<?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">IJMNTA</journal-id><journal-title-group><journal-title>International Journal of Modern Nonlinear Theory and Application</journal-title></journal-title-group><issn pub-type="epub">2167-9479</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ijmnta.2013.24029</article-id><article-id pub-id-type="publisher-id">IJMNTA-40276</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  The Global and Pullback Attractors for a Strongly Damped Wave Equation with Delays*
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>uoguang</surname><given-names>Lin</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>Fangfang</surname><given-names>Xia</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Guigui</surname><given-names>Xu</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Mathematics, Yunnan University, Kunming, China</addr-line></aff><aff id="aff2"><addr-line>School of Mathematics and Science, Kaili University, Kaili, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>gglin@ynu.edu.cn(UL)</email>;<email>xuguigui586@163.com(GX)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>29</day><month>11</month><year>2013</year></pub-date><volume>02</volume><issue>04</issue><fpage>209</fpage><lpage>218</lpage><history><date date-type="received"><day>October</day>	<month>13,</month>	<year>2013</year></date><date date-type="rev-recd"><day>November</day>	<month>13,</month>	<year>2013</year>	</date><date date-type="accepted"><day>November</day>	<month>21,</month>	<year>2013</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 study the global and pullback attractors for a strongly damped wave equation with delays when the force term belongs to different space. The results following from the solution generate a compact set.
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</p></abstract><kwd-group><kwd>Strongly Damped; Pullback Attractor; Global Attractor; Delays</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Let <img src="3-2340095\7936aeba-bebd-4ecb-8635-a3ca551d31e1.jpg" /> be a bounded domain with smooth boundary<img src="3-2340095\053813c3-ccfc-4a81-bb2a-92f24d57aee5.jpg" />, we study the following initial boundary value problem</p><disp-formula id="scirp.40276-formula78993"><label>(1.1)</label><graphic position="anchor" xlink:href="3-2340095\b58e1d80-2782-437c-b804-7f775a22ac7d.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="3-2340095\4b28c2b6-1217-4ab1-855d-a14d607fb499.jpg" /> is the source intensity which may depend on the history of the solution, <img src="3-2340095\c67c2ba4-80ee-4daa-939f-ab0314025ac6.jpg" />are the positive constants, <img src="3-2340095\f7ec0d2a-02c0-4e34-8e76-6e17cef5e27c.jpg" />is the initial value on the interval <img src="3-2340095\3bd0dbb2-079b-412f-a13f-d736c22adf33.jpg" /> where<img src="3-2340095\502134d6-7c89-4573-8292-af4281c59eea.jpg" />, and <img src="3-2340095\843e68c0-dbe5-4934-871d-1bd60b422f2a.jpg" /> is defined for <img src="3-2340095\3b4f919c-58df-4d86-95a1-34052654a445.jpg" /> as<img src="3-2340095\af56973b-49c1-4c46-9c48-4ab13a74db8a.jpg" />. The assumption on <img src="3-2340095\3fbd9de6-4813-4299-bcc5-fd2de4c59d64.jpg" /> and <img src="3-2340095\0dde4a61-7d21-4518-87d8-b19dfe3f09a7.jpg" /> will be specified later.</p><p>It is well known that the long time behavior of many dynamical system generated by evolution equations can be described naturally in term of attractors of corresponding semigroups. Attractor is a basic concept in the study of the asymptotic behavior of solutions for the nonlinear evolution equations with various dissipation. There have been many researches on the long-time behavior of solutions to the nonlinear damped wave equations with delays. The existence of random attractors has been investigated by many authors, see, e.g., [1-4]. A new type of attractor, called a pullback attractor, was proposed and investigated for non-autonomous or these random dynamical systems. The pullback attractor describing this attractors to a component subset for a fixed parameter value is achieved by starting progressively earlier in time, that is, at parameter values that are carried forward to the fixed value. see [5-20]. However, to our knowledge, in the case of functional differential equations of second order in time, there is only partial results.</p><p>Recently, In [<xref ref-type="bibr" rid="scirp.40276-ref5">5</xref>], some results on pullback and forward attractor for the following strongly damped wave equation with delays &#160;</p><p><img src="3-2340095\8d807637-e6bf-4d0f-a63c-edcd94879a88.jpg" /></p><p>have been analyzed.</p><p>In this work, first, we apply the means in [<xref ref-type="bibr" rid="scirp.40276-ref3">3</xref>] to provide the existence of global attractor, for the dynamical system generated by the initial value problem (1.1). The key is to deal with the nonlinear terms and the delay term is difficult to be handled, so we aimed at showing that it is dissipative and the solution is bounded and continuous with respect to initial value. Hence we can discover the global attractor. Then, we aim to obtain the pullback attractor. The technology we use is introduced in [<xref ref-type="bibr" rid="scirp.40276-ref1">1</xref>], that is, we divide the semigroup into two: the one is asymptotically close to 0, while the other is uniformly compact, so we can get the pullback attractor.</p><p>Now, we state the general assumptions for problem (1.1) on <img src="3-2340095\0ec71362-1675-40cd-8168-f7e621f51382.jpg" /> and<img src="3-2340095\593c5c13-6265-4f91-b05f-a3fb03524916.jpg" />.</p><p>Let<img src="3-2340095\1014c0a2-2193-4bb5-9305-f2acea33c0bb.jpg" />, then there exist positive constants <img src="3-2340095\a0a3f8d9-e9f3-4ac5-97fe-672d8ebfdbbc.jpg" /> such that the followings hold true</p><p>(G<sub>1</sub>).<img src="3-2340095\aa6fdebd-ec35-4349-8d8c-da9bb10cf366.jpg" />;</p><p>(G<sub>2</sub>).<img src="3-2340095\ddb7436d-a67a-4e40-be50-47d2ee53fc07.jpg" />;</p><p>(G<sub>3</sub>).<img src="3-2340095\33bfc90b-e4df-414d-a381-0296ab9cb733.jpg" />;</p><p>(G<sub>4</sub>).<img src="3-2340095\d1aa0fc3-6afb-4bc8-8c59-b77a1a61ccad.jpg" />;</p><p>(G<sub>5</sub>).<img src="3-2340095\85f1a905-35ab-4ed1-af8c-e6d558711747.jpg" />;</p><p>(G<sub>6</sub>).<img src="3-2340095\13d16e5c-d834-4934-876a-0875b0a0afaa.jpg" />;</p><p>(G<sub>7</sub>).<img src="3-2340095\a019dc88-df1d-4522-a6c8-de357a25828d.jpg" />.</p><p>For any<img src="3-2340095\5410d3c2-7455-42ee-aa11-cd8dbcedbf2d.jpg" />, set<img src="3-2340095\762ce32f-4696-48fa-aac7-c83b42057386.jpg" />, by<img src="3-2340095\2451d55a-9834-4bc7-9a1f-ac461175890d.jpg" />, there are <img src="3-2340095\124a38be-5359-4869-9b2a-6e039bf9f530.jpg" /> and<img src="3-2340095\e95bf437-1e8f-4c1c-82cb-039f5d9cb9b2.jpg" />, for any<img src="3-2340095\5ce55389-69dd-4ed2-b88c-a45e585c51ef.jpg" />, we have</p><p><img src="3-2340095\673f85e3-63d8-43e7-a123-7773abadf8b3.jpg" /></p><p>H<sub>1</sub>. <img src="3-2340095\2416abb5-9734-46ca-a378-2c95ab32fe66.jpg" />is continuous;</p><p>H<sub>2</sub>.<img src="3-2340095\7a99be8d-b94c-4712-8ed0-b96284777285.jpg" />;</p><p>H<sub>3</sub>. <img src="3-2340095\bd44df5d-f017-4845-b5ae-ae542670a2c4.jpg" />such that <img src="3-2340095\a2a0ac7d-e74d-451f-95be-3c38651a3a3d.jpg" /></p><p><img src="3-2340095\9ecdc19d-6c24-453e-8929-71d0b2aead28.jpg" /></p><p>H<sub>4</sub>. <img src="3-2340095\ebdee2af-60da-4b37-9ef6-c253525af848.jpg" />such that</p><p><img src="3-2340095\39a5d4ba-32e0-47a2-963a-e488f5bf4aba.jpg" /><img src="3-2340095\2fb52b7f-01d5-4792-b9ce-4d907ffbdf69.jpg" /></p><p>H<sub>5</sub>.<img src="3-2340095\61c63b4e-f35e-40d8-8012-bf0139fe6d7b.jpg" />, and there exists <img src="3-2340095\2731588d-d192-493b-afad-c515720d125a.jpg" /> such that, for any<img src="3-2340095\bdcae631-6519-4e2d-8e9e-ee4e4237a983.jpg" />, the Frechet derivative <img src="3-2340095\fe7e32ef-640b-432f-b928-a02f076822fe.jpg" /> satisfies</p><p><img src="3-2340095\12929b4a-3d6a-4777-bf7d-ce8db52f4735.jpg" /></p><p>The rest of this paper is organized as follows. In Section 2, we introduce basic concepts concerning global and pullback attractor. In Section 3, we obtain the existence of the global attractor. In Section 4, we obtain the existence of the pullback attractor.</p></sec><sec id="s2"><title>2. Preliminaries</title><p>In this section,firstly, we recall some basic concepts about the global attractor.</p><p>Definition 2.1 ([<xref ref-type="bibr" rid="scirp.40276-ref3">3</xref>]) Let <img src="3-2340095\c8801dcc-e95b-49db-9a58-4aae7f28f978.jpg" /> be a Banach space and</p><p><img src="3-2340095\829dbca3-f180-4d95-9913-2c757b40e251.jpg" />be a family of operators on<img src="3-2340095\1cb2df14-987b-4c37-8f17-753658a7b6e1.jpg" />. We say that <img src="3-2340095\bdbd7871-7962-4148-bdbf-170eeecf3c92.jpg" /> is norm-to-weak continuous semigroup on<img src="3-2340095\54f2eb91-6092-4a24-80f4-7299c52de38a.jpg" />, if <img src="3-2340095\2beb2047-0bd8-4886-91e4-24cdf430a432.jpg" /> satisfies:</p><p>[1)]<img src="3-2340095\48a2a8af-ac31-4838-8876-deeb999a7777.jpg" />;</p><p>[2)]<img src="3-2340095\5a877068-8064-4017-afbc-411c76bb6020.jpg" />;</p><p>[3)] <img src="3-2340095\0130ea13-f853-4555-aaa0-1149cc51a2b6.jpg" />if <img src="3-2340095\241cc7bb-7f4d-4743-b141-51a17ee60637.jpg" /> and <img src="3-2340095\98ab507f-94a9-47cf-80d6-d8315114e419.jpg" /> in<img src="3-2340095\9c188965-a13a-4d7d-9474-5c92ccfeec6f.jpg" />.</p><p><img src="3-2340095\8a7ef125-55c8-4911-b9cb-7a20631d4c5a.jpg" />The strong continuous semigroup and the weak semigroup are both the norm-to-weak continuous</p><p>Definition 2.2 ([<xref ref-type="bibr" rid="scirp.40276-ref3">3</xref>]) The semigroup <img src="3-2340095\05750be0-0e82-499e-a856-4672ee86421f.jpg" /> is called satisfying Condition (C) in <img src="3-2340095\76fae6e3-064b-4f55-97f4-218b6ac6e146.jpg" /> if and only if for any bounded set <img src="3-2340095\c107b932-8653-456c-8406-e1cb8f813489.jpg" /> of <img src="3-2340095\4e85ccd3-7d2f-430d-a30f-d051356e4647.jpg" /> and for any<img src="3-2340095\f173489d-cd2f-4fd2-975e-c322da903376.jpg" />, there exist a positive constant <img src="3-2340095\79c38742-2c0e-4912-ae1d-a49d3ce1f529.jpg" /> and a finite dimensional subspace <img src="3-2340095\e93d384f-d259-434d-9930-2633eaea22b7.jpg" /> of X, such that <img src="3-2340095\4256fef5-7b16-4c24-8b18-6fb5e5474c34.jpg" /> is bounded and</p><p><img src="3-2340095\6c936388-e59a-4faa-bcdc-42793542b869.jpg" /></p><p>where <img src="3-2340095\8062810e-d72e-47db-b180-2dcc1c10a591.jpg" /> is the canonical projector.</p><p>Lemma 2.1 ([<xref ref-type="bibr" rid="scirp.40276-ref3">3</xref>]) Let <img src="3-2340095\058cbf43-ca30-4eb7-9b5d-317de16bf5ff.jpg" /> be a Banach space and</p><p><img src="3-2340095\165354ea-535b-47d8-bfce-f2990572e709.jpg" />be a norm-to-weak continuous semigroup on<img src="3-2340095\0c5b4d11-e417-482e-8718-f4a9dbef33d4.jpg" />. Then <img src="3-2340095\c171129c-b71b-41fa-9de3-80d63cbf9024.jpg" /> has a global attractor in <img src="3-2340095\0d553e85-5b84-4acd-8995-ac038919843f.jpg" /></p><p>provided that the following conditions hold:</p><p>1) <img src="3-2340095\841c29b0-e427-453e-b96d-399f244bee05.jpg" />has a bounded absorbing set <img src="3-2340095\1c94c88c-66f8-49c6-8216-7ac5fedfb77f.jpg" /> in<img src="3-2340095\3e5d0c6e-1628-4e63-8a94-cef44eea78b3.jpg" />;</p><p>2) <img src="3-2340095\fdca5969-f519-47a6-84d7-082f7da771a1.jpg" />satisfies Condition (C) in<img src="3-2340095\376db7fb-e774-400f-81b4-5258e94b1707.jpg" />.</p><p>Then, we state the concepts and some result about the process and the pullback attractor.</p><p>Instead of a family of the one-parameter map<img src="3-2340095\ba57f30e-5cd5-4710-9a20-49e13fa5eac4.jpg" />, we need to use a two-parameter semigroup or process <img src="3-2340095\975c4a52-c326-4df6-8748-8464c20aefb0.jpg" /> on the complete metric space<img src="3-2340095\fa60fe88-902c-4b44-93c7-56d8e8e8f791.jpg" />, <img src="3-2340095\77e43f49-f912-4e14-918a-12bec2efd99e.jpg" />denotes the value of the solution at time <img src="3-2340095\b6aa34d5-d39f-4a02-921d-130d6867992e.jpg" /> which was equal to the initial value <img src="3-2340095\d29fd848-3681-4800-ae33-f5c0b62cde9e.jpg" /> at time<img src="3-2340095\c73d926c-637a-418b-8381-56fb9793ab54.jpg" />.</p><p>The semigroup property is replaced by the process composition property</p><p><img src="3-2340095\3058abbc-2192-411c-99e5-dcdc2369158b.jpg" /></p><p>and, obviously, the initial condition implies<img src="3-2340095\f5b52f4f-f7db-4020-badc-edce8b5b623a.jpg" />.</p><p>Definition 2.3 Let <img src="3-2340095\fb920e45-fb1b-4d40-8f37-ab076cb2f9b9.jpg" /> be the two-parameter semigroup or process on the complete metric space<img src="3-2340095\9afe23be-6cf7-468d-a9d2-6c3dc4c7db73.jpg" />. A family of compact set <img src="3-2340095\4d92a6fe-0bca-4e7e-8a73-246505fdd39a.jpg" /> is said to be a pullback attractor for <img src="3-2340095\ef090e6f-526b-4423-9579-8b1648c96d27.jpg" /> if, for all<img src="3-2340095\98e6dfa0-f349-4b78-91c7-cb3e6979cf52.jpg" />, it satisfies</p><p>[1)] <img src="3-2340095\2aa0b001-0c61-470e-a4c6-98b28d3190c7.jpg" />for all<img src="3-2340095\08264343-094a-425a-ba93-c6f29eca8c55.jpg" />, and</p><p>[2)]<img src="3-2340095\417e8c1e-be54-46fa-b335-9ccc5e9030ee.jpg" />, for all bounded<img src="3-2340095\72fbb946-07a2-4473-a137-898ce122d2ac.jpg" />, and all<img src="3-2340095\a82d8865-12b9-4090-bd79-b025da56e16d.jpg" />.</p><p>Definition 2.4 The family <img src="3-2340095\44bbe2dd-4266-4f36-bad0-ffbc1aa7faf8.jpg" /> is said to be</p><p>1) pullback absorbing with respect to the process<img src="3-2340095\ce7a9446-5c4c-44ca-842b-4b524af748b6.jpg" />, if for all <img src="3-2340095\738be62b-5fae-4eb1-b7b9-8dce28692720.jpg" /> and all bounded<img src="3-2340095\dffa8a1b-7610-4f7e-bd30-3676436efff9.jpg" />, there exists <img src="3-2340095\7a0afd52-4c01-4f22-b7df-1413e534f3ba.jpg" /> such that <img src="3-2340095\b7f316b9-1f26-4383-a26c-489ac7045401.jpg" /> for all<img src="3-2340095\9bdae35d-01bf-48ff-900e-a66d91f086dd.jpg" />;</p><p>2) pullback attracting with respect to the process<img src="3-2340095\7d940dbe-46c1-4761-8c25-df1f84fd90f7.jpg" />, if for all<img src="3-2340095\07f48ba3-7107-4e50-a38f-a19fc7683cfc.jpg" />, all bounded<img src="3-2340095\2cb93d8d-88a3-47e2-b7af-147ae2a6383b.jpg" />, and all<img src="3-2340095\20a771e2-a788-4668-9e40-1fe1e8ee55ec.jpg" />, there exists <img src="3-2340095\02658956-e6ee-412b-9f33-34ed3a7da6a0.jpg" /> such that for all <img src="3-2340095\e7eede06-2b4a-44ae-a445-5df1eb204df9.jpg" /></p><p><img src="3-2340095\1d078068-7908-4d03-83a1-f45084e9d38b.jpg" /></p><p>3) pullback uniformly absorbing (respectively uniformly attracting) if <img src="3-2340095\0b8aef8a-d2f2-4d0f-af41-e98b15fbefe3.jpg" /> in pact (a) (respectively <img src="3-2340095\460d5ca6-86c9-44f9-93f4-492e25fc5128.jpg" /> in part (b)) does not depend on the time<img src="3-2340095\f5545e07-1bb3-40d3-a8c6-aa2afc2cb187.jpg" />.</p><p>Theorem 2.1 Let <img src="3-2340095\43f348c9-4f0d-468a-b099-66c08cce424c.jpg" /> be a two-parameter process, and suppose <img src="3-2340095\4dcee2e0-578b-4b53-84af-a1e731299af8.jpg" /> is continuous for all<img src="3-2340095\23ab3119-756a-4202-80bb-6d5a92125fbb.jpg" />. If there exists a family of compact pullback attracting sets<img src="3-2340095\22e2c936-0cda-4b23-ac3f-4b44b5e87d2c.jpg" />, then there exists a pullback attractor<img src="3-2340095\5f4e73ea-2998-4447-b839-f4f769f6ad5c.jpg" />, such that <img src="3-2340095\cfa67736-1ec6-476a-8f9d-583d3db90bcd.jpg" /> for all<img src="3-2340095\c7de180e-b40b-4015-b305-daf97c12b2ac.jpg" />, and which is given by</p><p><img src="3-2340095\e4c6c30c-0ef8-4f44-ab4e-0d64d2ff7284.jpg" /></p><p>We set<img src="3-2340095\fa16fdab-5293-412c-b2a5-74bece4758e0.jpg" />, where<img src="3-2340095\d4592d38-edcc-47ff-8dd4-0c8f98ac1cf5.jpg" />, which are Hilbert spaces for the usual inner product and associated norms. we denote by <img src="3-2340095\95a3fbd5-04bb-42fc-b268-b9f214dc59ef.jpg" /> the first eigenvalue of <img src="3-2340095\f1d44526-39b4-4c3c-8923-bca180111e5e.jpg" /> in<img src="3-2340095\0180dafb-132e-4174-b649-369c33a3b27c.jpg" />.</p><p>Our problem can be written as a second-order differential equation in<img src="3-2340095\1f107590-5730-416b-baac-26de6e16565b.jpg" />:</p><disp-formula id="scirp.40276-formula78994"><label>(2.1)</label><graphic position="anchor" xlink:href="3-2340095\4bd62db2-444f-4db8-86d4-f5ae4ff34073.jpg"  xlink:type="simple"/></disp-formula></sec><sec id="s3"><title>3. Existence of the Global Attractor</title><p>In this section, our objection is to show that the well-posed of the solution and the existence of global attractor for the initial boundary value problem (1.1), we assume that<img src="3-2340095\1d158267-dece-4586-8294-c7f2c9598c7e.jpg" />.</p><p>Let <img src="3-2340095\0b47b15c-51a6-4b49-9559-f794c400d237.jpg" /> and<img src="3-2340095\e51321e7-5b2e-415a-84f8-4fa3c5cbc04a.jpg" />, then by the transformation<img src="3-2340095\80571b6b-2e4f-44b1-a6e3-7bf2fb5d2ce2.jpg" />. The initial boundary value problem (2.1) is equivalent to</p><disp-formula id="scirp.40276-formula78995"><label>(3.1)</label><graphic position="anchor" xlink:href="3-2340095\d5da8a15-2e0b-43b3-8f60-309061e9015f.jpg"  xlink:type="simple"/></disp-formula><p>with the initial value conditions</p><p><img src="3-2340095\fcdf6309-a98d-4f5f-b35a-3ecd50e7a47c.jpg" /></p><p>Theorem 3.1 Assume that the hypotheses on <img src="3-2340095\46250593-3784-4fb5-a046-2497dce3bfe4.jpg" /> and <img src="3-2340095\a747efd0-98b0-40de-8345-89b77dc718e5.jpg" /> hold for all <img src="3-2340095\6956cf27-0118-4c7e-8068-a5ce3d1dfdb8.jpg" /> and<img src="3-2340095\f8ec7697-d481-47cf-b147-0657966f0df1.jpg" />, <img src="3-2340095\7cce003c-1830-4d1f-9c30-0ead88722f88.jpg" />are the positive constants. Then the initial boundary value problem (3.1) has the unique solution <img src="3-2340095\56390a7a-6386-41df-bdff-e90549e2b17c.jpg" /> for all<img src="3-2340095\c0f439b9-5bd1-455f-8e0a-50eae216220f.jpg" />.</p><p>Proof. Taking the inner product of the Equation (3.1) with <img src="3-2340095\ce229d6d-d89c-4954-a196-ca4866386b87.jpg" /> in<img src="3-2340095\19692700-a49d-4419-bb8d-dbb5cfb3e325.jpg" />, we find that</p><disp-formula id="scirp.40276-formula78996"><label>(3.2)</label><graphic position="anchor" xlink:href="3-2340095\7598bf72-9825-48b6-9c5f-1c9f6ff9363d.jpg"  xlink:type="simple"/></disp-formula><p>Since <img src="3-2340095\6ba56a11-5f57-491f-b05c-bf30098ed6a4.jpg" /> and<img src="3-2340095\b83b08ce-4e88-450a-9b53-6b30bfcd4bb5.jpg" />we deal with the terms in (3.2) one by one as follows</p><disp-formula id="scirp.40276-formula78997"><label>(3.3)</label><graphic position="anchor" xlink:href="3-2340095\6c4ad33d-856f-490e-adf2-bd13046347b3.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.40276-formula78998"><label>(3.4)</label><graphic position="anchor" xlink:href="3-2340095\893e1564-fef0-49cf-86b0-be5f3d0578c6.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.40276-formula78999"><label>(3.5)</label><graphic position="anchor" xlink:href="3-2340095\9aa01371-f2e4-443d-9533-fccb6dbf8402.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.40276-formula79000"><label>(3.6)</label><graphic position="anchor" xlink:href="3-2340095\c043c218-e7b7-42cc-9648-b7eeeeecdbe5.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.40276-formula79001"><label>(3.7)</label><graphic position="anchor" xlink:href="3-2340095\b016411f-bd83-4039-b71f-b8b4b343cfa4.jpg"  xlink:type="simple"/></disp-formula><p>By (3.3)-(3.7), it follows from that</p><p><img src="3-2340095\6a1dd896-19fa-4b5f-826c-ae369bab4811.jpg" /></p><p>Since <img src="3-2340095\73b311e4-c02f-47c2-9826-d116b3eecdf3.jpg" /> and<img src="3-2340095\7c72fee2-5248-46a0-964d-ce89ba976eb4.jpg" />, this will imply<img src="3-2340095\3ff81dcd-4918-435f-8fc5-cc16417deacd.jpg" />, then we have</p><disp-formula id="scirp.40276-formula79002"><label>(3.8)</label><graphic position="anchor" xlink:href="3-2340095\5ae647c2-6c9e-4068-8d94-0a1e1e344ca7.jpg"  xlink:type="simple"/></disp-formula><p>Set<img src="3-2340095\601e6f1d-24e8-440e-a320-81412c67cab8.jpg" />, then (3.8) can be written as following</p><p><img src="3-2340095\d0e264b7-3241-46f4-ac13-7a39c803fd92.jpg" /></p><p>As our assumptions ensure that</p><p><img src="3-2340095\b9880f71-912e-4290-8c2b-48e1f91e1d45.jpg" />, then we can choose <img src="3-2340095\89fcc52b-cbce-4b13-9652-6c87a116a1e2.jpg" /> small enough such that</p><p><img src="3-2340095\63307795-3bc9-4aa9-b24a-d39204f2b356.jpg" />. For this choice, we have</p><p><img src="3-2340095\72fa8856-9fcf-45ce-8ae8-5ddf6dc83934.jpg" /></p><p>Hence, we can get the following inequality</p><p><img src="3-2340095\1f33871a-69c2-4169-9b3c-59cb0cee9c9f.jpg" /></p><p>By integrating over the interval<img src="3-2340095\66e23db9-e5ad-47a8-9ffe-8bcc60a36ec6.jpg" />, we deduce</p><disp-formula id="scirp.40276-formula79003"><label>(3.9)</label><graphic position="anchor" xlink:href="3-2340095\88d46390-321d-4ff5-8205-e77c8ba14777.jpg"  xlink:type="simple"/></disp-formula><p>Since</p><p><img src="3-2340095\3154d14a-81e0-4ef8-aa32-63185a67e095.jpg" /></p><p>So we can have</p><disp-formula id="scirp.40276-formula79004"><label>(3.10)</label><graphic position="anchor" xlink:href="3-2340095\3d06e525-177f-4dcc-b6be-57f4b72f4283.jpg"  xlink:type="simple"/></disp-formula><p>Noticing<img src="3-2340095\8078929d-c08f-49ca-aa26-1b9683360d9b.jpg" />, we obtain</p><disp-formula id="scirp.40276-formula79005"><label>(3.11)</label><graphic position="anchor" xlink:href="3-2340095\319869c6-8470-41f5-9292-3ba73768abf5.jpg"  xlink:type="simple"/></disp-formula><p>In the Bounded set<img src="3-2340095\d6a4b539-33ef-4738-85e8-011b9510a098.jpg" />, for any<img src="3-2340095\19532c78-8998-4e7d-a2d8-db9fb5d668b3.jpg" />, there exists a constant <img src="3-2340095\f068dc89-7df1-4416-bafd-893cf68d5739.jpg" /> such that</p><disp-formula id="scirp.40276-formula79006"><label>(3.12)</label><graphic position="anchor" xlink:href="3-2340095\b951365f-0ea9-4ad7-938e-116f796d2a68.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.40276-formula79007"><label>(3.13)</label><graphic position="anchor" xlink:href="3-2340095\74b01d04-affd-4450-8aad-5a8e96b90122.jpg"  xlink:type="simple"/></disp-formula><p>(3.10)-(3.13) means that</p><disp-formula id="scirp.40276-formula79008"><label>(3.14)</label><graphic position="anchor" xlink:href="3-2340095\3576dadc-7bf5-4946-baf2-202dd528690f.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.40276-formula79009"><label>(3.15)</label><graphic position="anchor" xlink:href="3-2340095\c8637575-d3bb-4b23-95d8-93910433fa35.jpg"  xlink:type="simple"/></disp-formula><p>Hence, by (3.12)-(3.14) and the choice of</p><p><img src="3-2340095\86d13cc1-3b4e-4aba-8fd8-ee392660c176.jpg" />, (3.9) can be rewritten</p><disp-formula id="scirp.40276-formula79010"><label>(3.16)</label><graphic position="anchor" xlink:href="3-2340095\fb78a75d-24f6-4f24-a812-d1d86c18f517.jpg"  xlink:type="simple"/></disp-formula><p>&#160;So we can get by (3.16)</p><p><img src="3-2340095\e640ac47-c632-489a-a832-26da05d39c40.jpg" /></p><p>which implies,for <img src="3-2340095\d5dc9f15-308a-48e1-a6e0-d7401235b7ee.jpg" /></p><disp-formula id="scirp.40276-formula79011"><label>(3.17)</label><graphic position="anchor" xlink:href="3-2340095\b9e4cf80-a1d0-4bd0-b72b-2ae08232bf72.jpg"  xlink:type="simple"/></disp-formula><p>If we denote</p><p><img src="3-2340095\2dc0c962-6ef1-4b1b-924c-97d798348492.jpg" />then (3.17) yields that</p><disp-formula id="scirp.40276-formula79012"><label>(3.18)</label><graphic position="anchor" xlink:href="3-2340095\b3c562c7-8a92-4c28-9701-a3a9d35214ce.jpg"  xlink:type="simple"/></disp-formula><p>which means that the initial boundary value problem (3.1) has the solution<img src="3-2340095\a6ca74fc-d705-4567-980f-74fb75025ce4.jpg" />.</p><p>Now, we prove the uniqueness of the solution. Assume that <img src="3-2340095\34794bd7-cb61-4047-a1f6-d91ddadbcf75.jpg" /> and <img src="3-2340095\d53b4947-b419-42fb-8cf4-2b5dcc77b89c.jpg" /> are the two solutions of the initial boundary value problem (3.1), <img src="3-2340095\7e7c51b3-ac45-4c04-b6d9-72f33e881f19.jpg" />are the corresponding initial value,we denote<img src="3-2340095\c91dd392-857c-422a-8492-26700dcbc349.jpg" />. Therefore we have</p><p><img src="3-2340095\00a722be-999a-4b6a-b0d8-491479eabb66.jpg" /></p><p>we take the inner product of the above equation with <img src="3-2340095\6cf67452-b3b3-44b8-9d4e-360d1a1e67e2.jpg" /> and we obtain</p><disp-formula id="scirp.40276-formula79013"><label>(3.19)</label><graphic position="anchor" xlink:href="3-2340095\8c66a631-81ac-4fad-992c-9dc4bbb875dc.jpg"  xlink:type="simple"/></disp-formula><p>Since</p><p><img src="3-2340095\496fc476-c26e-449d-9068-5c374980e8e9.jpg" /></p><p><img src="3-2340095\38d5aec6-0b07-4e3e-911e-aa3ab5088d27.jpg" /></p><p>So (3.20) can yields that</p><disp-formula id="scirp.40276-formula79014"><label>(3.20)</label><graphic position="anchor" xlink:href="3-2340095\3f28e156-bc42-4d73-8b43-70f39cc9c213.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.40276-formula79015"><label>(3.21)</label><graphic position="anchor" xlink:href="3-2340095\4a5948c3-9de5-4c10-9193-bd3bbdcd89ba.jpg"  xlink:type="simple"/></disp-formula><p><img src="3-2340095\be3def52-a2f1-418e-9863-ac57af3f9803.jpg" /></p><p>Integrating (3.21) over the interval<img src="3-2340095\56335726-b823-47a9-97cb-f6ba48ee3be2.jpg" />, we can get</p><p><img src="3-2340095\91f62e53-0d82-4317-b16c-bd5768634fd6.jpg" /></p><p>Set<img src="3-2340095\72fdb889-f939-4bc4-a26b-384288b73bb6.jpg" />, then we have</p><p><img src="3-2340095\9940fd33-2789-486a-a66a-e5d51a55db39.jpg" /></p><p>Combining the Gronwall Lemma, we get</p><disp-formula id="scirp.40276-formula79016"><label>(3.22)</label><graphic position="anchor" xlink:href="3-2340095\e7ecce0d-60f9-4950-873c-13b30e65b14d.jpg"  xlink:type="simple"/></disp-formula><p>If <img src="3-2340095\2f19e824-d8b1-4e44-9bfc-764af52c844e.jpg" /> stand for the same initial value, there has</p><p><img src="3-2340095\edff0643-fca1-4bb0-81bd-e5f25f852b51.jpg" /></p><p>that shows that</p><p><img src="3-2340095\59bd5ed9-8dbd-467f-8949-4a78cfddcac9.jpg" /></p><p>that is</p><p><img src="3-2340095\810abde9-667d-4ef6-b91d-493450d0b556.jpg" /></p><p>therefore</p><p><img src="3-2340095\ba9240df-d9db-4761-8015-f678544820b1.jpg" /></p><p>we get the uniqueness of the solution. So the proof of the theorem 3.1. has been completed.</p><p>By the theorem 3.1,we obtain the global smooth solution <img src="3-2340095\e2669f3a-c8c0-4d03-8ce8-50617e271970.jpg" /> continuously depends on the initial value<img src="3-2340095\aa82d490-dda9-4c91-8c82-93f56ad4218d.jpg" />, the initial boundary value problem (1.1) generates a continuous semigroup</p><p><img src="3-2340095\32722d57-7164-474a-8ede-408cf3308e05.jpg" />.</p><p>Then<img src="3-2340095\75c91c40-1363-4038-9959-90a815011b6c.jpg" /> is a bounded absorbing set for the semigroup <img src="3-2340095\42953f2f-72a1-40c0-9ee0-e108327e3d17.jpg" /> generated by (1.1).</p><p>Under the assumption on <img src="3-2340095\a1ea756a-7284-4094-bfc2-720773f99c44.jpg" /> and<img src="3-2340095\8fc0e090-2bf2-4eca-a555-0afd8c17ffa1.jpg" />, we can get the nonlinear term <img src="3-2340095\017bd79f-da72-4650-9ad3-0aebf0836b8e.jpg" /> is compact and continuous, <img src="3-2340095\44d422bb-07a4-48f4-9f71-094d717ab0eb.jpg" />is continuous. Next, our object is to show that the <img src="3-2340095\63a4c062-8292-4666-9875-076c70a4cdc0.jpg" /> semigroup <img src="3-2340095\ece10821-ecba-4f33-8fdd-af496176d9be.jpg" /> satisfies cindition C.</p><p>Theorem 3.2 Assume that the hypotheses on <img src="3-2340095\557c4114-ef15-403c-8442-4516439496d1.jpg" /> and <img src="3-2340095\4db85499-8dbd-4a4f-a24f-a7332fea3e36.jpg" /> hold for all<img src="3-2340095\e8aebff1-5dc0-4a6a-a5a7-d26c1871cfff.jpg" />, <img src="3-2340095\f9def4a3-73ff-44ed-964b-02b75f12fcc2.jpg" />are positive constants. Then the <img src="3-2340095\cf1baa68-0840-4cdb-8401-d6aa744f22d6.jpg" /> semigroup <img src="3-2340095\d758dd5e-032a-419e-9af7-8b67ac9e302e.jpg" /> associated with initial value problem (3.1) satisfies<img src="3-2340095\4b38a953-f928-4621-8e80-c2f76b8b82f1.jpg" />, that is, there exists <img src="3-2340095\1b8b9101-9b9d-4ce9-98df-b379f56e29dd.jpg" /> and <img src="3-2340095\460878d8-64db-4b44-90aa-beb258bbbee7.jpg" /> , for any <img src="3-2340095\9d1ff9bc-10eb-418a-8702-151c942c2f8d.jpg" /> such that</p><p><img src="3-2340095\5eebd522-af50-474b-8740-b62e465e5d41.jpg" /></p><p>Proof. Let <img src="3-2340095\bffafe29-d55b-44af-b432-a02b1efafed3.jpg" /> be the eigenvalues of <img src="3-2340095\a8bca98e-52f4-43a7-b0b3-c8ccb093819d.jpg" /> and <img src="3-2340095\9829ddf8-1bff-4eda-af50-26e0493bd022.jpg" /> be the corresponding eigenvectors, <img src="3-2340095\8213a8e4-5dbc-4974-aaaa-3c5ca6d74411.jpg" />, without loss of generality, we can assume that<img src="3-2340095\878ade82-39b0-46c0-8788-88d62d3d735f.jpg" />, and<img src="3-2340095\55c6186a-1263-4ff5-a072-352ead30c2a8.jpg" />.</p><p>It is well known that <img src="3-2340095\f653aac2-5136-4e19-b7c9-1f4f4545edc4.jpg" /> form an orthogonal basis of<img src="3-2340095\6486fa36-328f-4220-9b60-f361b04330f7.jpg" />. We write</p><p><img src="3-2340095\0d5c5c15-b4d6-4069-842e-60b7dce55c87.jpg" /></p><p>Since <img src="3-2340095\e2e11bbd-b4fb-4f1b-acab-10e6ae28108e.jpg" /> and <img src="3-2340095\2317f71d-729a-4ec6-97b7-41e3049b61f5.jpg" /> is compact, for any<img src="3-2340095\aa16b071-72ae-4394-9969-d64a96537ec3.jpg" />, there exists some <img src="3-2340095\45cacacb-ad2e-4125-8030-bd4135177401.jpg" /> such that</p><disp-formula id="scirp.40276-formula79017"><label>(3.23)</label><graphic position="anchor" xlink:href="3-2340095\30f5ca3c-0234-43f0-9b60-48888e21c714.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.40276-formula79018"><label>(3.24)</label><graphic position="anchor" xlink:href="3-2340095\21fe5ed6-61da-4d87-a02b-5dec82c9ce14.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="3-2340095\1ae81d8c-8213-43e6-9c20-ea93ea93acf8.jpg" /> is orthogonal projection and <img src="3-2340095\9003af03-c8fe-4d66-b7c8-bde34cff0154.jpg" /> is the radius of the absorbing set. For any<img src="3-2340095\ff6c3101-1ee2-4ae7-9251-5348b385cbc0.jpg" />, we write</p><p><img src="3-2340095\d564cefe-c007-4b64-b274-703468cd4d13.jpg" /></p><p>We note that</p><p><img src="3-2340095\3325999b-c992-41e2-9eb1-b0df130b77e1.jpg" /></p><p>Taking the inner product of the second equation of (3.1) with <img src="3-2340095\b42c9da9-d434-47a8-9d78-77168aa0b4fc.jpg" /> in<img src="3-2340095\e96dbeb9-d3a9-4dcb-9ba4-5c1dde6b6165.jpg" />, After a computation like in the proof of Theorem 3.1, we can yield that</p><disp-formula id="scirp.40276-formula79019"><label>(3.25)</label><graphic position="anchor" xlink:href="3-2340095\0b0a5575-aec8-474c-9671-592b26f1b1a5.jpg"  xlink:type="simple"/></disp-formula><p>This is the same as in the proof of the Theorem 3.1, except for a replacement of <img src="3-2340095\9813d03b-ab15-43c1-a38e-406dd1249727.jpg" /> with<img src="3-2340095\601d8e6f-270e-49cb-9cd0-d198497683c0.jpg" />. Combined with (3.23) , (3.24) and (3.4), then we have</p><p><img src="3-2340095\296bc47d-b01d-4705-9332-7dc4912f7039.jpg" /></p><p>Choose <img src="3-2340095\a6bf3108-f189-4042-845b-66949ace4986.jpg" /> , we can get</p><p><img src="3-2340095\f46e0e0b-922c-459c-80b8-8156c2483d31.jpg" /></p><p>By Gronwall lemma, we can obtain</p><p><img src="3-2340095\7bf25ea6-6c28-444a-a91d-4a22c237ac46.jpg" /></p><p>for all <img src="3-2340095\83a7bf26-3d48-4017-8c42-7d0132cce13c.jpg" /> and<img src="3-2340095\4fe4ad7b-f9ce-4b17-8648-3f3f8657fd31.jpg" />. This shows that Condition C is satisfied, and the proof is completed.</p><p>Due to Lemma 2.1, Theorem 3.1 and Theorem 3.2, we obtain the following Theorem</p><p>Theorem 3.3 Assume that the hypotheses on <img src="3-2340095\e06addfb-23ac-4d13-8e2a-b4c4cf49d126.jpg" /> and <img src="3-2340095\283d31ec-fba4-46fe-99ed-fc32aab86989.jpg" /> hold for all<img src="3-2340095\ae629638-0a82-422b-8a81-4c5f207be843.jpg" />, <img src="3-2340095\ec043256-98bd-4eb5-87c0-aa2884fb7599.jpg" />are positive constants. Then the <img src="3-2340095\2d6584b2-0341-46de-9229-6f6fc9d0b3bc.jpg" /> semigroup <img src="3-2340095\397378f3-a606-45cb-8013-1673f51f39e6.jpg" /> associated with initial value problem (3.1) has a global attractor in E. &#160;</p></sec><sec id="s4"><title>4. Existence of the Pullback Attractor</title><p>In this subsection, we assume that<img src="3-2340095\e26d0f77-a923-49f8-8d59-0e34c1bf8cac.jpg" />, we aim to study the pullback attractor for the initial value problem (1.1).</p><p>From Theorem 3.1, the initial value problem (1.1) generates a family two-parameter semigroup <img src="3-2340095\c93a4ca3-a8e8-403e-bbd4-5df54dbfd7ea.jpg" /> in<img src="3-2340095\529ba3b5-52a4-44f6-9206-aefcc6a6f90d.jpg" />, which can be defined by</p><p><img src="3-2340095\45799111-d589-4aaf-917a-25d855f301bb.jpg" /></p><p>Lemma 4.1 Let <img src="3-2340095\1ce54835-ea36-4353-b92d-fe1bffe636d8.jpg" /> be the two initial values for the problem (1.1), <img src="3-2340095\4fcaade2-6fb1-4b1a-a472-131d0616984f.jpg" />is the initial time, Denote by <img src="3-2340095\472b8faa-f079-417f-aab5-20b98b921192.jpg" /> and <img src="3-2340095\99382fc6-77f1-47fc-878f-856a4fb48426.jpg" /> the corresponding solutions to (1.1). Then, there exists a constant <img src="3-2340095\8d681a88-12f5-4571-838b-b220115fc8ca.jpg" /> which is independent of initial value value and time, such that the following estimates hold:</p><disp-formula id="scirp.40276-formula79020"><label>(4.1)</label><graphic position="anchor" xlink:href="3-2340095\28e7795b-a9e0-4dcb-b337-549da7efb27c.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.40276-formula79021"><label>(4.2)</label><graphic position="anchor" xlink:href="3-2340095\3f2cde81-6a27-4e08-8141-6405647bed57.jpg"  xlink:type="simple"/></disp-formula><p>Proof. We denote<img src="3-2340095\1cf03fe1-2fd2-4867-92d6-e5b11473b8c8.jpg" />, by (3.22), we can get (4.1) easily.</p><p>If we consider<img src="3-2340095\9bd338cc-a57f-4801-8ea5-9d0940105375.jpg" />, then <img src="3-2340095\75f1cf5d-7c1c-475b-9a48-1983d035baea.jpg" /> for any<img src="3-2340095\01e243fe-4f1c-4c70-b4e6-4c541e9099ac.jpg" />, and</p><p><img src="3-2340095\fcd7a969-3495-45d2-a52e-92902b8e5982.jpg" /></p><p>Thus,<img src="3-2340095\d8128511-b310-4d1f-a5d9-eb7151a98be8.jpg" />.</p><p>Theorem 4.1 The mapping <img src="3-2340095\2d18e754-f9b8-4a5e-9c3b-e21280788f2c.jpg" /> is continuous for any<img src="3-2340095\2046fe0e-9cf5-431c-85ed-382f5934de25.jpg" />.</p><p>Proof. Let <img src="3-2340095\2f9dfedc-2cc4-4012-916a-cec00afbb7e1.jpg" /> be the initial value for the problem (1.1) and<img src="3-2340095\2138990c-bde4-4d62-b03b-2547dd17aef3.jpg" />. Denote by <img src="3-2340095\528cdcd3-e633-4449-9207-dd28b4efd251.jpg" /> and <img src="3-2340095\81666f92-d274-4651-a216-978bb7e5faef.jpg" /> the corresponding solutions to (1.1). Then, writing again <img src="3-2340095\b330d9f2-ab59-4d73-91db-0bc2ed7f3477.jpg" /> we obtain the following. If<img src="3-2340095\58d85a0d-2bce-4cd7-93a8-9948b8b9ed31.jpg" />, then <img src="3-2340095\cde41bde-2706-4bb7-993a-b1d9fca1e33a.jpg" /> and</p><p><img src="3-2340095\53bcff2a-1252-49c8-b711-2e462f185cdb.jpg" /></p><p>Thus, we have</p><p><img src="3-2340095\1248e4ef-2b23-42b2-a6cb-acd689f5fa4f.jpg" /></p><p>whence</p><p><img src="3-2340095\c01fb2a1-90a4-453c-88aa-f0a62feb1e09.jpg" /></p><p>which implies the continuity of<img src="3-2340095\22bf9a97-97ca-4de6-99b4-60a79c6ec9b4.jpg" />.</p><p>Theorem 4.2 Assume that the hypotheses on <img src="3-2340095\ef925367-f2fd-4bd0-b1c4-0150fda6fe07.jpg" /> and <img src="3-2340095\e2cf01ee-d3fe-452d-b06b-c3379f9b1b72.jpg" /> hold with<img src="3-2340095\3851d240-bb75-4750-8bd1-f1300963443a.jpg" />, <img src="3-2340095\d0af2295-25d6-4102-825c-c051038638c0.jpg" />are the positive constants.</p><p>Suppose in addition that<img src="3-2340095\6ff0d4c9-e1f6-4797-8316-a282fb500f18.jpg" />. Then exists a family <img src="3-2340095\456bf619-3e1a-47f6-bad6-f09897a6ce19.jpg" /> of bounded sets in <img src="3-2340095\d30332b5-4925-496c-9c3f-d28092a7f0bc.jpg" /></p><p>which is uniformly pullback absorbing fir the process<img src="3-2340095\ece77675-6efc-46d0-b3f6-d74d175bfb0f.jpg" />. Moreover, <img src="3-2340095\4f67e11b-c3be-4513-9a80-fbcb130368ce.jpg" />for all<img src="3-2340095\e6409adb-57b7-4c33-acf3-de00a41b73bd.jpg" />, where <img src="3-2340095\d51388fd-199b-43ac-96ae-f540060e3c4d.jpg" /> is the bounded set in<img src="3-2340095\1b9f6bc1-aba1-4b8c-836e-5d7a3eef2f3d.jpg" />.</p><p>Proof. By (3.18), we can have</p><p><img src="3-2340095\8910a396-3857-46a5-8670-6db722d2d4ac.jpg" /></p><p>and, in particular,</p><disp-formula id="scirp.40276-formula79022"><label>(4.3)</label><graphic position="anchor" xlink:href="3-2340095\3570a9f3-45eb-43c9-bbc4-08b71a5cf62e.jpg"  xlink:type="simple"/></disp-formula><p>Moreover, as <img src="3-2340095\10383c3a-01b7-42a5-b2c6-2847799e7e75.jpg" /> and <img src="3-2340095\221c6dfb-456e-4204-b6d4-f68c33e1e664.jpg" /> for<img src="3-2340095\adb61a6c-7232-4e4b-b7f5-7cd29fbbbf42.jpg" />, then inequality (4.3) holds true for<img src="3-2340095\fdc843b3-997f-4acb-b33f-c10ae7f9b075.jpg" />.</p><p>If we take now<img src="3-2340095\c6e66083-1f31-4231-ae84-25479307289d.jpg" />, then for all <img src="3-2340095\f99a23d2-0fc4-48d3-bcd0-ca7fc9d2a6b1.jpg" /> we have <img src="3-2340095\118ef0ab-1ff4-4079-8241-2d26f1bf8cab.jpg" /> and so</p><disp-formula id="scirp.40276-formula79023"><label>(4.4)</label><graphic position="anchor" xlink:href="3-2340095\ccf71907-1eae-4164-ac7b-2d6d0c555c00.jpg"  xlink:type="simple"/></disp-formula><p>or, in other words,</p><p><img src="3-2340095\363c8bf9-a23c-461c-bc9d-5d0014ac0679.jpg" /></p><p>Therefore, there exists <img src="3-2340095\e2de1ce3-a734-443d-918c-bfbff308225b.jpg" /> such that</p><p><img src="3-2340095\205c80b3-f590-4ca3-9221-5ed982cef177.jpg" /></p><p>which means that the ball <img src="3-2340095\0a0a967b-57b0-48b0-9cc7-550d37057120.jpg" /> is uniformly pullback absorbing for the process<img src="3-2340095\e5afb135-0b93-4609-a9e1-e4207cefb51b.jpg" />.</p><p>Remark: On the one hand, observe that if <img src="3-2340095\eac18ce9-9780-49aa-95d9-cc7ebde52711.jpg" /> and<img src="3-2340095\f6624128-86dc-450e-807a-820431c1309c.jpg" />, then</p><p><img src="3-2340095\67caa570-2c48-411a-a96b-22b4f4f43107.jpg" /> and</p><p><img src="3-2340095\1716b9f5-730e-4a51-b4fe-23f8363a0c06.jpg" /> with</p><p><img src="3-2340095\15df9db2-5da3-43d6-88c6-f5936ee3e08b.jpg" />. As a sequence of (4.4) we have</p><p><img src="3-2340095\0b0b2e4a-0b83-4d0f-91e0-d410ca535b50.jpg" /></p><p>or ,we have <img src="3-2340095\532cf5f4-5781-48d4-8ce2-be13b70e4b3f.jpg" /></p><p><img src="3-2340095\a1b90283-b104-41ab-92d2-03f5019f756a.jpg" /></p><p>On the other hand, (4.3) implies,</p><p><img src="3-2340095\265accac-0160-46a0-95da-a08ddec038d1.jpg" />,</p><p><img src="3-2340095\27713d2a-26bb-48ff-b383-47ba4f167f14.jpg" /></p><p>Theorem 4.3 Under the assumption in Theorem 4.1. Then there exists a compact set <img src="3-2340095\1f2724c3-8994-4479-98cd-e12f982405f9.jpg" /> which is uniformly pullback attracting for the process<img src="3-2340095\f0dfdc83-4f0b-4460-9e8a-461031ccbf0e.jpg" />, and consequently, there exits the pullback attractor.</p><p><img src="3-2340095\589a648a-dae7-4ef6-88ba-859b173a1ef1.jpg" />. Moreover, <img src="3-2340095\e7d32780-fced-4e69-b349-2b0693d91eed.jpg" />for all<img src="3-2340095\f54fa62d-592c-4ad9-a373-607b53a45c4f.jpg" />.</p><p>Proof. For each<img src="3-2340095\72b92b0f-9882-40a5-b629-841721af122b.jpg" />, the norm</p><p><img src="3-2340095\31a9f730-d401-4cea-a5f0-9a8e1a09e5fa.jpg" />is equivalent to</p><p><img src="3-2340095\e65fb9cc-275b-4b5f-afe0-11a8a645a371.jpg" />. This allows us to obtain absorbing ball for the original norm by proving the existence of absorbing balls for this new norm for some suitable value of<img src="3-2340095\997daaa8-b50c-4621-8fca-67dc1cb9b4bd.jpg" />.</p><p>Indeed, let us denote<img src="3-2340095\5ef90ccd-0fce-4750-a643-467b2703c30e.jpg" />. Noticing that for <img src="3-2340095\fab7b181-5e71-4cbf-bb69-496a91391880.jpg" /> it follows that</p><p><img src="3-2340095\5a23486c-fd2b-4e20-b410-05436174c85f.jpg" /></p><p>we then have <img src="3-2340095\b66eb734-2220-45e9-9b3e-adaf7f6f203d.jpg" />.</p><p>Let <img src="3-2340095\2b67a871-c20a-4c50-97d5-b8b1037e4ea1.jpg" /> be a bounded set, i.e. there exists <img src="3-2340095\1c3671fa-95d7-4a1c-9ad5-30208e58d8fa.jpg" /> such that for any <img src="3-2340095\db237256-1b5e-4578-b3db-0e04f4df4cd0.jpg" /> it holds</p><p><img src="3-2340095\268f11d7-2d7c-43d8-aade-edb251bc9b7c.jpg" /></p><p>Denote by <img src="3-2340095\f5d24845-5f05-40b6-9e79-1167fca8992f.jpg" /> the solution of the problem (2.1), and consider the problems:</p><disp-formula id="scirp.40276-formula79024"><label>(4.5)</label><graphic position="anchor" xlink:href="3-2340095\08c35507-dc84-4170-ab24-595bd9e8a8e9.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.40276-formula79025"><label>(4.6)</label><graphic position="anchor" xlink:href="3-2340095\e6db5e0b-724d-4ecc-9c8f-52025b5e1956.jpg"  xlink:type="simple"/></disp-formula><p>From the uniqueness of the solution of problems (2.1), (4.5) and (4.6) it follows that</p><p><img src="3-2340095\efd04ccb-2690-4722-ae09-4c45b9232e9b.jpg" /></p><p>Consequently, <img src="3-2340095\d5b5f910-a303-4421-8cf0-4250da7a991a.jpg" />can be written as</p><p><img src="3-2340095\afd312cd-8f3e-4bda-a55a-a2e72ed14e0e.jpg" /></p><p>where <img src="3-2340095\807cce07-38ec-4a89-b2a6-77883506a08c.jpg" /> and <img src="3-2340095\610795b3-2125-41e4-b1c1-e8f245bccba4.jpg" /> are the solutions of (4.5) and (4.6) respectively.</p><p>First, thanks to (4.4), but with<img src="3-2340095\ab369adf-2931-437f-89ad-e5954ee528ee.jpg" />, it follows that</p><disp-formula id="scirp.40276-formula79026"><label>(4.7)</label><graphic position="anchor" xlink:href="3-2340095\1c9979d6-a652-46f8-822b-d8afe55c19f8.jpg"  xlink:type="simple"/></disp-formula><p>Furthermore, for <img src="3-2340095\1ec0b2d2-6735-4d78-83f0-cf887ff60fb7.jpg" /> and<img src="3-2340095\afc63546-506a-405b-9b55-ca57bafae8a5.jpg" />,</p><p><img src="3-2340095\93feb130-860a-4061-aaf4-9a6487fc7975.jpg" /></p><p>with<img src="3-2340095\3dbdcb92-a63b-43bb-ae2a-5d427261cf2c.jpg" />. Thus, Equation (4.7) implies in particular</p><p><img src="3-2340095\5e3e598a-1c48-4085-bfa2-77f051d2e806.jpg" /></p><p>Then we can obtain that</p><p><img src="3-2340095\17ef3759-50ad-4a7d-9a19-11f60a50aa87.jpg" /></p><p>whence,</p><p><img src="3-2340095\e9d7399b-779a-4d7f-9ba6-e2b676ee8092.jpg" /></p><p>Next, fix <img src="3-2340095\79d5d4b6-9598-41fc-ab27-333941267b5e.jpg" /> and denote</p><p><img src="3-2340095\e96ddaad-aa19-4112-a43d-f673227a6df3.jpg" /></p><p><img src="3-2340095\0fae79df-2296-4ce5-b828-a7b4423b2b9b.jpg" /></p><p>Then, for<img src="3-2340095\5f6c18e1-070d-407a-a36b-4a84222cf4ba.jpg" />,</p><disp-formula id="scirp.40276-formula79027"><label>(4.8)</label><graphic position="anchor" xlink:href="3-2340095\64aa431e-c2d4-4beb-80c4-43e436bf966c.jpg"  xlink:type="simple"/></disp-formula><p>and for<img src="3-2340095\eb8b7f26-f4d4-476b-a229-d4bcd7e6d8bf.jpg" />, we have</p><disp-formula id="scirp.40276-formula79028"><label>(4.9)</label><graphic position="anchor" xlink:href="3-2340095\64af6891-9669-4f50-b4c2-d63e119d1475.jpg"  xlink:type="simple"/></disp-formula><p>Then, we deduce from the assumption on <img src="3-2340095\672e72da-5a4d-4dbb-9bc5-dab80f041f54.jpg" /> that</p><p><img src="3-2340095\ac82b83d-d6de-43c8-85d7-9bf6c6a32343.jpg" />and</p><p><img src="3-2340095\47a41257-1022-4642-8434-1ab181443f83.jpg" />. Arguing as we did in order to obtain (4.8) and (4.9), we have</p><disp-formula id="scirp.40276-formula79029"><label>(4.10)</label><graphic position="anchor" xlink:href="3-2340095\acc5778c-5a65-4b29-bb1c-b04da3aac71c.jpg"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.40276-formula79030"><label>(4.11)</label><graphic position="anchor" xlink:href="3-2340095\e6e2ace4-293b-4394-b064-d7bb86b8c5e2.jpg"  xlink:type="simple"/></disp-formula><p>Let us denote</p><p><img src="3-2340095\54d335a8-d51a-4b3e-8f86-d847dc7e8a33.jpg" />and make use of the estimates in Theorem 4.2. On the one hand, for all<img src="3-2340095\42aefe55-2451-477f-a04c-f60eba01a15e.jpg" />,</p><p><img src="3-2340095\4ca2982b-55f0-4fb9-85ee-7df91213f444.jpg" /></p><p>but, as (4.4) and (4.7) ensure</p><p><img src="3-2340095\d0e5753b-0491-4f8f-a73e-ab9a169e0890.jpg" /></p><p>if we denote by</p><p><img src="3-2340095\371bf5ef-2ece-4485-91f8-3783ae288cae.jpg" /></p><p>then, in particular,</p><p><img src="3-2340095\1bd855a2-c346-43e5-8a80-8fd600aa5637.jpg" />.</p><p>Noticing that<img src="3-2340095\c9ecd0df-4ab5-43d3-9779-d3ff43552768.jpg" />, the Gronwall lemma leads us to</p><p><img src="3-2340095\a714f78f-2aab-4c61-9b98-138c298fff45.jpg" /></p><p>On the other hand, if<img src="3-2340095\38592ced-3c3d-46bc-b5f8-4b962001d4c0.jpg" />, we deduce that</p><p><img src="3-2340095\671c5a3c-e48b-4f0d-ab59-ce08bb82cde2.jpg" /></p><p>and, from (4.8) and (4.10),</p><p><img src="3-2340095\cab209eb-c192-4f02-97bb-6c35ae6820fd.jpg" /></p><p>Once again, the Gronwall lemma implies that</p><p><img src="3-2340095\88eddedf-ada8-470f-bce8-276f27ba884f.jpg" /></p><p>Then, there exists <img src="3-2340095\df063ee2-b5e1-4041-801c-24cf67c9ffe3.jpg" /> such that, if<img src="3-2340095\a00a21fd-6e30-460a-a613-019677e2b416.jpg" />,</p><p><img src="3-2340095\3dda7bb9-6fb0-4911-81be-4544dc5ab2fa.jpg" /></p><p>Recalling that<img src="3-2340095\0f0fa12d-e56d-4a3e-9129-60aecd9ea3ac.jpg" />, if we fix<img src="3-2340095\d524fa69-800f-4f1c-b52e-bc634d9110a7.jpg" />, take <img src="3-2340095\de29e4eb-637a-4981-97ca-b873055f9213.jpg" /> and denote <img src="3-2340095\65a34fae-456b-4449-af49-64616f679637.jpg" /> we have, provided <img src="3-2340095\1942a9b6-e937-488f-86ff-65b97077be63.jpg" /> is large enough, that &#160;</p><p><img src="3-2340095\016d1f8d-9d8e-432a-af87-8bfb26036c53.jpg" /></p><p>In conclusion, there exists <img src="3-2340095\e04eed22-8ab2-4462-811c-a14015a8c2a1.jpg" /> such that for all<img src="3-2340095\f4e8c1cb-8189-4fd7-8f64-809eb4b4a598.jpg" />, and all<img src="3-2340095\1909cd04-34e8-47b7-bda1-9a8afac3b1b4.jpg" />,</p><p><img src="3-2340095\1705fdf6-89f9-4fb1-8111-6181eb31a752.jpg" /></p><p>Denoting<img src="3-2340095\64acb122-cc4d-457c-9fec-e3a2820ee898.jpg" />, we have for all <img src="3-2340095\8b2cc69d-0697-4e82-a916-911801347bc8.jpg" /></p><p><img src="3-2340095\a6830231-2679-4c89-8acb-758969602c04.jpg" /></p><p>where</p><p><img src="3-2340095\58f66b39-c2d0-4e12-b132-a04560b217bd.jpg" />.</p><p>But as for all <img src="3-2340095\31f4a6b8-3f09-4019-b799-25bf8d73223e.jpg" /> and<img src="3-2340095\deac1f1f-5a08-4a79-b745-c24520a4c55c.jpg" />, we get <img src="3-2340095\991a8cf5-1d4c-418c-ba66-2e4ac16a97f9.jpg" /> and<img src="3-2340095\192a1911-4f86-4610-a73c-de6cd90cb751.jpg" />, and, consequently, for all <img src="3-2340095\4fcbe05d-2f63-427b-b7db-104511f8186d.jpg" /> and<img src="3-2340095\784394ec-72ef-4274-aeac-9fd950f50531.jpg" />,</p><p><img src="3-2340095\232c588c-5650-4b5d-8e8f-718325eefa23.jpg" /></p><p>which shows that</p><p><img src="3-2340095\827b46e7-ccc4-4493-8930-d1c9d151ba52.jpg" /></p><p>for all <img src="3-2340095\0a45f51b-3128-4064-8a07-cece49ced4d4.jpg" /> and<img src="3-2340095\66078a15-3d96-413a-803d-7b8de125b6be.jpg" />. This means that the all</p><p><img src="3-2340095\3d4ac1d5-8fef-478e-826b-a532b3a07c8c.jpg" />is the bounded set in <img src="3-2340095\702136f0-e2a0-4e06-9bd3-9d0247c163f1.jpg" /></p><p>which , in addition, is uniformly absorbing for the family of operators<img src="3-2340095\2c51a07e-cbad-4a4b-acdf-41bdd72b8886.jpg" />. As <img src="3-2340095\04eef518-b40e-4191-81e7-ddd89bb8cf53.jpg" /> is the bounded set in<img src="3-2340095\5349aa75-5af9-4876-84ad-712b35f3ac08.jpg" />, then there exists <img src="3-2340095\ec27bf04-bf9b-44a0-affd-142cc0574618.jpg" /> such that</p><p><img src="3-2340095\57e43a2e-a411-48b6-a3ac-067dc487faec.jpg" /></p><p>and, therefore, the bounded set <img src="3-2340095\702065ff-5b0d-4ec3-ac58-112acbdd9ef2.jpg" /> given</p><p><img src="3-2340095\84417ff3-ff7f-4d3b-bbf8-bd84ae426a07.jpg" /></p><p>is uniformly pullback absorbing for <img src="3-2340095\78b4a69c-f8c8-4f4f-bf3a-a1af69643424.jpg" /> in<img src="3-2340095\08094a92-024b-4b2c-94cb-db394a633450.jpg" />.</p><p>By Ascoli-Arzel&#224; theorem, we can prove that <img src="3-2340095\f8811f8a-6b92-4ff5-8a1a-60b1d6d14e03.jpg" /> is compact, so <img src="3-2340095\a687bc14-ab76-47dd-ba13-21015514bfe8.jpg" /> is a family of compact subsets in<img src="3-2340095\4a1a9372-ae08-4a50-95b7-1e8b3ff704d6.jpg" />, which is also uniformly pullback attracting for<img src="3-2340095\af9e4562-305d-4a3b-adc7-b82d9b46048f.jpg" />, and the proof has been completed.</p></sec><sec id="s5"><title>REFERENCES</title></sec><sec id="s6"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.40276-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">J. 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