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<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>the Distribution of COVID-19</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Yuriy Tymonin</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Kateryna Molodetska</string-name>
          <email>kateryna.molodetska@polissiauniver.edu.ua</email>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>Polissia National University</institution>
          ,
          <addr-line>Blvd Stary, Zhytomyr, 10008</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
      </contrib-group>
      <abstract>
        <p>Mathematical modelling of the COVID-19 epidemic is based on system dynamics and SIR models, which are not considered adequate. To overcome the shortcomings of modelling, a non-classical discipline, epidemic dynamics, is proposed. The epidemic should be viewed as an open, self-replicating dynamic system in epidemic dynamics. Epidemic dynamics models are based on a dynamic system model with an extended network of inverse relationship. This non-classical approach allows the tools of non-linear and non-equilibrium dynamics to be used and models of epidemic dynamics to be represented in the form of non-linear and nonstationary differential equations. The solutions of the equations are special COVID-19 distribution functions - functions of the flows and accumulation levels of the infected and the dead. The COVID-19 distribution functions show high accuracy in approximating the statistics, demonstrating the excellent adequacy of these functions in principle. The application of COVID-19 distribution functions makes it possible to quantitatively describe the basic concepts of an epidemic to carry out comparative parametric analysis of the distribution of diseases and predict the development of an epidemic. Epidemic dynamics models, approximation, parametric analysis of epidemic distribution Mathematical modelling of epidemic processes and the search for new drugs, vaccination and preventive measures contribute to disease control. In addition, quantitative model simulations can provide comparative analysis and predictions of temporal descriptions of key epidemic categories, such as the number of people who fall ill, recover, and die. Therefore, COVID-19 prevalence models are highly demanding to match statistical data and ensure that epidemic mechanisms and underlying conceptual descriptions are adequate.</p>
      </abstract>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>Introduction</title>
      <p>2022 Copyright for this paper by its authors.
they have been poorly linked to the formulation and solution of practical epidemiological problems.
Therefore, their use was inefficient. The author [6] reviewed a new methodology for mathematical
modelling of epidemics – “EPIDDINAMICS”. This methodology is based on the method of scientific
analogy in mapping the epidemic process with the process of "transfer" of matter in the equations of
mathematical physics. During an epidemic, a complex self-sustaining process of "transferring" a
population of a pathogen to a community of susceptible individuals is formed. The epidemic process in
this concept is described by a system of non-linear partial derivative equations, very "similar" to the
equations of hydrodynamics. However, analogies with hydrodynamics do not sufficiently reveal the
content of the self-sustaining process of disease spread.</p>
      <p>The nature of the COVID-19 coronavirus distribution statistics shows that the epidemic's dynamics
are highly like the logistic functions. Therefore, we note the application of logistic functions to
approximate a piece of given statistical information. The articles [7-10] use logistic-type models to
describe the spread of COVID-19. In [7], a mathematical model of the spread of the COVID-19
coronavirus epidemic is considered using a simplified logistic model describing the increase in cases.
The low accuracy of calculation results obtained in [7-8] can be attributed to the simplified
representations of logistic models used for modelling.</p>
      <p>Articles [9, 10] discuss the concept of modelling the spread of COVID-19 based on constrained
growth functions. In [9], the epidemic's wave structure, represented by a set of elementary epidemic
flows shifted along the time axis, is considered. However, the content of the articles does not sufficiently
reveal the mechanism of epidemic development, which reduces the accuracy of epidemic forecasts.
This issue can be explained by the classical methods of mathematical investigation of epidemic
processes. However, a fuller description of the epidemic development mechanism requires modern
nonclassical methods for studying complex systems involving non-linear and non-equilibrium dynamics.</p>
      <p>The article aims to develop mathematical models for the COVID-19 epidemic based on the
nonclassical approach using the methods and tools of non-linear and non-equilibrium dynamics. It allows
for the presentation of epidemic dynamics models in the form of non-linear and non-stationary
differential equations and dynamic models of system with an extended network of inverse relationship.
2.</p>
    </sec>
    <sec id="sec-2">
      <title>Models of Epidemic Dynamics</title>
      <p>The reason for the shortcomings of epidemic modelling is the simplification and inadequacy of the
mechanistic representations of system dynamics characteristic of classical mathematical modelling
methodology. In classical modelling methodology, it is common to represent the object of study using
the means of system dynamics [11-13] as epidemic dynamics. At the same time, an epidemic, a
progressive spread of infectious disease among people capable of causing an emergency, should be seen
as a complex systemic entity.
2.1.</p>
    </sec>
    <sec id="sec-3">
      <title>Main approaches</title>
      <p>Epidemic dynamics is a scientific discipline in the study of disease transmission processes that views
the epidemic as a complex open system, as a system dynamic viewed from a non-classical methodology.</p>
      <p>The core of epidemic dynamics is its model. Causality in large self-regulating systems reduces to
the action of a self-regulation program as a goal that ensures the reproduction of the system [Stepin]. It
enables the model of epidemic dynamics to be conceived of as a procedural reproduction system. A
model of epidemic dynamics in a non-classical methodology should have these properties:
• Openness means self-regulating systems are always open and exchange energy and substance
with the external environment (metabolism), due to which the processes of local order and
selforganization occur;
• Providing links with the environment through a network of linear and non-linear inverse
relationship;
• Conditions of equilibrium as a state of crisis;
• Non-equilibrium functioning outside of the equilibrium conditions
• Reproduction of the system through positive inverse relationship.</p>
      <p>The methods and tools of the theory of non-linear non-equilibrium dynamical systems are used to
describe the epidemic dynamics model. The epidemic dynamics model is based on a dynamical system,
a mathematical model of an object, process or phenomenon that neglects fluctuations and all other
statistical phenomena. A dynamic system is a system with a state. In this approach, a dynamical system
describes (in general) the dynamics of some process, namely, the process of a system moving from one
state to another. An epidemic dynamics model consists of abstract elements representing some
properties of the modelled system. The following elements are distinguished: integrator, adder, and
inverse relationship chains, which link the variables – flows and quantities of accumulations.
2.2.</p>
    </sec>
    <sec id="sec-4">
      <title>Variable patterns in epidemic dynamics</title>
      <p>•
•
unit time;
Epidemics are the transmission of viruses from ill people to those who are healthy and susceptible to
the disease. Statistics keep track of new cases – the number of people infected per day. An epidemic
process is characterized by an increase in the total number of infected people, counted cumulatively at
a specific date. Growth is limited by the number of people susceptible to the disease. The epidemic
dynamics model derives from a dynamic system model [16], which uses a linear dynamic system [19]
with inverse relationship. The main variables of the model:
 ( ) - an independent variable denoting the rate, flow of infected, those number of infected per
 ( ) - the dependent variable of the level of accumulation of infected (system state), denoting
the total number of infected over some time.</p>
      <p>A phenomenological inverse relationship coefficient complements the dynamic system model  .
Next model is an isolated design, usually used for linear systems

= 〈 ,  ,  〉, 
= ∫ 
,  =  ′.</p>
      <p>To use this model for open systems, it is necessary to: increase the number of inverse relationships and
relate them to the environment parameters. To extend the modelling capabilities of open systems, we
use a deployed scheme in the form of multi-circuit inverse relationship. Such a detailed dynamic model
of an open system provides a process description in abstract form and allows the construction of
non</p>
    </sec>
    <sec id="sec-5">
      <title>2.2.2. The flow of carriers of infection</title>
      <p>
        The carrier flow (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ) is also divided into two parts. One part relates to active spreaders and the other to
inactive spreaders, those who have died. This approach makes it possible to distinguish between fatal
cases and to consider the actual spreaders of infection. The flow of carriers is then equal to the difference
of the flow of infected minus the flow of deceased
      </p>
      <p>∓ =  + −  −,
linear differential equations.</p>
    </sec>
    <sec id="sec-6">
      <title>2.2.1. Deployment of a dynamic model</title>
      <p>
        (
        <xref ref-type="bibr" rid="ref1">1</xref>
        )
(
        <xref ref-type="bibr" rid="ref2">2</xref>
        )
(
        <xref ref-type="bibr" rid="ref3">3</xref>
        )
(
        <xref ref-type="bibr" rid="ref4">4</xref>
        )
The principle of dynamic model deployment is to decompose: the total flow of infected  into partial
variables and, similarly, the total phenomenological coefficient
      </p>
      <p>
        The complete flow of the infected as distributors of infection consists of elements. Following the
decomposition principle (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ), we distinguish two groups of elements based on facilitating the distribution
of infection. Then the total flow of the infected equals the difference of the incumbent carriers minus
the flow of loss of carriers
 = ∑   ,
      </p>
      <p>= ∑   .</p>
      <p>=  ∓ −  ̃,
where  ∓ - streams of carriers who facilitate the distribution of the infection;  ̃ - loss streams of carriers
who counteract the distribution of the infection.
where  + - is the flow of active carriers, reflecting new cases of infected persons in the process of
spreading infection (inflow of infected persons);  − - the flow of lethal cases (outflow of infected
persons).</p>
      <p>The flow of fatal cases is represented as a function of current infectious carriers  − =  ( +).</p>
    </sec>
    <sec id="sec-7">
      <title>2.2.3. Flow patterns</title>
      <p>
        Flow models (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ) describe the dependencies of the rate of infection on the number of people infected.
      </p>
      <p>
        These dependencies reflect the main patterns of epidemic processes. We describe the relationship
between flows and the environment using phenomenological coefficients. The relationship with the
environment can be linear and non-linear. For linear relationships, the flow (
        <xref ref-type="bibr" rid="ref5">5</xref>
        ) is proportional to the
number of infected with the inverse relationship coefficient
      </p>
      <p>For non-linear relationships, the inverse coefficient is a function of the derivatives of the</p>
    </sec>
    <sec id="sec-8">
      <title>2.2.5. Carrier loss flows</title>
      <p>Limit it to three types of loss and write an expression for the total flow
where  ̃ loss flows of certain types of carriers.</p>
      <p>
        The pattern of processes here is that loss flows are proportional to the number of spreaders, but this
relationship is not linear (
        <xref ref-type="bibr" rid="ref7">7</xref>
        ), and the coefficients of proportionality depend on the number of spreaders
  =   ( ),

 =    .
      </p>
      <p>=   ( ) .
 +( ) =  +</p>
      <p>( ),
 −( ) =  − ( ),
 ∓ = ( + −  −) ( ).</p>
      <p>̃ =  ̃0 +  ̃1 +  ̃2.</p>
      <p>
        ̃ ( ) =  ̃ ( ) ( ).
accumulation level variables
2.2.4. Patterns of carrier flows
(
        <xref ref-type="bibr" rid="ref5">5</xref>
        )
(
        <xref ref-type="bibr" rid="ref6">6</xref>
        )
(
        <xref ref-type="bibr" rid="ref7">7</xref>
        )
(
        <xref ref-type="bibr" rid="ref8">8</xref>
        )
(
        <xref ref-type="bibr" rid="ref10">9</xref>
        )
(
        <xref ref-type="bibr" rid="ref11 ref9">10</xref>
        )
The pattern of processes here is that the flows of carriers (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ) are proportional to the number of spreaders
of infection. Carrier flow patterns reflect a monotonic increase in the number of infected. We restrict
the group of linear (
        <xref ref-type="bibr" rid="ref6">6</xref>
        ) relationships to two types of inverse relationships, positive and negative  ∓ =
=  + −  −
1.
      </p>
      <p>The growth of an epidemic is mainly determined by the inflow of infected persons, which is
proportional to the number of people spreading the infection
where  + is the positive inverse coefficient, a measure of the growth in the number of infected.</p>
      <p>
        It follows from equation (
        <xref ref-type="bibr" rid="ref8">8</xref>
        ) that the number of people infected, and consequently the infectious
flow, grows exponentially without limit  ( ) =   + . This growth can be ensured if there is an
unlimited number of susceptible individuals regarded as the source of the infection. However, in
practice, the number of susceptible persons is limited, which poses the problem of a limited growth
      </p>
      <p>The flow of deaths, which reduces the growth of the epidemic, is proportional to the number of
model.</p>
      <p>2.
people infected
dead
where  − is the growth rate of fatal cases.</p>
      <p>
        The growth rates in (
        <xref ref-type="bibr" rid="ref8">8</xref>
        ) and (
        <xref ref-type="bibr" rid="ref10">9</xref>
        ) are constant coefficients, so these carrier flow models are linear
relationships. The flow of carriers (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ) is then equal to the difference between the flow of infected and
      </p>
      <p>
        The principle behind this non-linear relationship is that loss rates are proportional to the derivatives
of the number of infectious spreaders (
        <xref ref-type="bibr" rid="ref7">7</xref>
        ), so growth rates are functions that depend on the
phenomenological coefficients
      </p>
      <p>
        ̃ ( ) =   (  )( ). (
        <xref ref-type="bibr" rid="ref13">12</xref>
        )
Then the total loss flow equation (
        <xref ref-type="bibr" rid="ref11 ref9">10</xref>
        ) with (
        <xref ref-type="bibr" rid="ref12">11</xref>
        ) and (
        <xref ref-type="bibr" rid="ref13">12</xref>
        ) will appear as
      </p>
      <p>
        ̃( ) =  0 2( )+  1 ( ) ′ +  2 ( ) ′′. (
        <xref ref-type="bibr" rid="ref14">13</xref>
        )
      </p>
      <p>
        Consider the features of the loss components in the total loss flow equation (
        <xref ref-type="bibr" rid="ref14">13</xref>
        ) that describe the
dispersal of infectious agents in the environment.
      </p>
    </sec>
    <sec id="sec-9">
      <title>2.2.6. Zero-order loss flow models</title>
      <p>
        expression for the flow (
        <xref ref-type="bibr" rid="ref15">14</xref>
        ) in the form of
      </p>
      <p>
        ̃0( ) = {
Zero-order loss stream is a function proportional to the number (zero-order derivative) of infectious
spreaders, where the coefficient of proportionality depends on the number of spreaders  ̃0( ) =
=  0 (0)( )(
        <xref ref-type="bibr" rid="ref13">12</xref>
        ). The flow expression is then a non-linear relationship of the form
 ̃0( ) =  0 2( ). (
        <xref ref-type="bibr" rid="ref15">14</xref>
        )
      </p>
      <p>
        Zero-order flow models (
        <xref ref-type="bibr" rid="ref15">14</xref>
        ) solve the problem of limited epidemic growth, which results from the
limited source of the infected population and consists of the fact that the growth of the infected
population is limited to the number of persons  ̂ susceptible to the epidemic. This value can be regarded
as the source of infection in the environment. The introduction of a source limits the number of infected
to  ≤  ̂. When the limit is reached  =  ̂, the flow value falls by leaps and bounds to zero. Then the
expression for the flow of loss takes the form of a discontinuous function
 ̃0 ( ),  ( ) ≤  ̂; (
        <xref ref-type="bibr" rid="ref16">15</xref>
        )
0,  ( ) ≥  ̂.
      </p>
      <p>
        A gap in the expression for the loss flow is considered a catastrophe, leading to uncertainty in the
spread of infection. Given that flow gaps are not observed in practice, it is necessary to introduce a
source of infection into the model (
        <xref ref-type="bibr" rid="ref15">14</xref>
        ) to exclude a catastrophe (
        <xref ref-type="bibr" rid="ref16">15</xref>
        ). To do this, consider the infected
source capacity  ̅0 =  ̂ and the source action time  . Considering that  ̅0 = 1 we rewrite the
 0
 ̂
      </p>
      <p>
        The expression for the loss flow (
        <xref ref-type="bibr" rid="ref17">16</xref>
        ) considers the source of the infected, is a continuous function
of the number of infected and can be used to describe the limited growth of an epidemic.
 ̃0( ) =
 2( )
.
      </p>
      <p>
        (
        <xref ref-type="bibr" rid="ref17">16</xref>
        )
      </p>
    </sec>
    <sec id="sec-10">
      <title>2.2.7. First-order loss flow models</title>
      <p>
        According to (
        <xref ref-type="bibr" rid="ref13">12</xref>
        ), the growth rate is a function proportional to the first-order derivative of the number
of distributors  ̃1( ) =  1 (
        <xref ref-type="bibr" rid="ref1">1</xref>
        )( ). It follows that the flow expression is a non-linear relationship of the
form
      </p>
      <p>
        ̃1( ) =  1 ( ) (
        <xref ref-type="bibr" rid="ref1">1</xref>
        )( ). (
        <xref ref-type="bibr" rid="ref18">17</xref>
        )
      </p>
      <p>The proportionality factor  1 reflects the resistive properties of the environment, which inhibit the
spread of the flow of the infected.</p>
    </sec>
    <sec id="sec-11">
      <title>2.2.8. Second-order loss flow models</title>
      <p>
        The second-order loss rate is a function proportional to the second-order derivative of the number of
distributors  ̃2( ) =  2 (
        <xref ref-type="bibr" rid="ref2">2</xref>
        )( ), then the flow expression is a non-linear relationship of the form
 ̃2( ) =  2 ( ) (
        <xref ref-type="bibr" rid="ref2">2</xref>
        )( ). (18)
      </p>
      <p>The proportional coefficient  2 can be considered as the elasticity of the environment and reflects
the ability to generate oscillations during flow distribution.</p>
    </sec>
    <sec id="sec-12">
      <title>2.2.9. Differential equations of epidemic dynamics</title>
      <p>
        Given the expressions for the elements (
        <xref ref-type="bibr" rid="ref8">8</xref>
        ), (
        <xref ref-type="bibr" rid="ref10">9</xref>
        ) and (
        <xref ref-type="bibr" rid="ref17">16</xref>
        )-(18), we write the differential equation for the
total flow of infectious agents
 = (( + −  −)− ( 0 (0) +  1 (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) +  2 (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ))) .
 2  ′′ + (1 +  1 ) ′ +  2 = ( + −  −) . (20)
      </p>
      <p>̂</p>
      <p>Model (20) describes epidemic dynamics as a nonlinear, non-stationary differential equation. This
model reflects epidemic dynamics as a process system reproduces stably due to interaction with the
environment. Equation (20) has no analytical solutions, and numerical methods are used to solve it.
Solutions to equation (20) give the epidemic episode functions:
• The total infectiousness flow functions have a bell-shaped form;
• The functions of the number of infected (infection rate) are S-shaped.</p>
      <p>The epidemic dynamics functions have two equilibrium states:
• Initial equilibrium – unstable  (0) = 0,  (0)at  = 0;
• Final equilibrium – stable,  ( ) → 0,  ( ) →  ̅ at  → ∞.</p>
      <p>The epidemic dynamics functions vary over a range bounded by the equilibrium states, and then the
epidemic processes in the range are non-equilibrium and irreversible.</p>
      <p>Equilibrium of the system means that the growth of infected individuals stops, and the derivatives
tend towards zero. We obtain the equilibrium equation from the equation of epidemic dynamics (20)
with zero derivatives  ′′( ) = 0,  ′( ) = 0 and  ( ) ≠ 0
 ̅ (21)
 ̂</p>
      <p>The stable equilibrium equation is a parametric equation that relates the parameters of the
COVID19 distribution functions. The epidemic threshold is described by the expression</p>
      <p>̅ = ( + −  −) ̂ . (22)</p>
      <p>In many practical cases, it is possible to restrict oneself to first-order epidemic dynamics models,
which are derived from (20) at  ′′( ) = 0</p>
      <p>(1 +  1 ) ′ +  ̂2 = ( + −  −) . (23)</p>
      <p>In particular cases, equation (23) admits analytical solutions, but numerical finite-difference
methods are generally used to solve it. The solution of finite difference equations constructed by (23)
leads to discrete COVID-19 distribution functions.</p>
      <p>=  + −  −.</p>
    </sec>
    <sec id="sec-13">
      <title>2.2.10. Discrete distribution functions</title>
      <p>In the discrete COVID-19 distribution functions, the relations of the variables are described by the
discrete   +1 =   +   +1,   +1 =  +  , where  + = ( + −  −)×
 
× 1− ̅ is the equivalent variable for the growth rate of infected persons. Expressions for the discrete
1+ 1 
function of the infector flow and the number of people infected
  +1 = ( + −  −)11+−1 ̅    ;   +1 = (1 + ( + −  −)11+−1 ̅  )   ; (24)
 ̅ = ( + −  −) ̂ .</p>
      <p>The discrete COVID-19 distribution functions fit the statistics well, so they are used to model the
epidemic. Similarly to (24), the discrete flow and number of deaths functions are
  +1 = ( + −  −)11+−1 ̅    ;   +1 = (1 + ( + −  −)11+−1 ̅  )   ; (25)
 ̅ = ( + −  −) ̂ .</p>
    </sec>
    <sec id="sec-14">
      <title>Approximation of Statistical Data Covid-19 Distribution</title>
      <p>Discrete COVID-19 distribution functions are used to analyse and predict epidemics. These functions
are obtained by approximating statistical data. Two problems can be solved by approximating the
statistics:
• The total flow of infected people;
• The function of the number of infected.</p>
      <p>Ukraine [16] is chosen as an example to show how the calculated values of COVID-19 distribution
functions correspond to statistical data [16].
3.1.</p>
    </sec>
    <sec id="sec-15">
      <title>Approximations of Data on the Number of Infected</title>
    </sec>
    <sec id="sec-16">
      <title>Approximations of the Full Flow of Infected</title>
      <p>Approximation of the total flow of infected persons was performed using the example of the second
wave of COVID-19 spread in the time interval from 1.04 to 10.09 2020 according to the statistical data
given in [17, 18]. The approximating functions have the character of episodes (27), those of completed
processes, and the total flow is the sum of episodes. Figure 3 shows the results of the decomposition of
the complex flow into 4 episodes, those into 4 elementary f flows.</p>
    </sec>
    <sec id="sec-17">
      <title>Conclusions</title>
      <p>Research on the history of epidemic modelling shows that the main reason for the shortcomings of
mathematical modelling of epidemics (SIR, System Dynamics, “EPIDDINAMICS”) can be considered
as the application of the classical methodology characteristic of simple isolated systems. Therefore,
there is a problem associated with the transition of the modelling methodology from classical to
nonclassical positions, within which the epidemic should be considered an open self-replicating dynamic
system. This shift is associated with a new scientific approach to the study of disease transmission
processes, where epidemics are viewed as system dynamics from a non-classical methodology. This
scientific direction is called epidemic dynamics, the core of which is a reproducible procedural system.
A model of epidemic dynamics in a non-classical methodology would be open and reflect an exchange
of energy and matter with the external environment to enable reproduction in a nonequilibrium
functioning mode. The methods and tools of the theory of non-linear nonequilibrium dynamical systems
are used to describe the model of epidemic dynamics.</p>
      <p>The epidemic dynamics models are based on a dynamic system model with an extended feedback
network. This non-classical approach allows epidemic dynamics models are represented as non-linear
and non-stationary differential equations. Solutions to the equations - COVID-19 distribution functions
– are used for mathematical modelling and investigation of epidemic processes. Importantly, these
functions describe elementary complete epidemic processes - "epidemic episodes". The modelling
process begins by approximating epidemic statistics with discrete functions describing two "epidemic
episodes" types: flows and accumulations. Next, superpositions of unrelated epidemic episodes shifted
in time and described complex processes.</p>
      <p>This approach is consistent with agent-based modelling methodology, which has greater descriptive
power than classical models but requires a more detailed description of epidemic categories. The
application of COVID-19 distribution functions shows high accuracy in approximating statistical data,
demonstrating the excellent adequacy of these functions in principle. Applying COVID-19 distribution
functions enables quantitative description and analysis of epidemic processes and reliable forecasting.
Overall, applying COVID-19 distribution functions can help reduce the harm caused by a pandemic.
[18] Distribution COVID-19 in Ukraine (2021). URL: https://ru.wikipedia.org/wiki/.
[19] A. Comunian, R. Gaburro, and M. Giudici. Inversion of a SIR-based model: A critical analysis
about the application to COVID-19 epidemic. Physica D: Nonlinear Phenomena 413 (2020) 132674.
doi: 10.1016/j.physd.2020.132674.</p>
    </sec>
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