<!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>Equation of the Related Riemann-Hilbert-Privalov Problem with Zeros and Poles of the Coefficient in the Half-plane*</article-title>
      </title-group>
      <contrib-group>
        <aff id="aff0">
          <label>0</label>
          <institution>Odessa National Maritime University</institution>
          ,
          <addr-line>Odessa</addr-line>
          ,
          <country country="UA">Ukraine</country>
        </aff>
        <aff id="aff1">
          <label>1</label>
          <institution>Relevance</institution>
          ,
          <addr-line>Problem Statement</addr-line>
        </aff>
      </contrib-group>
      <pub-date>
        <year>1989</year>
      </pub-date>
      <fpage>0000</fpage>
      <lpage>0002</lpage>
      <abstract>
        <p>Various mathematics and mechanics questions are connected with the Riemann (Riemann-Hilbert-Privalov) problem from the theory of analytic functions. This justifies the relevance of the equation associated with the specified Riemann problem. Until now, the specificity of the location of the singular points of the rational coefficient of the equation has not been considered. The paper aims to obtain general formulas for solving abstract equations in the corresponding ring of rational functions, considering this specificity. The authors propose a way to solve an equation and a related problem. For the first time, the sought general formulas were established and proved to be simpler than those obtained earlier. The research indicates the signs when the use of these formulas is justified. The authors apply the general provisions of (1) the theory of rings and functional analysis, (2) the theory of linear operators, (3) equations in rings with factorization pairs, (4) the problem of factorization by subrings, and (5) the properties of the used ring of rational functions. The authors' approach is free from the theory of integrals (Cauchy and Fourier types), the requirements of the Hölder condition, and the index. In a similar situation, it applies to (1) integral equations of the Wiener-Hopf type and other equations of the convolution type, as well as to related functional equations; (2) to matrix equations that can be used in mechanics with projectors onto the corresponding subrings and unknown triangular matrices.</p>
      </abstract>
      <kwd-group>
        <kwd>2 Odessa State Academy of Buildings and Architecture</kwd>
        <kwd>Odessa</kwd>
        <kwd>Ukraine</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec-1">
      <title>-</title>
      <p>1.1</p>
    </sec>
    <sec id="sec-2">
      <title>Introduction</title>
      <p>
        The equations and problems considered in the paper are related to the corresponding
famous Riemann problem (Riemann-Hilbert, Riemann-Hilbert-Privalov) from the
theory of analytic functions, but for a narrower class of functions. This problem is
important in the theory of differential and integro-differential equations, integral
equations of convolution type, the corresponding differential equations of
mathematical physics, in the theory of elasticity, torsion problems, and others
        <xref ref-type="bibr" rid="ref1 ref10 ref13 ref2 ref3 ref4 ref5 ref7 ref8">(Akopyan &amp; Dashtoyan, 2013; Cherskij, P. Kerekesha &amp; D. Kerekesha, 2010;
Gahov, 1963; Gahov &amp; Cherskij, 1978; Krejn, 1958; Mhitaryan, 1968;
Mushelishvili, 1968; Popov, Kerekesha &amp; Kruglov, 1976; Voytik, Poletaev &amp;
Yatsenko, 2017)</xref>
        . Therefore, the authors develop (1) general provisions on the
solvability of equations associated with it or related problems; (2) ideas about the
possible results of the theory; (3) a way of considering the specifics. The research
analyzes the solvability, criteria, and formulas for solutions of an equation in the
corresponding ring of rational functions:
 ( ) +( ) +  −( ) =  ( );    ∈ ℂ ∪ {∞}.
(1)
      </p>
      <p>This equation for  =  ∈ {−∞, ∞} expresses the boundary conditions of the
following, called related, problem:</p>
      <p>For given rational coefficient functions  ( ),    ( ),   −∞ &lt;  &lt; ∞ find a pair
of rational functions  +( ) ∈ ℜ+,  −( ) ∈ ℜ − ,    ∈ ℂ. All poles of the first
one (if they exist) are located only inside the lower one; the second one is located
only inside the upper one of the half-plane bounded by the closed real axis and
satisfying the linear equation on this axis:
 ( ) +( ) +  −( ) =  ( );    ∈ {−∞; ∞}.”
(2)</p>
      <p>The closed real axis here is the contour [1]. The authors consider the case when
all zeros and poles of the coefficient  ( ) (if they exist) are located simultaneously
in the lower or upper half-plane of the extended complex plane.
1.2</p>
      <sec id="sec-2-1">
        <title>Analysis of Research and Publications</title>
        <p>
          The study of the Riemann-Hilbert problem’s solvability by exact methods goes back
to the works of I. I. Privalov, F. D. Gahov, Yu. I. Cherskij, M. G. Krejn, and others
          <xref ref-type="bibr" rid="ref4 ref5">(Gahov &amp; Cherskij, 1978; Krejn, 1958)</xref>
          . The connection between the theory of
integral equations of Wiener-Hopf type and this problem was first noted by I. M.
          <xref ref-type="bibr" rid="ref11">Rapoport (1948</xref>
          , 1949). Using the provisions of M. G. Krejn (1958, p. 114)
concerning the N. I. Mushelishvili book (1968), the authors conclude that this
problem was solved under the assumption that the additional Hölder condition for
functions on a contour is fulfilled. The apparatus of the Cauchy integral theorem,
an index, was often used. This can lead to the need to overcome serious analytical
difficulties, sometimes unjustified. Information of history elements to the Riemann
problem, integral equations of convolution type, is in the works of F. D. Gahov, Yu.
I. Cherskij, M. G. Krejn, and others
          <xref ref-type="bibr" rid="ref3 ref4 ref5">(Gahov, 1963; Gahov &amp; Cherskij, 1978; Krejn,
1958)</xref>
          . Here arises the question about easing restrictions. In M. G. Krejn work
(1958), new ideas and an indication of possible approaches to research based on the
theory of Banach algebras, under different assumptions and without the requirement
that the functions be Hölder, appeared for the first time. Related to the
RiemannHilbert problem, integral equations of convolution type, the study of abstract
equations with an arbitrary right-hand side in associative rings with a special pair
of subrings, and their realizations in concrete rings, the results of individual works
by G. S. Poletaev (1973–2020) and in co-authorship
          <xref ref-type="bibr" rid="ref13 ref9">(Poletaev, 1988; Voytik et al.,
2017)</xref>
          . The works by V. N. Akopyan &amp; L. L. Dashtoyan (2013); A. McNabb &amp; A.
Schumitzky (1972); and G. Ya. Popov, P. V. Kerekesha &amp; V. E. Kruglov (1976)
confirmed the relevance of a range of issues close to the Riemann-Hilbert problem.
Along with others, the case is important when in this type of problems and related,
the coefficients are rational functions
          <xref ref-type="bibr" rid="ref10 ref3 ref8">(Gahov, 1963; Mushelishvili, 1968; Popov et
al., 1976)</xref>
          . However, it does not consider the specifics of the case when the zeros
and poles of the coefficient of a related problem and the equation under
consideration are simultaneously located in one of the half-planes of the extended
complex plane. Therefore, the search for solutions to equations (1) in the considered
setting is relevant.
1.3
        </p>
      </sec>
      <sec id="sec-2-2">
        <title>Research Objective</title>
        <p>
          The research aims to establish the form of general formulas for solutions of abstract
equations (1), considering the specifics of assumptions in cases where the
coefficient  ( ) is a function of the considered ring of rational ones. Moreover, a
function, all zeros, and poles of which (if they exist) are finite, immaterial, and are
concentrated simultaneously either inside the upper half-plane or the lower
halfplane of the extended complex plane. The aim can be achieved using the
corresponding statements and theorems, decision formulas established in the works
of the abovelisted authors
          <xref ref-type="bibr" rid="ref13 ref5 ref6 ref9">(Krejn, 1958; McNabb &amp; Schumitzky, 1972; Poletaev,
1988; Voytik et al., 2017)</xref>
          .
2
2.1
        </p>
      </sec>
    </sec>
    <sec id="sec-3">
      <title>Materials and Methods</title>
      <sec id="sec-3-1">
        <title>Designations, Definitions, and General Provisions</title>
        <p>The current research uses designations and statements from the works of the
abovementioned authors. The symbol  denotes an arbitrary commutative and
associative ring with unit  . Let  +,  − - be the commuting projectors  →  .
Therefore:</p>
        <p>0: =  + −(=  − +),  ∓: =  ∓ −  0,  ∗: =  + +  −.</p>
        <p>For any subset  ⊆  let us denote  ∓, 0: =  ∓, 0 ;  ∓: =  ∓ ;  ∗ =  + +  −;
 ∗ =  + +  −. For any element  ∈  , we assume:</p>
        <p>∓, 0: =  ∓, 0 ,  ∓: =  ∓ ,  ∗: =  ∗ .</p>
        <p>
          Definition 1. A pair of subrings ( +,  −) of a ring  with unit  will be called a
factorization pair [FP], if it is generated in force in  commuting projectors
 +,    −: ∓ =  ∓( ), and the following axioms
          <xref ref-type="bibr" rid="ref6">(McNabb &amp; Schumitzky, 1972)</xref>
          :
 ∈  0  =  ∓ ∩  ± ;
(*)
 0(=  ∓ ±) - is the ring homomorphism  +and  − in  0;
 + −,     − + ⊆  + +  −
(: =  ∗).
        </p>
        <p>(**)
(***)
Definition 2. Any ring</p>
        <p>with unit  1′, considered together with a fixed FP of
the subrings  2′  , in other words, subrings with axiomatically specified properties
(*), (**), (***), will be called a “ring with a factorization pair” or, in short - a ring
with FP.
2.2</p>
      </sec>
      <sec id="sec-3-2">
        <title>Factorization of an Element of a ring by its Factorization Pair</title>
        <p>namely:
Let us say that the element  ∈  admits factorization in the commutative ring  by
the factorization pair  2′ =  2− 20 2+ (– by the FP  2′ =  2− 20
 2+), if there are elements
+ ∈  +,  0 ∈  0,  − ∈  − such that:  =  + 0 −. This factorization is called,
1. Correct factorization факторизацией [CF], if</p>
        <p>invertible in their subrings, respectively;
2. Normalized factorization [NF], if  0 =  0 =  ;</p>
        <p>
          only one normalized correct factorization.
3. Normalized regular factorization [NRF] if it is CF and  0 =  0 =  . The correct
factorization of an element from  − by the FP  1−′ 10′ 1+′ +
 2+′ 20′ 2−′ =  + +
 − can be normalized
          <xref ref-type="bibr" rid="ref6 ref9">(McNabb &amp; Schumitzky, 1972; Poletaev, 1988)</xref>
          . There is
+ ∈  +,  0 ∈  0,  − ∈  − - are
of all rational functions of a complex variable  ∈ ℂ, all whose poles (if they exist)

are finite and immaterial. The limits of functions from ℜ
 at infinity exist and are
finite. Let ℜ+ ( ℜ−) – be subsets of functions from ℜ , all poles of which (if they


exist) are located inside the lower (upper) half-plane  −( +), respectively
          <xref ref-type="bibr" rid="ref5">(Krejn,
1958, pp.14–15)</xref>
          . It can be shown that ℜ±,0 =  ±,0(ℜ ), where  0: =  + −(=

ℜ - ring with FP (ℜ+, ℜ−). For any function A(z) ∈ ℜ the decomposition is true:
        </p>
        <p>Let us establish formulas for solutions for (1) considering corresponding to the
 − +), ℜ0 = ℜ+

   ∩ ℜ−,</p>
        <p>( ): =  0 +  +( ) +  −( ).
research objective.
3
3.1</p>
      </sec>
    </sec>
    <sec id="sec-4">
      <title>Results</title>
      <sec id="sec-4-1">
        <title>Main Result</title>
        <p>
          Results of individual works by G. S. Poletaev (1973–2020) and in co-authorship
          <xref ref-type="bibr" rid="ref13 ref9">(Poletaev, 1988; Voytik et al., 2017)</xref>
          suggest that the following is true:
Theorem 1. Let the function  ( ) ∈   have no real zeros and 
→ ∞
 ( ) =
≠  . If, in this case, the element inverse in   is the function  − ( ) admits
a normalized regular factorization:  − ( ) =   +( )   ( )   −( ),  ∈ ℂ ∪ {∞}
concerning the factorization pair ( +, −), then the abstract equation (1) and the
problem concerning  +( ) ∈  +,  −( ) ∈  −, for any right-hand side of B(z)∈
  , в   are uniquely solvable. The formulas find their only solution:
 +( ) =  +( )   0 [ −( ) +( ) ]+,
 −( ) =  −( ) + ( −
        </p>
        <p>( ))−1[ −( ) +( )]− ,   ∈ ℂ ∪ {∞}, (3)
where:
 0:=  0( ) =   ∈ ℂ.</p>
        <p>Using theorem 1, let us establish a statement corresponding to the research
objective.</p>
        <p>Theorem 2. Let the function A(z)∈ℜ с  0:=  0 ( ) = 
( 1, 2 ∈    ), for which: in the case 1):</p>
        <p>≠ 0 has no real zeros and all its zeros and poles (for existence) are located:
1) only inside the lower, or 2) only inside the upper, from the half-planes  −, + of
the extended complex plane, bounded by a closed real axis. Then for it there exists
in   the inverse - function  −1( ) ∈ ℜ
 and there is a normalized correct
factorization of  −1( ) =  +( ) 0( ) −( ),  ∈ ℂ ∪ {∞} by the factorization pair
 →∞
 ( ) = =
 −( ) = 1,  ∈ ℂ ∪ {∞};
  +( ) = [ −1( ) 0]+ =  −1( ) 0,
 0:= [ ( )]0,</p>
        <p>0( ) = [ 0]−1:= [ −1( )]0,
and in case 2) it will be:
 +( ) = 1 ,   0( ) = [ 0] −1,
 −( ) = [ 0 −1( )] − =  0 −1( ),  ∈ ℂ ∪ {∞}.</p>
        <p>For arbitrary  ( ) ∈ ℜ</p>
        <p>there is a unique solution to equation (1) and the
problem. This solution in case 1) can be found according to following the formulas:
 +( ) =  −1( ) +( ),  −( ) =  −( ),   ∈ ℂ ∪ {∞};
and in case 2) - according to the formulas:
 +( ) = [ −1( ) +( )] +,</p>
        <p> 
 −( ) =  −( ) +  ( )[ −1( ) +( )] −,   ∈ ℂ ∪ {∞}.
and
the
assumptions,
in</p>
        <p>case</p>
        <p>Proof. Under the conditions of theorem 2, for the coefficient  ( ) ∈ ℜ there
exists an inverse in ℜ , and by virtue of the definitions of the subrings ℜ +</p>
        <p>,  ℜ −
1)  ( ),  −1( ) ∈ ℜ+,

and
in
case
2)  ( ),   −1( ) ∈ ℜ−. Therefore, there is a normalized correct factorization of

 −1( ) =  +( ) 0( )  −( ),  ∈ ℂ ∪ {∞} over the factorization pair ( 1, 2 ∈
   ), which will be: in the case 1)  +( ) = [ −1( ) 0)]+ ==  −1( ) 0,   0:=
[ ( )] 0,   0( ) = [ 0]−1 = [ −1( )] 0,  −( ) = 1,  ∈ ℂ ∪ {∞}; and in case 2)
 +( ) = 1,  0( ) = [ 0]−1,  −( ) = [ 0 −1( )]− =  0 −1( ),  ∈ ℂ ∪ {∞}.
Therefore, by theorem 1, for an arbitrary right-hand side  ( ) ∈ ℜ there is a
(4)
(5)</p>
      </sec>
      <sec id="sec-4-2">
        <title>3.2 Example</title>
        <p>In this case,
unique solution in ℜ to equation (1) and the problem. It can be found by formulas
(3), which, in case 1), give:
 +( ) =  −1( ) 0 [ 0]−1 [1 ⋅  +( )]+  =  −1( )  +( ),</p>
        <p>−( ) =  −( ) + (1)−1[1 ⋅  +( )]− =  −( ).</p>
        <p>The formulas (4) are valid. In case 2), from the same formulas (3), it follows that:
 +( ) = 1 ⋅ [ 0]−1[ 0 −1( )  +( )]+ = [ −1( )  +( )]+,
 −( ) =  −( ) + [ 0]−1 ( )[ 0 −1( ) +( )]− =</p>
        <p>=  −( ) +  ( )[ −1( ) +( )]− ,
that is, formulas (5) are valid. The theorem is proved.</p>
        <p>Consequence. Under the conditions of theorem 2, equation (1) and the problem
with the right-hand side  ( ) = 1,   ( ) ∈ ℜ ,  ∈ ℂ ∪ {∞} have in ℜ the only
solution  +( ),   − ( ). In case 1) from theorem 2, it can be found by the formulas:
 +( ) =  −1( ),  − ( ) = 0,  ∈ ℂ ∪ {∞},
(6)
and in case 2) - according to the following formulas:</p>
        <p>+( ) = [ −1( )]0 = [ 0]−1,   − ( ) =  ( )[ −1( )]−,  ∈ ℂ ∪ {∞}. (7)
The transformation of the second of equalities (7) can be represent in the as:
 +( ) = [ 0( )]−1,   − ( ) = 1 −  ( )[ 0]−1,  ∈ ℂ ∪ {∞}. (8)
Let us find a solution to an equation of the form (1) and problem in ℜ for:
11 2−33 −22 5 +5 .</p>
        <p>( ) = 3 2−24 −45 ;  ( ) =  2+22 −120
 0 = 131;  ( ) = 31(1(−−3 ))(( −−52 )) ;  −1( ) = 13(1(−−3 ))(( −−52 ));</p>
        <p>5( +  )
 ( ) = ( + 10 )( + 12 ) =  +( ) =  +( ),</p>
        <p>−( ) = 0 =  −( ).</p>
        <p>In this example, all zeros and poles of the function  ( ) are located in the upper
half-plane. Thus,  ( ),  −1( ) ∈ ℜ− and, by virtue of theorem 2, formulas (5) are
applicable. Using these formulas, let us find a unique solution to equation (1) and
the problem in the form:</p>
        <p>3( − 3 )( − 5 ) 5( +  ) + +
 +( ) = 11( −  )( − 2 ) ⋅ ( + 10 )( + 12 ) =</p>
        <p> 15(z − 3i)(z − 5i)(z + i) 
=
11(z − i)(z − 2i)(z + 10i)(z + 12i) </p>
        <p>+
,
 −( ) =</p>
        <p>5( +  )
( + 10 )( + 12 ) −
+
11 ( −  )( − 2 )
3 ( − 3 )( − 5 )</p>
        <p>×
⋅
⋅
×
3( − 3 )( − 5 )
11( −  )( − 2 )</p>
        <p>5( +  )
( + 10 )( + 12 )
=
 =</p>
        <p>⋅
5
(−467 + 1363 )</p>
        <p>.</p>
        <p>8008  2 − 8 − 15</p>
        <p>By substitution in (1), one can make sure that the solution is actually found. The
desired solution is as follows:</p>
        <p>
          X+ (z) =
225
In the range of questions related to integral equations of the convolution type and
the Riemann problem, research methods based on the integral theory (Cauchy type)
are distinguished by a significant analytical barrier. It is quite challenging to bring
research to the level of observable theorems. In different classes of assumptions, it
is often necessary to rebuild the theory from scratch. Examples of new approaches
go back, particularly to the research of M. G.
          <xref ref-type="bibr" rid="ref5">Krejn (1958)</xref>
          . Simultaneously, it is
sometimes possible to simplify and obtain the final results and exact formulas for
solutions to equation (1). This is how the current research is carried out. Using a
new approach, the authors obtained a general solvability theorem that considers the
specifics of the assumptions and contains convenient solution formulas. The
resulting theorem is consistent with the stated objective. The authors note that the
special nature of the used FP ring can be both a strength and a weakness of the
research. The proposed approach is simpler and more efficient to use. Other authors
did not have similar results.
        </p>
        <p>The authors have reflected the research results in many publications. With the
received materials (abstract and specific), they participated in scientific conferences
of the following structures:
1. Kherson National Technical University (KNTU) in Kherson (Ukraine);
2. Taras Shevchenko National University of Kyiv (KNU);
3. National Technical University of Ukraine “Igor Sikorsky Kyiv Polytechnic</p>
        <p>Institute” (NTUU KPI) in Kyiv (Ukraine);
4. Bauman Moscow State Technical University (BMSTU) in Moscow (Russia);
5. Odessa State Academy of Civil Engineering and Architecture in Odessa
(Ukraine) (2015–2020), and others.</p>
        <p>Experts showed a significant interest to the obtained results.
5</p>
      </sec>
    </sec>
    <sec id="sec-5">
      <title>Conclusion</title>
      <p>The paper considers the specifics of the assumptions about the location of the
singular points of the rational coefficient of equation (1). The authors obtained final
results that are easy to use, and the main results of the research are consistent with
the objective. For the first time, under the conditions of theorem 2, signs are
established that consider the specifics of assumptions about the coefficients of
equation (1) and general formulas (4)-(8) of solutions in ℜ . They are more

convenient than the ones obtained by the authors earlier. The results are applicable
when studying the existence, uniqueness, or non-uniqueness of solutions, their
construction for specific equations of the form (1), and corresponding related
problems. Their practical significance lies in the possibility of facilitating their use
for finding solutions of specific equations of the considered form and demonstrating
a new general approach. The new research methodology for this problem is also of
practical interest. Other researchers did not use the proposed method in the
considered ring. The authors want to study the cases further when factorization
concerning the factorization pair for  −1( ) is not correct. The expansion of classes
of equations, examples of rings with factorization pairs, the expansion of the scope
of the approach based on the approximation of functions, and applied aspects are
also promising. The obtained results indicate the fruitfulness of the approach from
the theory of equations in rings with factorization pairs for the considered issues
and
problems.</p>
      <p>According
to
assumptions, they
deepen
the
fundamental
understanding of issues related to the Riemann problem and simplify the process of
solving specific examples. The formulation of the problem of solvability of the
equation, considering the specifics of the location of the singular points of the
rational coefficient, is given for the first time and the “circular” approach to the
research. It demonstrates the possibility of a unified approach based on the
provisions on equations in rings with FP and provides an opportunity to see the
interpretation and results of research.</p>
    </sec>
  </body>
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