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    <article-meta>
      <title-group>
        <article-title>Modeling and Decision Support for the Firms' Pricing Policy under a Chaotic Dynamic of Market Prices</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Ekaterina V. Orlova</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Ufa State Aviation Technical University</institution>
          ,
          <addr-line>Ufa</addr-line>
          ,
          <country country="RU">Russia</country>
        </aff>
      </contrib-group>
      <abstract>
        <p>The article presents the results of the study of nonlinear market prices dynamic, simulated using game theory model, maps and theory of bifurcation. Market pricing is presented as a two-dimensional map. Qualitative analyses of the rms' pricing system properties using the xed points, analysis of the trajectories near these xed points were ful lled Simulation of the market prices dynamic showed that the xed point of the map coincides with the local Nash equilibrium, so the analysis of the stability of Nash equilibrium was done based on the maps' xed points sustainability analysis. Numerical simulation results were visualized, bifurcations of the xed point were identi ed and transition from periodic to chaotic mode was demonstrated. Sustainability analysis was carried out with using Jacobian. The mechanism for the pricing decision support, allowing under a chaotic market dynamics to ensure maximum e ciency of the rms was proposed.</p>
      </abstract>
      <kwd-group>
        <kwd>nonlinear economic dynamics</kwd>
        <kwd>visualization of chaos</kwd>
        <kwd>pricing decision making</kwd>
        <kwd>xed point stability criteria</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>-</title>
      <p>The last two decades the scienti c literature has been widely discussing the
concept of deterministic chaos, chaotic dynamics occurring in di erent systems.
Di erent approaches and methods for chaos control in theoretical and applied
problem solution are suggested. At the same time a lot of attention is given to
managing the impact of low power, meaning that the system has a number of
characteristics, inherent properties and laws which allow to achieve expected
results using weak management actions (without spending of signi cant resources).</p>
      <p>In a number of studies of nonlinear systems dynamic (physical, chemical,
biological, economic), it was found that the dynamic chaos mode is a typical
phenomenon. Chaotic properties are manifested in a variety of systems, and if
the chaos is not found, the reasons for this may be either the existence of chaos
in a small area of the parameter space, or it is out of range of parameters.</p>
      <p>Research associated with the problems of predictability of chaotic systems,
control of system dynamics and stabilization of chaos is rapidly developing in
di erent elds. Theoretical and applied studies in these elds have revealed an
unexpected property of chaotic dynamical systems: they are controlled by
external actions [3,13,18,21]. That is, by smaller impacts it is possible to signi cantly
a ect the dynamics of chaotic systems, to stabilize their dynamics, transferring
it from the chaotic mode to the required periodic mode.</p>
      <p>In relation to economic systems the following studies in the eld of chaos
control were conducted: [1, 2, 5{8, 11, 12, 14, 15, 19, 20]. Chaos control is proposed
on the basis of production cost reduction [2], an increase in investment
activity [11, 19], or control impacts are con rmed on the basis of revealed connection
between the previous and current variables values, i. e. by e ective use of
feedback [2, 19, 22].
2</p>
      <p>Phenomenon of Chaotic Market Dynamic: the Model
Chaotic systems are a class of uncertain models that di ers from deterministic
and stochastic systems in their properties [4]. In deterministic systems it is
possible to build the future system trajectory from the initial state to in nite time
interval. In stochastic systems it is possible to estimate the future system state
into short time interval,determined by the prediction accuracy.</p>
      <p>We consider a duopoly as a market model, when two rms-producers
cooperate on the market, and the pricing process is controlled by price (which
rms o er there di erential products to consumers) change. Further it will be
illustrated that the pricing system is chaotic and then we will o er the decision
support model for stabilization market prices dynamic.</p>
      <p>The main precondition of the model:
{ The model of duopoly (model of price competition) with a di erentiated
product in which the consumer demand function is given a utility function
with constant elasticity of substitution is used;
{ Pricing dynamics is modeled as a map (recurrence relations);
{ Modeling of pricing decisions is realized with using the game theory and
methods of nonlinear dynamic.</p>
      <p>The model designations: i 2 I { producer's number; pi { price of the i-th
producer ( rm); qi { the volume of sales of i-th producer; qi(p) { demand for
the product of i-th producer; ci { unit costs for the product of i-th producer;
i(p) = (pi ci) qi(p) { pro t of i-th producer.</p>
      <p>Prices vector p = (pi ; i 2 I) is a local Nash equilibrium when it satis es the
following conditions of local maxima conditional of the pro t function:</p>
      <p>The strategy of i-th producer is a price changing, which is proportional to
the change of its pro ts with some constant ki &gt; 0 in order to maximize their
e ectiveness, i. e. to achieve the global sustainable Nash equilibrium. The model
of competitive interaction of rms described by two-dimensional system of
differential equations was o ered in [16, 17] and represented as:
8
&gt;&lt; p1(t + 1) = p1(t) + k1 ( p12(t)p2(t)+2c1p1(t)p2(t)+c1p22(t)) ;</p>
      <p>
        (p21(t)+p1(t)p2(t))2
&gt;: p2(t + 1) = p2(t) + k2 ( p1(t)p22(t)+2c2p1(t)p2(t)+c2p12(t)) ;
(p22(t)+p1(t)p2(t))2
(
        <xref ref-type="bibr" rid="ref1">1</xref>
        )
where p1(t), p2(t) are product prices of rst and second producers at discrete
time t; second terms in both equations show the prices changing in period t, and
how this changing will a ect the price in the next period (t + 1). Parameters k1
and k2 characterizes the prices increasing due to changes in the rms' pricing
policy; c1 and c2 represents a production cost of the rst and second producer
respectively.
      </p>
      <p>
        Nash equilibrium, characterized by a pair of prices p1 and p2, is the solution
of the following equations:
8
&lt; p1 = c1 + c1
: p2 = c2 + c2
q
q
1 + Ap21 ;
1 + Ap12 :
(
        <xref ref-type="bibr" rid="ref2">2</xref>
        )
Analyze the evolution of the system (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) according to the parameter values k1,
k2, A1, A2 identify the area of stability, bifurcations and chaos. Such analysis has
been made based on the known analytical and graphical criteria of dynamic chaos
[10, 13]: the Lyapunov exponents, bifurcation diagrams, attractors of the system
by varying the system parameters. Then, in order to control the system dynamic
on the basis of the revealed laws, it is necessary to nd the method for parameters
changing in order to provide an expected mode of the system dynamic. For each
rm, this means the monitoring and controlling of their costs Ai and changing
in pro t for the period and the selection of appropriate control ki. In practice
this means the variation of price, which causes both rms to balance interests,
i. e. the Nash equilibrium.
      </p>
      <p>From the economic point of view, this means that rms choose the mode (and
parameters), which will lead to a change in the market, resulting in price levels
will evolve predictable dynamic. If such control is permissible, then a transition
to the market equilibrium will proceed, that ensure for each rm the maximum
e ectiveness.</p>
      <p>
        The xed point (p10; p20) of the system (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) is a point which goes into itself
under a single iteration of the map and is determined on the basis of equations:
(
p10 = f (p10; p20);
p20 = g(p10; p20);
where f { the function p1(t + 1) of p1(t) and p2(t), g { the function p2(t + 1)
of p1(t) and p2(t) of the map (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ).
      </p>
      <p>
        The decision of the latter system of equations will obviously be the same as
the solution of the system (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ). Therefore, the xed point of map (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) coincides
with the Nash equilibrium, for a certain competitive interaction between rms.
The nature of the stability of a xed point is de ned by its multipliers, which are
the eigenvalues of the perturbation matrix (Jacobian) and their number is equal
to the dimension of the display. The bifurcation analysis and stability analysis
of two-dimensional maps is carried out on the basis of parameters { invariants
of Jacobi matrix. For the two-dimensional map there are track and Jacobian
of Jacobi matrix. Jacobi matrix of the dynamic system (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) at a xed point is
as follows:
      </p>
      <p>
        Mc =
Eigenvalues of this matrix are multiples of the map (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) 1 and 2, for which
the relation is performed: 2 S + J = 0, where S and J { two invariants of
Jacobi matrix { track and Jacobian, also S = 1 + 2, J = 1 2. In accordance
with a triangle of stability [9], the conditions of stability of a xed point are
presented as:
We form the prices Nash equilibrium p1 and p2, and nd the conditions to achieve
and maintain this balance for given costs Ai. If we x a cost A1,vA2 at the
level 0.07 and 0.12 respectively, the Nash equilibrium prices (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) are: p1 = 0:15;
p2 = 0:23. Jacobi matrix (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) at this point would be:
      </p>
      <p>Mc =
1
61k1
30:5k1
19:8k2 + 4 &gt; 0;</p>
      <p>
        The solution of this system of inequalities that de ne the triangle of stability
for the xed point of the two-dimensional map prices (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ), is shown in Fig. 1.
      </p>
      <p>Thus, the identi ed area of admissible values of adaptive price parameters k1
and k2 is highlighted in gray. To ensure the stability of the Nash price equilibrium
(0.15; 0.23) in the conditions of the given cost values of both rms at 0.07 and
0.12 will allow the use of such rms adaptation strategy, which is based on a set
of adaptation options combinations that are within the acceptable area.</p>
      <p>As soon as the control parameters deviate from the permissible values, there
occurs the equilibrium stability loosing and the system goes to another unstable
mode { chaos. That is, in any initial price of rms if they use a pricing
strategy in accordance with the values determined above, the rm de nitely reaches
the Nash equilibrium. These pricing values are not able to change the Nash
price equilibrium, so to increase the e ciency the rm should use the proposed
decisions.</p>
      <p>
        Figure 2 shows the chaotic attractors of system (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) in terms of unit costs
A1 = 0:07; A2 = 0:12 and variations in the parameters k1, k2. For instance, when
the values of the chaotic attractor of price adaptation parameters are k1 = 1,
k2 = 1:15 it demonstrates the chaotic pricing system dynamic. This mode is
determined by nonlinear system properties and manifests itself in an exponentially
rapid divergence of initially close trajectories in a bounded phase space.
      </p>
      <p>The chaotic nature of the prices system dynamics is due to the instability of
the phase trajectories, the growth of small initial perturbations in time, mixing
elements of the phase space and, as a consequence, leads to unpredictable system
dynamic over long term.</p>
      <p>In making pricing decisions in addition to the criterion of economic e ciency
the rms must take into account the objective nature of the market dynamics
as a whole and take into account the possibility of a chaotic regime of market
dynamics.</p>
      <p>Results and conclusions
The described approach for rms pricing using the methods of game theory,
nonlinear dynamics and bifurcation theory provides a new perspective on the
dynamics of the process of competitive interaction of the rms and makes it
possible to conduct a qualitative and visual analysis of the system properties
with help of the singular points of the phase space ( xed points) and to analyze
the systems trajectories near these xed points.</p>
      <p>It is shown that the market pricing system has complex and diverse types of
dynamics, so that the structure of the phase space and its dependence on the
parameters of this structure are very complex. The phase space of the system is
heterogeneous and has two basic types of system dynamic { stability and chaos.</p>
      <p>Prices dynamics is modeled using a two-dimensional map; coordination of
rms' pricing decisions is based on monitoring the stability of the Nash
equilibrium. The analysis of the developed model shows that the Nash equilibrium
coincides with the map xed point prices. Therefore, the analysis of Nash
equilibrium stability is carried out on the basis of the analysis of the map xed
points sustainability. Numerical simulations are demonstrated the existence of
xed point bifurcations. Chaos in market pricing model means that when one
rm change its price even slightly this can lead to unpredictable market prices
changing of another producers and total market in long term. Therefore, all
producers must have the tools of chaos control.</p>
      <p>In order to avoid unexpected chaotic dynamics in market prices the
mechanism for decision making support is o ered and is based on the price changing
proportional to marginal pro t changing of each rm. These mechanism would
ensure the stability of the Nash equilibrium, and therefore would balance the
rms' economic interests, would coordinate price decisions and maintain
maximum rms e ciency.</p>
      <p>
        For the complex research and analysis of rms competitive interaction we use
the author program for modeling and visualization of nonlinear pricing dynamics
and decision support in rms price strategies. The program is designed to
simulate the strategic cooperation in the rms pricing process, use a four-parameter
map and form the optimal pricing policy in oligopoly, provided the e ective
control and decision making under prices chaotic dynamics. The program has the
following functions:
{ Assessment of local Nash equilibrium of prices;
{ Identi cation of bifurcations of xed price points in the map;
{ Identi cation of modes of stability and dynamical chaos in pricing;
{ Identi cation of transition scenarios to dynamical chaos;
{ Forming the pricing decisions, ensuring stable mode of market prices
dynamic.
12. Loskutov, A.Y.: Non-linear optimization of chaotic dynamics of the market.
Economics and Mathematical Methods 46(
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13. Loskutov, A.Y., Mikhailov, A.S.: Fundamentals of the Theory of Complex Systems.
      </p>
      <p>Institute of Computer Science, Moscow { Izhevsk, Russia (2007)
14. Moon, F.: Chaotic Oscillations: Introductory Course for Scientists and Engineers.</p>
      <p>Mir, Moscow, Russia (1990)
15. Neimark, Y.I., Ostrovsky, A.V.: On some models of pricing in the market economy.</p>
      <p>
        Izvestiya VUZ. Applied Nonlinear Dynamics 6, 35{41 (1999)
16. Orlova, E.V.: Model for economic interests agreement in duopoly's making pricing
decision. Computer Research and Modeling 7(
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17. Orlova, E.V.: Concept for industrial and economic systems management based on
criteria coordination of interested agents. Program Engineering 2, 86{96 (2016)
18. Ostrovsky, A.A.: About one class of models of competitive pricing in the market
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19. Puu, T.: Nonlinear Economic Dynamics. Springer Berlin Heidelberg, Berlin,
Heidelberg (1991)
20. Puu, T.: Attractors, Bifurcations, and Chaos: Nonlinear Phenomena in Economics.
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21. Schuster, H.G., Just, W.: Deterministic chaos : an introduction. Wiley-VCH,
Weinheim (2005)
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