<?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.2012.26053</article-id><article-id pub-id-type="publisher-id">APM-24363</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>
 
 
  Some Symmetry Results for the A-Laplacian Equation via the Moving Planes Method
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>hongbo</surname><given-names>Fang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Anna</surname><given-names>Wang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>School of Mathematical Sciences, Ocean University of China, Qingdao, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>fangzb7777@hotmail.com(HF)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>09</day><month>11</month><year>2012</year></pub-date><volume>02</volume><issue>06</issue><fpage>363</fpage><lpage>366</lpage><history><date date-type="received"><day>July</day>	<month>3,</month>	<year>2012</year></date><date date-type="rev-recd"><day>September</day>	<month>1,</month>	<year>2012</year>	</date><date date-type="accepted"><day>September</day>	<month>8,</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 this paper, we are concerned with a positive solution of the non-homogeneous A-Laplacian equation in an open bounded connected domain. We use moving planes method to prove that the domain is a ball and the solution is radially symmetric.
 
</p></abstract><kwd-group><kwd>Symmetry; A-Laplacian; Moving Planes Method; Overdetermined Boundary Value Problem</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In this paper, we are going to study the symmetry results for the overdetermined problem</p><disp-formula id="scirp.24363-formula7744"><label>(1.1)</label><graphic position="anchor" xlink:href="1-5300169\8c32fa41-0f00-49ba-a123-f01db695e890.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24363-formula7745"><label>(1.2)</label><graphic position="anchor" xlink:href="1-5300169\f4791309-5ecc-4c19-8e1d-4f516bbff1eb.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24363-formula7746"><label>(1.3)</label><graphic position="anchor" xlink:href="1-5300169\7c96e053-aa52-4144-a0a6-d89e4b4fc28f.jpg"  xlink:type="simple"/></disp-formula><p>Here <img src="1-5300169\e836baa1-720c-43e8-a105-4735914bb8a6.jpg" /> is a bounded connected open subset of <img src="1-5300169\df7ca9ab-eff7-48a0-942d-cfde71f374c5.jpg" /> with <img src="1-5300169\d3f50099-0387-488d-880b-ce0f8dc3ea1e.jpg" /> boundary and <img src="1-5300169\b0e45999-e836-442f-9aa8-12130e76561e.jpg" /> is a point in<img src="1-5300169\c57ff67d-a380-4b33-a243-cd17b90c1746.jpg" />. The function <img src="1-5300169\b15b1a77-e571-4ace-9fe8-cd4678dd344c.jpg" /> satisfies the regularity requirement</p><disp-formula id="scirp.24363-formula7747"><label>(1.4)</label><graphic position="anchor" xlink:href="1-5300169\8a4252ea-5384-422b-9eb3-3a046b990926.jpg"  xlink:type="simple"/></disp-formula><p>and the (possibly degenerate) elliptic condition</p><disp-formula id="scirp.24363-formula7748"><label>(1.5)</label><graphic position="anchor" xlink:href="1-5300169\4f246aa5-6eaa-4387-b93c-d7ee3ac80534.jpg"  xlink:type="simple"/></disp-formula><p><img src="1-5300169\ca2ab413-7638-4dd3-ab28-530f2bbcb4b8.jpg" />is a continuously differentiable function. <img src="1-5300169\81271341-176d-40df-b62f-860fce3a4187.jpg" />is a constant and <img src="1-5300169\e1a0919d-fa8f-4329-bc2e-af2c69deecbc.jpg" /> denotes the inner normal to<img src="1-5300169\a9d2bdda-6cec-44f0-b13a-959ca4e45c3e.jpg" />.</p><p>J. Serrin proved the radial symmetry for positive solutions of the equation <img src="1-5300169\a778334f-0ee4-405d-b912-01d2e1c6e418.jpg" /> in <img src="1-5300169\21fac8b3-bb7a-44b4-919f-8c086ab5401c.jpg" /> with the same overdetermined boundary conditions as the above problem, see [<xref ref-type="bibr" rid="scirp.24363-ref1">1</xref>]. N. Garofalo and J. Lewis extended Serrin’s result to a larger class of elliptic equations possibly degenerate, including the following p-Laplacian equation</p><p><img src="1-5300169\bfaf7d87-01d8-4b1c-9ebc-6a379ea0e96c.jpg" />with the same boundary conditionssee [<xref ref-type="bibr" rid="scirp.24363-ref2">2</xref>]. For the overdetermined elliptic boundary value problem <img src="1-5300169\fe24d339-d414-4cee-b0ca-9e90f772b129.jpg" /> in <img src="1-5300169\6fd6f54d-7545-45a4-8c58-ac00790cc2aa.jpg" />with the same overdetermined boundary conditions as above, I. Fragala, I. F. Gazzaola and B. Kawohl used the geometric approach which relies on a maximum principle for a suitable Pfunction, combined with some geometric arguments involving the mean curvature of <img src="1-5300169\19a45161-b79c-40a5-af07-32a598686281.jpg" /> to prove that if the above problem admits a solution in a suitable weak sense, then <img src="1-5300169\6de53f41-8975-464f-bfcd-79f989beb907.jpg" /> is a ball, see [<xref ref-type="bibr" rid="scirp.24363-ref3">3</xref>]. A. Farina and B. Kawohl obtained the same result under removing the strong ellipticity assumption in [<xref ref-type="bibr" rid="scirp.24363-ref4">4</xref>] and a growth assumption in [<xref ref-type="bibr" rid="scirp.24363-ref2">2</xref>] on the diffusion coefficient A, as well as a starshapedness assumption on <img src="1-5300169\eb97b0f0-e56b-4892-9aa6-08c40f0b4951.jpg" /> in [<xref ref-type="bibr" rid="scirp.24363-ref3">3</xref>], see [<xref ref-type="bibr" rid="scirp.24363-ref5">5</xref>]. A. Firenze considered the positive solution of problem (1.1)-(1.3) when it is a p-Laplacian equation in an open bounded connected subset <img src="1-5300169\72be0fb3-2b11-4145-b27b-d187b7aa74ba.jpg" /> of <img src="1-5300169\75c003c1-8fee-4137-ab3b-94828ae8e514.jpg" />with <img src="1-5300169\73c15677-a365-47bd-be97-64e3dbf87b2a.jpg" /> boundary, see [<xref ref-type="bibr" rid="scirp.24363-ref6">6</xref>]. All of the above motivated us to extend the symmetry result to the non-homogeneous A-Laplacian equation.</p><p>Our main result is that for the problem (1.1)-(1.3), if u has only one critical point in<img src="1-5300169\3225ade7-5623-4aea-b471-493413eab24d.jpg" />, then <img src="1-5300169\902f917d-9398-4787-a68e-9cf62ad41858.jpg" /> is a ball and u is radially symmetric.</p><p>Section 2 of this paper is devoted to the main result and a more general version of this theorem. In Section 3, we will present the proof of the main theorem.</p><p>Some components, such as multi-leveled equations, graphics, and tables are not prescribed, although the various table text styles are provided. The formatter will need to create these components, incorporating the applicable criteria that follow.</p></sec><sec id="s2"><title>2. Preliminaries and Statement of Results</title><p>In this section we give some lemma that we shall use and present our main result.</p><p>Lemma 2.1. (The boundary lemma at corner) (Lemma 2 in [<xref ref-type="bibr" rid="scirp.24363-ref1">1</xref>]) Let <img src="1-5300169\287bd314-2fe4-4556-9296-509dec194734.jpg" /> be a domain with C<sup>2</sup> boundary and <img src="1-5300169\50275bf0-f799-427b-8002-1bb9508737bb.jpg" /> be a hyperplane containing the normal to <img src="1-5300169\2df743fe-9319-41ba-b3f8-ea33d279ae8a.jpg" /> at some point<img src="1-5300169\05982d38-7777-402a-b15d-3ad24a1ffdbe.jpg" />. Let <img src="1-5300169\2b344e0e-2756-4ffc-9660-95e622d150ba.jpg" /> denote the portion of <img src="1-5300169\dcc5d835-b59f-457b-aaca-891f343f0092.jpg" /> lying on some particular side of<img src="1-5300169\f4919a18-d87a-4f7a-8215-2514ad5f8065.jpg" />.</p><p>Suppose that<img src="1-5300169\24525d4e-b7a5-411f-85b2-d022569f1bb2.jpg" /> is of class <img src="1-5300169\f45f3103-ac0e-42d5-bdec-4db0656d5512.jpg" /> in the closure of <img src="1-5300169\b7e8373f-6440-4f5c-a777-1216176aa1b0.jpg" /> and satisfies the elliptic inequality</p><p><img src="1-5300169\579265dc-4017-47fd-bded-68144dae924b.jpg" />, <img src="1-5300169\63105374-f331-4563-a6c4-bb45c35696c2.jpg" /></p><p>where the coefficients are uniformly bounded. We assume that the matrix <img src="1-5300169\e9a93770-1d80-49cd-9add-d6b6e01ede0b.jpg" /> is uniformly definite</p><p><img src="1-5300169\b375efa4-0dc1-465f-9ef3-853a9eb24625.jpg" />, <img src="1-5300169\76040187-bccc-4dbc-b7a2-d09733a4a2f1.jpg" />and that</p><p><img src="1-5300169\212d3b4c-88dd-4ddf-83c3-5e0afa394e0f.jpg" />, <img src="1-5300169\eaed05d0-1b08-415f-a82c-f6d74d422c35.jpg" />where <img src="1-5300169\c78e8205-d2ce-4dae-a322-2995cf6ed7f7.jpg" /> is an arbitrary real vector, <img src="1-5300169\6b9d8fee-990b-4a23-bea5-c280f4194971.jpg" />is the unit normal to the plane<img src="1-5300169\4afc03ec-0aa8-4034-9e0c-5bd30a82db97.jpg" />, and <img src="1-5300169\c23c688e-0a7e-4b69-ba10-4fa7b71dd78d.jpg" /> is the distance from<img src="1-5300169\d8b82948-667e-419c-814d-baf846ea0a9f.jpg" />. Suppose also <img src="1-5300169\518049df-d400-4c67-bdd2-87a4771c214e.jpg" /> in <img src="1-5300169\890b6894-a8dd-4270-b050-2ae83633f9fd.jpg" /> and <img src="1-5300169\f6287aa6-5d25-438c-a35e-dce978528f4d.jpg" /> at<img src="1-5300169\16027f8a-6f04-4465-915b-1891a77c0b6e.jpg" />. Let <img src="1-5300169\a557c89b-9533-44c7-879d-1cab77882237.jpg" /> be any direction at <img src="1-5300169\aa56f182-c4dd-4fa2-af69-ec67ab62e96d.jpg" /> which enters <img src="1-5300169\a0025c7a-a9ba-46cc-9428-d83eb0e92ec5.jpg" />nontangentially. Then</p><p><img src="1-5300169\4a02c9bb-8919-4c8c-99c5-58b140c82972.jpg" />or <img src="1-5300169\dca032df-4c96-43b8-abc5-8261f868010c.jpg" /> at<img src="1-5300169\6ec5c301-31e4-414f-80d3-65b9830a8b00.jpg" />unless<img src="1-5300169\af43085a-56bc-4146-802d-725fe981e64f.jpg" />.</p><p>Our main results are as follows:</p><p>Theorem 2.2. Let <img src="1-5300169\b4dc7f83-42b9-48d6-b1c4-3d230429213f.jpg" /> be a bounded connected open subset of <img src="1-5300169\c5e06612-8def-4a80-b068-0a76b0a1eb13.jpg" />with <img src="1-5300169\fbcec2fe-2713-4ca3-85fd-ea68d946c730.jpg" />boundary and let <img src="1-5300169\e10477d6-fd08-4189-b0c9-6c7c2d23ff3e.jpg" /> be a point in</p><p><img src="1-5300169\a804cd6b-32b4-4758-b3f6-37966b92da82.jpg" />. Let<img src="1-5300169\dc1100c5-6a9a-420f-af8e-5dd16e30769b.jpg" />, <img src="1-5300169\2e4916d1-c2fe-4166-b13a-44972199e4d0.jpg" />, be a strictly positive solution of the following overdetermined boundary value problem</p><disp-formula id="scirp.24363-formula7749"><label>(2.1)</label><graphic position="anchor" xlink:href="1-5300169\262069ef-7042-4355-8f3a-5f8fbb230291.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24363-formula7750"><label>(2.2)</label><graphic position="anchor" xlink:href="1-5300169\29900c8c-6bec-44a4-9cd1-209597b5c886.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.24363-formula7751"><label>(2.3)</label><graphic position="anchor" xlink:href="1-5300169\03f95eb7-7c89-4e56-8389-dde0c3c0ad1d.jpg"  xlink:type="simple"/></disp-formula><p>Here <img src="1-5300169\ae8ea848-bba3-4ab3-918f-db13663a6006.jpg" /> is a continuously differentiable function, <img src="1-5300169\2575acde-f034-496f-b70f-070a0bfd03b4.jpg" />and</p><disp-formula id="scirp.24363-formula7752"><label>. (2.4)</label><graphic position="anchor" xlink:href="1-5300169\70cc7ef2-0d90-4941-a2c1-f9c9c46cba9d.jpg"  xlink:type="simple"/></disp-formula><p>c is a constant and <img src="1-5300169\7d852218-81cd-4861-af5f-0c760b606a66.jpg" /> denotes the inner normal to<img src="1-5300169\c5d2a0bf-4d8c-4ecd-94c4-3ed10acebed7.jpg" />. Assume</p><disp-formula id="scirp.24363-formula7753"><label>(2.5)</label><graphic position="anchor" xlink:href="1-5300169\0dc6350a-8481-4939-a120-b6055c484435.jpg"  xlink:type="simple"/></disp-formula><p>then <img src="1-5300169\46ac49f0-9fbe-4dd3-b09e-2e5ef8d67fb3.jpg" /> is a ball and <img src="1-5300169\7c28fde8-e1e0-4200-873b-af49e4f44cdc.jpg" /> is radially symmetric.</p><p>The following remark is a general version of the theorem. It can be viewed as an extension result of p-Laplacian too. As the proof is similar to Theorem 2.2, we omit it.</p><p>Remark 2.3. Let <img src="1-5300169\15e0e270-f1b4-4aad-9a8d-1b9d0318bec0.jpg" /> be as in Theorem 2.2 and D be a subset of<img src="1-5300169\803839f0-c35b-471e-b88f-517dd41805fc.jpg" />. Let <img src="1-5300169\7d127e3a-b60d-4261-a689-b54fbe398381.jpg" /> be a strictly positive solution of Equation (2.1) in <img src="1-5300169\e09a08e7-33ee-4c2a-9e7a-4ed9b050e54a.jpg" />and verify the boundary conditions; Assume that <img src="1-5300169\427803ce-133a-4e61-b2f6-3e93f14f7242.jpg" /> is the critical set of<img src="1-5300169\be3ba4ac-2929-4e85-b6b8-d26c1b37cee0.jpg" />, then if <img src="1-5300169\113e5a05-c1b4-430d-8d6d-5b0bbfe9ad5e.jpg" /> denotes the convex hull of<img src="1-5300169\d56b2a46-a513-49b3-8b54-45caed90a6cd.jpg" />1) the normal line to <img src="1-5300169\4d60f814-f56e-4c41-956f-09e43c289756.jpg" /> at an arbitrary point of <img src="1-5300169\24e6bb1c-805a-422f-9656-5962573b00aa.jpg" /> intersects<img src="1-5300169\45cbfe5f-01de-4c3b-b4c4-7ab09a44d23a.jpg" />;</p><p>2) if <img src="1-5300169\435a31e1-9e3b-4a53-afd9-bc772b0a9e56.jpg" /> is a support plane to <img src="1-5300169\b282fc73-65f2-4ba2-873e-9271be256230.jpg" /> through <img src="1-5300169\71b082cd-d2bd-4f43-89c1-838e4e3cf304.jpg" /> and <img src="1-5300169\90296018-45dc-4b1a-83da-56831269047e.jpg" /> is a ray from A orthogonal to <img src="1-5300169\e4dcab0e-8176-4b20-8fc1-70e2e2dba962.jpg" /> which lies in the half-space determined by <img src="1-5300169\2200c7d3-95d9-4604-9afd-c2cdfb09a9c0.jpg" />not containing<img src="1-5300169\38e428ea-15bd-4366-86f2-ed2afb230718.jpg" />, then <img src="1-5300169\7374d7fb-160a-4e9e-86f5-ed11a40c0d49.jpg" /> intersects <img src="1-5300169\2843cf23-f1ff-4e5f-84c7-f540ec6754fe.jpg" /> exactly in one point.</p><p>In what follows we assume that the origin <img src="1-5300169\ecd39858-aa2a-4d77-ad29-b5f190d4d2db.jpg" /> of the coordinates system is an interior point of<img src="1-5300169\54322058-5f36-45ee-91bd-380c7ee5b727.jpg" />, and we denote with <img src="1-5300169\288a70dd-2b72-4dfc-b98c-fb47a0292c0e.jpg" /> the closure of the ball centered in <img src="1-5300169\569fea87-628c-4eb2-98da-cd847e98fabf.jpg" /> with radius<img src="1-5300169\ca0165a3-5e2d-4762-aa50-c400cd2a2a34.jpg" />.</p><p>Theorem 2.4. Assume that the hypotheses of Theorem 2.2 hold and furthermore assume that</p><p><img src="1-5300169\f6aa6da6-aa86-4ac9-89ff-34562bcd9339.jpg" /></p><p>for some positive<img src="1-5300169\1e11216e-5a2d-4eed-9de8-23979e2daf8a.jpg" />. Then 1) <img src="1-5300169\e90714fb-808f-41bc-baf4-e913fc7d99c5.jpg" />is starshaped with respect to<img src="1-5300169\953320d7-eb3e-4943-a2c9-2a86fb8f18d1.jpg" />;</p><p>2) if</p><p><img src="1-5300169\0a1ab184-1485-4e90-bd17-df546b80dca4.jpg" />;</p><p><img src="1-5300169\f0d47b32-8699-44e6-a1eb-d74304fe8d2f.jpg" />;</p><p>then</p><p><img src="1-5300169\f2a4a1cf-6f74-4b7d-ba67-eaa40dcac48e.jpg" />.</p></sec><sec id="s3"><title>3. Proof of Theorem 2.1</title><p>The technique we are going to use is the moving planes method. For the detailed description about moving planes method, see [<xref ref-type="bibr" rid="scirp.24363-ref1">1</xref>].</p><p>Proof. Step 1: To prove <img src="1-5300169\d7cf61ea-cc1f-46a8-b808-7d6a9f49a6f5.jpg" /> is a ball.</p><p>If we can demonstrate that for any point Q on<img src="1-5300169\dbbd3de3-84e2-4aee-92b1-8c8865e02c3b.jpg" />, P lies on the normal line to <img src="1-5300169\664629ac-fa5d-44cc-9acc-f0ef5cddb550.jpg" /> at Q, then <img src="1-5300169\a81e4d17-8f8d-41a3-a4db-85fda98f8d41.jpg" /> is a ball with centre P. To do this, we argue by contradiction.</p><p>Assume that there exists a point <img src="1-5300169\40e00bda-ae83-434b-8acd-3406b3fe067a.jpg" /> such that the normal line <img src="1-5300169\b96adf9a-c8db-4bcb-98a1-c6c7cb8425ed.jpg" /> to <img src="1-5300169\1d914372-a76e-4386-912f-ef3f4eb1d736.jpg" /> at Q does not contain P. We choose a coordinate system in <img src="1-5300169\dc959985-f0d9-4988-8d46-6180295343c0.jpg" /> such that <img src="1-5300169\45cc53c0-7d99-443a-ac24-1f5c07605278.jpg" />, <img src="1-5300169\9832ae8d-5fe4-4834-a218-f316a53ded0b.jpg" />, and the x<sub>n</sub> axis coincides with r.</p><p>When we use the moving planes method, we choose a family of hyperplanes normal to the <img src="1-5300169\f874c607-2fe2-4b79-9db0-302d2343c2b5.jpg" /> axis. Define hyperplan <img src="1-5300169\5e4ab6f4-8182-48a8-aa8a-1a9c8697c7a2.jpg" /> for any positive<img src="1-5300169\3a1cb3ae-3374-43f0-b4db-3d97651a1c4c.jpg" />; Let <img src="1-5300169\512133db-c4cb-47a2-a824-8fd9839965a2.jpg" /> be the infimum of <img src="1-5300169\df392e1a-cdda-41aa-b536-15a20c35d434.jpg" /> such that<img src="1-5300169\7f5446db-dad5-4556-8679-2d2705c5b3da.jpg" />; Define <img src="1-5300169\0b17d161-9cbf-4c69-aa5f-11df3b3c4e0c.jpg" /> for <img src="1-5300169\fcae1686-f63b-4b57-8bff-d69e5932406c.jpg" /> and we denote by <img src="1-5300169\151370b2-349b-4b20-922e-653a24a5c846.jpg" /> the reflection <img src="1-5300169\ff5c9fc4-5af8-4406-b5d4-40a2d31dac16.jpg" /> in<img src="1-5300169\f648963b-7c2a-4d07-aa6a-2384c338c342.jpg" />. Since <img src="1-5300169\6f0390d3-7979-4f2c-941b-77a188e9cc6f.jpg" /> is<img src="1-5300169\de6117fa-2951-4682-a750-0ab3ccea9f95.jpg" />, for some <img src="1-5300169\2717ca46-c3e9-4dc3-b51e-c316e6d12b0b.jpg" /> close to<img src="1-5300169\76bc6a36-4ca0-4477-b89d-7734f1028f97.jpg" />, v, we have</p><disp-formula id="scirp.24363-formula7754"><label>(3.1)</label><graphic position="anchor" xlink:href="1-5300169\ec32c7d3-960b-4f2e-8886-a8d317f8e289.jpg"  xlink:type="simple"/></disp-formula><p>As <img src="1-5300169\3f0db13b-52c1-4041-b4f9-26a4aa5ab676.jpg" /> decreases, condition (3.1) holds until one of the following facts happens:</p><p>1) <img src="1-5300169\0e398e1f-7662-454a-9d98-79e55c4ac1f8.jpg" />is internally tangent to <img src="1-5300169\95f3ecf5-561c-41d1-b487-44e4344e923c.jpg" /> at some point of<img src="1-5300169\83c2edb2-f4a2-419e-9083-36a6bcb03461.jpg" />;</p><p>2) <img src="1-5300169\ce2295fe-8efe-48ea-b4d0-6a2a46242644.jpg" />intersects <img src="1-5300169\4775e10a-9305-4a47-b189-1a33dee9b493.jpg" /> at some point of<img src="1-5300169\18efee06-dda9-4a3a-9b95-6880832bbe2f.jpg" />.</p><p>Let <img src="1-5300169\41778d47-7ea3-4161-a732-1c8ae49943c3.jpg" /> be the greatest value of<img src="1-5300169\72ed1de1-e882-4952-87cc-9003793546bb.jpg" />, <img src="1-5300169\b66d7cc4-f3d0-4f2c-a226-b4717bfeb2c7.jpg" />, such that either condition a) or b) is true. Since <img src="1-5300169\cbdd5321-f99b-4264-8d0a-bf76ebbcfaf4.jpg" /> is orthogonal to <img src="1-5300169\44a02919-935d-4c2f-a2ba-bacd31357fae.jpg" /> at<img src="1-5300169\b3a1d7cd-e71a-4446-b909-acc6ffb896f5.jpg" />, we have <img src="1-5300169\e1dda3dd-3722-4642-8f06-83508d452d57.jpg" /> and then <img src="1-5300169\a74dcd13-ea9d-46e3-af89-2dc1a548e0c5.jpg" /> for any <img src="1-5300169\b146ab9d-3959-4998-9834-fc495ba721cc.jpg" /> in<img src="1-5300169\92b8dcf7-6346-4c23-a053-ac09610f8df0.jpg" />. This is the crucial point of our proof. We have found a direction such that as the moving plane <img src="1-5300169\268a948f-2a71-4d6e-8ccf-6282a780a650.jpg" /> moves from <img src="1-5300169\ff9c1004-8018-4483-a04b-561fa315e671.jpg" /> to the critical position<img src="1-5300169\396a9974-a19f-4faf-a892-f21c5e0c6077.jpg" />, it never intersects<img src="1-5300169\5ea1f493-669c-4d65-9daa-50b8690dcf5d.jpg" />, so that the moving planes method may be applied.</p><p>Let <img src="1-5300169\86e495eb-e12f-41da-abda-5852bf3b49f3.jpg" /> be the reflected point of x in<img src="1-5300169\e9be2799-e933-466d-bacc-a40afd09de88.jpg" />. We defined</p><p><img src="1-5300169\c2b6bbb1-3455-4c64-b43c-33300fda081f.jpg" />for<img src="1-5300169\cccd9053-b89b-49d6-b103-1c881a1b9a68.jpg" />, <img src="1-5300169\59e845d8-ee6e-4b28-a2a8-37a96166ebf1.jpg" />,</p><p><img src="1-5300169\2f86426d-67f4-45fd-9e95-e1a5ec59f61e.jpg" /></p><p>From Equation (2.1) we have for<img src="1-5300169\26e273a3-bce4-42e9-9278-23aa98aa9023.jpg" />,</p><disp-formula id="scirp.24363-formula7755"><label>(3.2)</label><graphic position="anchor" xlink:href="1-5300169\31927fb1-cb98-4114-ba6f-be171cb23384.jpg"  xlink:type="simple"/></disp-formula><p>By the definition of v, we obtain</p><disp-formula id="scirp.24363-formula7756"><label>(3.3)</label><graphic position="anchor" xlink:href="1-5300169\5434857b-d3e7-4cc3-a412-b231a31ef5c0.jpg"  xlink:type="simple"/></disp-formula><p>Differencing Equations (3.2) and (3.3) yields</p><disp-formula id="scirp.24363-formula7757"><label>(3.4)</label><graphic position="anchor" xlink:href="1-5300169\8b0e657e-4c9a-4af6-baef-cda764109c4a.jpg"  xlink:type="simple"/></disp-formula><p>Meanwhile, (3.4) can also be rewritten into</p><disp-formula id="scirp.24363-formula7758"><label>(3.5)</label><graphic position="anchor" xlink:href="1-5300169\67c18254-f49f-489a-84a3-f666d316caa3.jpg"  xlink:type="simple"/></disp-formula><p>Denote<img src="1-5300169\68abbc1b-8f51-4f63-ab36-ba176baf1f30.jpg" />, <img src="1-5300169\cdc13a81-3b79-41d9-9269-4f83f29107c9.jpg" />,</p><p><img src="1-5300169\d0606957-9882-4ac9-b68d-8fdebf5f624a.jpg" />.</p><p>Let</p><p><img src="1-5300169\9cfa898f-18ad-4ce7-95a1-2a63fdce3fed.jpg" /></p><p>By the mean value theorem, it follows from (3.5) that</p><disp-formula id="scirp.24363-formula7759"><label>(3.6)</label><graphic position="anchor" xlink:href="1-5300169\554cffb9-2277-4ee2-8107-ff35fb1fc6f9.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="1-5300169\60c648be-e269-484f-a596-9a2217123f01.jpg" />, <img src="1-5300169\5b8f1e7f-eb34-46bd-9c5e-32b5d50d2d03.jpg" />and c are certain functions depending on u and f. Here the matrix <img src="1-5300169\23da0b25-37df-4a81-a3d7-a364f5b05acb.jpg" /> is uniformly positive definite, since both expressions <img src="1-5300169\d3522b5c-eccb-44b9-8cff-323150c4171a.jpg" /> and <img src="1-5300169\7edbabf1-3c61-4d12-bdeb-03b4ab4d0127.jpg" /> have this property (recall that Equation (2.1) is elliptic). So (3.6) is uniformly elliptic with bounded coefficients far from<img src="1-5300169\43381dbb-73cf-4d02-8409-05e79db74b28.jpg" />, i.e. in <img src="1-5300169\06792453-7ed5-46f9-bdd2-dc81d6d533c8.jpg" /> where <img src="1-5300169\2212e540-5782-4783-a626-568f50386404.jpg" /> is a ball centered in with radius<img src="1-5300169\7d1cf3ab-4dbe-4895-93aa-131bfb3191dc.jpg" />, for any positive<img src="1-5300169\5ddf0c58-0aa1-4c04-8171-5029a14d2695.jpg" />.</p><p>From the boundary condition (2.3) on the normal derivative of<img src="1-5300169\cc957ec0-1a3d-40f3-a1a6-bd199276ca9a.jpg" />, it follows that</p><p><img src="1-5300169\21f300e4-cc10-46c7-8454-e8b5f41d90d8.jpg" />in <img src="1-5300169\8980e16e-a8bc-492a-9f64-fe48f365e5a1.jpg" /> (3.7)</p><p>for some <img src="1-5300169\9ad6af82-3e9b-450a-95c0-780130785dd4.jpg" /> sufficiently close to<img src="1-5300169\8e6aefc9-41b1-4d10-a7e0-5d29e0024555.jpg" />. Let</p><p><img src="1-5300169\bc8516f0-b8dc-47c5-a0e3-d4eb06a79afd.jpg" />. We prove<img src="1-5300169\e86a60f1-0611-45a9-82cb-b0444bbea60e.jpg" />.</p><p>Assume<img src="1-5300169\30c81f89-8026-4b31-84ff-0f33c52fae78.jpg" />, by continuity, <img src="1-5300169\f8f977cd-5a0a-4761-81e9-1a26462c7c22.jpg" />in<img src="1-5300169\c8df9762-2cdf-48b0-a952-3af665ae7b27.jpg" />. On the other hand, since <img src="1-5300169\74cb2851-5c31-4c74-819d-311443e1fc68.jpg" /> is not symmetric with respect to<img src="1-5300169\13f84638-8d95-49af-ae90-932f0777be92.jpg" />, <img src="1-5300169\ebec5e5e-34e1-4345-b05a-d1c2d62ab8c3.jpg" />in<img src="1-5300169\d096544d-68f4-49ab-9e69-f63ada1df670.jpg" />. By the strong version of the maximum principle, we obtain <img src="1-5300169\b740c530-d030-4f3e-bd19-3c96b215d475.jpg" /> in</p><p><img src="1-5300169\eeb56369-bf31-4474-84ad-50a945da65ef.jpg" />. Next we observe that <img src="1-5300169\08f624d9-37c8-4135-8d3a-47f5d25bf748.jpg" /> can not be a critical point for w since <img src="1-5300169\fad1cbff-514a-44bf-aa8a-16791dc8e84b.jpg" /> while</p><p><img src="1-5300169\1d9ff9a0-6d80-4e70-bd5b-9d21dc756ee0.jpg" />. So as <img src="1-5300169\38877526-f27e-4e2c-9ab2-45db7804685c.jpg" /> is arbitrarily small, it is <img src="1-5300169\0257afbf-4066-4564-a140-79b569e2fa47.jpg" /></p><p>in<img src="1-5300169\27f07500-b722-4a02-8041-7bb41085edf0.jpg" />. Since<img src="1-5300169\16df2ebf-a7ce-4e15-9b7b-91eb126d184e.jpg" />, we may apply the Hopf lemma to <img src="1-5300169\b3099fd2-ffdf-4df5-a464-3191a59f0ea3.jpg" /> at each point of<img src="1-5300169\0d232446-e2cb-4b59-a2b3-4b93ddaa8630.jpg" />, we get</p><p><img src="1-5300169\ff7eee10-7482-44c4-815e-bb6fa07c06fc.jpg" />on <img src="1-5300169\35743963-4ad5-44c4-9a32-7a33eae376ef.jpg" />&#160;&#160;&#160;&#160;&#160;&#160;&#160;&#160;&#160; (3.8)</p><p>The plane <img src="1-5300169\6bc30e26-9a5e-4741-a8e7-d12601b4bef1.jpg" /> is not normal to <img src="1-5300169\908f3f79-1d71-472c-97e1-c93d21e3b79a.jpg" /> at any point, then from inequality (3.8) and the boundary condition (2.3) on the normal derivative of<img src="1-5300169\a2ad2558-df84-45c5-b0a1-e4038ee1dc7f.jpg" />, we get</p><disp-formula id="scirp.24363-formula7760"><label>(3.9)</label><graphic position="anchor" xlink:href="1-5300169\bae01e1a-dba3-4df2-aecb-31cf2ac455a7.jpg"  xlink:type="simple"/></disp-formula><p>By the definition of<img src="1-5300169\1e7cd327-1512-4ef1-99a4-083f3a5a92d7.jpg" />, there exists a sequence <img src="1-5300169\012a825f-a12b-487b-954a-938fbf0d3346.jpg" /> such that <img src="1-5300169\37fc59fd-4a93-4b78-8363-dfe77f2aed5c.jpg" /> and</p><disp-formula id="scirp.24363-formula7761"><label>(3.10)</label><graphic position="anchor" xlink:href="1-5300169\4acd9392-ac1b-4525-8734-abb2101c1b9c.jpg"  xlink:type="simple"/></disp-formula><p>Let <img src="1-5300169\d228613c-28c1-4ccb-b930-aff26d34fe0d.jpg" /> be a limit point for x<sub>n</sub> in the closure of<img src="1-5300169\fa71d30d-14fa-4f43-b5a8-a0e01d0a75a8.jpg" />by continuity<img src="1-5300169\2481d52c-93f3-4592-9560-16653770d6f0.jpg" />, thus<img src="1-5300169\08ba70a4-623c-49a5-bc98-ba9c83e06b03.jpg" />. But from inequality (3.10) and the mean value theorem we get <img src="1-5300169\ee94ce9d-7a2d-4b37-811c-b5f40d75e758.jpg" /> and this contradicts condition (3.9).</p><p>So <img src="1-5300169\0d04c588-8724-4fd4-aa1e-4d1317675ed9.jpg" /> is proved.</p><p>Now we will prove that u must be symmetric with respect to<img src="1-5300169\fa437e65-b8b7-429d-b307-f46dc6e58577.jpg" />. Assume <img src="1-5300169\08e2a8bb-f4f7-4932-a8bb-b91c14a62af4.jpg" /> in<img src="1-5300169\6fb04bfe-d208-4c10-89d7-0c1ce42f5f6d.jpg" />, so as we did for<img src="1-5300169\748c4b45-46fd-455a-b995-0f7036cfaafc.jpg" />, we infer <img src="1-5300169\fad5f337-0f2c-4290-a4c4-a0623f74096c.jpg" /> in<img src="1-5300169\b4ba30e6-c0f3-4c25-956f-1d9ca9fbb5be.jpg" />.</p><p>Assume next that condition a) holds, then <img src="1-5300169\4bda0a84-4ac6-4138-8ae4-1c1b55e216dd.jpg" /> is internally tangent to <img src="1-5300169\3e7f07b1-45b7-45c2-b9f1-26fc9c2bcbdc.jpg" /> at some point<img src="1-5300169\1696d9f4-173b-4543-bc5d-09f10dc3575e.jpg" />, where<img src="1-5300169\17778811-24a3-459f-ba92-343af18d9c9d.jpg" />. Since P is an interior point of<img src="1-5300169\59e0daec-2f2e-42be-8a33-576d55657012.jpg" />, <img src="1-5300169\a2ad9308-5e11-45a4-8d5b-f771eefaa6ef.jpg" />, so that we can apply the Hopf lemma to w at M and we obtain</p><p><img src="1-5300169\7165b6ed-01d0-4913-9cc3-ccfacc80f511.jpg" />;</p><p>where <img src="1-5300169\0beeef91-29d6-46c8-bdd4-d972144838de.jpg" /> is the inner normal to <img src="1-5300169\98e77b96-c4ed-4f5e-8755-a6f2b5a0c0e5.jpg" /> at M. For</p><p><img src="1-5300169\f135d180-225f-4598-b057-4a63bff33122.jpg" /></p><p>we get the contradiction. Hence condition 2) must be true, i.e. <img src="1-5300169\c3f33260-76bd-49e3-ae18-949a2aadd881.jpg" />is orthogonal to <img src="1-5300169\068389af-ac2e-43f0-ade2-34aeb6f54c29.jpg" /> at some point B. From the boundary condition (2.3) and the definition of w it follows that all the first and second derivatives of w vanish at B. On the other hand, as<img src="1-5300169\f043101d-3563-4838-aa8e-58d58e15d789.jpg" />, Equation (3.6) is uniformly elliptic with bounded coefficents in a neighborhood of B, so that the boundary lemma at corner in [<xref ref-type="bibr" rid="scirp.24363-ref1">1</xref>] lemma 2, may be applied to w. Let s be a direction which enters<img src="1-5300169\26e2f4ed-66a4-42d7-8f91-2c68f6c4407c.jpg" /> nontangentially at B, then by the Serrin’s lemma</p><p><img src="1-5300169\6257223b-222c-4e61-bcba-b6ba4d908169.jpg" />or <img src="1-5300169\431431eb-4c3d-4ce8-b497-cd6bc2cd125c.jpg" /></p><p>Then we have again a contradiction with the derivatives of w at B, so <img src="1-5300169\135e2e03-3eda-4104-beea-f915d17304c1.jpg" /> in<img src="1-5300169\6cccab04-7822-4b48-a643-ac357d2b06b5.jpg" />. But this last inequality can not be true since otherwise w would be a function symmetric in <img src="1-5300169\1be21e12-af13-483b-b1e9-ae851c9db5cd.jpg" /> whose only critical point is not on<img src="1-5300169\ab894fd4-c8bc-4ce8-ac9e-04d9670b4da8.jpg" />.</p><p>This completes the proof of Theorem 2.1.</p></sec><sec id="s4"><title>REFERENCES</title></sec><sec id="s5"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.24363-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">J. Serrin, “A Symmetry Problem in Potential Theory,” Archive for Rational Mechanics and Analysis, Vol. 43, No. 4, 1971, pp. 304-318. doi:10.1007/BF00250468</mixed-citation></ref><ref id="scirp.24363-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">N. Garofalo and J. Lewis, “A Symmetry Result Related to Some Overdetermined Boundary Value Problems,” American Journal of Mathematics, Vol. 111, No. 1, 1989, pp. 9-33. doi:10.2307/2374477</mixed-citation></ref><ref id="scirp.24363-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">I. Fragala, I. F. Gazzaola and B. Kawohl, “Overdetemined Boundary Value Problems with Possibly Degenerate Ellipticity: A Geometry Approach,” Mathematische Zeitschrift, Vol. 254, No. 1, 2006, pp. 117-132. 
doi:10.1007/s00209-006-0937-7</mixed-citation></ref><ref id="scirp.24363-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">G. A. Philippin, “Application of the Maximum Principle to a Variety of Problems Involving Elliptic Differential Equations,” In: P. W. Schaefer, Ed., Maximum Principles and Eigenvalue Problems in Partial Differential Equations, Pitman Research Notes in Mathematics Series, Longman SciTech., Harlow, 1988, pp. 34-48.</mixed-citation></ref><ref id="scirp.24363-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">A. Farina and B. Kawohl, “Remarks on an Overdetermined Boundary Value Problem,” Calculus of Variations and Partial Differential Equations, Vol. 31, No. 3, 2008, pp. 351-357.</mixed-citation></ref></ref-list></back></article>