<!DOCTYPE article PUBLIC "-//NLM//DTD JATS (Z39.96) Journal Archiving and Interchange DTD v1.0 20120330//EN" "JATS-archivearticle1.dtd">
<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Computer research of nonlinear stochastic models with migration flows</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Anastasia V. Demidova</string-name>
          <email>demidova_av@rudn.university</email>
          <xref ref-type="aff" rid="aff1">1</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Olga V. Druzhinina</string-name>
          <xref ref-type="aff" rid="aff2">2</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Olga N. Masina</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Ekaterina D. Tarova</string-name>
          <email>katerina.tarova@yandex.ru</email>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Bunin Yelets State University Communards str.</institution>
          <addr-line>28, Yelets, 399770, Russian Federation</addr-line>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>Department of Applied Probability and Informatics Peoples' Friendship University of Russia Miklukho-Maklaya str.</institution>
          <addr-line>6, Moscow, 117198, Russian Federation</addr-line>
        </aff>
        <aff id="aff2">
          <label>2</label>
          <institution>Federal Research Center “Computer Science and Control” of Russian Academy of Sciences Vavilov str.</institution>
          <addr-line>44, building 2, Moscow, 119333, Russian Federation</addr-line>
        </aff>
      </contrib-group>
      <pub-date>
        <year>2019</year>
      </pub-date>
      <fpage>26</fpage>
      <lpage>37</lpage>
      <abstract>
        <p>The problems of the design methods extension and computer research of nondeterministic ifnite-dimensional population models describing migration flows are studied. The significant dificulties arise in the construction of high dimension dynamic models in the course of analytical research. Computer research allows not only to obtain the results of numerical experiments to search for trajectories and estimate the parameters of deterministic models, but also to reveal the efects caused by stochasticization. The model parameters are estimated and local phase portraits are constructed for the initial four-dimensional migration-population model. The transition from the vector ordinary diferential equation to the corresponding stochastic diferential equation is performed. The structure of the stochastic model is described on the basis of applying the method of constructing self-consistent stochastic models. As a tool for the study of population-migration models, a software package is used to solve numerically the diferential equations systems using modified Runge-Kutta methods. The software package allows numerical experiments based on the implementation of algorithms for generating trajectories of multidimensional Wiener processes and multipoint distributions and algorithms for solving stochastic diferential equations. The comparative analysis of the computer research results obtained for stochastic models is carried out. The properties of migration-population systems in deterministic and stochastic cases are characterized. The comparison of the results obtained for the three-dimensional and four-dimensional cases is carried out. The efects inherent in models with migration flows are revealed.The obtained results can be applied to the problems of modeling and forecasting the behavior of multidimensional systems describing the migration flows.</p>
      </abstract>
      <kwd-group>
        <kwd>and phrases</kwd>
        <kwd>computer modeling</kwd>
        <kwd>nonlinear models of migration flows</kwd>
        <kwd>stochasticization of one-step processes</kwd>
        <kwd>symbolic representation algorithms</kwd>
        <kwd>symbol computing libraries</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>-</title>
      <p>Copyright © 2019 for the individual papers by the papers’ authors. Copying permitted for private and
academic purposes. This volume is published and copyrighted by its editors.</p>
      <p>In: K. E. Samouylov, L. A. Sevastianov, D. S. Kulyabov (eds.): Selected Papers of the IX Conference
“Information and Telecommunication Technologies and Mathematical Modeling of High-Tech Systems”,
Moscow, Russia, 19-Apr-2019, published at http://ceur-ws.org</p>
    </sec>
    <sec id="sec-2">
      <title>1. Introduction</title>
      <p>The construction and study of the models with migration are devoted to the work
of various authors (see, for example, [1–3]). In [2–6] migration flows in deterministic
population is considered. The analysis of distributed multidimensional population
models taking into account cross-migration is carried out in papers [7–10]. Migration
mechanisms can be described by both linear and non-linear functions, and lead to
diferent efects [2, 11]. In [3, 5, 11, 12] the issues of qualitative behavior and sustainability
of population-migration models are studied. In [13–15] a qualitative analysis of a
three-dimensional non-deterministic model with migration is performed. To study
the model, a combination of known methods of synthesis and analysis of models and
a method for constructing stochastic self-consistent models are used [16]. In [12] a
methodological support is developed for the analysis and synthesis of multidimensional
nonlinear dynamic models describing migration flows taking into account the efects of
broadband parametric and additive noise. The stability of stationary states is studied
and the efects obtained for stochastic models are interpreted. The model examples
show a comparison of the migration-population systems properties in deterministic and
stochastic cases and the efects due to stochastic broadband perturbations are revealed.</p>
      <p>When modeling population-migration systems, various software tools are used that
present wide possibilities for building computer models and carrying out computational
experiments. However, many software products do not contain libraries for numerical
and symbolic calculations and do not have suficient computational complexity. In this
regard, in the study of the population-migration systems models, the application of
mathematical packages and general-purpose programming languages [17–19] is relevant.
In [20] suficient conditions are proposed for the uniform stability of the equilibrium
states of a four-dimensional non-linear model of population dynamics. In [21] the
Maxima mathematical package is used to study the stability of this model. One of
the instrumental software tools for studying population-migration models is a software
package for the numerical solution of diferential equations systems using modified Runge
– Kutta methods. The specified complex was developed in [22, 23]. The software package
allows numerical experiments based on the implementation of algorithms for generating
trajectories of multidimensional Wiener processes and multipoint distributions and
algorithms for solving stochastic diferential equations.</p>
      <p>The several types of four-dimensional models with migration flows are studied in
this paper. A comparative analysis of the computer research results obtained for
threedimensional and four-dimensional stochastic models with migration flows is carried
out. A comparison is made of the qualitative properties of four-dimensional models,
taking into account changes in migration rates, as well as intraspecific and interspecific
interaction coeficients. The properties of the models in the deterministic and stochastic
cases are characterized. As a tool for the study of the models, a software package in the
Python language using the NumPy and SciPy libraries is used.</p>
      <p>2.</p>
    </sec>
    <sec id="sec-3">
      <title>Deterministic Migration Models</title>
      <p>A nonlinear model is considered that is described by a system of ordinary diferential
equations of the form:</p>
      <p>
        The following notation is used in (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ): 1, 3 and 4 is the population density of
competing species in the area of the forma 1 (area 1), 2 is the population density
(
        <xref ref-type="bibr" rid="ref1">1</xref>
        )
in the area of the form 2 (area 2), 13, 14, 31, 34, 41, 43 &gt; 0 are the coeficients of
species competition in the area of 1,  &gt; 0 and  &gt; 0 are the coeficients of the migration
of species between two areas, while area 2 is a refuge and  ̸=  .
      </p>
      <p>
        In the model (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) the first two equations describe the dynamics of one type taking
into account migration processes. The first equation sets the dynamics in the first area,
the second one sets the dynamics in the second area. The third and fourth equations
describe the dynamics of the second and third types, interacting as competitors with
the first type in the first area. Previously, we studied the three-dimensional model (two
species, the first species migrated to another area, and in the first area it competed with
the second type).
      </p>
      <p>
        In the case when 13 = 31, 14 = 41, 34 = 43, the model (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) takes view
At the same migration rates  =  =  from (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) we get a model of the form
where 1 and 3 are the density of populations of competing species in the area of the
form 1 (area 1), 2 is the population density in the area type 2 (area 2), 13 &gt; 0 is the
coeficient of competition of species in the area 1. The results of the analysis of the (
        <xref ref-type="bibr" rid="ref4">4</xref>
        )
model and the generalized stochastic model are presented in [13–15]. The model (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ) is a
generalization of the model considered in [3], in the case when the migration rates are
diferent.
      </p>
      <p>
        The numerical experiment for the model (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ) is carried out with the help of the
developed software for the study and numerical solution of systems of ordinary and
stochastic diferential equations using the Runge–Kutta method [22, 23]. The library is
written in Python using the NumPy and SciPy modules. The models (
        <xref ref-type="bibr" rid="ref1">1</xref>
        )–(
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) and their
stochastic generalizations are studied using this software package.
      </p>
      <p>
        For the numerical experiment of the deterministic model, the following sets of
parameters are chosen: the initial values 1(0) = 0.5, 2(0) = 1.0, 3(0) = 0.5 for
the three-dimensional model and 1(0) = 0.5, 2(0) = 1.0, 3(0) = 0.5,4 = 0.7 for a
(
        <xref ref-type="bibr" rid="ref2">2</xref>
        )
(
        <xref ref-type="bibr" rid="ref3">3</xref>
        )
(
        <xref ref-type="bibr" rid="ref4">4</xref>
        )
four-dimensional model, the values of the parameters 13 = 1.2, 14 = 0.5, 34 = 1.4,
 = 1.5,  = 0.2.
      </p>
      <p>
        Fig. 1 presents solution trajectories for (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) and (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ) models with the specified initial
values and parameter values in the time interval [0,40]. The efect of an additional
competitor on the migration flow is shown. The introduction of an additional competitor
corresponding to the phase variable 4, leads to a decrease in both the density of the
migrating population in both areas and the density of the competitor corresponding to
the variable 3.
      </p>
      <p>
        With the values of the parameters 13 = 0.9, 14 = 0.4, 34 = 0.8, 34 = 0.6,
41 = 0.5, 43 = 0.7,  = 0.25,  = 0.3 in the model (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) there are the following equilibria:
1(0, 0, 0, 0), 2(
        <xref ref-type="bibr" rid="ref1">0, 0, 0, 1</xref>
        ), 3(
        <xref ref-type="bibr" rid="ref1">0, 0, 1, 0</xref>
        ), 4(0, 0, 0.69, 0.517), 5(0.63, 0.949, 0.4957, 0),
6(0.75, 0.98, 0.043, 0.595). Here 1,  5 are unstable nodes, 2 − 4 are saddles, 6 is a
stable node.
      </p>
      <p>
        Consider the models (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) and (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) with the same set of migration velocity values for these
models, but with diferent sets of intraspecific and interspecific interaction coeficients.
Solution trajectories for the model (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) with the values of the parameters 13 = 0.9,
14 = 0.4, 31 = 0.8, 34 = 0.6, 41 = 0.5, 43 = 0.7 and the trajectories of solutions for
the model (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) with 13 = 1, 14 = 0.6, 34 = 0.7 in the time interval [0, 25] is presented
in fig. 2. For models (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) and (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) the initial values are (1(0), 2(0), 3(0), 4(0)) =
(0.3, 0.7, 1.1, 0.8), values of migration speeds  = 0.25,  = 0.3. In fig. 2 a record of the
form (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ),  = 1, 2, 3, 4, indicates the trajectory corresponding to the phase variable 
for the model (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ), a record of the form (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) denotes the trajectory corresponding to
the phase variable  for the model (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ).
      </p>
      <p>
        As a result of a comparative analysis of the solution trajectories of (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) and (
        <xref ref-type="bibr" rid="ref2">2</xref>
        )
presented in fig. 2:
1) in the model (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) the population of 4 is dying out, the population density of 1 is
increasing, and the population density of 3 is decreasing;
2) for the models (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) and (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) favorable conditions are created in the second area, and
the population density of 2 increases;
3) in the model (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) competition intensified, which led to the extinction of the 4
population and the improvement of living conditions for the 1 and 3 populations.
      </p>
      <p>
        For the values of the parameters 13 = 1.2, 14 = 0.5, 34 = 1.4,  = 0.3 in model (
        <xref ref-type="bibr" rid="ref3">3</xref>
        )
there are the following equilibrium positions: 1(0, 0, 0, 0), 2(
        <xref ref-type="bibr" rid="ref1">0, 0, 0, 1</xref>
        ), 3(
        <xref ref-type="bibr" rid="ref1">0, 0, 1, 0</xref>
        ),
4(0, 0, 0.42, 0.42), 5(
        <xref ref-type="bibr" rid="ref1 ref1">1, 1, 0, 0</xref>
        ), 6(0.76, 0.94, 0, 0.62). Here 2 − 5 are saddles, 1 is
an unstable node, 6 is a stable node.
      </p>
      <p>
        Consider the models (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) and (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) taking into account the coincidence of the intraspecific
and interspecific interaction for these models. Note that in the model (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) in the general
case  ̸=  , and in the model (
        <xref ref-type="bibr" rid="ref3">3</xref>
        )  =  . Solution trajectories for models (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) and (
        <xref ref-type="bibr" rid="ref3">3</xref>
        )
with the values of the parameters 13 = 1.2, 14 = 0.5, 34 = 1.4 and the initial values
(1(0), 2(0), 3(0), 4(0)) = (0.5, 1, 0.8, 1) in the time interval [0, 25] are presented
in fig. 3. For the model (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) the values of migration speeds  = 1.5,  = 0.2, for the
model (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) the value of migration speed  = 0.3. In fig. 3 the record of the form (
        <xref ref-type="bibr" rid="ref3">3</xref>
        )
denotes the trajectory corresponding to the phase variable  for the model (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ).
      </p>
      <p>
        As a result of a comparative analysis of the solution trajectories of the (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) and (
        <xref ref-type="bibr" rid="ref3">3</xref>
        )
models shown in fig. 3, the following conclusions are obtained:
1) in the model (
        <xref ref-type="bibr" rid="ref3">3</xref>
        )the population density 4 increased insignificantly, and the
population density 1 decreased, while the population 3 in both models is rapidly
dying out;
2) as the migration rate increases, the model (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) in the second area creates more
favorable conditions than in the model (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ), so the population density 2 increases
significantly.
      </p>
      <p>
        For a series of parameter sets, stationary states of the model (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) are found. It is
established that for the values of the parameters 13 = 1.2, 14 = 0.5, 34 = 1.4,  = 1.5,
 = 0.2 in the model (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) the following stationary states exist: 1(0, 0, 0, 0), 2(
        <xref ref-type="bibr" rid="ref1">0, 0, 0, 1</xref>
        ),
3(
        <xref ref-type="bibr" rid="ref1">0, 0, 1, 0</xref>
        ), 4(1.18, 0.29, 0, 0), 5(0, 0, 0.42, 0.42), 6(0.93, 0.25, 0, 0.53). In addition,
the system is linearized in the vicinity of stationary states and the stability on the
ifrst approach is investigated. For the model (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) the projections of the phase portraits
(1, 2) are shown in fig. 4. The projections of the phase portraits (1, 2) in the vicinity
of equilibrium positions are shown in fig. 5. The projections of the phase portraits
(1, 3) are shown in fig. 6.
      </p>
      <p>3.</p>
    </sec>
    <sec id="sec-4">
      <title>Stochastic Migration Models</title>
      <p>
        Questions of constructing and studying a stochastic model for a three-dimensional
system with regard to migration are considered in the works [13–15]. In this paper,
stochastization of (
        <xref ref-type="bibr" rid="ref1">1</xref>
        )–(
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) models is carried out using the method of constructing
selfconsistent stochastic models [16]. The basis of this method is combinatorial methodology.
This method involves recording the system under study as an interaction scheme, i.e. a
symbolic record of all possible interactions between elements of the system. For this, the
a) 1 b) 2
c) 3 d) 4
d) 5Figure 6. Phase portraits for the model (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ).d) 6
system state operators and the system state change operator are used. Then we can get
the drift and difusion coeficients for the Fokker–Planck equation, which allows to write
the equation itself and its equivalent stochastic diferential equation in the Langevin
form.
      </p>
      <p>However, an increase in the dimension and complexity of the system under study leads
to the complexity of the analytical conclusion of the necessary coeficients of the Fokker–
Planck equation. As a solution to this problem, a software implementation is developed
for obtaining the coeficients of the Fokker–Planck equation from interaction schemes
using a symbolic computation system. This software implementation is a modification
of the stochastization method for one-step processes in the computer algebra system
described in [24]. This implementation is introduced as a module into a software package
developed earlier for the numerical study of deterministic and stochastic models [22].</p>
      <p>The following is the algorithm for obtaining the symbolic notation of a stochastic
diferential equation (Algorithm 1).</p>
      <p>Algorithm 1. Getting the system of diferential equations from the interaction
scheme</p>
      <p>Initial parameters: interaction scheme.</p>
      <p>Result: system of diferential equations in the form of Langevin.</p>
      <p>Start:
1. Getting the system state operators from the interaction scheme.
2. Getting the change of the system state.
3. Getting the transition intensities.
4. Record the coeficients of the Fokker–Planck equation.
5. Record the system of diferential equations.
end</p>
      <p>To implement the described algorithm, SymPy [17], computer computing system
is used, which is a powerful symbolic computation library for the Python language.
In addition, the output data obtained using the SymPy library can be transferred for
numerical calculations using the NumPy [19] library and SciPy [18].</p>
      <p>
        To obtain a stochastic model corresponding to the models (
        <xref ref-type="bibr" rid="ref1">1</xref>
        )–(
        <xref ref-type="bibr" rid="ref3">3</xref>
        ), it is necessary to
write the interaction scheme, which is as follows:
      </p>
      <p>→− 2,  = 1, 4;
 +  →− ,  = 1, 4;
 + →−−
The values of the coeficients for each of the models are given in the table 1.</p>
      <p>The first line corresponds to the natural reproduction of the species in the absence
of other factors, the second line symbolizes intraspecific competition, and the third one
is interspecific competition. The last line corresponds to the description of the species
migration process from one area to another. Then, expressions for the coeficients of the
Fokker–Planck equation are obtained for this interaction scheme using the developed
software (fig. 7).</p>
      <p>
        Further, the coeficients are transferred to the appropriate module of the software
complex for the numerical solution of the constructed stochastic diferential equation.
For the numerical experiment of the obtained stochastic model, the parameters are
chosen, the same as for the numerical analysis of the deterministic model (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ). Fig. 8
presents the trajectories of average values for 100 realizations for the specified initial
values and parameter values in the time interval [0, 40].
      </p>
      <p>A numerical experiment showed the closeness of trajectories for stochastic and
deterministic cases. Similarly to the deterministic case, the mean values trajectories
of diferent implementations of the stochastic diferential equation solutions go to the</p>
      <p>
        Coeficients for the interaction scheme
(
        <xref ref-type="bibr" rid="ref5">5</xref>
        )


stationary mode, retain the character and values of the stationary state are weakly
distinguished.
      </p>
      <p>A series of numerical experiments is carried out using diferent sets of model
parameters. For each set, we analyzed the stationary states and constructed the trajectories of
solutions. Taking into account the characteristic cases, the peculiarities of the influence
of an additional competitor on the dynamics of the migrating population are revealed
and the efects of stochastization of one-step processes are described.</p>
      <p>4.</p>
    </sec>
    <sec id="sec-5">
      <title>Conclusions</title>
      <p>A computer study of nonlinear models with migration flows made it possible obtain
the results of numerical experiments on trajectory search and parameter estimation in the
case of high dimensionality of models, as well as to reveal efects due to stochasticization.
The estimation of the influence of an additional competitor type on the dynamics, stability
and level of migration in the multidimensional model is obtained. A comparative analysis
of computer simulation results showed that with an increase in the rate of migration
in the second area, more favorable conditions are created, which leads to a significant
increase in the number of the second population. At the same time, competition in
the first area is increasing, which leads to the extinction of one of the population. The
comparison of the results obtained for the three-dimensional and four-dimensional cases.
The software package developed in the Python language using the NumPy and SciPy
libraries is demonstrated suficient eficiency for computer studies of multidimensional
nonlinear migration models. Numerical experiments using problem-oriented software
show the closeness of the trajectories types for stochastic and deterministic cases. The
results obtained can be applied to the problems of computer modeling of ecological,
demographic and socio-economic systems.</p>
    </sec>
    <sec id="sec-6">
      <title>Acknowledgments</title>
      <p>The publication has been prepared with the support of the “RUDN University
Program 5-100” (Demidova A.V., numerical analysis).</p>
    </sec>
  </body>
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