 Research
 Open access
 Published:
Analysis of two mechanisms of telomere maintenance based on the theory of gNetworks and stochastic automata networks
BMC Genomics volume 21, Article number: 587 (2020)
Abstract
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Background Telomeres, which are composed of repetitive nucleotide sequences at the end of chromosomes, behave as a division clock that measures replicative senescence. Under the normal physiological condition, telomeres shorten with each cell division, and cells use the telomere lengths to sense the number of divisions. Replicative senescence has been shown to occur at approximately 50–70 cell divisions, which is termed the Hayflick’s limit. However, in cancer cells telomere lengths are stabilized, thereby allowing continual cell replication by two known mechanisms: activation of telomerase and Alternative Lengthening of Telomeres (ALT). The connections between the two mechanisms are complicated and still poorly understood.
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Results In this research, we propose that two different approaches, GNetworks and Stochastic Automata Networks, which are stochastic models motivated by queueing theory, are useful to identify a set of genes that play an important role in the state of interest and to infer their previously unknown correlation by obtaining both stationary and joint transient distributions of the given system. Our analysis using GNetwork detects five statistically significant genes (CEBPA, FOXM1, E2F1, cMYC, hTERT) with either mechanism, contrasted to normal cells. A new algorithm is introduced to show how the correlation between two genes of interest varies in the transient state according not only to each mechanism but also to each cell condition.
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Conclusions This study expands our existing knowledge of genes associated with mechanisms of telomere maintenance and provides a platform to understand similarities and differences between telomerase and ALT in terms of the correlation between two genes in the system. This is particularly important because telomere dynamics plays a major role in many physiological and disease processes, including hematopoiesis.
Background
The introduction of Stochastic Automata Networks (SANs) [1] has led researchers to explore an efficient solution of finite multicomponent Markov chains of potentially very high dimension. The main idea of the SAN formalism is to employ Kronecker algebra operations for generating the infinitesimal generator (also known as an intensity matrix or transition rate matrix) of a Markov chain in a product form in order to ease the problem of dimensionality and the complexity of the vectormatrix product [2, 3]. Specifically, a compact representation using tensor product and sums of matrices of the form, which is formally proved in [1]
provides the transition rates of a timecontinuous Markov chain of the type just described. Notation: N is the number of automata, R is the number of synchronizations, and L_{i} and M_{r,i} are matrices containing information about the local transitions and the effect of the synchronization r on the automaton i, respectively. N_{r,i} is the normalizing matrix of M_{r,i}, and ⊗ and ⊕ denote, respectively, the (generalized) tensor product and tensor sum [4]. Notation will be discussed in detail in the following section.
For a decade after SAN introduction, many outstanding analytical results have been proved. For example, Plateau and Stewart [5] proved in year 2000 that a productform steadystate distribution for SANs without synchronizations exists, as long as some numerical conditions related to local balance are satisfied. Prior to that, Boujdaine et al. in 1997 [6] considered a special class of SAN having limited synchronization, and proved a sufficient condition for existence of stationary distribution, by applying properties of Kronecker sum. Note that classic queuing networks such as Jackson’s networks and GNetworks with positive and negative customers [7] fall under this special class.
Most analyses and applications of SANs focus on finding steadystate distribution of queuing system models. To our knowledge, correlation analysis in SANs is rarely examined, although correlation quantifies the degree of interrelatedness of two automata. It contributes to the understanding of how the association of two automata changes with time according to the state of interest, with the behavior of other automata in the system simultaneously considered. In the current study, we first examine the exactform of an infinitesimal generator for GNetworks with positive and negative customers. Then it is applied to a gene regulatory network (GRN) having five genes related to the onset of cancer in order to show the timedependent dynamics of transition rates and correlation between two particular genes of interest. Throughout this paper, our analysis is based on timecontinuous Markov chains, but we note that most results are valid in the timediscrete case provided complications such as periodicity are excluded.
Stochastic automata network
The SAN consists of a number of automata, which are correlated by synchronizing transitions. Each automaton has states and transitions. The state space of the system is the Cartesian product of the states of the automata [6]. There exist two types of transitions: local and synchronizing.

1.
Transition in one automaton may initiate a new simultaneous transition in another automaton. Such transitions are collectively referred to as synchronizing transitions. In one synchronizing transition, two automata are paired. The first is called a master automaton; it affects the state of another automaton as its state changes. The second is called a slave automaton; it is affected by its master automaton [8].

2.
In any given automaton, transitions not classified as synchronizing transitions are local transitions. Such transitions only change the state of one automaton.
In the SAN, two assumptions are made. First, the time to transition is exponentially distributed, and second, that a multidimensional Markov chain represents the SAN, although a particular automaton may not be Markovian itself. Then the (global) infinitesimal generator (the matrix of time derivatives at 0 of the transition probabilities), which reflects a change in transition probability from one state to another, is given by Eq. 1, with notation explained in Table1.
Specifically, each matrix in Q is defined as follows:

L_{i} is a local normalized transition rate matrix of automaton i; thus
$$\begin{array}{*{20}l} L_{i}[m,n] \geq 0 \;\; \text{if} \;\; m \neq n \;\;\; \text{and} \;\;\; \sum_{n = 1}^{N} L_{i}[m,n] = 0 \end{array} $$ 
For each synchronizing transition, for all i∈{1,2,⋯,N},M_{r,i}=I_{K}, where I_{K} is an identity matrix of size K, except for the case when r is two indices corresponding to master and slave automaton. Therefore
$$ {{{}\begin{aligned} \bigotimes_{i=1}^{N} \; M_{r,i} & = I_{K} \otimes \cdots \otimes I_{K} \otimes \left(D_{r, msr(r)}  \bar{D}_{r, msr(r)} \right) \\ & \;\;\;\;\; \otimes I_{K} \otimes \cdots \otimes I_{K} \otimes E_{r, sl(r)} \otimes I_{K} \otimes \cdots \otimes I_{K} \end{aligned}}} $$where msr(r) and sl(r) are indices for master automaton and slave automaton, respectively, in the r^{th} synchronization. Here, D_{r,msr(r)} denotes the transition rate matrix due to the r^{th} synchronizing event on the master automaton, and \(\bar {D}_{r, msr(r)}\) is its diagonal matrix. E_{r,sl(r)}, the transition probability matrix, is the effect of the r^{th} synchronizing event on the automaton sl(r).
$${{\begin{aligned} D_{r,msr(r)} [m, n] & \geq 0 \; \text{if} \; m \neq n \; & \text{and} \; & \sum_{n=1}^{N} D_{r,msr(r)} [m, n] & = 0 \;, \; \forall \; m \\ E_{r, sl(r)}[m,n] & \geq 0 \; \forall \; m, n & \text{and} \; & \sum_{n = 1}^{N} E_{r, sl(r)}[m,n] & = 1 \;, \forall \; m \end{aligned}}} $$ 
A normalizing matrix \(\bigotimes _{i=1}^{N} \; N_{i, r}\) is a (K^{N}×K^{N})dimensional diagonal matrix, whose the l^{th} diagonal element is the negative sum of the l^{th} row of \(\bigotimes _{i=1}^{N} \; M_{r,i} \).
GNetworks with positive and negative customers
Gelenbe or GNetworks [9], devised by Erol Gelenbe, are Markovian stochastic models grounded in queueing network theory [10]. They were extensively applied to study probability models of various objects [11–18]. However they are particularly appropriate to construct GRNs, as they introduce a novel notion called a ‘negative customer’, which can be biologically interpreted as a repression signal [19]. GNetworks model the number of positive customers, which is mRNA expression level biologically, in an automaton or a gene having an infinite state space. Positive and negative customers synchronously move from a master gene to a slave gene within the system with transition probabilities, \(p_{msr(r), sl(r)}^{+}\) and \(p_{msr(r), sl(r)}^{}\), respectively. It implies that there are two types of the synchronizing transition. Note that the behavior of positive customers identical to that of positive customers in Jackson networks [20]. In contrast, negative customers function distinctively as follows: they are not accumulated and instantaneously leave a queue after the completion of their tasks. If a negative customer arrives at a nonempty queue, it destroys one current positive customer. However if the queue is empty, then the negative customer disappears without locally affecting the queue. Both types of customers arrive at the i^{th} gene from outside of the system at rates \(\lambda _{i}^{+}\) and \(\lambda _{i}^{}\), respectively. It is assumed that service disciplines are the same for all queue [21], and the service times for each queue i are independent and identically exponentially distributed with rates μ_{i}∈(0,∞) for i=1,2,⋯,N. Figure 1 visually illustrates four activities of mRNA and/or protein molecules, and Table 2 suggests how the biological terms that refer to these activities can be identified with those used in GNetworks.
GNetworks have an advantageous property of being analytically tractable because of the existence of productform stationary distributions under the typical Markov Chain assumptions as shown in Eq. 2 [7, 22].
Let x={x_{1},x_{2},⋯,x_{N}} be the vector of nonnegative integers representing the state of the network. Then the timedependent vector, {x(t):t≥0}, is a continuoustime Markov chain, which satisfies the system of ChapmanKolmogorov equations [23]. Element x_{i}(t),1≤i≤N, of vector x(t)=(x_{1}(t),x_{2}(t),⋯,x_{N}(t)), is the number of customers (or the mRNA expression level) of gene i at time t. It has been proved that the joint steadystate distribution π(x) of x(t), has the form of a product of stationary distributions of each queue,
each satisfying the balance equation of the GNetworks [23–25], i.e.
for i=1,2,⋯,N. It implies that the stationary probability for each positive recurrent state is expressed in the terms of a product of functions depending solely on the state of a single queue.
According to [8], matrices constituting the global infinitesimal generator Q are defined as follows in the terms of customerrelated rates:
where

I : Identity matrix

Upp : Matrix with entries 0 except the main upper diagonal which is 1

Low : Matrix with entries 0 except the main lower diagonal which is 1

\(I_{1}^{0}\) : Identity matrix except the first diagonal element which is 0

\(I_{K}^{0}\): Identity matrix except the K^{th} diagonal element which is 0
Results
This section consists of two parts. The first part shows the mathematical result that derives the correlation between two genes utilizing Kronecker algebra. The second part contains the biological results based on the application of the mathematical result to the gene regulatory network associated with telomere biology.
Mathematical result: derivation of joint transient distribution of two automata
If Q is the infinitesimal generator and P(t) is the transition probability matrix of a finite Markov chain, we can derive a set of differential equations called Kolmogorov’s forward equations, in the form of P^{′}(t)=P(t)·Q. Solution of the forward equation is given in this case by the power series expansion that converges for any square matrix Q:
The resulting (1×K^{N})dimensional timedependent state probability vector at time t has the form
where π(t) is a state probability vector at time t [26]. In order to find a joint state probability vector π_{i,j}(t) of two automata, say i and j, we introduce two matrices C_{i,j} and \(C^{*}_{i,j}\), which are (K^{N}×K^{2}) and (K^{2}×K^{N})dimensional, respectively. After several steps of calculation, we obtain
where, for all i≠j, i,j=1,2,⋯,N, C_{i,j} and \(C^{*}_{i,j}\) are defined by
Note that the (1×K)dimensional matrix \(1_{K}^{T} = \left [\begin {array}{llll} 1 & 1 & \cdots & 1 \end {array}\right ]\) indicates the matrix transpose of 1_{K}. This results in
where
Therefore Eq. 6 finally becomes
Equation 8 implies that a timedependent joint state probability vector π_{i,j}(t) can be easily calculated, once the infinitesimal generator, Q, of the entire system is obtained.
We can then form a (K×K)dimensional table that describes the joint probabilities for each time point t. Based upon it, the association between two genes for all t is evaluated using the Pearson productmoment correlation coefficient [27]. It implies the correlation of a pair of genes in the regulatory system varies by each time (each generation of cells) as shown in Fig. 2.
Application to the gene regulatory networks
GRNs and parameters from gNetworks
In this research, we use a GRN provided in Fig. 3. It consists of 5 statistically significant genes associated with telomere maintenance, which are discovered by (modified) Abnormal Pathway Detection Algorithm (APDA) based on GNetworks [18]. (See Methods for detailed information on the modification). We explore the correlation between a pair of genes, e.g., CEBPA and hTERT, which is not apparent from Fig. 3. On the biology side, Kirwan et al. in 2009 [28] reported that mutations in hTERT within 4 of 20 families were identified in familial acute myeloid leukemia (AML). It is known that the mutation of CEBPA is one of the important factors in AML and its prognosis [29]. However the direct relationship between CEBPA and AML is still not satisfactorily understood. The joint state probability vector of two genes, which can be calculated from Eq. 9, is expected to show the flow of probabilities for the K^{2}–tuples of mRNA expression levels at each fixed time t, and thereby illustrates the relationship between any two genes.
In this case, the number of automata is equal to N=5, while the number of synchronizing events is equal to R=7. We limit the number of gene expression levels to K=7 for two reasons. The first is that, because the data are normalized, there are few genes with a mRNA expression level of 7 or higher. Furthermore, the memory limitations enforce it. In this paper, we assume that pairs of genes are highly positively correlated at the initial time point; that is
Note that this matrix needs to be transformed into a (1×K^{2})dimensional joint state probability vector as π_{ij}(t) in Eq. 9. Tables 3 and 4 exhibit the values of parameters that are required to build the infinitesimal generator Q. They are estimated and optimized according to the APDA [18] based on GNetworks. Specifically, values in Table 3 allow to calculate a joint probability vector π_{i,j}(t), under the normal condition, with the Table 4 contains information for malignant (ALT or active telomerase) cells. The three families of parameters, \(\lambda _{i}^{+}, \lambda _{i}^{}\) and μ_{i} for all i, are identical for both normal and ALT cells, while transition probabilities, \(p_{{ij}}^{+}, p_{{ij}}^{}\) and d_{i}, are different between the cell types. Transition probabilities are deciding factors in correlation coefficients based on Eq. 9 and the rates of convergence to stationarity in GNetworks.
Simulation study using estimated parameters
Estimated and/or assumed values of the parameters listed in Tables 3 and 4 determine the infinitesimal generator, Q, and the steadystate distribution of each gene. Developed on the global balance equation of GNetworks [23] and the exponentiallydistributed holding times of Markov chains [30], the empirical cumulative density function (ECDF) was exploited to confirm that parameter estimation via the APDA is appropriate aligning with the theory of GNetworks. We compare the ECDF of simulated data utilizing values in Tables 3 and 4 and the theoretical cumulative density function (CDF) based on q_{i} in Eq. 3. The algorithm for the simulation is explained in detail in Methods.
The ECDF, usually denoted by \(\hat {F}_{n} (x)\), is associated with cumulative frequency of observations (empirical sampled data). It is a nonparametric estimator of the underlying CDF of a random variable of interest and is formally defined as follows:
where \(\mathbb{1}_{\left [ \cdot \right ]}\) is an indicator function. That is, the ECDF is a step function that increases by \(\frac {1}{n}\) at each datum. The stationary probability distribution of each gene in GNetworks is in the geometric productform as stated in Eq. 2, which results in the following tail of the theoretical CDF, T(x_{i}):
Figure 4 (and Fig. 9) illustrates how the ECDF of hTERT utilizing estimated/assumed values of the parameters (Tables 3 and 4) converges to the theoretical CDF regardless of cell types. Similar patterns are obtained for all 5 statistically significant genes in this research.
Correlation between a pair of genes
We discuss the similarities or differences in the correlation of two genes between normal and malignant cells with either active telomerase or ALT. Figure 5 based on Eq. 9 illustrates the following:

First, Fig. 5 demonstrates the change of correlation between a pair of genes in the given system over time in normal cells and ALT (malignant) cells. We can then infer both the trend of correlation between a pair of genes and the speed to the transient state, i.e., before it reaches a steady state. Due to the productform stationary probability distribution of network state in the theory of GNetworks, the correlation coefficient becomes 0 when the system becomes stationary [31]. Assuming that the pair of genes are positively correlated at time 0, the positive correlation persists over time in both types of cells (normal and ALT) and practically reaches 0 (the steady state) approximately at t=0.8. As shown in the figure, the patterns of correlation between each pair of genes do not noticeably differ among the types of cells (normal or malignant with either ALT or active telomerase shown), although they are dissimilar from one pair to another within the same type of cells. For example, the correlation between CEBPA and FOXM1 in a transient state is stronger than that of cMyc and hTERT, and it reaches a steady state more slowly in all cell types.

Second, Eq. 9 uncovers the interactions between (1) CEBPA and hTERT, (2) FOXM1 and hTERT and (3) FOXM1 and E2F1, which are unknown in Fig. 3. The pattern in Fig. 5, which is analogous to Fig. 7, delineates that the relationship of the three pairs of genes is similar regardless of the mechanisms by which telomeres maintain their sufficient lengths. However, within the same condition of cells, the magnitude of correlation and the speed to the steady state vary by interactions. It is supported by the interaction of CEBPA and hTERT, which is relatively weaker than that of other pairs, even though its trend over time is indistinguishable by the cell types.
Note that if we conversely assume that a pair of genes are highly negatively correlated at the initial time point, then the negative correlation prevails over time as shown in Fig. 8.
Discussion
One important advantage of using mathematical modeling to understand dynamics of a biological system is that the model can be a costeffective and timesaving supplement or even a substitute for laboratory experiments in which patterns of the system are delicate and complex. Especially the stochastic approach is useful to quantify the role of fluctuations in the behavior of the system of interest. In this paper, we propose that a stochastic paradigm involving GNetworks and Stochastic Automata Networks both stemming from queuing theory, can contribute to the analysis of similarities and differences between telomerase activation and ALT using genes related to telomere maintenance. However, there are the following two caveats.

First, correlation coefficient, whose sign relies upon the initial joint state probability vector π_{ij}(0) in our example, evaluates the strength of the evidence for a relationship of two genes but does not determine causal relationships. In other words, even if a positive correlation between CEBPA and hTERT in ALT cells is revealed, it is not known which gene activates another one.

Second, the dimension of the infinitesimal generator, Q, which is a function of tensor products, can be enormously large, with the corresponding matrix being sparse depending on the number of states of each queue. The state space used in this research is relatively small. Computations in larger dimensions can be made practical by using Compressed Sparse Row and a number of methods for the approximation of the matrix exponential [32] such as Krylovtype techniques.
Conclusion
In spite of the caveats discussed in the previous section, the APDA based on GNetworks initially introduced in [18] can suggest a set of statistically significant genes (CEBPA, FOXM1, E2F1, cMYC, hTERT) in cells with either telomerase or ALT compared to normal cells from preexisting GRNs. We further confirmed that the APDA satisfactorily estimates the parameters, which decide the rates of convergence to stationarity as the ECDF of the simulated data using the estimated parameters approaches to theoretical CDF using q_{i∈{1,2,⋯,N}} as time progresses. Further, our correlation analysis based on SANs helps to infer the link between genes in various conditions that has not yet been discovered through experiments. We prove that our mathematical expression (Eq. 9) allows analytically calculating the correlation coefficients between any pair of genes in the given system at every time point and compare them in various types of cells for an order relation. Specifically in our example, the trend of correlation among genes in the system is not influenced by the mechanism (telomerase vs. ALT) by which telomeres maintain their sufficient lengths, even though the trend differs from one pair to another within the same type of cells. To conclude, this study provides a platform to detect significant genes and infer the previously unknown connection among them by applying modeling techniques borrowed from queueing theory. This is particularly important because telomere dynamics plays a major role in many physiological and disease processes, including hematopoiesis.
Methods
Detailed proof of Eq. 9
If Q is the infinitesimal generator and P(t) is the transition probability matrix of a finite Markov chain, we can derive a set of differential equations called Kolmogorov’s forward equations, in the form of P^{′}(t)=P(t)·Q
P(0) initial condition is P(0)=I, where I is an identity matrix having the same dimension as Q [33], consistent with
Solution of the forward equation for finite Markov chains is given by the power series expansion that always converges for any square matrix Q:
where · denotes l_{1}norm, and H(t) is is a linear operator with  H(t) =o(t), as t→0. When the infinitesimal generator, Q, is irreducible, its transition probability matrix, P(t) defined in Eq. 11, is strictly positive for each time t>0. It signifies that as the trajectory length N approaches to the limit, at least one transition between any pair of states will almost surely happen without regard to the sparsity of Q [34]. Note that 0=π·Q are a set of S linear equations, which is usually used to detect the stationary distribution π, if such one exists [26].
A formal solution to the time dependent state probability vector is defined as
where π(t) is a state probability vector at time t [35, 36]. In order to find a joint state probability vector π_{i,j}(t) of two automata, say i and j, we introduce two matrices called C_{i,j} and \(C^{*}_{i,j}\), which are (K^{N}×K^{2}) and (K^{2}×K^{N})dimensional matrices, respectively. Then based on Eq. 12, we achieve
Here, C_{i,j} and \(C^{*}_{i,j}\) are defined as follows respectively:
where
and
where
Note that \(1_{K}^{T}\) indicates the matrix transpose of 1_{K}, and we have
This results in
where
Therefore Eq. 13 finally becomes
Equation 14 implies that a timedependent joint state probability vector π_{i,j}(t) can be easily calculated, once the (global) infinitesimal generator of the entire system is obtained.
Once π_{i,j}(t) of two genes is obtained, we then can form a (K×K)dimensional contingency table that describes the joint probability for each time point t. Based upon it, the association between two genes for all t is evaluated using the Pearson productmoment correlation coefficient.
Application to telomere maintenance
Data description
Gene expression data (GSE14533) were obtained from the National Center for Biotechnology Information Gene Expression Omnibus (http://www.ncbi.nlm.nih.gov/geo/). Data includes expression gene levels of 3 types of cells: 18 ALT cell lines, 16 telomerasepositive cell lines and 4 normal (fibroblast) cell lines. Initially, the gene expression levels of 29 genes (hTERT, CRY2, FOXM1, cMYC, SOCS1, AHNAK, HDAC5, TK1, S100A4, LMO4, PRKD1, PER2, PRKCA, CEBPA, E2F1, RBPJ, TOMM20, AIP, EHD1, TGOLN2, TTC17, LAMP2, ATP5D, ADGRL1, LASP1, RPRD1A, HNRNPA3, KAT2A, STK24) were extracted from the data according to [37]. However, only 5 significant genes (CEBPA, E2F1, FOXM1, cMYC, hTERT) (connected to statistically significant edges) in either telomerasepositive or ALT cells compared to the normal cells, discovered by APDA based on GNetworks [18], have been included in this research. Note that the data were first normalized to the 50^{th} percentile to guarantee the identical medians across all samples. Then they were normalized again and scaled with mean 3 and variance 1 [18, 38]. Table 5 and Fig. 6 outline the data in detail.
Modification of the aPDA
We adopt APDA introduced originally in [18], but slight modification of assumptions on \(\lambda _{i}^{+}\) and \(\lambda _{i}^{}\) is added in this research as follows:

Define initiating genes as genes which do not receive any customer from other genes but send a customer to others within the system.

The arrival rate of negative customers from the external system, denoted by \(\lambda _{i}^{}\), of the initiating genes is assumed to be 0. This assumption enables the initiating genes to maintain their customers; thereby to be consistently activated.

The arrival rate of positive customers from the external system is defined as follows:
$${{\begin{aligned} \lambda_{i}^{+} = \left\{\begin{array}{ll} D_{i}^{\; in} + 3 \;\;\;\;\; &, \;\;\; \text{if} \;\; i \; \in \; \left\{ \text{Indices of noninitiating genes} \right\} \\ \frac{\bar{x}_{i}}{\bar{x}_{i} + 1} \times \mu_{i} \;\;\;\;\; &, \;\;\; \text{if} \;\; i \in \left\{ \text{Indices of initiating genes} \right\} \end{array}\right. \end{aligned}}} $$where \(\bar {x}_{i}\) is the average mRNA expression level of the gene i in normal cell lines. Here, \(D_{i}^{\; in}\) represents the indegree of gene i, which is the number of edges incoming to node i. The purpose of adding 3 to the noninitiating genes is to prevent the numerator of q_{i} from becoming 0. The definition of \(\lambda _{i}^{+}\) for the initiating genes stems from the following logic: the indegree, arrival rate of the negative customers from the external system and transition probabilities of an initiating gene are all 0; that is,
$$\begin{array}{*{20}l} D_{i}^{\; in} \; &= \; \lambda_{i}^{} \; = \; p_{{ji}}^{+} \; = \; p_{{ji}}^{} \; = \; 0 \;\; \text{for} \; i \in\\& \left\{ \text{Indices of initiating genes} \right\}. \end{array} $$In such cases, the parameters of stationary distribution in Eq. 3 are \(q_{i} = \frac {\lambda _{i}^{+}}{\mu _{i}} \), resulting in \(\lambda _{i}^{+} = q_{i} \times \mu _{i} \) for all i∈{Indices of initiating genes}. Because the numerical value of q_{i} is unknown yet, we estimate it based on the property of the geometric distribution with parameter (1−q_{i}) as follows:
$$\begin{array}{*{20}l} \bar{x}_{i} & = \frac{1  \left(1  q_{i} \right)}{1  q_{i}} = \frac{q_{i}}{1  q_{i}} \\ \Rightarrow \;\;\; \bar{q}_{i} & = \frac{\bar{x}_{i}}{1 + \bar{x}_{i}} \end{array} $$(16)Equation 16 finally leads to the definition of \(\lambda _{i}^{+}\) for i∈{Indices of initiating genes}. Note that, according to Eq. 3, \(\bar {q}_{i}\) describes the estimate of the steadystate probability that there is at least one mRNA of the gene i [18].
Rules and assumptions of other parameters (shown in Table 2) in this research are identical to those in [18].
Algorithm: simulation study
According to the global balance equation of GNetworks [23–25], a movement of mRNA expression levels of a gene in small time Δt is decided by one of the 4 cases as shown in Table 6.
Algorithm 1 contains the details of the simulation assessing the estimated parameter values from the APDA.
Appendix: supplementary figures/tables
Availability of data and materials
Data used in this research can be downloaded from the National Center for Biotechnology Information Gene Expression Omnibus. Further details are in the Data description section.
Abbreviations
 ALT:

Alternative lengthening of telomeres
 SAN:

Stochastic automata network
 GRN:

Gene regulatory network
 APDA:

Abnormal pathway detection algorithm
 AML:

Acute myeloid leukemia
 ECDF:

Empirical cumulative density function
 CDF:

Cumulative density function
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Acknowledgments
We thank Dr. Khanh Dinh of the department of Statistics at Rice University (currently at Columbia University) for help with Fortran programming.
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This article has been published as part of BMC Genomics Volume 21 Supplement 9, 2020: Selected original articles from the Sixth International Workshop on Computational Network Biology: Modeling, Analysis, and Control (CNBMAC 2019): genomics. The full contents of the supplement are available online https://bmcgenomics.biomedcentral.com/articles/supplements/volume21supplement9.
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This research was supported by National Institute of Health grant 5R01HL128173. The funding agency played no part in neither any aspect of the study, nor the decision to publish. Publication costs were funded in part by the Rice University Libraries Open Access Publishing Fund.
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All authors contributed to the development and implementation of the mathematical result. blueKL analyzed the data for the application part and produced the numerical results/plots using R. She wrote the first draft of the paper. MK revised the draft for submission. All authors read and approved the final manuscript.
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Lee, K.H., Kimmel, M. Analysis of two mechanisms of telomere maintenance based on the theory of gNetworks and stochastic automata networks. BMC Genomics 21 (Suppl 9), 587 (2020). https://doi.org/10.1186/s12864020069379
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DOI: https://doi.org/10.1186/s12864020069379