<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2023.114059</article-id><article-id pub-id-type="publisher-id">JAMP-124321</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Matrix Boundary Value Problem on Hyperbola
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Shaohua</surname><given-names>Fan</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>School of Science, Tianjin University of Technology and Education, Tianjin, China</addr-line></aff><pub-date pub-type="epub"><day>13</day><month>04</month><year>2023</year></pub-date><volume>11</volume><issue>04</issue><fpage>884</fpage><lpage>890</lpage><history><date date-type="received"><day>6,</day>	<month>March</month>	<year>2023</year></date><date date-type="rev-recd"><day>15,</day>	<month>April</month>	<year>2023</year>	</date><date date-type="accepted"><day>18,</day>	<month>April</month>	<year>2023</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  We study a special class of lower trigonometric matrix value boundary value problems on hyperbolas. Firstly, the pseudo-orthogonal polynomial on hyperbola is given in bilinear form and it is shown that it is the only one. Secondly, a special boundary value problem of lower triangular matrix is presented and transformed into four related boundary value problems. Finally, Liouville theorem and Painlev&#233; theorem and pseudo-orthogonal polynomials are used to give solutions.
 
</p></abstract><kwd-group><kwd>Hyperbola</kwd><kwd> Matrix Boundary Value Problem</kwd><kwd> Orthogonal Polynomial</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In some references [<xref ref-type="bibr" rid="scirp.124321-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.124321-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.124321-ref3">3</xref>] , the boundary value problem (Riemann-Hilbert problem) of analytic functions on finite curves is discussed, but the research on infinite curves is not deep enough. In [<xref ref-type="bibr" rid="scirp.124321-ref4">4</xref>] , the author discusses the Riemann boundary value problem on the positive real axis and generalizes the concept of the generalized principal part.</p><p>The Riemann-Hilbert method is a brand-new method for studying orthogonal polynomials formed in recent 20 years. In 1992, FoKas A S, Its A R and Kitaev A V constructed a matrix-valued Riemann-Hilbert boundary value problem in [<xref ref-type="bibr" rid="scirp.124321-ref5">5</xref>] , the only solution of which is the orthogonal polynomial on the real axis. In 1993, Deift P and Zhou X introduced the Riemann-Hilbert boundary value problem of oscillatory type in [<xref ref-type="bibr" rid="scirp.124321-ref6">6</xref>] , and applied it to the study of orthogonal polynomials. Therefore, the Riemann-Hilbert method was formed [<xref ref-type="bibr" rid="scirp.124321-ref6">6</xref>] .</p></sec><sec id="s2"><title>2. Preliminary</title><p>In this paper, the right branch of the Hyperbola x 2 − y 2 = 1 is denoted by default to L, which is regarded as the image of the function x = φ ( y ) = y 2 + 1 , and L is oriented from top to bottom.</p><p>Denote by l a the point φ ( a ) + i a and ∞ &#177; respectively its upper and lower infinite ends. Then ℂ consists of two connected components, the right part S + and the left part S − .</p><p>We use bilinear form to replace inner product on hyperbola, which is a common way. For example, [Lu J K, 1993] gives the solvable condition of singular integral equation by this way; for example, Delft P. defined a polynomial group similar to orthogonal polynomials in bilinear form in [<xref ref-type="bibr" rid="scirp.124321-ref7">7</xref>] , and we studied similar polynomial groups on hyperbola:</p><p>Let w ( t ) be a nonzero weight function. We introduce bilinear form in polynomial space Π n with degree no more than n:</p><p>( f , g ) = ∫ L w ( t ) f ( t ) g ( t ) d t , f , g ∈ Π n (1)</p><p>Take a group of bases 1 , t , t 2 , ⋯ , t n in Π n and make Schmidt orthogonalization on this group of bases, then we have</p><p>p 0 ( z ) = 1 ( ∫ L w d t ) 1 2</p><p>p 1 ( z ) = t − ( t , p 0 ) ( p 0 , p 0 ) p 0 ( t − ( t , p 0 ) ( p 0 , p 0 ) p 0 , t − ( t , p 0 ) ( p 0 , p 0 ) p 0 ) 1 2</p><p>⋮</p><p>p n ( z ) = t n − ( t n , p n − 1 ) ( p n − 1 , p n − 1 ) p n − 1 − ⋯ − ( t n , p 1 ) ( p 1 , p 1 ) p 1 − ( t n , p 0 ) ( p 0 , p 0 ) p 0 ( A n , A n )</p><p>where A n = t n − ( t n , p n − 1 ) ( p n − 1 , p n − 1 ) p n − 1 − ⋯ − ( t n , p 1 ) ( p 1 , p 1 ) p 1 − ( t n , p 0 ) ( p 0 , p 0 ) p 0 , If ( p n , p n ) is always not zero, then this process can always be carried out. Finally, we get a pseudo-orthogonal polynomial group with a weight function of p 0 , p 1 ( z ) , ⋯ , p n ( z ) on L:</p><p>P k ( z ) = 1 α k p k ( z ) , k = 0 , 1 , ⋯ , n , (2)</p><p>where α k is the first coefficient of p k ( z ) , then P k ( z ) is a pseudo-orthogonal polynomial of degree k with the first coefficient of 1. Obviously, the pseudo-orthogonal polynomial group P 0 , P 1 ( z ) , ⋯ , P n ( z ) is unique.</p><p>Definition 1. Let f is defined on L, if there is some positive real number a, such that</p><p>| f ( t ′ ) − f ( t ″ ) | ≤ M | 1 t ′ − 1 t ″ | μ ,       t ′ , t ″ ∈ l ∞ + l a ⌢ ∪ l a l ∞ − ⌢ (3)</p><p>where M and 0 &lt; μ ≤ 1 are definite constants, then denoted by f ∈ H ^ μ ( ∞ ) , and if f ∈ H μ ( L ) , then denoted by f ∈ H ^ μ ( L ) . If f ∈ H ^ μ ( ∞ ) and f ( ∞ ) = 0 , then denoted by f ∈ H ^ 0 μ ( ∞ ) , or f ∈ H ^ 0 ( ∞ ) . Moreover, if t λ f ∈ H ^ 0 ( ∞ ) , then denoted by f ∈ H ^ λ , 0 ( ∞ ) .</p><p>Definition 2 Let f is a function defined on L. There exists t → ∞ such that</p><p>f ( t ) = f * ( t ) t ν ,</p><p>where v is a real number and f * is a bounded function, then denoted by f ∈ O v ( ∞ ) .</p><p>Definition 3 If F is holomorphic in the complex plane cut by the Hyperbola, then denoted by F ∈ A ( ℂ \ L ) .</p><p>Definition 4 Let f be a locally integrable function on L. If</p><p>( C [ f ] ) ( z ) = 1 2 π i ∫ L f ( τ ) τ − z d τ ,     z ∈ ℂ \ L (4)</p><p>is integrable, it is called the Cauchy-type integral with kernel density f on L, and the Cauchy principal value integral with kernel density f is defined by</p><p>( C [ f ] ) ( t ) = 1 2 π i ∫ L f ( τ ) τ − t d τ = lim r → 0 + 1 2 π i ∫ | y − a | &gt; 0 f ( ( φ ( y ) + i y ) ) ( φ ′ ( y ) + i y ) φ ( y ) + i y − t d y (5)</p><p>where t = φ ( a ) + i a ∈ L , if the integral exists.</p><p>Ref [Wang Ying, 2017], below we introduce the concept of a generalized main part.</p><p>Definition 5 Let F ∈ A ( ℂ \ L ) . If there exists an entire function E ( z ) such that</p><p>lim z → ∞ [ F ( z ) − E ( z ) ] = 0 . (6)</p><p>and then E ( z ) is called the generalized principal part of F ( z ) at ∞ , denoted by G .P [ F , ∞ ] .</p><p>Reference [<xref ref-type="bibr" rid="scirp.124321-ref8">8</xref>] proves the generalized principal part of Cauchy integral at infinity and Plemelj formula.</p><p>Theorem 1 [<xref ref-type="bibr" rid="scirp.124321-ref8">8</xref>] If f ∈ H ( L ) ∩ O v ( ∞ ) ( v &gt; 0 ) is locally integrable on L. Then</p><p>G .P [ C [ f ] , ∞ ] = 0 . (7)</p><p>Theorem 2 [<xref ref-type="bibr" rid="scirp.124321-ref8">8</xref>] If f ∈ H ^ μ ( L ) , then the boundary values of the Cauchy-type integral C [ f ] exist and have the following Plemelj formula:</p><p>( C [ f ] ) &#177; ( t ) = &#177; 1 2 f ( t ) + 1 2 π i ∫ L f ( τ ) τ − t d τ . (8)</p></sec><sec id="s3"><title>3. Matrix Value Riemann Boundary Value Problem</title><p>In this paper, we consider the Riemann boundary value problem of lower trigonometric matrix on hyperbola.</p><p>Let</p><p>Φ ( z ) = ( Φ 1 , 1 ( z ) Φ 1 , 2 ( z ) Φ 2 , 1 ( z ) Φ 2 , 2 ( z ) ) (9)</p><p>be a matrix-valued function defined on subset Ω of the complex plane ℂ , and each element Φ j , k be a function defined on Ω . If every element Φ j , k of Φ satisfies the same property, then Φ is said to have its corresponding property, such as Φ ∈ A ( ℂ \ L ) , G .P [ Φ , ∞ ] ( z ) , Φ ∈ H ( L ) .</p><p>Problem (boundary value problem of lower trigonometric matrix value function) Find the matrix-valued partitioned holomorphic function Φ with L as the jump curve, such that</p><p>{ Φ + ( t ) = ( 1 0 w ( t ) 1 ) Φ − ( t ) , t ∈ L , G .P [ Ξ Φ , ∞ ] ( z ) = I , (10)</p><p>where</p><p>Ξ ( z ) = ( z − n 0 0 z n ) , (11)</p><p>I is the identity matrix of 2 &#215; 2, w ∈ H μ ( L ) ∩ H ^ 2 n , 0 ( ∞ ) .</p><p>We can convert (10) into four related Riemann boundary value problems:</p><p>{ Φ 1 , 1 + ( t ) = Φ 1 , 1 − ( t ) , t ∈ L , G .P [ z − n Φ 1 , 1 , ∞ ] = 1 , (12)</p><p>{ Φ 1 , 2 + ( t ) = Φ 1 , 2 − ( t ) , t ∈ L , G .P [ z − n Φ 1 , 2 , ∞ ] = 0 , (13)</p><p>{ Φ 2 , 1 + ( t ) = Φ 2 , 1 − ( t ) + w ( t ) Φ 1 , 1 − ( t ) , t ∈ L , G .P [ z n Φ 2 , 1 , ∞ ] = 0 , (14)</p><p>{ Φ 2 , 2 + ( t ) = Φ 2 , 2 − ( t ) + w ( t ) Φ 1 , 2 − ( t ) , t ∈ L , G .P [ z n Φ 2 , 2 , ∞ ] = 1. (15)</p><p>Obviously, (12) is a Liouville problem. It is known from Painlev&#233; theorem that Φ 1 , 1 ( z ) is analytic over the entire complex plane. Because G .P [ z − n Φ 1 , 1 , ∞ ] = 1 , it is known from the generalized Liouville theorem that</p><p>Φ 1 , 1 ( z ) = P n ( z ) , (16)</p><p>where P n ( z ) is a polynomial with a leading coefficient of 1 and a degree of n.</p><p>By (16), we have</p><p>{ Φ 2 , 1 + ( t ) = Φ 2 , 1 − ( t ) + w ( t ) P n ( t ) , t ∈ L , G .P [ z n Φ 2 , 1 , ∞ ] = 0 , (17)</p><p>Obviously (17) is a jump problem with L as the jump curve. Let</p><p>ψ ( z ) = C [ w P n ] ( z ) = 1 2 π i ∫ L w ( τ ) P n ( τ ) τ − z d τ ,                 z ∈ L , (18)</p><p>by w ∈ H μ ( L ) ∩ H ^ 2 n , 0 ( ∞ ) ,</p><p>w P n ∈ H μ ( L ) ∩ H ^ n , 0 ( ∞ ) . (19)</p><p>Therefore, by Plemelj formula (8) and Theorem 1, we can know that ψ ( z ) is a partitioned holomorphic function with L as the jump curve, and satisfies:</p><p>{ ψ + ( t ) = ψ − ( t ) + ω ( t ) P n ( t ) , t ∈ L , G .P [ ψ , ∞ ] ( z ) = 0 , (20)</p><p>let F ( z ) = Φ ( z ) − ψ ( z ) , then F is a partitioned holomorphic function with L as the jump curve and satisfies:</p><p>{ F + ( t ) = F − ( t ) , t ∈ L , G .P [ F , ∞ ] = 0, (21)</p><p>Obviously problem (21) is a zero-order Liouville problem, its solution is F ( z ) = 0 , so</p><p>Φ 2 , 1 ( z ) = C [ w P n ] ( z ) = 1 2 π i ∫ L w ( τ ) P n ( τ ) τ − z d τ ,   z ∈ ℂ \ L (22)</p><p>if and only if condition G .P [ z n Φ 2 , 1 , ∞ ] = 0 is satisfied. By</p><p>z n Φ 2 , 1 ( z ) = 1 2 π i ∫ L w ( τ ) P n ( τ ) ( z n − τ n ) τ − z d τ + 1 2 π i ∫ L w ( τ ) P n ( τ ) τ n τ − z d τ = − ∑ k = 0 n − 1 z k 2 π i ∫ L w ( τ ) P n ( τ ) τ n − 1 − k d τ + 1 2 π i ∫ L w ( τ ) P n ( τ ) τ n τ − z d τ , (23)</p><p>and Theorem 1 and (19), it can be seen that G .P [ z n Φ 2 , 1 , ∞ ] = 0 is equivalent to</p><p>1 2 π i ∫ L w ( τ ) P n ( τ ) τ k d τ = 0 , k = 0 , 1 , ⋯ , n − 1 . (24)</p><p>Obviously (13) is the Liouville problem, similar to (12) we have</p><p>Φ 1 , 2 ( z ) = q n − 1 ( z ) (25)</p><p>where q n − 1 ( z ) is a polynomial of order not exceeding n − 1 .</p><p>By (16), we have</p><p>{ Φ 2 , 2 + ( t ) = Φ 2 , 2 − ( t ) + w ( t ) q n − 1 ( t ) , t ∈ L , G .P [ z n Φ 2 , 2 , ∞ ] = 1. (26)</p><p>Obviously, (26) is a fixed-order jump problem, similar to (15). It can be seen that its solution is</p><p>Φ 2 , 2 ( z ) = C [ w q n − 1 ] ( z ) = 1 2 π i ∫ L w ( τ ) q n − 1 ( τ ) τ − z d τ ,   z ∈ ℂ \ L (27)</p><p>if and only if condition</p><p>{ 1 2 π i ∫ L w ( τ ) q n − 1 ( τ ) τ k d τ = 0 , k = 0 , 1 , ⋯ , n − 2 , 1 2 π i ∫ L w ( τ ) q n − 1 ( τ ) τ n − 1 d τ = − 1 , (28)</p><p>is satisfied.</p><p>Let q n − 1 = λ P n − 1 , then</p><p>1 2 π i ∫ L ω ( τ ) λ P n − 1 P n − 1 = − 1 , (29)</p><p>that is,</p><p>λ = − 2 π i ∫ L ω ( τ ) P n − 1 2 ( τ ) d τ (30)</p><p>then q n − 1 is a pseudo-orthogonal polynomial of degree n − 1 on L with respect to the weight function w.</p><p>Definition 6</p><p>f * ( z ) = 1 2 π i ∫ L ω ( τ ) f ( τ ) τ − z d τ ,               z ∉ L , (31)</p><p>we call it the companion function of f with respect to the weight function w.</p><p>Theorem 3 If w ∈ H μ ( L ) ∩ H ^ 2 n , 0 ( ∞ ) , then the lower triangular matrix-valued Riemann boundary value problem (10) has a solution, and its solution has the following form:</p><p>Φ ( z ) = ( P n ( z ) λ P n − 1 ( z ) P n * ( z ) λ P n − 1 * ( z ) ) , (32)</p><p>where P n ( z ) is a polynomial with a leading coefficient of 1 and a degree of n, and P n * is the companion function of P n with respect to the middle weight function w.</p><p>Proof: If (10) has a solution, it can be seen from the previous discussion that its solution is of the form (32).</p><p>Conversely, the polynomial with pseudo-orthogonal and leading coefficient 1 is unique, and by reversing each previous step, we get that Φ is the solution of (10), that is, (10) has and only one set of solutions (32).</p><p>The matrix-valued boundary value problem (10) is characterized by the pseudo-orthogonal polynomial P n on L with respect to the weight function w and the leading coefficient is 1. Therefore, we call this problem the Riemann-Hilbert characteristic characterization of the orthogonal polynomial of the weight function w on hyperbola, or P n is the characteristic orthogonal polynomial of the matrix-valued boundary value problem (10), please refer to [Deift P, 2011] for details.</p></sec><sec id="s4"><title>Conflicts of Interest</title><p>The author declares no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s5"><title>Cite this paper</title><p>Fan, S.H. (2023) Matrix Boundary Value Problem on Hyperbola. Journal of Applied Mathematics and Physics, 11, 884-890. https://doi.org/10.4236/jamp.2023.114059</p></sec></body><back><ref-list><title>References</title><ref id="scirp.124321-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Gakhov, F.D. (1977) Boundary Value Problems. Nauka, Moscow.</mixed-citation></ref><ref id="scirp.124321-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Lu, J.K. (1993) Boundary Value Problems for Analytic Functions. World Scientific, Singapore. https://doi.org/10.1142/1701</mixed-citation></ref><ref id="scirp.124321-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Muskhelishvili, N.I. (1953) Singular Integral Equations. 2nd Edition, P. Noordhoff N. V., Groningen.</mixed-citation></ref><ref id="scirp.124321-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Wang, Y., Duan, P. and Du, J.Y. (2017) Riemann Boundary Value Problems on Positive Real Axis. Science in China: Mathematics, 47, 887-918. https://doi.org/10.1360/N012016-00146</mixed-citation></ref><ref id="scirp.124321-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Fokas, A.S., Its, A. and Kitaev, A.V. (1992) The Isomonodromy Approach to Matric Models in 2D Quantum Gravity. Communications in Mathematical Physics, 147, 395-430. https://doi.org/10.1007/BF02096594</mixed-citation></ref><ref id="scirp.124321-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Deift, P. and Zhou, X. (1993) A Steepest Descent Method for Oscillatory Riemann—Hilbert Problems. Asymptotics for the MKdV Equation. Annals of Mathematics, 137, 295-368. https://doi.org/10.2307/2946540</mixed-citation></ref><ref id="scirp.124321-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">Deift, P., Its, A. and Krasovsky, I. (2011) Asymptotics of Toeplitz, Hankel, and Toeplitz + Hankel Determinants with Fisher-Hartwig Singularities. Annals of Mathematics, 174, 1243-1299. https://doi.org/10.4007/annals.2011.174.2.12</mixed-citation></ref><ref id="scirp.124321-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">Wei, Y.Q. and Liu, H. (2023) Properties of Cauchy Integral on the Hyperbola. Journal of Ningxia Normal University, 44, 6-12.</mixed-citation></ref></ref-list></back></article>