<?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">APM</journal-id><journal-title-group><journal-title>Advances in Pure Mathematics</journal-title></journal-title-group><issn pub-type="epub">2160-0368</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/apm.2013.31A024</article-id><article-id pub-id-type="publisher-id">APM-27539</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>
 
 
  Poincar&#233; Problem for Nonlinear Elliptic Equations of Second Order in Unbounded Domains
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>uochun</surname><given-names>Wen</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>LMAM, School of Mathematical Sciences, Peking University, Beijing, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>wengc@math.pku.edu.cn</email></corresp></author-notes><pub-date pub-type="epub"><day>30</day><month>01</month><year>2013</year></pub-date><volume>03</volume><issue>01</issue><fpage>172</fpage><lpage>177</lpage><history><date date-type="received"><day>September</day>	<month>27,</month>	<year>2012</year></date><date date-type="rev-recd"><day>November</day>	<month>2,</month>	<year>2012</year>	</date><date date-type="accepted"><day>November</day>	<month>10,</month>	<year>2012</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>
 
 
   In [1], I. N. Vekua propose the Poincar&#233; problem for some second order elliptic equations, but it can not be solved. In [2], the authors discussed the boundary value problem for nonlinear elliptic equations of second order in some bounded domains. In this article, the Poincar&#233; boundary value problem for general nonlinear elliptic equations of second order in unbounded multiply connected domains have been completely investigated. We first provide the formulation of the above boundary value problem and corresponding modified well posed-ness. Next we obtain the representation theorem and a priori estimates of solutions for the modified problem. Finally by the above estimates of solutions and the Schauder fixed-point theorem, the solvability results of the above Poincar&#233; problem for the nonlinear elliptic equations of second order can be obtained. The above problem possesses many applications in mechanics and physics and so on.
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</p></abstract><kwd-group><kwd>Poincar&#233; Boundary Value Problem; Nonlinear Elliptic Equations; Unbounded Domains</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Formulation of the Poincar&#233; Boundary Value Problem</title><p>Let D be an <img src="4-5300326\7fb3f193-d097-4467-8b3a-92e16f91579b.jpg" />-connected domain including the infinite point with the boundary <img src="4-5300326\85bc0c01-2c85-42e6-909c-7ae2cbb34820.jpg" /> in<img src="4-5300326\e674188a-37ee-4786-a111-264c8ed0a3e7.jpg" />where<img src="4-5300326\c4075f53-453e-4a22-b647-9896abc64143.jpg" />. Without loss of generality, we assume that D is a circular domain in<img src="4-5300326\8e282a5a-08fb-49c3-a27e-abb38a38f5a1.jpg" />, where the boundary consists of <img src="4-5300326\1f89b9e9-fa25-4d52-8cb2-a74e0f581ec2.jpg" /> circles<img src="4-5300326\f1cb72b9-f934-46f3-86c7-3fc67db6503e.jpg" />, <img src="4-5300326\7a52da82-3dd3-4b53-b424-58ee831a1ff6.jpg" />and<img src="4-5300326\b00b3f02-ccd8-4839-bc8e-e93fade8b9d8.jpg" />. In this article, the notations are as the same in References [1-8]. We consider the second order equation in the complex form</p><disp-formula id="scirp.27539-formula96672"><label>(1.1)</label><graphic position="anchor" xlink:href="4-5300326\9478dc0c-887c-420d-bcc1-a1275f603641.jpg"  xlink:type="simple"/></disp-formula><p>satisfying the following conditions.</p><p>Condition C. 1)<img src="4-5300326\9ba4c732-6667-485f-b62e-27423d80a24f.jpg" />, <img src="4-5300326\27373b95-e7bb-4cd8-b6e1-3983a9932a1d.jpg" />are continuous in <img src="4-5300326\df1657d8-0bba-4fb4-bb45-8bd5d8245b4c.jpg" /> for almost every point <img src="4-5300326\85ba90f1-ea71-4eae-b2a6-a395c5d0c120.jpg" /> and <img src="4-5300326\504b699a-fd61-46f6-95af-9e124fd0867b.jpg" /> for <img src="4-5300326\4e1bfb72-fab3-41d0-8e4e-2fee8e6122b7.jpg" /></p><p>2) The above functions are measurable in <img src="4-5300326\43a07872-90f7-4d62-8300-0ddbbe1b5aac.jpg" /> for all continuous functions <img src="4-5300326\3bd8aeff-02b5-4777-870e-1d8567a9c838.jpg" /> in<img src="4-5300326\940a2ca7-b82a-4193-85d0-fc4729d6f8b0.jpg" />, and satisfy</p><disp-formula id="scirp.27539-formula96673"><label>(1.2)</label><graphic position="anchor" xlink:href="4-5300326\a8e748d2-5485-476d-9113-6b18e3c4fe79.jpg"  xlink:type="simple"/></disp-formula><p>in which <img src="4-5300326\7032dc67-99e8-4717-bbf1-2a64e78eb31f.jpg" /> <img src="4-5300326\ecd1b528-388c-412c-b6e2-490120aa4965.jpg" /> are non-negative constants.</p><p>3) The Equation (1.1) satisfies the uniform ellipticity condition, namely for any number <img src="4-5300326\25d3f656-bf37-4283-974e-e9238a73d280.jpg" /> and w, U<sub>1</sub>, <img src="4-5300326\f3598414-cd11-4fac-ac84-de93bb70b81c.jpg" />the inequality</p><p><img src="4-5300326\a9d4e445-d9ac-4139-89bd-f6b5d3d7054e.jpg" /></p><p>for almost every point <img src="4-5300326\29736031-41f2-424f-9c23-eba9c0b44a63.jpg" /> holds, where <img src="4-5300326\8ba0846e-a2b3-4b6f-8bed-cbdfa7d037c5.jpg" /> is a non-negative constant.</p><p>4) For any function<img src="4-5300326\86c8dcf7-cc21-4743-95dc-37c089e933e2.jpg" />, <img src="4-5300326\26ed0307-a641-4e0d-95ad-e13daf421861.jpg" />, <img src="4-5300326\4eaaca2e-c232-4c91-b41e-49fe89716483.jpg" />satisfies the condition</p><p><img src="4-5300326\31e7e32d-860b-4c4f-9ea7-5b41be766c2d.jpg" /></p><p>in which <img src="4-5300326\0c7e68c8-ec08-4f5a-852f-a9930ecceba6.jpg" /> satisfy the condition</p><disp-formula id="scirp.27539-formula96674"><label>(1.3)</label><graphic position="anchor" xlink:href="4-5300326\03e4c7c7-0ce5-4896-806b-8b4fd4a9c2c0.jpg"  xlink:type="simple"/></disp-formula><p>with a non-negative constant<img src="4-5300326\7a57dc1f-2754-402d-b520-6be790aecfe9.jpg" />.</p><p>Now, we formulate the Poincar&#233; boundary value problem as follows.</p><p>Problem P. In the domain D, find a solution <img src="4-5300326\8f382ed9-02b8-4b84-944c-9fa92a1fc090.jpg" /> of Equation (1.1), which is continuously differentiable in<img src="4-5300326\8e427090-8bd2-4bf4-ad1c-f48e3587ccdb.jpg" />, and satisfies the boundary condition</p><disp-formula id="scirp.27539-formula96675"><label>(1.4)</label><graphic position="anchor" xlink:href="4-5300326\2790c1ec-db49-4126-a1b2-025567b31792.jpg"  xlink:type="simple"/></disp-formula><p>in which <img src="4-5300326\42325232-d0ef-4eee-83c4-d0e535144477.jpg" /> is any unit vector at every point on<img src="4-5300326\120e4426-a3fa-4a97-8084-d30a6ac572a9.jpg" />, <img src="4-5300326\2f5cf0a8-12d5-4f98-8414-ddae067cdec2.jpg" /><img src="4-5300326\4c25964f-666c-4f5d-b860-feb3eed8f58d.jpg" />and <img src="4-5300326\02ee8e7b-3e68-453b-b3b1-3f5affbac9c1.jpg" /> are known functions satisfying the conditions</p><disp-formula id="scirp.27539-formula96676"><label>(1.5)</label><graphic position="anchor" xlink:href="4-5300326\7939e755-c214-4938-a2e9-fadfb41ac193.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="4-5300326\8b03a78d-415d-4749-a766-21f9bca8ad12.jpg" />, <img src="4-5300326\ce87b953-177a-4134-aeaf-4e40ad5172ed.jpg" />, <img src="4-5300326\a78824f7-56f9-4d00-876d-58d23dda9f98.jpg" />, <img src="4-5300326\5b9a2ca2-462d-4fb3-a1c2-e060ac67ca8b.jpg" />are non-negative constants.</p><p>If <img src="4-5300326\e4c58322-9036-47f4-a9b7-582a5117d983.jpg" /> and <img src="4-5300326\184491f8-e772-4ad1-bad5-199d52474677.jpg" /> on<img src="4-5300326\ce4e77a8-dc99-4cc7-a902-606a384cbb95.jpg" />, where n is the outward normal vector on<img src="4-5300326\619ae911-8e2d-443e-b884-043ebc6b2b8d.jpg" />, then Problem P is the Dirichlet boundary value problem (Problem D). If <img src="4-5300326\eac13b6b-543e-4576-9247-79475c59a483.jpg" /> and <img src="4-5300326\45447144-c730-4ed7-bdba-93862ac8396a.jpg" /> on<img src="4-5300326\44308b69-d64c-43c9-ab08-6d9a550b66c7.jpg" />, then Problem P is the Neumann boundary value problem (Problem N), and if<img src="4-5300326\548544df-312c-48ee-8d18-72db23397263.jpg" />, and <img src="4-5300326\1be9b2cc-9608-4f64-8c2c-15ff8f0909e9.jpg" /> on<img src="4-5300326\95bf4f66-3975-427f-8136-5465fecf2684.jpg" />, then Problem P is the regular oblique derivative problem, i.e. the third boundary value problem (Problem III or O). Now the directional derivative may be arbitrary, hence the boundary condition is very general.</p><p>The integer</p><p><img src="4-5300326\5373718e-23e7-436c-ac63-9241f181f954.jpg" /></p><p>is called the index of Problem P. When the index <img src="4-5300326\35d7e778-b985-4a2a-b8e1-23c4f54f25df.jpg" /> Problem P may not be solvable, and when <img src="4-5300326\74e340d9-7d20-47ab-97cb-b9f69ffa71a0.jpg" /> the solution of Problem P is not necessarily unique. Hence we consider the well-posedness of Problem P with modified boundary conditions.</p><p>Problem Q. Find a continuous solution <img src="4-5300326\28770b6e-437a-4f3c-996c-3619e15684a0.jpg" /> of the complex equation</p><disp-formula id="scirp.27539-formula96677"><label>(1.6)</label><graphic position="anchor" xlink:href="4-5300326\27d9cae5-cfc8-43c3-b767-242e5004af05.jpg"  xlink:type="simple"/></disp-formula><p>satisfying the boundary condition</p><disp-formula id="scirp.27539-formula96678"><label>(1.7)</label><graphic position="anchor" xlink:href="4-5300326\ae261206-32cb-45b6-8695-2509df149f99.jpg"  xlink:type="simple"/></disp-formula><p>and the relation</p><disp-formula id="scirp.27539-formula96679"><label>(1.8)</label><graphic position="anchor" xlink:href="4-5300326\468a523a-8daf-45ab-8d5e-fe6ac4c4318a.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="4-5300326\7bf70a68-e78b-4366-9094-5bde4bb7961d.jpg" /> are appropriate real constants such that the function determined by the integral in (1.8) is single-valued in<img src="4-5300326\62db8f3f-6df9-4abf-af52-6a0fca05f6a9.jpg" />, and the undetermined function <img src="4-5300326\364cbd8a-4d9e-407d-a994-d7f47c5b2f28.jpg" /> is as stated in</p><p><img src="4-5300326\04cc4bdf-3bf7-4d7e-905a-934ab5c157a1.jpg" /></p><p>in which<img src="4-5300326\b4c38fc3-2042-439f-a20c-09a6a4a2754a.jpg" />, <img src="4-5300326\11f313df-0880-4c1a-bf26-d511219b5fa5.jpg" />are unknown real constants to be determined appropriately. In addition, for <img src="4-5300326\2d029f00-2035-4a0d-9c55-a658482728f5.jpg" /> the solution <img src="4-5300326\2adaed9a-2694-4fdf-8a03-62fb71d3b61c.jpg" /> is assumed to satisfy the point conditions</p><disp-formula id="scirp.27539-formula96680"><label>(1.9)</label><graphic position="anchor" xlink:href="4-5300326\e7464ce6-a3ab-4edc-9a2d-bc88a6c1ac8f.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="4-5300326\5abb58c5-259d-44ca-ae81-a519d002fdae.jpg" /></p><p>are distinct points, and <img src="4-5300326\4c29a929-ad6c-41c4-a9c8-448e842648bd.jpg" /> are all real constants satisfying the conditions</p><disp-formula id="scirp.27539-formula96681"><label>(1.10)</label><graphic position="anchor" xlink:href="4-5300326\a1172aae-de73-4f44-b8d6-ea8abaa08b79.jpg"  xlink:type="simple"/></disp-formula><p>for a non-negative constant<img src="4-5300326\520b47f1-8ec1-4286-a942-1e740f0e6edb.jpg" />.</p></sec><sec id="s2"><title>2. Estimates of Solutions for the Poincar&#233; Boundary Value Problem</title><p>First of all, we give a prior estimate of solutions of Problem Q for (1.6).</p><p>Theorem 2.1. Suppose that Condition C holds and ε = 0 in (1.6) and (1.7). Then any solution <img src="4-5300326\93f48b82-e92e-4c60-91d1-e87de1c32680.jpg" /> of Problem Q for (1.6) satisfies the estimates</p><disp-formula id="scirp.27539-formula96682"><label>(2.1)</label><graphic position="anchor" xlink:href="4-5300326\291992a5-aa9a-4dfd-977c-826eb4c04cdb.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.27539-formula96683"><label>(2.2)</label><graphic position="anchor" xlink:href="4-5300326\e4f41ec6-4479-40ef-aa58-3ea76123dbd6.jpg"  xlink:type="simple"/></disp-formula><p>in which</p><p><img src="4-5300326\bd723c64-17e9-4cc6-af3f-caa0f1e54ec4.jpg" /></p><p><img src="4-5300326\40338d46-048a-44a2-a9c8-a55756b04158.jpg" /></p><p><img src="4-5300326\01f97ced-be92-44e2-98ed-155b23e74830.jpg" /></p><p>Proof. Noting that the solution <img src="4-5300326\13593330-c0ee-4ca0-9693-1df8654ebe9e.jpg" /> of Problem Q satisfies the equation and boundary conditions</p><disp-formula id="scirp.27539-formula96684"><label>(2.3)</label><graphic position="anchor" xlink:href="4-5300326\d6c229eb-7157-4f79-8a6d-67754984c4f0.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.27539-formula96685"><label>(2.4)</label><graphic position="anchor" xlink:href="4-5300326\ed2fd06a-fa43-4f06-8d07-30e94fcf580a.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.27539-formula96686"><label>(2.5)</label><graphic position="anchor" xlink:href="4-5300326\e0a7d8ad-c1f3-44e6-895c-96ac285f549c.jpg"  xlink:type="simple"/></disp-formula><p>according to the method in the proof of Theorem 4.3, Chapter II, [<xref ref-type="bibr" rid="scirp.27539-ref2">2</xref>] or Theorem 2.2.1, [<xref ref-type="bibr" rid="scirp.27539-ref5">5</xref>], we can derive that the solution <img src="4-5300326\cd640c75-299d-47f0-9ca5-531db31f1916.jpg" /> satisfies the estimates</p><disp-formula id="scirp.27539-formula96687"><label>(2.6)</label><graphic position="anchor" xlink:href="4-5300326\393c472f-5399-4c5b-97dc-843bd4a099e4.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.27539-formula96688"><label>(2.7)</label><graphic position="anchor" xlink:href="4-5300326\87c54357-7c3a-43a7-a383-1bcf5ad02c5d.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="4-5300326\7c9fac5b-71e2-4400-b35e-7c50809e1bd5.jpg" /></p><p>and</p><p><img src="4-5300326\c4003345-5ed2-4499-8d7a-ad61ca9407c8.jpg" /></p><p>From (1.8), it follows that</p><disp-formula id="scirp.27539-formula96689"><label>(2.8)</label><graphic position="anchor" xlink:href="4-5300326\79f84f75-64a6-4862-8bd2-b4757445f33f.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.27539-formula96690"><label>(2.9)</label><graphic position="anchor" xlink:href="4-5300326\6b724b5d-6355-4668-98df-0e6091fef122.jpg"  xlink:type="simple"/></disp-formula><p>in which <img src="4-5300326\1e6e5fc1-8184-4009-86c5-9e2be80663b6.jpg" /> is a non-negative constant. Moreover, it is easy to see that</p><disp-formula id="scirp.27539-formula96691"><label>(2.10)</label><graphic position="anchor" xlink:href="4-5300326\3495adf1-0ff5-4c94-b021-360d9e58e401.jpg"  xlink:type="simple"/></disp-formula><p>Combining (2.6)-(2.10), the estimates (2.1) and (2.2) are obtained.</p><p>Theorem 2.2. Let the Equation (1.6) satisfy Condition C and <img src="4-5300326\7638442a-03a8-41e9-9e94-a6d3b5495a74.jpg" /> in (1.6)-(1.7) be small enough. Then any solution <img src="4-5300326\ddca6d0a-4bef-4a45-8389-279a79414d5c.jpg" /> of Problem Q for (1.6) satisfies the estimates</p><disp-formula id="scirp.27539-formula96692"><label>(2.11)</label><graphic position="anchor" xlink:href="4-5300326\edd83f7a-3e32-497f-94b8-c15c34a6c416.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.27539-formula96693"><label>(2.12)</label><graphic position="anchor" xlink:href="4-5300326\4071e5cf-9bb9-4088-aad4-90c1c1ab3474.jpg"  xlink:type="simple"/></disp-formula><p>here <img src="4-5300326\83d1ff5e-3e7c-4c3d-a38a-ab74a7a2e050.jpg" /> are as stated in Theorem 2.1,</p><p><img src="4-5300326\3583ef28-2f77-4315-9a33-4a6d7ec4ef45.jpg" /></p><p>Proof. It is easy to see that <img src="4-5300326\dc15212a-918e-4d37-a09a-424b0836b38b.jpg" /> satisfies the equation and boundary conditions</p><disp-formula id="scirp.27539-formula96694"><label>(2.13)</label><graphic position="anchor" xlink:href="4-5300326\a035bbcd-ac37-4afe-b3b2-8f3f677b3c00.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.27539-formula96695"><label>(2.14)</label><graphic position="anchor" xlink:href="4-5300326\3b1e492f-5b8c-4fb5-98d5-e4eab65c4471.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.27539-formula96696"><label>(2.15)</label><graphic position="anchor" xlink:href="4-5300326\8987d7f5-f592-4953-9437-14b67e75f7a6.jpg"  xlink:type="simple"/></disp-formula><p>Moreover from (2.6) and (2.7), we have</p><disp-formula id="scirp.27539-formula96697"><label>(2.16)</label><graphic position="anchor" xlink:href="4-5300326\67254560-077b-4ef5-a151-49f0dbeffe22.jpg"  xlink:type="simple"/></disp-formula><p>and from (2.8)-(2.10), it follows that</p><disp-formula id="scirp.27539-formula96698"><label>(2.17)</label><graphic position="anchor" xlink:href="4-5300326\ea70b668-1b9d-4b7a-a562-8d93a753c0b0.jpg"  xlink:type="simple"/></disp-formula><p>If the positive constant <img src="4-5300326\a682fe55-744e-479e-843f-41ff3f8bd5af.jpg" /> is small enough such that<img src="4-5300326\c22444f3-9bfa-4df3-ad9d-725d4bf11950.jpg" />, then the first inequality in (2.17) implies that</p><disp-formula id="scirp.27539-formula96699"><label>(2.18)</label><graphic position="anchor" xlink:href="4-5300326\1de78dbe-0490-43e3-a157-79256d14bcd2.jpg"  xlink:type="simple"/></disp-formula><p>Combining (2.8) and (2.18), we obtain</p><disp-formula id="scirp.27539-formula96700"><label>(2.19)</label><graphic position="anchor" xlink:href="4-5300326\0cecfc36-6678-4ee1-afc4-04b8ecd6712b.jpg"  xlink:type="simple"/></disp-formula><p>which is the estimate (2.11). As for (2.12), it is easily derived from (2.9) and the second inequality in (2.17), i.e.</p><disp-formula id="scirp.27539-formula96701"><label>(2.20)</label><graphic position="anchor" xlink:href="4-5300326\8f489e0d-0e67-4944-82f6-c5e7a640cc1f.jpg"  xlink:type="simple"/></disp-formula></sec><sec id="s3"><title>3. Solvability Results of the Poincar&#233; Boundary Value Problem</title><p>We first prove a lemma.</p><p>Lemma 3.1. If <img src="4-5300326\4bbe0065-4fdf-44cf-b085-6bfade6a50b3.jpg" /> satisfies the condition stated in Condition C, then the nonlinear mapping G:</p><p><img src="4-5300326\df52c119-9bcc-4600-865a-68b2d239fdd0.jpg" /></p><p>defined by <img src="4-5300326\d41d7a54-7599-4acc-a8b7-db5d503ebb1c.jpg" /> is continuous and bounded</p><disp-formula id="scirp.27539-formula96702"><label>(3.1)</label><graphic position="anchor" xlink:href="4-5300326\b4affbd8-c4f1-4f4d-b4b1-116f09db4c76.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="4-5300326\3982da87-a5f5-4ef6-96a4-075d380a6dc9.jpg" /></p><p>Proof. In order to prove that the mapping<img src="4-5300326\e9ef16ba-296b-4f05-8b94-a0f18854147b.jpg" />:</p><p><img src="4-5300326\570b4e34-442b-49b3-b044-a60d636c3a9d.jpg" /></p><p>Defined by <img src="4-5300326\75470969-da4b-41d7-9350-2f77277e09a2.jpg" /> is continuous, we choose any sequence of functions <img src="4-5300326\2905cedb-6d7c-4f55-92e8-aa38e336c552.jpg" /></p><p><img src="4-5300326\c9c62c14-3a2a-4611-9d52-60abb1b2c3ae.jpg" /></p><p>such that</p><p><img src="4-5300326\fdc0fc48-9102-47da-9df1-13e06872172b.jpg" /></p><p>as <img src="4-5300326\7527e25f-2006-4723-8493-831d7736a6bc.jpg" /> Similarly to Lemma 2.2.1, [<xref ref-type="bibr" rid="scirp.27539-ref5">5</xref>], we can prove that</p><p><img src="4-5300326\50e16818-f53f-4e56-be00-fcc17467c41d.jpg" /></p><p>possesses the property</p><disp-formula id="scirp.27539-formula96703"><label>(3.2)</label><graphic position="anchor" xlink:href="4-5300326\350f4c11-c982-4d74-8681-bd0e115896ca.jpg"  xlink:type="simple"/></disp-formula><p>And the inequality (3.1) is obviously true.</p><p>Theorem 3.2. Let the complex Equation (1.1) satisfy Condition C, and the positive constant <img src="4-5300326\5c2d7467-88c2-4261-a3aa-2578465a2410.jpg" /> in (1.6) and (1.7) is small enough.</p><p>1) When<img src="4-5300326\9d97959d-f33d-4531-9040-f685b44fbe3b.jpg" />, <img src="4-5300326\7b032919-7c6c-44d4-ba4d-9363be2c122e.jpg" />, Problem Q for (1.6) has a solution<img src="4-5300326\fcac7d7b-8b14-449e-bfe3-59b4753dbe40.jpg" />, where<img src="4-5300326\5596958b-8410-46cd-a92b-ea18646ea0ac.jpg" />, <img src="4-5300326\00093a8a-c6ff-44c1-b146-99ec283c623a.jpg" />, <img src="4-5300326\8b51c3d2-e075-4940-984e-0460abaf4220.jpg" />is a constant as stated before.</p><p>2) When <img src="4-5300326\8bc96578-34a4-4bd5-af2c-794a2ba7a7c6.jpg" /> Problem Q for (1.6) has a solution<img src="4-5300326\144d0db4-424a-42ae-80bb-a42203721896.jpg" />, where <img src="4-5300326\c36f3533-c449-4e46-947d-ef1d03f80266.jpg" /> provided that</p><disp-formula id="scirp.27539-formula96704"><label>(3.3)</label><graphic position="anchor" xlink:href="4-5300326\f391e09c-6126-411e-a78c-fcca7b8b0415.jpg"  xlink:type="simple"/></disp-formula><p>is sufficiently small.</p><p>3) If <img src="4-5300326\57815a0e-786d-4007-bbcd-6c4fb35035d3.jpg" /> satisfy the conditions,&#160; i.e. Condition C and for any functions <img src="4-5300326\f5c82658-a36d-42af-a9c3-7d511a68a99f.jpg" /></p><p><img src="4-5300326\493a5c8e-1ef0-49cf-a7d5-dd1ffd5c8e99.jpg" />and<img src="4-5300326\c8e6efa7-4110-488f-8c30-7c2097902694.jpg" />, there are</p><disp-formula id="scirp.27539-formula96705"><label>(3.4)</label><graphic position="anchor" xlink:href="4-5300326\af42f677-0d56-41c7-988e-97f63b8e75b9.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="4-5300326\6e0a465e-5938-4e4f-b117-bd6e48f6fc94.jpg" /></p><p><img src="4-5300326\15cd0a09-8171-403a-9955-16fa3151e375.jpg" />is a sufficiently small positive constant, then the above solution of Problem Q is unique.</p><p>Proof. 1) In this case, the algebraic equation for t is as follows</p><disp-formula id="scirp.27539-formula96706"><label>(3.5)</label><graphic position="anchor" xlink:href="4-5300326\d20dd9cc-b741-415f-a534-a6aac341afce.jpg"  xlink:type="simple"/></disp-formula><p>where M<sub>6</sub>, M<sub>7</sub> are constants as stated in (2.11) and (2.12). Because<img src="4-5300326\c764ae58-4893-44fd-b911-eb76a5cea23e.jpg" />, <img src="4-5300326\d872bcdc-3e52-47fe-b6b6-46b7aa71dca1.jpg" />, the Equation (3.5) has a unique solution <img src="4-5300326\699d26d8-edf2-4e69-a779-7978db2f400e.jpg" /> Now we introduce a bounded, closed and convex subset B<sup>*</sup> of the Banach space <img src="4-5300326\616fd63b-13d4-44cb-92af-4b8d4a0768ce.jpg" /> <img src="4-5300326\72768a56-79d4-411d-91f9-6f09d4d794b4.jpg" /> whose elements are of the form <img src="4-5300326\f2e2aceb-28ac-4d43-9433-16a6a73f10fa.jpg" /> satisfying the condition</p><disp-formula id="scirp.27539-formula96707"><label>(3.6)</label><graphic position="anchor" xlink:href="4-5300326\4f4801c2-e80a-4673-a0ce-ce3c140be2e5.jpg"  xlink:type="simple"/></disp-formula><p>We choose a pair of functions <img src="4-5300326\2e427c8d-0996-4cef-a672-be1ea1c03def.jpg" /> and substitute it into the appropriate positions of</p><p><img src="4-5300326\daf6e142-93f5-4cbe-a5c9-4297e143681b.jpg" />, <img src="4-5300326\9553e60a-b182-40ff-995d-f845d61eb8d9.jpg" />in (1.6) and the boundary condition (1.7), and obtain</p><disp-formula id="scirp.27539-formula96708"><label>(3.7)</label><graphic position="anchor" xlink:href="4-5300326\46a07534-6a02-4bc6-8200-fa47405d7b9a.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.27539-formula96709"><label>(3.8)</label><graphic position="anchor" xlink:href="4-5300326\abf980cc-c858-48f5-a965-3a95652245f8.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="4-5300326\a31f1272-27be-406e-9ffe-743b08b224b3.jpg" /></p><p>In accordance with the method in the proof of Theorem 1.2.5, [<xref ref-type="bibr" rid="scirp.27539-ref5">5</xref>], we can prove that the boundary value problem (3.7), (3.8) and (1.6) has a unique solution<img src="4-5300326\e6b07b59-49da-4a3c-890d-d40def2441b1.jpg" />. Denote by <img src="4-5300326\3b064418-200b-4316-af3a-1046af763340.jpg" /> the mapping from <img src="4-5300326\c677c41d-dad2-4588-97d2-6557b89fe614.jpg" /> to<img src="4-5300326\2b1f929a-6fec-4d2b-a1d6-ffa3c7cb1ae4.jpg" />. Noting that</p><p><img src="4-5300326\6b7f18dd-211e-455f-b15b-c9d6238560b7.jpg" /></p><p>provided that the positive number <img src="4-5300326\99563a99-fb17-4e01-b330-8af8006702fd.jpg" /> is sufficiently small, and noting that the coefficients of complex Equation (3.7) satisfy the same conditions as in Condition C, from Theorem 2.2, we can obtain</p><disp-formula id="scirp.27539-formula96710"><label>(3.9)</label><graphic position="anchor" xlink:href="4-5300326\71dc975e-aa7d-4245-b0e2-bb6a29df833b.jpg"  xlink:type="simple"/></disp-formula><p>This shows that T maps B<sup>*</sup> onto a compact subset in B<sup>*</sup>. Next, we verify that T in B<sup>*</sup> is a continuous operator. In fact, we arbitrarily select a sequence <img src="4-5300326\24a516f4-3c5b-49f5-86dc-48a7c1b31853.jpg" /> in B<sup>*</sup>, such that</p><disp-formula id="scirp.27539-formula96711"><label>(3.10)</label><graphic position="anchor" xlink:href="4-5300326\8233c481-cbf8-4b92-812c-7107d3fa11e5.jpg"  xlink:type="simple"/></disp-formula><p>By Lemma 3.1, we can see that</p><disp-formula id="scirp.27539-formula96712"><label>(3.11)</label><graphic position="anchor" xlink:href="4-5300326\9a91071c-e0d9-46b3-92c4-0585ff770290.jpg"  xlink:type="simple"/></disp-formula><p>Moreover, from</p><p><img src="4-5300326\79e2d1ff-e340-411e-91f3-7dd09fcfd957.jpg" />,</p><p><img src="4-5300326\df5f4b1a-e75c-47ed-b621-866cedc890d8.jpg" />it is clear that <img src="4-5300326\e976b6c4-3d3d-47a6-9896-41315c59a1b3.jpg" /> is a solution of Problem Q for the following equation</p><disp-formula id="scirp.27539-formula96713"><label>(3.12)</label><graphic position="anchor" xlink:href="4-5300326\8d1281c7-7577-4717-8a4e-b017e3c1871d.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.27539-formula96714"><label>(3.13)</label><graphic position="anchor" xlink:href="4-5300326\2d17f4ce-da8d-4385-bc32-2f67286b2f4b.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.27539-formula96715"><label>(3.14)</label><graphic position="anchor" xlink:href="4-5300326\3933e011-f095-419d-a837-b57ea03d5505.jpg"  xlink:type="simple"/></disp-formula><p>In accordance with the method in proof of Theorem 2.2, we can obtain the estimate</p><disp-formula id="scirp.27539-formula96716"><label>(3.15)</label><graphic position="anchor" xlink:href="4-5300326\5c62b319-c392-43f8-92d9-7fb8f43a52c1.jpg"  xlink:type="simple"/></disp-formula><p>in which <img src="4-5300326\d2c2e342-9795-4df1-8020-5faf15518a3c.jpg" /> From (3.10), (3.11) and the above estimate, we obtain</p><p><img src="4-5300326\af70f364-6a33-417f-8775-0fe81d455ae5.jpg" />as <img src="4-5300326\2e61d63f-546d-4035-921d-6aaa960b7918.jpg" /></p><p>On the basis of the Schauder fixed-point theorem, there exists a function <img src="4-5300326\67739b4d-79e6-40a0-8ddc-622982667c6d.jpg" /> such that<img src="4-5300326\e43035ff-6f45-4cd3-adce-972ef6b39f9a.jpg" />, and from Theorem 2.2, it is easy to see that<img src="4-5300326\039255fb-cd75-4471-8513-797f4e5414a7.jpg" />, <img src="4-5300326\10688554-2704-457f-9e73-7890f1b4c2b8.jpg" />, and</p><p><img src="4-5300326\8955ecea-514b-41ed-95ad-5d908f4826a3.jpg" />is a solution of Problem Q for the Equation (1.6) and the relation (1.8) with the condition<img src="4-5300326\20096fa8-5d48-4770-bb86-231168bc9ec5.jpg" />,<img src="4-5300326\e6a3e91c-8e06-432a-9ded-69598810e81a.jpg" />.</p><p>In addition, if <img src="4-5300326\4e50c803-3cb2-47cc-a392-e42097e1137b.jpg" /> in<img src="4-5300326\5308c89a-2466-4eb7-acf5-81925aa6d8fa.jpg" />where <img src="4-5300326\e0820d5f-9f9e-41a0-b6c4-8d0e9f8cbb2e.jpg" /> then the above solvability result still hold by using the above similar method.</p><p>2) Secondly, we discuss the case: <img src="4-5300326\a7e3456f-d56e-4bda-a0f7-d5e263834486.jpg" />In this case, (3.5) has the solution <img src="4-5300326\58c15429-b817-494b-a7e4-bf08ca5ab950.jpg" /> provided that M<sub>9</sub> in (3.3) is small enough. Now we consider a closed and convex subset <img src="4-5300326\184ee11c-f6f0-4816-acc5-bb6ab39bee53.jpg" /> in the Banach space <img src="4-5300326\25294d72-bfd8-4001-b9a2-0b525e37ef1f.jpg" /> i.e.</p><disp-formula id="scirp.27539-formula96717"><label>(3.16)</label><graphic position="anchor" xlink:href="4-5300326\389dfe30-db3e-4682-b4db-a7b6e289388f.jpg"  xlink:type="simple"/></disp-formula><p>Applying a method similar as before, we can verify that there exists a solution</p><p><img src="4-5300326\4fbb9251-cbf2-48b7-bbf1-f29bb4a0c281.jpg" /></p><p>of Problem Q for (1.6) with the condition <img src="4-5300326\fb1d9a4f-24ad-4c7e-a74e-b97c70a52af0.jpg" /></p><p>Moreover, if <img src="4-5300326\0fd26d15-2198-462b-b8b3-3feb2a628a41.jpg" /> in D, where</p><p><img src="4-5300326\cf6f7700-56a8-4414-8c4b-cd9c20ce8924.jpg" />, <img src="4-5300326\2c067b71-d96d-4e84-846d-e2e60955eca1.jpg" />, j = 1, 2. Under the same condition, we can derive the above solvability result by the similar method.</p><p>3) When <img src="4-5300326\7de01d4c-435b-47b4-a589-0d619457c5c2.jpg" /> satisfies the condition (3.4), we can verify the uniqueness of solutions in this theorem. In fact, if<img src="4-5300326\a3e4e78a-f569-4faf-9e37-27a076375e00.jpg" />, <img src="4-5300326\a45ded0e-3982-4a65-b46a-693c67b0c10c.jpg" />are two solutions of Problem Q for the Equation (1.6), then</p><p><img src="4-5300326\e483aa12-f07e-4405-b2ae-2ffe5be94593.jpg" /></p><p>satisfies the equation and boundary conditions</p><disp-formula id="scirp.27539-formula96718"><label>(3.17)</label><graphic position="anchor" xlink:href="4-5300326\5f34b838-7dde-4fcc-89f5-3d353bda79e2.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.27539-formula96719"><label>(3.18)</label><graphic position="anchor" xlink:href="4-5300326\6c8bffb1-d210-4599-846d-3a5f593249cb.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.27539-formula96720"><label>(3.19)</label><graphic position="anchor" xlink:href="4-5300326\1c71c9e8-50d2-4002-8295-ce190fe12ceb.jpg"  xlink:type="simple"/></disp-formula><p>in which<img src="4-5300326\7576ded4-9d68-4a22-a7af-e224833fd1d6.jpg" />. Similarly to Theorem 2.2, we can derive the following estimates of the solution <img src="4-5300326\f50349ce-17e0-44fc-b3e0-7453ed31d44a.jpg" /> for complex Equation (3.17):</p><disp-formula id="scirp.27539-formula96721"><label>(3.20)</label><graphic position="anchor" xlink:href="4-5300326\26d6ef4e-71e2-41f1-938f-9da2daec8533.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.27539-formula96722"><label>(3.21)</label><graphic position="anchor" xlink:href="4-5300326\5a3e7bdc-110c-4120-9188-af3b40639f34.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="4-5300326\25d12068-b37c-4f73-93ef-932be1aad70c.jpg" /></p><p><img src="4-5300326\0ef70ca7-c55a-474f-8a1c-7b6d55d6bead.jpg" /></p><p>are two non-negative constants, <img src="4-5300326\375d54cf-ac24-4849-be0a-749062fdd64f.jpg" />Moreover the estimate</p><disp-formula id="scirp.27539-formula96723"><label>(3.22)</label><graphic position="anchor" xlink:href="4-5300326\7654c7c2-af5e-4029-90d0-ee16516350f5.jpg"  xlink:type="simple"/></disp-formula><p>can be derived. Provided that the positive constant <img src="4-5300326\02ca9b12-759c-4ff4-9e31-984ec7da6a32.jpg" /> is small enough such that<img src="4-5300326\81073a9c-02e9-4a5a-9180-8339fa73fcf4.jpg" />, from (3.22) it follows<img src="4-5300326\995a91d8-9310-49db-a258-0f618c394279.jpg" />, i.e. <img src="4-5300326\9414ff00-7b72-47b9-bf10-068220332faf.jpg" />in D. This completes the proof of the theorem.</p><p>From the above theorem, the next result can be derived.</p><p>Theorem 3.3. Under the same conditions as in Theorem 3.2, the following statements hold.</p><p>1) When the index K &gt; N, Problem P for (1.1) has N solvability conditions, and the solution of Problem P depends on <img src="4-5300326\e0fbc6bf-7db3-42c0-895d-649a9ef0ca60.jpg" /> arbitrary real constants.</p><p>2) When <img src="4-5300326\df15dcb8-db9b-488b-9981-20d646eba35d.jpg" /> Problem P for (1.1) is solvable, if <img src="4-5300326\f08d2f77-0f41-45c6-9a78-80f0c33b5248.jpg" /> solvability conditions are satisfied, and the solution of Problem P depends on <img src="4-5300326\d38e05a4-4df3-4e49-90c5-bc40ca88d1f3.jpg" /> arbitrary real constants.</p><p>3) When K &lt; 0, Problem P for (1.1) is solvable under <img src="4-5300326\f219c60c-1d0a-4083-95e4-bda02e88633a.jpg" /> conditions, and the solution of Problem P depends on 1 arbitrary real constant.</p><p>Moreover, we can write down the solvability conditions of Problem P for all other cases.</p><p>Proof. Let the solution <img src="4-5300326\94424c38-d5c0-4a4b-b1dc-2164f735c35e.jpg" /> of Problem Q for (1.6) be substituted into the boundary condition (1.7) and the relation (1.8). If the function<img src="4-5300326\465c9632-a2a1-450a-80c9-c125b5b5f5db.jpg" />, i.e.</p><p><img src="4-5300326\a9e95a4d-0967-48cf-97ae-fcd9c4f24d73.jpg" /></p><p>and<img src="4-5300326\c0ca8c34-0dff-42ab-a511-d2d407f617f8.jpg" />, <img src="4-5300326\1c4f6dc2-5970-438e-8573-f10302e87ec4.jpg" />, then we have <img src="4-5300326\99f29cca-df6d-4ef0-b8b9-d6df6108c8f6.jpg" /> in D and the function <img src="4-5300326\0b0f08f2-c3e8-4efd-b013-d1a9aff773bc.jpg" /> is just a solution of Problem P for (1.1). Hence the total number of above equalities is just the number of solvability conditions as stated in this theorem. Also note that the real constants b<sub>0</sub> in (1.8) and <img src="4-5300326\25ee1a8d-81de-4d9d-8502-0a7d59315bd1.jpg" /> in (1.9) are arbitrarily chosen. 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