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<article xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta />
    <article-meta>
      <title-group>
        <article-title>Weak Chaos and Controllability Conditions in Discrete Systems</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <string-name>Sergey Dashkovskiy</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Oleksandr Boichuk</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Oleksandr Pokutnyi</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <contrib contrib-type="author">
          <string-name>Olena Polishchuk</string-name>
          <xref ref-type="aff" rid="aff0">0</xref>
        </contrib>
        <aff id="aff0">
          <label>0</label>
          <institution>University of Wu ̈ rzburg, Institute of mathematics</institution>
          ,
          <addr-line>40 Emil Fischer str., Wu ̈ rzburg, 97074</addr-line>
          ,
          <institution>Germany Institute of Mathematics of the National Academy of Sciences</institution>
          ,
          <addr-line>3 Tereschenkivska Street, Kyiv-4, 01024</addr-line>
          ,
          <institution>Ukraine Taras Shevchenko University</institution>
          ,
          <addr-line>4d Glushkova Street, Kyiv, 03022</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
      </contrib-group>
      <fpage>96</fpage>
      <lpage>101</lpage>
      <abstract>
        <p>Report is devoted to obtaining the conditions of the input-to-state stability for the discrete linear systems in the Banach and Hilbert spaces. For the nonlinear boundary-value problem we found a necessary condition for the existence of bounded solutions. Such condition was obtained with using of the system of operator equations for generating elements. Moreover, conditions of the controllability and reachability were obtained with using of the operator matrix equation. Estimates on the norms of solutions were obtained under assumption that the corresponding linear interconnected system admits a discrete dichotomy. For the boundary-value problem conditions of solvability were obtained and examples of boundary conditions were represented. Controllability conditions were obtained in the case when the corresponding set of controls are constant. We consider the so-called resonance ill-posed problem when the uniqueness can be disturbed, and corresponding linear interconnected system can have solutions not for any righthand sides.</p>
      </abstract>
      <kwd-group>
        <kwd>1 Moore-Penrose pseudoinverse operator</kwd>
        <kwd>weakly nonlinear equation</kwd>
        <kwd>boundary-value problem</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>1. Introduction</title>
      <p>Weakly nonlinear boundary-value problems for the discrete equations plays an important role in
the qualitative theory of dynamical systems. We consider conditions of the solvability for such
interconnected systems with linear boundary conditions. Interconnected systems use as a model for
investigations in applied sciences (see [1]). Moreover, the notion of input-to-state stability with
corresponding estimates for such system is a very popular direction in the last years (see [2]). That’s
why we obtain input-to-state stability estimates and corresponding controllability conditions. It should
be noted that this work is additional. We formulate general statement of the problem in nonlinear case
but represent and prove the main results only in linear case. In the future works we use these results for
investigating of nonlinear case and try to formulate chaotic conditions (in the weaklier sense than in
[4]- [10]). It should be noted the papers [11], [12].
1.1.</p>
    </sec>
    <sec id="sec-2">
      <title>Statement of the problem</title>
      <p>Consider the following interconnected system of nonlinear equations</p>
      <p>
        ( + 1,  )=   ( )  ( ,  )+   ( )  ( )+ ℎ ( )+
+    ( 1( ,  ), … ,   −1( ,  ),   +1( ,  ), … ,   ( ,  )), 
,  = ̅1̅̅,̅̅
with boundary conditions
(
        <xref ref-type="bibr" rid="ref1">1</xref>
        )
(A.3),
    (∙,  )=   ,
where   ( ),   ( )∶  →  - are a set of bounded operators, from the Banach space B into itself.
      </p>
      <p>Assume that</p>
      <sec id="sec-2-1">
        <title>It means that:</title>
        <p>|||  ||| =   ∈ ||  ( )|| &lt; + ∞, |||ℎ ||| =   ∈ ||ℎ ( )|| &lt; +∞,</p>
        <p>
          :  ∞( ,  )→ 
are the linear and bounded operators which translates bounded solutions of (
          <xref ref-type="bibr" rid="ref1">1</xref>
          ) into the Banach space
BS, αi are the elements of Banach space BS. We find conditions of the existence of bounded solutions
(
          <xref ref-type="bibr" rid="ref1">1</xref>
          ), (
          <xref ref-type="bibr" rid="ref2">2</xref>
          ) which turn (ε = 0) in one of the bounded solutions of generating boundary-value problem
 0( + 1)=   ( ) 0( )+   ( )  ( )+ ℎ ( ), ∈  ,  = ̅1̅̅,̅̅ (
          <xref ref-type="bibr" rid="ref3">3</xref>
          )
        </p>
        <p>
          0(∙)=   . (
          <xref ref-type="bibr" rid="ref4">4</xref>
          )
        </p>
        <p>
          First, we formulate the conditions for the existence of bounded solutions of the equation (
          <xref ref-type="bibr" rid="ref3">3</xref>
          ) and
boundary value problem (
          <xref ref-type="bibr" rid="ref3">3</xref>
          ), (
          <xref ref-type="bibr" rid="ref4">4</xref>
          ). The corresponding homogeneous system of difference equations has
the following form:
        </p>
        <p>
          ( + 1)=   ( )  ( ). (
          <xref ref-type="bibr" rid="ref5">5</xref>
          )
It should be noted that an arbitrary solution of a homogeneous system can be represented as:   ( )=
Φ ( ,  )  ( ),  ≥  , where:
        </p>
        <p>( − 1)  ( − 2)…   ( ),   &gt; 
Φ ( ,  )= { ,   = 
.</p>
      </sec>
      <sec id="sec-2-2">
        <title>It is clear, that</title>
      </sec>
      <sec id="sec-2-3">
        <title>Also, we denote</title>
        <p>Φ ( , 0 )=   ( − 1)  ( − 2)…   (0).</p>
        <p>( ):= Φ ( , 0)and   (0)=  .</p>
        <p>
          Traditionally [12], the mappings Φ ( ,  )are called the evolutionary operators of the problem
(
          <xref ref-type="bibr" rid="ref5">5</xref>
          ). Suppose that the system (
          <xref ref-type="bibr" rid="ref5">5</xref>
          ) is exponentially dichotomous [4, 12] on the semiaxes  + and  − with
projectors   and   in the space B respectively, which means that there are projectors
{
{
  ( 2 =   )and   ( 2 =   ),
 1,2 ≥ 1, 0 &lt;  1(,2) &lt; 1
        </p>
        <p>−
||  ( )   −1( )|| ≤  1 ( 1( ))</p>
        <p>,  ≥ 
||  ( )( −   ) −1( )|| ≤  1 ( 1( )) − ,  ≥  ,</p>
        <p>−
||  ( )   −1( )|| ≤  2 ( 2( ))</p>
        <p>,  ≥ 
 −
||  ( )( −   ) −1( )|| ≤  2 ( 2( ))
,  ≥  ,
constants
such that
for arbitrary  ,  ∈  + (dichotomy on  +).
for arbitrary  ,  ∈  − (dichotomy on  −).</p>
      </sec>
    </sec>
    <sec id="sec-3">
      <title>2. Main results. Linear case. Banach space case</title>
      <p>
        In this part we obtain the necessary and sufficient conditions of the existence of the sets of bounded
solutions for the linear generating boundary-value problems (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ), (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ) and controllability conditions.
      </p>
    </sec>
    <sec id="sec-4">
      <title>2.1. Bounded solutions. Linear case</title>
      <p>We formulate an auxiliary lemma which we will use when obtaining the main results (first lemma
directly follows from the well-known results of [4], [12]).
projectors   and   respectively, and the operators</p>
      <p>
        Lemma 1. Suppose that a homogeneous system is dichotomous on the semi-axes  + and  − with
  =   − ( −   ): 
→ 
are generalized invertible [5]. The solutions of the equation (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) bounded on the entire axis  exist if
and only if the following conditions are satisfied:
If the conditions (
        <xref ref-type="bibr" rid="ref6">6</xref>
        ) hold, the set of bounded solutions has the following view:
      </p>
      <p>∑+=∞−∞   ( + 1)(ℎ ( )+   ( )  ( ))= 0.
 0

( ,   )=   ( )    (  )  + (  [ℎ +     ])( ),   ∈</p>
      <p>
        where   are generalized inverse Green’s operators [12, 13] on  with the following properties:
(    [ℎ +     ])( )=   ( )  ( )+ ℎ ( ),  ∈  ,
(
        <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="ref9">9</xref>
        )
(
        <xref ref-type="bibr" rid="ref10">10</xref>
        )
where
(    )( )≔   ( + 1)−   ( )  ( ):  ∞( ,  )→  ∞( ,  ),
  ( + 1)=
      </p>
      <p>−1( + 1),
 −are generalized inverse to the operators   ,
projectors   (  )=  −  −  and     =  −    − (see [3], [13]),</p>
      <p>Remark 2. It should also be noted that if bounded solutions are united together at zero as follows:
  (0 + )=   (0 − )+   ,
which project space B on the kernels  (  )of the operators   and the subspaces    ≔  ⊝  (  )
respectively ( =    ⨁ (  )).</p>
      <p>Remark 1. We have the following estimates for the norm of the solutions:
|| 0( ,   )|| ≤  1( 1) ||  (  )  || +  1( 1) || −|| ( 1 
1−  11 + 1 −2   22)(|||ℎ ||| + |||  ||| |||  |||)+
 1 (1+  1−( 1) )
1−  1</p>
      <p>(|||ℎ ||| + |||  ||| |||  |||),  ≥ 0,
|||  ||| |||  |||)+  2 (1+  2−( 2)− +1)</p>
      <p>1−  2
From these inequalities follows the estimates
|| 0( ,   )|| ≤  2( 2)− ||  (  )  || +  2( 2)− || −|| ( 1 
1− 11 + 1 −2   22)(|||ℎ ||| +
(|||ℎ ||| + |||  ||| |||  |||),  ≤ 0.
||| 0||| ≤   ||  (  )  || +   || −|| ( 1</p>
      <p>1−  11 + 1 −2 22)(|||ℎ ||| + |||  ||| |||  |||)+
+   11+− Λ21 (|||ℎ ||| + |||  ||| |||  |||),
where   = 
{ 1,  2},  1 = 
{ 1,  2},  2 = 
{ 1,  2}.
where   are the elements of Banach space, then we obtain a bounded solutions for the problem with a
jump.</p>
      <p>
        Let us find the solvability condition of the generating boundary-value problem (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ), (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ). Suppose that
condition (
        <xref ref-type="bibr" rid="ref6">6</xref>
        ) is satisfied. Substitute expression (
        <xref ref-type="bibr" rid="ref7">7</xref>
        ) in the boundary condition (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ). Then we obtain the
operator equations which can be represented in the following form:
where   =     (∙)   ( (  )):  →  . If the operators   are generalized invertible [6], then equation
(
        <xref ref-type="bibr" rid="ref11">11</xref>
        ) is solvable [6] if and only if the following conditions are satisfied:
      </p>
      <p>=   −   (  [ℎ +     ])(∙),</p>
      <p>
        (  −   (  [ℎ +     ])(∙))= 0,
where 
  =  −     − (

(
        <xref ref-type="bibr" rid="ref11">11</xref>
        ) have the following forms
      </p>
      <sec id="sec-4-1">
        <title>Thus, we obtain the following theorem.</title>
        <p>
          =  (  )⨁   ). Under conditions (
          <xref ref-type="bibr" rid="ref12">12</xref>
          ) the sets of solutions of the system
  =   −(  −   (  [ℎ +     ])(∙))+   (  ) 
 ̅,
 ̅ .
        </p>
        <p>
          Theorem 1. Under condition (
          <xref ref-type="bibr" rid="ref6">6</xref>
          ) boundary-value problem (
          <xref ref-type="bibr" rid="ref3">3</xref>
          ), (
          <xref ref-type="bibr" rid="ref4">4</xref>
          ) has bounded solutions if and
only if the conditions (
          <xref ref-type="bibr" rid="ref12">12</xref>
          ) are satisfied. The sets of bounded solutions have the following form:
  ( ,  ̅)=   ( )    (  )  (  ) ̅+ ( ̅[ℎ +     ,   ])( ),
where ( ̅[ℎ +     ,   ])( )are generalized Green’s operators in the form
        </p>
        <p>( ̅[ℎ +     ,   ])( )= (  [ℎ +     ])( )+
+   ( )    (  )</p>
        <p>−(  −   (  [ℎ +     ])(∙)).</p>
        <p>
          Remark 3. It should be noted that the operators   in (
          <xref ref-type="bibr" rid="ref2">2</xref>
          ) can be for example represent two-point
or multi-point boundary-value problems:
        </p>
      </sec>
    </sec>
    <sec id="sec-5">
      <title>2.2. Bounded solutions. Nonlinear case</title>
      <p>
        Using theorem 1 we can obtain necessary condition of the existence of the sets of bounded solutions
for the nonlinear boundary-value problem (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ), (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ). Suppose that generating boundary-value problem
(
        <xref ref-type="bibr" rid="ref3">3</xref>
        ), (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ) is solvable. It means that the conditions (
        <xref ref-type="bibr" rid="ref6">6</xref>
        ), (
        <xref ref-type="bibr" rid="ref12">12</xref>
        ) are satisfied. In this case we can easily obtain
the following theorem.
      </p>
      <p>
        Theorem 2. (Necessary condition). Suppose that conditions (
        <xref ref-type="bibr" rid="ref6">6</xref>
        ), (
        <xref ref-type="bibr" rid="ref12">12</xref>
        ) (the sets of solutions (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ), (
        <xref ref-type="bibr" rid="ref4">4</xref>
        )
has the form (
        <xref ref-type="bibr" rid="ref13">13</xref>
        )) are satisfied and nonlinear problem (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ), (
        <xref ref-type="bibr" rid="ref2">2</xref>
        ) has bounded solutions. Then  ̅ from the
Banach space B (see (
        <xref ref-type="bibr" rid="ref13">13</xref>
        )) satisfy the following operator system for the generating elements:
(
        <xref ref-type="bibr" rid="ref11">11</xref>
        )
(
        <xref ref-type="bibr" rid="ref12">12</xref>
        )
(
        <xref ref-type="bibr" rid="ref13">13</xref>
        )
(14)
(15)
where  ,   ∈  ,   ( )∈  ( , 
conditions at the infinity:
    (∙)=  1 
 →−∞   ( )+  2 

→+∞   ( ).
      </p>
      <p>
        Moreover, boundary-value problems (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ), (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ) in the represented form are the systems of independent
boundary-value problems. We can consider more general linear boundary conditions (instead of (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ))
),  = ̅1̅̅,̅̅ are linear and bounded operators. Another example is
in the forms:
the condition (15).
      </p>
      <p>∑</p>
      <p>=1    0(∙)=  ,    .</p>
      <p>In such way we obtain boundary-value problem with components of system  0 which can connect by
+∞</p>
    </sec>
    <sec id="sec-6">
      <title>2.3. Controllability conditions</title>
      <p>= ∑+=∞−∞   ( + 1)  ( ),   = − ∑+=∞−∞   ( + 1)ℎ ( ),</p>
      <p>=     1  (  [  ])(∙),   =     1(  −   (  [ℎ ])(∙)).</p>
      <p>We can rewrite the systems of operator equations (16), (17) in the form of matrix operator equation
 =  ,  0:   → ( ×  1) ,  ∈   ,  ∈ ( ×  1) ,
where
 0 =
(
[ 11]
0
0</p>
      <p>0
[ 22]</p>
      <p>…
0
,
 = ( …2),
If the operator  0 is generalized invertible [6], then we can obtain the following theorem.
Theorem 2. (Reachability conditions). Under condition</p>
      <p>
        ( 0∗) = 0,
the linear generating boundary-value problem (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ), (
        <xref ref-type="bibr" rid="ref4">4</xref>
        ) is controllable. The sets of controls can be
represented in the following form:
 =  0− +   ( 0) , for any  = ( 11,  12,  21,  22, … ,  1,  2)∈ ( ×  1) .
      </p>
      <p>
        Remark 4. Substituting solutions (20) in (
        <xref ref-type="bibr" rid="ref13">13</xref>
        ) we obtain the set of bounded solutions with
corresponding set of controls u.
      </p>
      <p>
        Theorem 3. (Input-to-state stability conditions (see [1]-[3]). It is easy to show that under conditions
of the existence of bounded solutions from the inequalities (
        <xref ref-type="bibr" rid="ref8">8</xref>
        ), (
        <xref ref-type="bibr" rid="ref9">9</xref>
        ) we have the following estimates for
any bounded solution of (
        <xref ref-type="bibr" rid="ref3">3</xref>
        ), (
        <xref ref-type="bibr" rid="ref4">4</xref>
        )
|| 0( ,  ̅)|| ≤   ( 1) (||  (  )  (  ) ̅|| + ||  ||)+   (|||ℎ |||)+   (|||  ||||||  |||),  ≥ 0,
|| 0( ,  ̅)|| ≤   ( 2)− (||  (  )  (  ) ̅|| + ||  ||)+   (|||ℎ |||)+   (|||  ||||||  |||),  ≤ 0,
with corresponding constants   and functions   .
      </p>
      <p>Remark 5. Presented theorem gives us conditions of the input-to-state stability and chaoticity (see
also [1],[11]).
[ 1
 1]
 = [ 22] .</p>
      <p>…
 
([  ])
(17)
(18)
(19)
(20)</p>
      <p>
        Remark 6. It should be noted that in more general case the linear and bounded operators   can
translate bounded solutions of (
        <xref ref-type="bibr" rid="ref1">1</xref>
        ) into different spaces (instead of BS we can use   , where   are
Banash spaces and   ≠   ).
      </p>
    </sec>
    <sec id="sec-7">
      <title>3. Acknowledgements</title>
      <p>The authors would like to thank the conference organizers for the opportunity to make report at the
conference DSMSI 2023.</p>
    </sec>
    <sec id="sec-8">
      <title>4. References</title>
    </sec>
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