<?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">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2016.718189</article-id><article-id pub-id-type="publisher-id">AM-73044</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>
 
 
  Asymptotic Formulas of the Solutions and the Trace Formulas for the Polynomial Pencil of the Sturm-Liouville Operators
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>A.</surname><given-names>Adiloglu Nabiev</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Mathematics, Cumhuriyet University, Sivas, Turkey</addr-line></aff><author-notes><corresp id="cor1">* E-mail:</corresp></author-notes><pub-date pub-type="epub"><day>02</day><month>12</month><year>2016</year></pub-date><volume>07</volume><issue>18</issue><fpage>2411</fpage><lpage>2417</lpage><history><date date-type="received"><day>October</day>	<month>25,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>December</month>	<year>25,</year>	</date><date date-type="accepted"><day>December</day>	<month>28,</month>	<year>2016</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>
 
 
  This work studies the asymptotic formulas for the solutions of the Sturm-Liouville equation with the polynomial dependence in the spectral parameter. Using these asymptotic formulas it is proved some trace formulas for the eigenvalues of a simple boundary problem generated in a finite interval by the considered Sturm-Liouville equation.
 
</p></abstract><kwd-group><kwd>Sturm-Liouville Equation</kwd><kwd> Asymptotic Formulas for Solutions</kwd><kwd> Spectral Parameter</kwd><kwd> Eigenvalue</kwd><kwd> Boundary Value Problem</kwd><kwd> Trace Formula</kwd><kwd> Fractional Integrals and  Derivatives</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Consider the differential equation</p><disp-formula id="scirp.73044-formula30"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x2.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x3.png" xlink:type="simple"/></inline-formula> are complex valued functions and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x4.png" xlink:type="simple"/></inline-formula> is a complex parameter.</p><p>Differential equations of type (1) often appear in connection with some spectral problems and nonlinear evolution equations (see [<xref ref-type="bibr" rid="scirp.73044-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.73044-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.73044-ref3">3</xref>] ). In the case <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x5.png" xlink:type="simple"/></inline-formula> the equation is the classical Sturm-Liouville equation and in this case there are a wide class of spectral problems and inverse spectral problems which were investigated by constructing integral representations for the independent solutions of the Sturm-Liouville equation (see [<xref ref-type="bibr" rid="scirp.73044-ref4">4</xref>] ). We studied in [<xref ref-type="bibr" rid="scirp.73044-ref5">5</xref>] , the solutions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x6.png" xlink:type="simple"/></inline-formula> of the Equation (1) satisfying the initial conditions</p><disp-formula id="scirp.73044-formula31"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x7.png"  xlink:type="simple"/></disp-formula><p>and it is proved that in the sectors of complex plane</p><disp-formula id="scirp.73044-formula32"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x8.png"  xlink:type="simple"/></disp-formula><p>the solutions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x9.png" xlink:type="simple"/></inline-formula> have the following integral representations:</p><disp-formula id="scirp.73044-formula33"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x10.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x11.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x12.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x13.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x14.png" xlink:type="simple"/></inline-formula>belong to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x15.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x16.png" xlink:type="simple"/></inline-formula> respectively. Moreover, if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x17.png" xlink:type="simple"/></inline-formula> denotes Riemann-Liouville fractional derivative of order <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x18.png" xlink:type="simple"/></inline-formula> (see [<xref ref-type="bibr" rid="scirp.73044-ref6">6</xref>] ) with respect to t, i.e.</p><disp-formula id="scirp.73044-formula34"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x19.png"  xlink:type="simple"/></disp-formula><p>then for all <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x20.png" xlink:type="simple"/></inline-formula> the functions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x21.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x22.png" xlink:type="simple"/></inline-formula> belong to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x23.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x24.png" xlink:type="simple"/></inline-formula> respectively. Furthermore, the following equalities are valid:</p><disp-formula id="scirp.73044-formula35"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x25.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula36"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x26.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.73044-formula37"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x27.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula38"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x28.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula39"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x29.png"  xlink:type="simple"/></disp-formula><p>In the present paper we use the above facts about special solutions of the Equation (1) to obtain some trace formulas for the boundary value problem generated by the Equation (1) in the segment <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x30.png" xlink:type="simple"/></inline-formula> with simple boundary conditions</p><disp-formula id="scirp.73044-formula40"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x31.png"  xlink:type="simple"/></disp-formula></sec><sec id="s2"><title>2. Asymptotic Formulas and the Trace Formulas</title><p>Using (2), (3) and (4) it is easy to prove the following theorem where we seek two solutions which have special representations.</p><p>Theorem 1. If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x32.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x33.png" xlink:type="simple"/></inline-formula> then the Equation (1) has solutions</p><disp-formula id="scirp.73044-formula41"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x34.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.73044-formula42"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x35.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.73044-formula43"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x36.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula44"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x37.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula45"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x38.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula46"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x39.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula47"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x40.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula48"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x41.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula49"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x42.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula50"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x43.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula51"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x44.png"  xlink:type="simple"/></disp-formula><p>Since the solutions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x45.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x46.png" xlink:type="simple"/></inline-formula> are linearly independent for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x47.png" xlink:type="simple"/></inline-formula> we have</p><disp-formula id="scirp.73044-formula52"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x48.png"  xlink:type="simple"/></disp-formula><p>for the solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x49.png" xlink:type="simple"/></inline-formula> of the Equation (1) with initial conditions</p><disp-formula id="scirp.73044-formula53"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x50.png"  xlink:type="simple"/></disp-formula><p>Then the Theorem 1 gives</p><disp-formula id="scirp.73044-formula54"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x51.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.73044-formula55"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x52.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula56"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x53.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula57"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x54.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula58"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x55.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula59"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x56.png"  xlink:type="simple"/></disp-formula><p>Now let us connect the Equation (1) to the boundary conditions</p><disp-formula id="scirp.73044-formula60"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x57.png"  xlink:type="simple"/></disp-formula><p>In [<xref ref-type="bibr" rid="scirp.73044-ref2">2</xref>] it is obtained the asymptotic formulas for the eigenvalues <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x58.png" xlink:type="simple"/></inline-formula> of the boundary value problem (1)-(2). Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x59.png" xlink:type="simple"/></inline-formula> be a characteristic function of this boundary value problem. Then</p><disp-formula id="scirp.73044-formula61"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x60.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.73044-formula62"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x61.png"  xlink:type="simple"/></disp-formula><p>Let us consider the circles <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x62.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x63.png" xlink:type="simple"/></inline-formula> is sufficiently large integer. On circles <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x64.png" xlink:type="simple"/></inline-formula> the functions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x65.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x66.png" xlink:type="simple"/></inline-formula> are</p><p>bounded by the constants independent of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x67.png" xlink:type="simple"/></inline-formula>. So we have that the module of the maximum of the function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x68.png" xlink:type="simple"/></inline-formula> approaches to zero when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x69.png" xlink:type="simple"/></inline-formula>. Hence, if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x70.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x71.png" xlink:type="simple"/></inline-formula> are the series of eigenvalues of the problem (1), (18) we have</p><disp-formula id="scirp.73044-formula63"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x72.png"  xlink:type="simple"/></disp-formula><p>Using (19) and (20) we compute the integrals on the right hand side of the Equation (21) and prove the following theorem.</p><p>Theorem 2. If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x73.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x74.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x75.png" xlink:type="simple"/></inline-formula> are the series of eigenvalues of the boundary value problem (1), (18) then</p><disp-formula id="scirp.73044-formula64"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x76.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula65"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x77.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula66"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x78.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula67"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x79.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x80.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x81.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x82.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x83.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x84.png" xlink:type="simple"/></inline-formula> are constants defined by the help of the functions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x85.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x86.png" xlink:type="simple"/></inline-formula>. Here</p><disp-formula id="scirp.73044-formula68"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x87.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula69"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x88.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula70"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/10-7403446x89.png"  xlink:type="simple"/></disp-formula><p>in which the numbers <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x90.png" xlink:type="simple"/></inline-formula> are defined from the asymptotic equality</p><disp-formula id="scirp.73044-formula71"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x91.png"  xlink:type="simple"/></disp-formula><p>From Theorem 2 we have that if the Fourier series <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x92.png" xlink:type="simple"/></inline-formula> are conver-</p><p>gent and denoting their sums by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/10-7403446x93.png" xlink:type="simple"/></inline-formula> we obtain the following regularized trace formulas for the eigenvalues of the boundary value problem (1), (18):</p><disp-formula id="scirp.73044-formula72"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x94.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula73"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x95.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula74"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x96.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.73044-formula75"><graphic  xlink:href="http://html.scirp.org/file/10-7403446x97.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3"><title>Cite this paper</title><p>Adiloglu Nabiev, A. (2016) Asymptotic Formulas of the Solutions and the Trace Formulas for the Polynomial Pencil of the Sturm-Liouville Operators. Applied Mathematics, 7, 2411-2417. http://dx.doi.org/10.4236/am.2016.718189</p></sec></body><back><ref-list><title>References</title><ref id="scirp.73044-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Alonso, M. (1980) Schrodinger Spectral Problems with Energy-Dependent Potentials as Sources of Nonlinear Hamiltonian Evolution Equations. Journal of Mathematical Physics, 21, 2342-2349. https://doi.org/10.1063/1.524690</mixed-citation></ref><ref id="scirp.73044-ref2"><label>2</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>Yordanov</surname><given-names> R. </given-names></name>,<etal>et al</etal>. (<year>1984</year>)<article-title>About Some Spectral Properties of the Schrodinger Equation with an Energy Dependent Potential Generating Fully Integrable Hamiltonian Systems</article-title><source> Annals de L’Universite de Sofia “Kliment Ohridski” Faculte de Mathematiques et Mecanique</source><volume> 78</volume>,<fpage> 1</fpage>-<lpage>29</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.73044-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Jaulent, M. and Jean, C. (1982) Solution of a Schrodinger Inverse Scattering Problem with a Polynomial Spectral Dependence in the Potential. Journal of Mathematial Physics, 23, 258-266. https://doi.org/10.1063/1.525347</mixed-citation></ref><ref id="scirp.73044-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">Marchenko, V.A. (1997) Sturm-Liouville’s Operators and Their Application. Kiev.</mixed-citation></ref><ref id="scirp.73044-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">Guseinov, I.M., Nabiev, A.A. and Pashayev, R.T. (2000) Transformation Operators and Asymptotic Formulas for the Eigenvalues of a Polynomial Pencil of Sturm-Liouville Operators. Siberian Journal of Mathematics, 41, 453-464. https://doi.org/10.1007/BF02674102</mixed-citation></ref><ref id="scirp.73044-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">Samko, S.G., Kilbas, A.A. and Marichev, O.M. (1987) Integral and Derifatives of Fractional Order and Its Applications. Minsk, Nauka and Tekhnika.</mixed-citation></ref></ref-list></back></article>