Volume 9 Supplement 9

## Proceedings of the Fifth Annual MCBIOS Conference. Systems Biology: Bridging the Omics

# Time-dependent ARMA modeling of genomic sequences

- Jerzy S Zielinski
^{1}Email author, - Nidhal Bouaynaya
^{1}Email author, - Dan Schonfeld
^{2}and - William O'Neill
^{3}

**9(Suppl 9)**:S14

**DOI: **10.1186/1471-2105-9-S9-S14

© Zielinski et al; licensee BioMed Central Ltd. 2008

**Published: **12 August 2008

## Abstract

### Background

Over the past decade, many investigators have used sophisticated time series tools for the analysis of genomic sequences. Specifically, the correlation of the nucleotide chain has been studied by examining the properties of the power spectrum. The main limitation of the power spectrum is that it is restricted to stationary time series. However, it has been observed over the past decade that genomic sequences exhibit non-stationary statistical behavior. Standard statistical tests have been used to verify that the genomic sequences are indeed not stationary. More recent analysis of genomic data has relied on time-varying power spectral methods to capture the statistical characteristics of genomic sequences. Techniques such as the evolutionary spectrum and evolutionary periodogram have been successful in extracting the time-varying correlation structure. The main difficulty in using time-varying spectral methods is that they are extremely unstable. Large deviations in the correlation structure results from very minor perturbations in the genomic data and experimental procedure. A fundamental new approach is needed in order to provide a stable platform for the non-stationary statistical analysis of genomic sequences.

### Results

In this paper, we propose to model non-stationary genomic sequences by a time-dependent autoregressive moving average (TD-ARMA) process. The model is based on a classical ARMA process whose coefficients are allowed to vary with time. A series expansion of the time-varying coefficients is used to form a generalized Yule-Walker-type system of equations. A recursive least-squares algorithm is subsequently used to estimate the time-dependent coefficients of the model. The non-stationary parameters estimated are used as a basis for statistical inference and biophysical interpretation of genomic data. In particular, we rely on the TD-ARMA model of genomic sequences to investigate the statistical properties and differentiate between coding and non-coding regions in the nucleotide chain. Specifically, we define a quantitative measure of randomness to assess how far a process deviates from white noise. Our simulation results on various gene sequences show that both the coding and non-coding regions are non-random. However, coding sequences are "whiter" than non-coding sequences as attested by a higher index of randomness.

### Conclusion

We demonstrate that the proposed TD-ARMA model can be used to provide a stable time series tool for the analysis of non-stationary genomic sequences. The estimated time-varying coefficients are used to define an index of randomness, in order to assess the statistical correlations in coding and non-coding DNA sequences. It turns out that the statistical differences between coding and non-coding sequences are more subtle than previously thought using stationary analysis tools: Both coding and non-coding sequences exhibit statistical correlations, with the coding regions being "whiter" than the non-coding regions. These results corroborate the evolutionary periodogram analysis of genomic sequences and revoke the stationary analysis' conclusion that coding DNA behaves like random sequences.

## Background

Understanding the statistical properties of genomic sequences helps recreate the dynamical processes that led to the current DNA structure, and determine gene-related diseases like cancer and Alzheimer disease. For instance, based on the view that non-coding DNA exhibits long-range correlations [1–6], Li [7] proposed an expansion-modification model of gene evolution. The model incorporates the two basic features of DNA evolution: (i) sequence elongation due to gene duplication and (ii) mutations. It can be shown that the limiting sequence created by this dynamical process exhibits a long-range correlation structure, as attested by a 1/*f*^{
α
}spectrum, where the exponent *α* is a function of the probability of mutation. To understand the relationship between the DNA correlation structure and possible gene abberations, Dodin et al. [8] designed a simple correlation function intended to visualize the regular patterns encountered in DNA sequences. This function is used to revisit the intriguing question of triplet repeats with the aim of providing a visual estimate of the propensity of genes to be highly expressed and/or to lead to possible aberrant structures formed upon strand slippage.

Statistical analysis of genomic sequences has, however, relied, for a long time, on signal processing techniques for stationary signals (correlation and power spectrum) [2, 4, 9, 10], and statistical tools for slowly-varying trends within stationary signals (Detrended Fluctuation Analysis or DFA) [1, 5, 6]. Stationarity can be argued as a valid assumption for time-series of short duration. However, such an assumption rapidly loses its credibility in the enormous databases maintained by various genome projects. Standard statistical tests (e.g., Priestley's test for stationarity) have been used to verify that genomic sequences are not stationary and the nature of their non-stationarity varies and is often more complex than a simple trend [11, 12]. Subsequently, more recent analysis of genomic data [1] has relied on time-varying power spectral methods (the evolutionary spectrum and periodogram) to capture the statistical characteristics of genomic sequences [11, 12]. The main difficulty in using time-varying spectral methods is that they are extremely unstable and very noisy. Typically, the power spectrum and the evolutionary spectrum are averaged over time in order to obtain smooth and less jittery curves. Moreover, as was pointed out in [13], the evolutionary spectrum is restricted to the class of oscillatory processes. A stochastic process, *X*(*t*), is oscillatory if it has a representation of the form

*X*(*t*) = ∫ *A*(*t*, *λ*)*e*^{2iπλt}*dZ*(*λ*), (1)

Where *Z*(*λ*) is an orthogonal increment process, and the evolutionary power spectrum of the process is defined by *P* (*t*, *λ*) = |*A*(*t*, *λ*)|^{2}. This definition of the evolutionary power spectrum has the following disadvantages [13]:

**(i)** It is not uniquely defined for a given non-stationary process.

**(ii)** The estimation procedure for the evolutionary spectrum depends greatly on the nature of theamplitude function *A*(*t*, *λ*), which is not known a priori.

**(iii)** An increase in the number of observations does not provide added information on the local behavior of the evolutionary spectrum, and thus does not improve estimation accuracy.

*x*(

*t*), when driven by the innovation,

*w*(

*t*), is no longer shift-invariant; the parameters of the impulse response,

*h*

_{ u }, of this system are time-dependent so that

The existence of a time-varying ARMA representation of this process is ensured by two theorems due, independently, to Grenier [15] and Huang and Aggarwal [16]. The uniqueness of the TD-ARMA representation is obtained by constraining the ARMA model to be invertible, but this leads to conditions on the time-varying impulse response {*h*_{
u
}(*t*)} and its inverse (namely to be absolutely summable at any time *t*), which cannot be easily expressed in terms of the time-dependent coefficients of the ARMA model. In this paper, we estimate the time-dependent coefficients of the general TD-ARMA model using mean-squares, least-squares and recursive least-squares algorithms. The mean-squares estimation leads to generalized Yule-Walker type equations [15]. Once the non-stationary parameters are estimated (as time series), we use them to provide a basis for statistical inference by defining an index of randomness, which quantitatively assesses how close the non-stationary signal is to white noise. Our simulation results on various gene sequences show that (i) both the coding and non-coding segments of a gene are not random, and (ii) the coding segments are "closer" to random sequences than non-coding segments. Our results support the view that both coding and non-coding sequences are not random [11, 12, 9, 17–20], and revokes the stationary study that maintains that non-coding DNA sustains long-range correlations whereas coding DNA behaves like random sequences [1–3, 5, 6, 10].

## Methods

### Numerical representation of genomic sequences

*u*(

*i*), which they termed "DNA walk". The DNA walk is defined by the rule that the walker steps up (

*u*(

*i*) = +1) if a pyrimidine resides at position

*i*, and steps down (

*u*(

*i*) = -1) otherwise. Voss [9] represents a DNA sequence by four binary indicator sequences, which indicate the locations of the four nucleotides A, T, C and G. Berthelsen et al. [21] proposed a two-dimensional representation of DNA sequences, characterized by a Hausdorff dimension (also called fractal dimension) that is invariant under (i) complementarity, (ii) reflection symmetry, (iii) compatibility and (iv) substitution symmetry of A͘T and C↔G. The corresponding embedding assignment is given by A = (-1; 0), T = (1; 0), C = (0; -1) and G = (0; 1). In this paper, since we are interested in time-dependent ARMA modeling of one-dimensional non-stationary genomic sequences, we adopt the widely used "DNA walk" map proposed by Peng et al [1]. The DNA walk provides a nice graphical representation for each gene. For instance, Figure 1 shows the structure of the Human gene 276 located in chromosome 1, and its DNA walk is displayed in Fig. 2.

### Time-dependent ARMA model

*x*[

*n*]}, can be represented by finite-order time-varying ARMA processes of the form

*N*is the length of the sequence

*x*[

*n*],

*a*

_{ i }[

*n*] and

*b*

_{ i }[

*n*] are the time-dependent model parameters,

*p*and

*q*are the model orders and

*w*[

*n*] is a white noise process. Observe that the coefficients

*a*

_{ i }[

*n*] and

*b*

_{ i }[

*n*] appear with an argument

*n*-

*i*depending on

*i*. This is purely arbitrary since any time origin can be chosen, without restraining the generality of the model. We assume that the time-dependent coefficients

*a*

_{ i }[

*n*] and

*b*

_{ i }[

*n*] can be expressed as linear combinations of some basis functions ${\{{f}_{k}[n]\}}_{k=0}^{m}$,

The advantage of the basis parametrization is clear from the fact that the identification of the time-dependent coefficients *a*_{
i
}[*n*] and *b*_{
i
}[*n*] reduces to the identification of the constant coefficients ${\left\{{c}_{i,k}\right\}}_{k=0}^{m}$ and ${\left\{{d}_{i,k}\right\}}_{k=0}^{m}$, and therefore the linear non-stationary problem reduces to a linear time-invariant problem. The basis functions ${\{{f}_{k}[n]\}}_{k=0}^{m}$ do not have to be limited to the standard choices of Legendre, Fourier, or the prolate spheroidal basis but can also take advantage of any prior information, such as the presence of a jump in the coefficients at a known instant [22].

### Estimation of the time-dependent ARMA coefficients

From Eqs. (4) and (5), the unknown parameters of the TD-ARMA model are the weights of the linear combinations defining each time-varying parameter. The linearity is the key to the algorithms proposed in this paper. We will derive mean-squares, least-squares and recursive least-squares solutions to estimate the time-dependent coefficients ${\{{a}_{i}[n]\}}_{i=1}^{p}$ and ${\{{b}_{j}[n]\}}_{j=1}^{q}$.

#### Mean-squares estimation

and define the vector

*X* [*n*] = [*f*_{0}[*n*]*x*[*n*], ⋯, *f*_{
m
}[*n*]*x*[*n*]]^{
t
}, (7)

^{ t }stands for the transpose of a vector or a matrix. It is possible to derive for this process orthogonality conditions similar to the stationary ARMA model conditions [23]. Observe that the process

*v*[

*n*], defined in Eq. (6), is orthogonal to [

*w*[

*n*-

*q*- 1],

*w*[

*n*-

*q*- 2], ⋯]; hence, it is orthogonal to

*x*[

*n*-

*q*-

*i*] for all

*i*> 0, and orthogonal to

*X*[

*n*-

*q*-

*i*] for all

*i*> 0 [22]. This orthogonality condition leads to a generalized Yule-Walker equation [22]

Although the process *x* [*n*] is non-stationary, the stationarity and ergodicity of the process *w* [*n*], together with the linearity of the model, allow us to replace in Eq. (8) the expectation by a summation. However, although consistent, the above estimator is often considered a poor one [22].

#### Least-squares estimation

Equations (4) and (5) can be written in vector format as follows

*a*_{
i
}[*n*] = **f**^{
t
}[*n*] **c**_{
i
}, and *b*_{
i
}[*n*] = **f**^{
t
}[*n*] **d**_{
i
},

Define

**u**^{
t
}[*n*] = *x* [*n*] **f**^{
t
}[*n*], and **v**^{
t
}[*n*] = *w* [*n*] **f**^{
t
}[*n*].

Using this vector notation, Eq. (3) can be written as

*x* [*n*] + **u**^{
t
}[*n* - 1] **c**_{
1
}+ ⋯ + **u**^{
t
}[*n* - *p*] **c**_{
p
}= *w* [*n*] + **v**^{
t
}[*n* - 1] **d**_{
1
}+ ⋯ + **v**^{
t
}[*n* - *q*] **d**_{
q
} (9)

Or equivalently

*x* [*n*] + *φ*^{
t
}[*n*] *θ* = *w* [*n*], (10)

where *φ*^{
t
}[*n*] is the row vector

*φ*^{
t
}[*n*] = [**u**^{
t
}[*n* - 1], ⋯, **u**^{
t
}[*n* -*p*], - **v**^{
t
}[*n* - 1], ⋯, **v**^{
t
}[*n* -*q*]],

and

θ= [**c**_{
1
}, ⋯,**c**_{
p
}, **d**_{
1
}, ⋯, **d**_{
q
}]^{
t
}.

Observe that the vector *θ* contains all the unknowns of the TD-ARMA model. Writing Eq. (10) for *n* = 0, 1, ⋯, *N* - 1 leads to

**x = Φ** θ **+ w**, (11)

The least-squares solution of Eq. (11) is given by

θ **= (Φ**^{
t
}**Φ)**^{
-1
} **Φ**^{
t
}**x** (12)

To overcome the computational complexity associated with the least-squares estimation (involving in particular the inversion of a square (*m* + 1)(*p* + *q*) × (*m* + 1)(*p* + *q*) matrix), we opted for a recursive least-squares estimation as follows.

#### Recursive least-squares estimation

The initial conditions can be chosen arbitrarily.

### Index of randomness

Over the past decade, there has been a flow of conflicting papers about the long-range power-law correlations detected in eukaryotic DNA [1–3, 5, 6, 9–12, 17–20]. The controversy is generated by conflicting views that either advocate that non-coding DNA sustains long-range correlations whereas coding DNA behaves like random sequences [1, 10, 2, 3, 5, 6], or maintains that both coding and non-coding DNA exhibit long-range power-law correlations [11, 12, 9, 17–20]. Based on the analysis of the time-dependent power spectrum of genomic sequences, Bouaynaya and Schonfeld [11, 12] showed that the statistical differences between coding and non-coding sequences are more subtle than previously concluded using stationary analysis tools. In fact they found that both coding and non-coding sequences are non-random. However, coding sequences are "whiter" than non-coding sequences.

*a*

_{ i }[

*n*] and

*b*

_{ i }[

*n*]. Consider the system function,

*H*(

*z*), of a stationary ARMA model (whose coefficients

*a*

_{ i }and

*b*

_{ i }are constant, i.e., independent of time). We know that

_{2}distance) the zeros and poles are, the flatter is the spectrum of the process. Following the same reasoning locally for non-stationary processes, we define the curve of randomness,

*CR*[

*n*], of the non-stationary process

*x*[

*n*] by

*r*

_{ k }[

*n*],

*p*

_{ k }[

*n*]). Observe that the case

*p*<

*q*is obtained from the

*p*>

*q*case by interchanging the roles of

*r*

_{ k }and

*p*

_{ k }, and the indices

*p*and

*q*. The curve of randomness defined in Eq. (17) is a measure of how close the zeros and the poles of the system function are, and therefore, is a measure of how flat the system function is, and how close is the process from a white noise. The index of randomness,

*IR*(

*p*,

*q*), of a TD-ARMA(

*p*,

*q*), is then defined as the average of the curve of randomness, i.e.,

*x*[

*n*] +

*a*[

*n*- 1]

*x*[

*n*- 1] =

*w*[

*n*] +

*b*[

*n*]

*w*[

*n*- 1]) is given by

Observe that the index of randomness of a white noise process is equal to zero. We say that the sequence *x*_{1} [*n*] with index of randomness *IR*_{1} is more random than the sequence *x*_{2} [*n*] with index of randomness *IR*_{2} if the index of randomness of the former is lower than the index of randomness of the latter, i.e., *IR*_{1} <*IR*_{2}.

## Results

*rarmax*, which implements the recursive least-squares algorithm for TD-ARMA models. The choice of the orders

*p*and

*q*of the model were determined experimentally as follows: For each genomic sequence, we computed 100 TD-ARMA models corresponding to the orders (1, 1) up to (10, 10). The best model was chosen to be the one that minimizes the average squared error between the actual and the fitted sequences. Our extensive simulations on various DNA sequences from different organisms show that most of the sequences are best fitted with low-order TD-ARMA models, e.g., TD-ARMA(1,1), TD-ARMA(1,2) and TD-ARMA(2,1). Figure 3 shows the DNA walk of the Human gene 276 and its TD-ARMA(1,1) fitted sequence. Observe that the TD-ARMA(1,1) model accurately fits this gene sequence. The estimated time-varying coefficients

*a*[

*n*] and

*b*[

*n*] are displayed in Fig. 4 for both the coding and non-coding regions of this gene. Their statistical differences are not clear from the plot of the time-series coefficients. The curves of randomness of the coding and non-coding regions are displayed in Fig. 5. Table 1 shows the index of randomness of various gene sequences. For concise representation, the column titles have been abbreviated as follows: "C. length" (resp."N.C. length") denotes the length (in base pairs) of the coding (resp. non-coding) segment of the gene. The total length of the gene is the sum of the lengths of its coding and non-coding regions. "C. (

*p*,

*q*)" (resp. "N.C. (

*p*,

*q*)") denotes the optimal TD-ARMA parameters (

*p*,

*q*) for the coding (resp. non-coding) region of the gene. Finally, "C. IR" (resp. "N.C. IR") is the index of randomness of the coding (resp. non-coding) segment of the gene. Observe that, in all considered genes, the index of randomness of both the coding and non-coding segments are strictly positive, and the index of randomness of the coding region is consistently lower than the index of randomness of the non-coding region (recall that the index of randomness of a white noise is zero). These observations bring to bear two important conclusion: (i) Both the coding and non-coding sequences are not random, as attested by an index of randomness greater than zero. (ii) The coding sequences are "whiter" than the non-coding sequences. This conclusion revokes previous work on statistical correlation of DNA sequences, which, based on stationary time-series analysis, presumed that coding DNA behaves like random sequences [1–3, 5, 6, 10]; and supports the conflicting view that both coding and non-coding sequences are not random [11, 12, 9, 17–20]. In particular, our conclusion is in accordance with the evolutionary periodogram analysis conducted in [11, 12].

Index of Randomness of the Coding and Non-Coding segments of Various Gene Sequences

Gene NIH accession number | C. length | C. ( | C. IR | N.C. length | N.C. ( | N.C. IR |
---|---|---|---|---|---|---|

Ashbya gossypii (fungus) AE016815 | 180953 | (1,1) | 0.9466 | 674919 | (1,1) | 0.9860 |

Aspergillus fumigatus (form of fungus) CM000169 | 1227993 | (2,1) | 0.9870 | 1835394 | (1,1) | 1.0683 |

Candida albicans (form of yeast) AP006852 | 373390 | (1,1) | 1.0282 | 570789 | (1,1) | 1.0429 |

Candida albicans AP006852 | 373390 | (1,1) | 1.0282 | 570789 | (3,1) | 1.0429 |

fission yeast GI:157310483 | 753661 | (1,1) | 1.0402 | 1654671 | (1,1) | 1.0642 |

fruit fly AE002620 | 21399 | (1,1) | 1.0084 | 1222832 | (1,2) | 1.1075 |

fruit fly AE002725 | 11316 | (1,1) | 1.0145 | 659655 | (1,1) | 1.0320 |

Homo sapiens hs-gene277 NG-004750 | 1639 | (1,1) | 1.0688 | 6573 | (1,1) | 1.0808 |

Homo sapiens hs-gene276 NG-004750 | 1536 | (1,1) | 1.0603 | 6672 | (1,1) | 1.0627 |

## Conclusion

In this paper, we modelled the non-stationary genomic sequences by a time-dependent autoregressive moving average (TD-ARMA) model. By expressing the time-dependent coefficients as linear combinations of parametric basis functions, we were able to transform a linear non-stationary problem into a linear time-invariant problem. Subsequently, we proposed three methods to estimate the time-dependent coefficients: Mean -square, least-squares, and recursive least-squares algorithms. Based on the estimated TD-ARMA coefficients, we defined an index of randomness to quantify the degree of randomness of both coding and non-coding sequences. We found that both coding and non-coding sequences are not random. However, a higher index of randomness attests that coding sequences are "whiter" than non-coding sequences. These results corroborate the evolutionary periodogram analysis of genomic sequences performed in [11] and [12], and revoke the stationary analysis' conclusion that coding DNA behaves like random sequences.

## Declarations

### Acknowledgements

The publication of this paper was partially supported by the Arkansas IDeA Networks of Biomedical Research Excellence (INBRE).

This article has been published as part of *BMC Bioinformatics* Volume 9 Supplement 9, 2008: Proceedings of the Fifth Annual MCBIOS Conference. Systems Biology: Bridging the Omics. The full contents of the supplement are available online at http://www.biomedcentral.com/1471-2105/9?issue=S9

## Authors’ Affiliations

## References

- Peng CK, Buldyrev SV, Goldberger AL, Havlin S, Sciortino F, Simons M, Stanley HE: Long-range correlations in nucleotide sequences. Nature. 1992, 356 (6365): 168-170.View ArticlePubMedGoogle Scholar
- Buldyrev SV, Goldberger AL, Havlin S, Mantegna RN, Matsa ME, Peng CK, Simons M, Stanley HE: Long-range correlation properties of coding and noncoding DNA sequences: GenBank analysis. Physical Review E. 1995, 51: 5084-5091.View ArticleGoogle Scholar
- Stanley HE, Buldyrev SV, Goldberger AL, Havlin S, Peng CK, Simons M: Scaling features of noncoding DNA. Physica A. 1999, 273: 1-18.View ArticlePubMedGoogle Scholar
- Li W, Holste D: Universal 1/f noise, crossovers of scaling exponents, and chromosome-specific patterns of guanine-cytosine content in DNA sequences of the human genome. Physical Review E. 2005, 71: 041910-View ArticleGoogle Scholar
- Podobnik B, Shao J, Dokholyan NV, Zlatic V, Stanley HE, Grosse I: Similarity and dissimilarity in correlations of genomic DNA. Physica A. 2006, 373: 497-502.View ArticleGoogle Scholar
- Carpena P, Bernaola-Galvan P, Coronado AV, Hackenberg M, Oliver JL: Identifying chracteristic scales in the human genome. Physical Review E. 2007, 75: 032903-View ArticleGoogle Scholar
- Li W: Expansion-modification systems: a model for spatial 1/f spectra. Physical Review A. 1991, 43 (10): 5240-5260.View ArticlePubMedGoogle Scholar
- Dodin G, Levoir P, Cordier C: Triplet Correlation in DNA Sequences and Stability of Heteroduplexes. Journal of Theoretical Biology. 1996, 183: 341-343.View ArticlePubMedGoogle Scholar
- Voss RF: Evolution of long-range fractal correlations and 1/f noise in DNA base sequences. Physical Review Letters. 1992, 68: 3805-3808.View ArticlePubMedGoogle Scholar
- Li W, Kaneko K: Long-range correlation and partial 1/f spectrum in a noncoding DNA sequence. Europhysics Letters. 1992, 17: 655-View ArticleGoogle Scholar
- Bouaynaya N, Schonfeld D: Non-Stationary Analysis of Genomic Sequences. IEEE Statistical Signal Processing Workshop. 2007, Madison, WI, 200-204.Google Scholar
- Bouaynaya N, Schonfeld D: Non-stationary Analysis of Coding and Non-coding Regions in Nucleotide Sequences. IEEE Journal of Selected Topics in Signal Processing. 2008Google Scholar
- ADAK S: Time-dependent spectral analysis of nonstationary time series. Journal of the American Statistical Association. 1998, 93 (444): 1488-1501.View ArticleGoogle Scholar
- Cramer H: On some classes of nonstationary stochastic processes. Proceedings of the Berkeley Symppsium on Math, Statistics, and Probability. 1961, Los Angeles, CAGoogle Scholar
- Grenier Y: Rational nonstationary spectra and their estimation. ASSP Workshop on Spectral Estimation. 1981Google Scholar
- Huang NC, Aggarwal JK: On linear Shift-variant digital filters. IEEE Transactions on Circuits and Systems. 1980, 27 (8): 672-679.View ArticleGoogle Scholar
- Prabhu VV, Claverie JM: Correlations in intronless DNA. Nature. 1992, 359-782.Google Scholar
- Chatzidimitriou-Dreismann CA, Larhammar D: Long-range correlations in DNA. Nature. 1993, 361: 212-View ArticlePubMedGoogle Scholar
- Pande VS, Grosberg AY, Tanaka T: Nonrandomness in protein sequences – evidence for a physically driven stage of evolution. Proceedings of the National Academy of Sciences. 1994, 91 (26): 12972-12975.View ArticleGoogle Scholar
- Guharay S, Hunt BR, York JA, White OR: Correlations in DNA sequences across the three domains of life. Physica D. 2000, 146 (1–4):Google Scholar
- Berthelsen CL, Glazier JA, Skolnick MH: Global fractal dimension of human DNA sequences treated as pseudorandom walks. Physical Review A. 1992, 45 (12): 8902-8913.View ArticlePubMedGoogle Scholar
- Grenier Y: Time-Dependent ARMA Modeling of Nonstationary Signals. IEEE Transactions on Acoustics, Speech, and Signal Processing. 1983, 31 (4): 899-911.View ArticleGoogle Scholar
- Hayes MH: Statistical digital signal processing and modeling. Wiley. 1996Google Scholar
- Ljung L: System Identification – Theory for the User. 2006, Prentice Hall, secondGoogle Scholar

## Copyright

This article is published under license to BioMed Central Ltd. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.