack of analytic foundation. Some research has attempted to establish and improve analytical aspects of these empirical approaches [16]. In [17], an alternative algorithm for EMD is introduced based on iterating certain filters, such as Toeplitz filters. The results of iterative filtering are similar to those of the conventional sifting process. Although the authors of [17] do not claim superiority for their method, it lays down a mathematical framework for an alternative approach to EMD. The convergence of iterative filtering EMD is studied in [18]. A variant of EMD to decompose multiscale data is proposed in [19]. This work provides some theoretical understanding of EMD for a class of multiscale data and introduces two algorithms, Newton-Raphson-based EMD and ODE-based EMD, as the variations of the sifting process. The decomposition of multiscale data based on EMD is pursued in [20] inspired by the compressed sensing theory. The sparsest representation of multiscale data is sought within the largest possible dictionary constructed of IMFs. The problem is formulated as a non-linear *L*^{1} optimization, and an iterative algorithm is proposed to solve it. Noise and perturbation in data may cause numerical instability in this method. Daubechies et al. developed a method which captures the philosophy of EMD and decomposes special functions in a defined class [21]. This method employs a combination of wavelet analysis and reallocation technique called synchrosqueezing transform which aim to sharpen a time-frequency representation. Synchrosqueezed wavelet transform is also investigated for signal sampling and denoising applications in multicomponent signal analysis [22]. In [23], an algorithm for AM-FM parameter estimation is proposed based on the iterated application of the Hilbert transform to amplitude envelopes obtained by adaptively low-pass filters. Furthermore, the IF of AM-FM components can be calculated by *a posteriori* adaptive segmentation of the acquired phase signal. Another iterative AM-FM decomposition is suggested in [24] using the quasi-harmonic model (QHM) for quasi-harmonic signals such as voiced speech.

There are various parametric approaches to extract IFs of multicomponent signals. One common approach is based on signal segmentation, while some simplifying assumptions such as constant frequency seem logical in each segment. Then, an estimator is designed to estimate the model parameters segment by segment. In [25], the maximum windowed likelihood (MWL) criterion is used to estimate the AM-FM components. The high non-linearity of this method makes the necessary optimization difficult. Another parametric approach is based on the statistical modeling of the signal according to its statistical attributes and assumptions. Speech signals are statistically modeled as AM-FM signals, and the extended Kalman filter (EKF) is applied for demodulation [3]. The idea of EKF is also exploited in [26]. Polynomial phase signal (PPS) modeling is another parametric approach which is employed for AM-FM signals [27].

The interpretations and estimation of instantaneous frequencies embedded in a multicomponent signal have been controversial [28]. Three different approaches are proposed to estimate the IFs after the decomposition stage. In the first approach, the Hilbert transform is exploited to get the analytic signal whose phase is differentiated to find the IF [10]. The energy operator (TKEO) is utilized in the second approach [12], and the third one is based on TFD [11, 29]. Different definitions of IF are considered in these approaches, and consequently, their results are not necessarily equivalent. In [28] and [30], the different definitions and estimation methods are compared and discussed. The main contribution of this paper is to develop a novel approach based on the expansion of time-varying systems by orthogonal rational functions. The method introduced in [31] is extended and improved to be applied as the essence of the new method for IF estimation. An adaptive segmentation procedure in the proposed algorithm allows us to estimate the IFs locally. The decomposition is performed using orthogonal rational functions.

## 2 Problem statement

*N*

_{c}is the number of components.

*A*

_{ k }(

*t*) and

*θ*

_{ k }(

*t*) are time-varying envelope and time-varying phase of the

*k*th component respectively, and the instantaneous frequency denoted by

*f*

_{ k }(

*t*) is defined from

*θ*

_{ k }(

*t*) :

*x*(

*t*):

*g*

_{ k };

*k*= 1, 2, ⋯,

*K*} should represent the oscillation modes in signal, for which the instantaneous frequency is meaningfully definable. Accordingly, each term represents a valid IF of the multicomponent signal. The main idea to attain such decomposition is expanding the corresponding system of the AM-FM signal in the complex plane. Since the transfer function of a realistic linear system has a rational representation, it can be expanded by orthogonal rational functions in the complex

*z*-plane. Returning back to the time-domain, each rational function is equivalent to a generalized exponential basis and represents one valid oscillation term or resonance. To perform this procedure, we should specify the generating system of the AM-FM signal. The corresponding system of a non-stationary signal is modeled by a linear time-varying (LTV) system [32]. LTV models have been applied to describe non-stationary signals [33, 34]. Our proposed method is developed based on this approach of modeling. Let us consider the discrete-time AM-FM signal

*x*[

*n*], obtained by time sampling of

*x*(

*t*) at the rate of

*f*

_{s}. Its generating system is modeled as a LTV system, which can be described by a bivariate function to characterize the input-output linear relationship [32]. Hence, a bivariate discrete-time impulse response,

*h*[

*m*,

*n*], is considered, where

*n*and

*m*are two independent time instants, representing the time variable of the signal and the time variable of the system, respectively. Taking the

*Z*-transform of

*h*[

*m*,

*n*] with respect to the time variable of the signal,

*H*(

*m*,

*z*) is obtained which denotes the generating system of

*x*[

*n*]. The orthogonal rational basis has been investigated for the decomposition of linear time-invariant (LTI) systems [35] and should be generalized to expand the time-varying generating system of the AM-FM signal as follows:

where {*G*_{
k
}(*m*, *z*);*k* = 1, 2, ⋯, *K*} is a rational basis. Fortunately, to find the orthogonal rational functions for system expansion, it is not necessary to have the system’s transfer function with all the details. The knowledge of poles or logical assumptions about them are sufficient to extract a proper basis [35].

## 3 Orthogonal rational functions

*a priori*information to describe the desired space being spanned by a rational basis. Let us consider a set of

*M*time-varying poles, {

*ξ*

_{ k }[

*m*],

*k*= 1, …,

*M*}. We can make a first-order IIR transfer function by each pole. So, a basis set is constructed including all specified poles, but not orthogonal. The Blaschke products [35] formed by these poles are two-dimensional functions,

*z*, two-dimensional functions are obtained:

*z*in the complex domain. The inner product of each pair of these functions is a function of time,

*m*:

Utilizing the Cauchy integral implies that *d*_{
kl
}[ *m*] is zero at each snapshot, *m*, for *k* ≠ *l*. Taking the inverse *Z*-transform of *G*_{
k
}(*m*, *z*) produces *g*_{
k
}[ *m*, *n*]. Since the *Z*-transform and its inverse are homomorphic transforms, these functions would preserve orthogonality with respect to *n*. Two problems remain to be studied. At first, the underlying time-varying poles of the corresponding LTV system should be determined. Secondly, univariate terms should be extracted from bivariate functions, *g*_{
k
}[ *m*, *n*], to express the oscillation modes of *x*[ *n*]. These issues are resolved simultaneously by adaptive segmentation which is addressed in the following section.

## 4 Time-varying modeling

*x*[

*n*], is modeled by a time-varying autoregressive (TVAR) of order

*M*:

{*a*_{
m
}[ *n*], *m* = 1, …, *M*} are the time-varying parameters, and *ν*[ *n*] is the zero-mean innovation process, also addressed as a modeling error. The most general case of this model is where the parameters are completely uncorrelated at each time sample. Therefore, each time sample of *x*[ *n*] would be represented by *M* unknown coefficients; hence, it is not a practical approach. Based on a common practical assumption, the non-stationary signal is approximately regarded locally stationary or quasi-stationary. This assumption implies that the parameters of the TVAR model are correlated, and the coefficients are supposed to be constant in subintervals of the total time span, referred to as segments. This model is called a block stationary AR model [34]. For multicomponent AM-FM signals whose IAs and IFs are slowly time-varying or piecewise-constant, the segmentation strategy is applicable. By virtue of this assumption, a real multicomponent AM-FM signal over its support is considered as a superposition of temporarily more limited signals with constant frequencies. These intervals can generally have various lengths, and different methods from fixed-length windowing to adaptive segmentation algorithms are introduced to determine the borders of the segments [23]. In the proposed method, the segmentation is performed adaptively from the aspect of TVAR parameter estimation.

### 4.1 Segmentation procedure

*N*samples is segmented into

*L*blocks with various lengths:

*ℓ*= 1, …,

*L*and

*n*

_{0}= 0. The TVAR coefficients are supposed to be constant in each segment. The mean square error in the

*ℓ*th segment is given by

where {*a*_{ℓ, m}, *m* = 1, …, *M*} are the TVAR coefficients of the *ℓ* th segment. The boundaries of each segment are determined such that the error *J*_{
ℓ
} remains under a specified threshold. The segmentation algorithm operates as follows. At the start of each stage, the length of the current segment (say *ℓ*) is considered the minimum possible length, equal to the order of the TVAR model, i.e., *n*_{
ℓ
} = *n*_{ℓ-1} + *M*. The TVAR coefficients, *a*_{ℓ, m}, are estimated by the recursive least squares (RLS) technique, and the error in (10) is computed. If it is still greater than the pre-specified threshold, the length of the segment increases by one sample, and the calculations are repeated. This procedure continues by one-sample increment in each stage until the error falls below the threshold. Now, the boundaries and the length of the current segment are determined, and the procedure starts over the next time sample for another segment establishment. This algorithm runs through the entire signal repeatedly and stops at the end of the data batch. The question arises here about the threshold setting and how it can affect the accuracy of the IF estimation. This issue is scrutinized in the succeeding subsection separately. Once the TVAR parameters are estimated, the corresponding time-varying poles, denoted by {*ξ*_{
k
}[ *m*], *k* = 1, …, *M*}, are obtained by applying the *Z*-transform of (8) with respect to *n*.

### 4.2 Error analysis

*ε*

_{ θ }, sets off an error in signal:

*e*[

*n*] whose instantaneous amplitude is absolute error of modeling is also an AM-FM signal:

*η*[

*n*] such that |

*e*[

*n*] | is restrained lower than it, i.e., |

*e*[

*n*] | <

*η*[

*n*]. If we substitute |

*e*[

*n*] | by (16), the following inequality holds:

*η*[

*n*] is constant over the entire signal, larger phase errors can occur when IA becomes smaller. Therefore, the threshold should vary adaptively, adjusted to the envelope of the observed signal. In other words, the locally normalized error for each segment is a proper threshold. Since the IA evolves slowly, its mean or minimum amount during the segment can be utilized for normalization. The normalized threshold is denoted by $\stackrel{\u0304}{\eta}$ for brevity:

*ε*[

*n*] | is obtained from (15):

*ε*

_{ θ }) under control, the error of IF is consequently controlled. By definition (2), IF is the derivative of instantaneous phase, which is a difference equation in the discrete-time situation:

where *ω*[ *n*] = 2*π* *f*[ *n*] is the instantaneous frequency in radian per second, and *T*_{s} denotes the sampling time. In the worst case, the maximum phase errors of two consecutive instants accumulate. Thus, the maximum error of IF is 2*ε*_{
θ
}*f*_{s}. For example, if $\stackrel{\u0304}{\eta}=1{0}^{-3},$ then from (21), the maximum phase error is almost 10^{-3}, and the absolute error of IF is at most 0.2*%* of the sampling frequency. This error can be controlled by arbitrary selection of $\stackrel{\u0304}{\eta}.$ A smaller threshold leads to wider segments, in which the assumption of constant frequency is no longer respected. Our experiments verified that the condition of piecewise-constant frequency for slowly varying IFs is satisfied for $\stackrel{\u0304}{\eta}$ in the order of 10^{-3}∼10^{-2}.

## 5 Estimation framework

*G*

_{ k }(

*m*,

*z*) in (6). Then, bivariate functions, {

*g*

_{ k }[

*m*,

*n*],

*k*= 1, …,

*M*}, are produced by taking the inverse Z-transform. Now, the one-dimensional basis is extracted from the existing bivariate functions to achieve a one-dimensional expansion for

*x*[

*n*] as in (3). The basis

*g*

_{ k }[

*n*] is constructed by the concatenation of truncated pieces of bivariate functions,

*g*

_{ k }[

*m*,

*n*], based on the result of the segmentation procedure:

where *L* is the number of total segments, and *W*_{
ℓ
}[ *n*] is an arbitrary weighting window over the *ℓ* th segment. It is supposed that during this block, the corresponding pole remains equal to *ξ*_{
k
}[ *m*_{
ℓ
}]. Each resultant function, *g*_{
k
}[ *n*], is a valid oscillation mode for which IF is definable. Thus, the estimation of the embedded IFs is achieved through the IF estimation of the extracted functions. To estimate the IF, linear regression of the phase for each segment is computed by applying the weighted linear least squares technique on a first-order polynomial model. The abrupt changes in the phase which can affect the IF estimation severely are an important issue. While the consecutive segments derived from different rows of *g*_{
k
}[ *m*, *n*] are concatenated, there may be some phase discontinuities over the resultant bases in the junctions of segments. Such discontinuities in the phase trajectory cause serious deficiency in the IF estimation which appears as spikes over the resultant IFs. To remedy this problem, a proper data window such as the Hamming window is chosen as *W*_{
ℓ
}[ *n*] in (23), which controls the effect of borderline samples. The Hamming window is commonly utilized as an analysis window in audio and speech processing [24, 27].

*M*) is twice the number of components (

*N*

_{c}). Nonetheless, to improve the estimation of time-varying poles in the presence of noise, we should have

*M*>2

*N*

_{c}. Therefore, extraneous poles appear besides the valid poles. A minimum distance classifier [38] is applied to assign the poles of the resonances in each segment and distinguish them from the invalid poles. The perturbation of the poles due to the estimation error of TVAR coefficients is investigated mathematically in the succeeding section. The steps of the proposed algorithm are summarized as follows:

- 1.
Adaptive segmentation of the AM-FM signal based on TVAR modeling and computation of underlying time-varying poles.

- 2.
Assignment of the poles to the components by minimum distance classifier.

- 3.
Employing the time-varying poles to construct oscillation terms,

*g*_{ k }[*n*]. - 4.
Fitting a linear model to the phase of each segment of

*g*_{ k }[*n*] to estimate the IF.

In this novel method of IF extraction, the Hilbert transform that is a global operator is not employed. Additionally, a linear model is applied to the phase of components segment by segment in spite of differentiating throughout. It makes the proposed method less sensitive to phase changes. Therefore, the adaptive segmentation is advantageous for both decomposition and frequency estimation.

## 6 Pole perturbation

*p*(

*ℓ*,

*z*) be the polynomial of AR model in the

*ℓ*th segment whose roots are time-varying poles:

*a*

_{ℓ,0}= 1. If the perturbation

*Δ*

*a*

_{ℓ,i}occurs in the

*i*th coefficient,

*a*

_{ℓ,i}, the polynomial (24) changes to

*ξ*

_{ k }[

*m*

_{ ℓ }] by

*Δ*

*ξ*

_{ k }[

*m*

_{ ℓ }], which may be real or complex. Let us denote the perturbed roots by ${\stackrel{~}{\xi}}_{k}\left[\phantom{\rule{0.3em}{0ex}}{m}_{\ell}\right]={\xi}_{k}\left[\phantom{\rule{0.3em}{0ex}}{m}_{\ell}\right]+\Delta {\xi}_{k}\left[\phantom{\rule{0.3em}{0ex}}{m}_{\ell}\right]\phantom{\rule{0.3em}{0ex}}:$

*k*th pole and its perturbation are denoted by

*ξ*

_{ k }and

*Δ*

*ξ*

_{ k }, respectively, and their arguments are neglected for brevity. When

*Δ*

*ξ*

_{ k }→ 0, the above equation is simplified by employing Taylor’s expansion:

*p*

^{′}(

*ℓ*,

*z*) is the first derivative of

*p*(

*ℓ*,

*z*) with respect to

*z*. This equation expresses the linear relation between perturbation in poles and perturbation in coefficients:

*Δ*

*a*

_{ℓ,i}and

*Δ*

*ξ*

_{ k }as random variables, their variances, respectively ${\sigma}_{{a}_{\ell ,i}}^{2}$ and ${\sigma}_{{\xi}_{k}}^{2}$, are related linearly,

*p*

^{′}(

*ℓ*,

*ξ*

_{ k }) from (24), the ratio of the variances is given by

*ξ*

_{ k }| < 1,

*k*= 1, …,

*M*, the ratio in (30) takes its maximum value for

*i*=

*M*. This means that the perturbation in the coefficient of the highest order in the polynomial has the most effect on misplacing the poles. This maximum value for each pole is defined as its variance ratio:

*γ*_{
k
} is the variance ratio of *ξ*_{
k
} which indicates the robustness of this pole. This parameter only depends on the positions of the underlying poles, which are determined by AM-FM signal characteristics.

## 7 Experimental evaluation

The proposed method is implemented on both synthetic and real-world signals, and its performance is compared to the results of two previously introduced methods.

### 7.1 Synthetic data

*α*

_{1}= -2,

*β*

_{1,1}= 10

^{3},

*β*

_{1,2}= 5 × 10

^{3},

*β*

_{1,3}= -20 × 10

^{3}and

*α*

_{2}= -5,

*β*

_{2,1}= 5 × 10

^{3},

*β*

_{2,2}= - 3 × 10

^{3},

*β*

_{2,3}= 0. The two following IFs are embedded in this AM-FM signal:

*T*

_{s}= 50

*μ*s intervals, so the sampling frequency is

*f*

_{s}= 20 kHz. Since the absolute values of the instantaneous frequencies increase over time, a limited span of signal is observed to avoid aliasing. The algorithm is run over

*N*= 2,000 samples of the signal. The corresponding system has four time-varying complex poles {

*ξ*

_{1}[

*m*], …,

*ξ*

_{4}[

*m*]} in conjugate pairs. There are two conjugate pairs, and each pair represents one oscillation component. Consequently, four complex functions,

*g*

_{1}[

*n*], …,

*g*

_{4}[

*n*], are extracted whose phases yield desired IFs.

*g*

_{1}[

*n*] and

*g*

_{2}[

*n*] are common resonances, which means that their IFs have equal absolute values, but opposite signs.

*g*

_{3}[

*n*] and

*g*

_{4}[

*n*] determine the second IF likewise. The adaptive segmentation procedure divides the data batch into

*L*= 45 segments with different lengths. The threshold of error in the segmentation procedure is set to 0.001. The coefficients of the TVAR model and, accordingly, the time-varying poles are estimated through the RLS algorithm with the forgetting factor of 0.98. Figure 1 demonstrates the estimated IFs denoted by ${\widehat{f}}_{i};i=1,2$ besides the original IFs. ${\widehat{f}}_{1}$ and ${\widehat{f}}_{2}$ track the original IFs very closely. The step-like variation, produced by segmentation, is obvious. For quantitative evaluation, the relative mean absolute error (MAE) of IF estimation is computed for ${\widehat{f}}_{1}$ and ${\widehat{f}}_{2},$ and illustrated in Tables 1 and 2, respectively.

**Relative MAE (%) for the estimation of the first instantaneous frequency,**
f
_{
1
}
**(**
t
**)**

SNR | EEMD-HT | QHM | Proposed method |
---|---|---|---|

| 0.57 | 0.06 | 0.53 |

30 dB | 1.49 | 0.83 | 1.62 |

10 dB | 79.68 | 44.03 | 40.74 |

**Relative MAE (%) for the estimation of the second instantaneous frequency,**
f
_{
2
}
**(**
t
**)**

SNR | EEMD-HT | QHM | Proposed method |
---|---|---|---|

| 0.17 | 0.03 | 0.09 |

30 dB | 0.46 | 0.24 | 0.19 |

10 dB | 21.54 | 8.30 | 3.23 |

*f*

_{2}and

*f*

_{1}, respectively. MAEs of the estimation of IFs are recorded in Tables 1 and 2. The estimation errors of QHM are also provided in these tables for comparison. The analysis window of 64 samples and hop step of one sample is considered for this algorithm.

*∞*), the order of the TVAR model,

*M*, is equal to 4. Since higher error is imposed on pole estimation for stronger noise,

*M*should increase to alleviate this problem. We have

*M*= 24 for SNR = 30 dB and SNR = 10 dB. Figure 3 depicts the MAE of IF estimation with respect to

*M*for both components. It demonstrates that the error decreases remarkably as the order increases. However, there are more poles for higher orders which raise the error of classification routine and consequently the total error of estimation. Thus, there is a compromise to select the optimum order. In Figure 3, MAEs of ${\widehat{f}}_{1}$ and ${\widehat{f}}_{2}$ are minimum at

*M*= 24 and

*M*= 28, respectively.

*γ*

_{1}, …,

*γ*

_{4}(31) for each segment in Figure 4. The variance ratios of the poles in a conjugate pair are very close to each other or even equal in some segments.

*γ*

_{3}and

*γ*

_{4}, corresponding to

*ξ*

_{3}and

*ξ*

_{4}or the second resonance, are smaller than

*γ*

_{1}and

*γ*

_{2}. This means that the poles corresponding to the first oscillation component are more sensitive to the noise. This observation justifies why the MAE for ${\widehat{f}}_{1}$ (Table 1) deteriorates more than the MAE of ${\widehat{f}}_{2}$ (Table 2) due to the noise.

*f*

_{2}, is reduced by 4.8 kHz, i.e.,

*β*

_{2,1}= 1, 200 in (32). In this case, two IFs are closer and intersect each other. Both IFs are depicted in Figure 5. The proposed method is implemented in the same condition, and the results of estimation are exhibited in Figure 5, besides the original IFs. This method can track both IFs, and the intersection in their trajectories is handled properly. The degradation of estimation, especially around the crossover junction, is obvious by comparing Figures 5 and 1, but the trajectories are not missed and the estimated IFs are improved with time. This advantage arises from the step of pole classification in the proposed algorithm.

### 7.2 Real-world signal

*L*= 76 unequal blocks. The threshold of the segmentation procedure, $\stackrel{\u0304}{\eta}$, is set to 0.01. The extracted IFs are illustrated in the same figure of the STFT spectrum by black marks. The estimated IF tracks the frequency of dominant oscillations. In Figure 7, the IFs are demonstrated in addition to the results of EEMD-HT and QHM. Nine IMFs are extracted through EEMD, but the first and the second ones are valid resonances whose IFs are displayed. The relative standard deviation of added noise is set to 0.2, and the number of ensembles is 100. It takes several samples for EEMD-HT to resolve two IFs. Furthermore, the local variations and spikes in the results of EEMD-HT and QHM are noticeable. By contrast, the IFs of the proposed method are piecewise-constant, and no spike appears due to the segmentation. The lengths of the segments and consequently the variations of the resultant IFs (flatness or volatility) are controllable by the threshold selected in the segmentation procedure.

## 8 Conclusion

The analytical approach developed for extraction of oscillation modes of multicomponent non-stationary signals is founded on several facts which are summarized herein. Firstly, the decomposition of a multicomponent signal is considered as a signal expansion and investigated from this point of view. Secondly, the equivalent time-varying system of the non-stationary signal is modeled by TVAR and expanded by the orthogonal rational functions. Finally, oscillation modes are constructed, employing these bivariate rational functions, and their IFs are estimated. For this purpose, the evolution of the time-varying poles is considered piecewise-constant which imposes the same approximation in frequency estimation. The threshold parameter in the adaptive segmentation algorithm controls this approximation and governs the flatness of estimated IF against volatility.

The order of the TVAR model or equivalently the number of time-varying poles is another parameter which is set properly to confront the noise. Because this method utilizes the poles of the generating system of the AM-FM signal, the distortions on the amplitude, like noise, affect the estimation results mildly in comparison to those of the empirical methods. Although the noise degrades the estimation of underlying poles, it can be controlled by the order of the TVAR model. Simulations reveal the superiority of this method in the presence of noise. The controlling parameters in the proposed method yield some degree of freedom to adjust it for different realistic applications. Its capability to extract the embedded IFs in audio signals is illustrated.

## Declarations

## Authors’ Affiliations

## References

- Santhanam B, Maragos P: Multicomponent AM-FM demodulation via periodicity-based algebraic separation and energy-based demodulation.
*IEEE Trans Commun*2000, 48(3):473-490. 10.1109/26.837050View ArticleGoogle Scholar - Jang S, Loughlin P: AM-FM interference excision in spread spectrum communications via projection filtering.
*EURASIP J Appl. Signal Process*2001, 4: 239-248.View ArticleGoogle Scholar - Lu S, Doerschu P: Nonlinear modeling and processing of speech based on sums of AM-FM formant models.
*IEEE Trans. Signal Process*1996, 44(4):773-782. 10.1109/78.492530View ArticleGoogle Scholar - Bester M, Collen P, Richard G, David B: Estimation of frequency for AM-FM models using the phase vocoder framework.
*IEEE Trans. Signal Process*2008, 56(2):505-517.MathSciNetView ArticleGoogle Scholar - Grimaldi M, Cummins F: Speaker identification using instantaneous frequencies.
*IEEE Trans. Audio Speech Lang. Process*2008, 16(6):1097-1111.View ArticleGoogle Scholar - Kubo Y, Okawa S, Kurematsu A, Shirai K: Temporal AM-FM combination for robust speech recognition.
*Speech Commun*2011, 53: 716-725. 10.1016/j.specom.2010.08.012View ArticleGoogle Scholar - Loizou C, Murray V, Pattichis M, Seimenis I, Pantziaris M, Pattichis C: Multiscale amplitude-modulation frequency-modulation (AM-FM) texture analysis of multiple sclerosis in brain MRI images.
*IEEE Trans. Inform. Technol. Biomed*2011, 15(1):119-129.View ArticleGoogle Scholar - Murray V, Rodriguez P, Pattichis M: Multiscale AM-FM demodulation and image reconstruction methods with improved accuracy.
*IEEE Trans. Image Process*2010, 19(5):1138-1152.MathSciNetView ArticleGoogle Scholar - Cohen L:
*What is a multicomponent signal? Paper presented at the of IEEE international conference on acoustic, speech and signal processing (ICASSP).*USA; 23–26 Mar 1992:113-116.Google Scholar - Boashash B: Estimating and interpreting the instantaneous frequency of a signal-part1: fundamentals.
*Proc. IEEE*1992, 80(4):520-538. 10.1109/5.135376View ArticleGoogle Scholar - Lovell B, Williamson R, Boashash B: The relationship between instantaneous frequency and time-frequency representations.
*IEEE Trans. Signal Process*1993, 41(3):1458-1461. 10.1109/78.205756View ArticleGoogle Scholar - Maragos P, Kaiser F, Quatieri T: Energy separation in signal modulations with application to speech analysis.
*IEEE Trans. Signal Process*1993, 41(10):3024-3051. 10.1109/78.277799View ArticleGoogle Scholar - Bovik A, Maragos P, Quatieri T: AM-FM energy detection and separation in noise using multiband energy operator.
*IEEE Trans. Signal Process*1993, 41(12):3245-3265. 10.1109/78.258071View ArticleGoogle Scholar - Huang N, Shen Z, Long S, Wu M, Shih H, Zheng Q, Yen N, Tung C, Liu H: The empirical mode decomposition and the Hilbert spectrum for nonlinear and non-stationary time series analysis.
*Proc. R. Soc. London*1998, 454: 903-995. 10.1098/rspa.1998.0193MathSciNetView ArticleGoogle Scholar - Wu Z, Huang N: Ensemble empirical mode decomposition: a noise-assisted data analysis method.
*Adv. Adaptive Data Anal*2009, 1(1):1-41. 10.1142/S1793536909000047View ArticleGoogle Scholar - Deléchelle E, Lemoine J, Niang O: Empirical mode decomposition: an analytical approach for sifting process.
*IEEE Signal Process. Lett*2005, 12(11):764-767.View ArticleGoogle Scholar - Lin L, Wang Y, Zhou H: Iterative filtering as an alternative algorithm for empirical mode decomposition.
*Adv. Adaptive Data Anal*2009, 1(4):543-560. 10.1142/S179353690900028XMathSciNetView ArticleGoogle Scholar - Wang Y, Zhou Z: On the convergence of iterative filtering empirical mode decomposition.
*Excursions in Harmonic Anal*2013, 2: 157-172.MathSciNetView ArticleGoogle Scholar - Hou T, Yan M: A variant of the EMD method for multi-scale data.
*Adv. Adaptive Data Anal*2009, 1(4):483-516. 10.1142/S179353690900031XMathSciNetView ArticleGoogle Scholar - Hou T, Shi Z: Adaptive data analysis via sparse time-frequency representation.
*Adv. Adaptive Data Anal*2011, 3(1):1-28.MathSciNetView ArticleGoogle Scholar - Daubechies I, Lu J, Wu H: Synchrosqueezed wavelet transforms: an empirical mode decomposition-like tool.
*Appl. Comput. Harmonic Anal*2011, 30(2):243-261. 10.1016/j.acha.2010.08.002MathSciNetView ArticleGoogle Scholar - Meignen S, Oberlin T, McLaughlin S: A new algorithm for multicomponent signals analysis based on synchrosqueezing: with an application to signal sampling and denoising.
*IEEE Trans. Signal Process*2012, 60(11):5787-5798.MathSciNetView ArticleGoogle Scholar - Gianfelici F, Biagetti G, Crippa P, Turchetti C: Multicomponent AM-FM representations: an asymptotically exact approach.
*IEEE Trans. Audio Speech Lang. Process*2007, 15(3):823-837.View ArticleGoogle Scholar - Pantazis Y, Rosec O, Stylianou Y: Adaptive AM-FM signal decomposition with application to speech analysis.
*IEEE Trans. Audio Speech Lang. Process*2011, 19(2):290-300.View ArticleGoogle Scholar - Gazor S, Rashidi Far R: Adaptive maximum windowed likelihood multicomponent AM-FM signal decomposition.
*IEEE Trans. Audio Speech Lang. Process*2006, 14(2):479-491.View ArticleGoogle Scholar - Pai W, Doerschuk C: Statistical AM-FM models, extended Kalman filter demodulation, Cramer-Rao bounds and speech analysis.
*IEEE Trans. Signal Process*2000, 48(8):2300-2313. 10.1109/78.852011View ArticleGoogle Scholar - Jabloun M, Leonard F, Vieira M, Martin N: A New flexible approach to estimate the IA and IF of nonstationary signals of long-time duration.
*IEEE Trans. Signal Process*2007, 55(7):3633-3644.MathSciNetView ArticleGoogle Scholar - Huang N, Wu Z, Long S, Arnold K, Chen Z, Blank K: On instantaneous frequency.
*Adv. Adaptive Data Anal*2009, 1(2):177-229. 10.1142/S1793536909000096MathSciNetView ArticleGoogle Scholar - Khan N, Boashash B: Instantaneous frequency estimation of multicomponent nonstationary signals using multiview time-frequency distributions based on the adaptive fractional spectrogram.
*IEEE Signal Process. Lett*2013, 20(2):157-160.View ArticleGoogle Scholar - Vakman D: On the analytic signal, the Teager-Kaiser energy algorithm, and other methods for defining amplitude and frequency.
*IEEE Trans. Signal Process*1996, 44(4):791-797. 10.1109/78.492532View ArticleGoogle Scholar - Sebgahti M, Amindavar H:
*A novel analytical approach to orthogonal bases extraction from AM-FM signals. Paper presented at the IEEE international conference on acoustic, speech and signal processing (ICASSP).*Czech Republic; 22–27 May 2011:3820-3823.Google Scholar - D’Angelo H:
*Linear Time-Varying Systems, Analysis and Synthesis*. Boston: Allyn and Bacon; 1970.Google Scholar - Martin N: An AR spectral analysis of non-stationary signals.
*Signal Process*1986, 10: 61-74. 10.1016/0165-1684(86)90065-4MathSciNetView ArticleGoogle Scholar - Hopgood J, Rayner P: Blind single channel deconvolution using nonstationary signal processing.
*IEEE Trans. Speech Audio Process*2003, 11(5):476-488. 10.1109/TSA.2003.815522View ArticleGoogle Scholar - Heuberger P, Van den Hof P, Wahlberg B:
*Modeling and Identification with Rational Orthogonal Basis Functions*. London: Springer; 2005.View ArticleGoogle Scholar - Ninness B, Gustafsson F: A unifying construction of orthonormal bases for system identification.
*IEEE Trans. Automatic Control*1997, 42(4):515-521. 10.1109/9.566661MathSciNetView ArticleGoogle Scholar - O’Brien Jr. R, Iglesias P: On the poles and zeros of linear time-varying systems.
*IEEE T Circuits-I*2001, 48(5):565-577. 10.1109/81.922459MathSciNetView ArticleGoogle Scholar - Duda R, Hart P, Stork D:
*Pattern Classification*. New York: Wiley; 2000.Google Scholar - Meng Q, Yuan M, Zhao J: Empirical AM-FM decomposition of auditory signals.
*J. Acoust. Soc. Am*2012., 131(4): doi:10.1121/1.4708214Google Scholar

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