<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2012.312256</article-id><article-id pub-id-type="publisher-id">AM-25441</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>
 
 
  A Model of Spatial Spread of an Infection with Applications to HIV/AIDS in Mali
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>uaténi</surname><given-names>Diallo</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>Yaya</surname><given-names>Koné</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>Jérôme</surname><given-names>Pousin</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Faculté des Sciences et Techniques, USTTB, Bamako, Mali</addr-line></aff><aff id="aff2"><addr-line>Institut Camille Jordan, INSA de Lyon, Lyon, France</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>ouateni@yahoo.fr(UD)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>12</day><month>12</month><year>2012</year></pub-date><volume>03</volume><issue>12</issue><fpage>1877</fpage><lpage>1881</lpage><history><date date-type="received"><day>July</day>	<month>27,</month>	<year>2012</year></date><date date-type="rev-recd"><day>November</day>	<month>21,</month>	<year>2012</year>	</date><date date-type="accepted"><day>November</day>	<month>29,</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 introduce a classical SI model to capture the spread of an infectious disease within a population. More precisely, the spatial diffusion of HIV/AIDS in a population is modeled. For that, we assume that the spread is due to the anarchical comportment of infected individuals along a road, especially, “lorry drivers”. The question which consists of the control of the infection is also addressed. Infected individuals moving from a town to another one, the diffusion is then anisotropic with a main direction of propagation, namely the road direction. Using a semi-group argument and a maximum principle, the uniqueness of a solution to the problem is established. This solution is also estimated. We end this paper by considering some numerical experiments in the case of HIV/AIDS spread in Mali along a road connecting two towns.
 
</p></abstract><kwd-group><kwd>Spacial Spread of Infections; Controlability; Maximum Principle</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Let <img src="6-7401010\79eea4e9-a4fd-4ad7-b095-e13ff4ff69f7.jpg" /> be an open bounded lipschitzian domain of <img src="6-7401010\8b59eb23-b51a-4d62-84d0-e3cab0798691.jpg" /> satisfying the cone property in which it will be assumed that the population is fixed. To describe the disease transmission, a traditional <img src="6-7401010\b7536ac3-b84b-4382-a70d-2003b0bae1c7.jpg" /> model is introduced. Each member of the population is supposed to belong to one of the these two classes: Susceptible individuals (denoted by<img src="6-7401010\42e033c1-9c2b-4988-ab83-2ff049c2ed15.jpg" />) or Infected individuals (denoted by<img src="6-7401010\1c26fd45-6e83-40b8-b1dd-b4b3b57559ba.jpg" />). Each individual which begins in the class<img src="6-7401010\34cb5c77-782e-44dc-9022-2fb0288b65bb.jpg" />, moves to the class<img src="6-7401010\4c491be9-309e-42a4-970a-5cf2a08a3391.jpg" />, having had a contact with an infected person. Infected individuals eventually recover from the disease due to a medical treatment. The disease is assumed to be transmitted from infected to susceptible individuals with a probability<img src="6-7401010\15ba0512-7786-4a46-8c39-f02578373242.jpg" />, by a “mass action” contact term and spreads spatially with the coefficient<img src="6-7401010\7345293b-3656-442b-9deb-1ea0eb59101c.jpg" />. The infected individuals are assumed to recover at a per capita rate of<img src="6-7401010\e4c2d418-9ae9-4fbb-86ea-c6e2dabb4020.jpg" />. Demographic changes are neglected under the assumption that the duration of the epidemic is short in comparison with the average life span of an individual. Assuming these assumptions to be relevant, we suppose that the following holds: there are positive constants</p><p><img src="6-7401010\f63dfed0-a652-4275-9c1c-4f0a0926c512.jpg" /></p><p>such that functions <img src="6-7401010\1641be98-a32a-4de7-8f8c-2ac0700ed8a7.jpg" /> and satisfy: <img src="6-7401010\890ac5f8-e999-45af-8219-780e29a1b9e2.jpg" /></p><p><img src="6-7401010\9cb6c509-b30f-48d9-b636-24d55cde9043.jpg" /></p><p><img src="6-7401010\9d2e9267-60c5-47ad-8192-ab1f1de7245e.jpg" /></p><p><img src="6-7401010\ea800e4e-49b5-43d5-9fd4-a1a722566558.jpg" /></p><p>At an initial time<img src="6-7401010\4361112d-220e-41f3-aa1b-562b6c4fbe57.jpg" />, we have two nonnegative, regular <img src="6-7401010\f6353c74-2af9-450d-b280-21e592263b9d.jpg" /> functions satisfying:</p><p><img src="6-7401010\e3be7784-90b0-47a2-b945-7486f424ca5c.jpg" />;<img src="6-7401010\5ebfbe19-3681-4faf-ba04-9a187e1937bc.jpg" />.</p><p>The no flux boundary conditions mean that the system is isolated.</p><p>The propagation of the disease for a fixed <img src="6-7401010\305e3b30-1702-4818-8784-7097b5b10471.jpg" /> is governed by the following simple model:</p><disp-formula id="scirp.25441-formula125016"><label>(1)</label><graphic position="anchor" xlink:href="6-7401010\7d297237-e9f0-47d7-a90d-7e83b407a030.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="6-7401010\70a618e5-d844-48cf-8fe2-2a5b58ed5ddb.jpg" /> denotes the outward normal vector to<img src="6-7401010\bef1872e-b013-4f2e-9077-2119fc386223.jpg" />.</p><p>System (1) has also been used to modelling chemistry reactions (with a different sign in reaction term) [<xref ref-type="bibr" rid="scirp.25441-ref1">1</xref>] or combustion phenomenon.</p><p>Even if the dynamics of the system (1) is quite simple, the question we address in this work is: are there parameters that allow to control the system in a finite time in case where the spacial diffusion is directed? In [<xref ref-type="bibr" rid="scirp.25441-ref2">2</xref>] a model structured by spatial position in a bounded onedimensional environment is proposed and analyzed. The spatial mobility is assumed to be governed by random diffusion with coefficients <img src="6-7401010\611d40bd-6278-42d6-8e00-06b1ba870ebd.jpg" /> and <img src="6-7401010\732600d8-a19c-4a0d-a050-0390152138da.jpg" /> for the susceptible and infected individuals, respectively.</p><p>In the present paper, the susceptible population doesn’t move away, so that its diffusion coefficient is equal to zero. Many other models of epidemics with spatial diffusion are studied, see for example [3,4].</p><p>The paper is organized as follows:</p><p>In Section 2 some a priori estimates are derived for the solution <img src="6-7401010\45e9e8d0-51da-4983-96f4-7097b04880e4.jpg" /> of the system (1). In Section 3 the existence and uniqueness of solutions are studied. In Section 4, the existence of coefficients <img src="6-7401010\4e63136e-f919-48f2-9455-98269cdd5398.jpg" /> and <img src="6-7401010\31e28e46-589d-4d82-83ad-57744d02ff3a.jpg" /> allowing to control the system (1) in a finite time is derived. This section is ended with some numerical results which take into account the data of the spread of VIH/AIDS in Mali.</p></sec><sec id="s2"><title>2. A Priori Estimates</title><p>We denote by <img src="6-7401010\3410387b-534c-4cfd-8e04-317de0078875.jpg" /> (respectively,<img src="6-7401010\b6d9ce98-1249-447a-8df7-9ebd4ff21e48.jpg" />) the classical Sobolev space of order 1 (respectively, Sobolev space of order 2) [<xref ref-type="bibr" rid="scirp.25441-ref5">5</xref>]. Let <img src="6-7401010\22badaa3-dd67-443b-9a8b-91c4dfff8292.jpg" /> be fixed. By integrating the first equation of the system (1) we obtain</p><disp-formula id="scirp.25441-formula125017"><label>(2)</label><graphic position="anchor" xlink:href="6-7401010\808c09c9-e4db-4ac7-b1ac-1dc6413427ec.jpg"  xlink:type="simple"/></disp-formula><p>Definition 2.1. A pair of functions <img src="6-7401010\0932dffa-5bcd-47c9-8ffa-9c984172d2ea.jpg" /> defined on <img src="6-7401010\bd2dab68-d1a7-4a5d-b55e-0a6843e504e5.jpg" /> is said to be a solution to the system (1) whether</p><p><img src="6-7401010\af3b52dd-bcf4-42cf-b69c-453d62a7812a.jpg" /></p><p><img src="6-7401010\d9b4490e-a0ed-438f-ba61-e81feb5141b9.jpg" /></p><p>Lemma 2.2. Let <img src="6-7401010\d03402df-e040-41f5-89c5-5ab341144df7.jpg" /> be a solution of the system (1), then the following holds:</p><p><img src="6-7401010\9a1207bb-760c-4650-aec7-1e936bf86e3d.jpg" /></p><disp-formula id="scirp.25441-formula125018"><label>(3)</label><graphic position="anchor" xlink:href="6-7401010\c482d606-2ddd-4413-aa5c-443f962e0545.jpg"  xlink:type="simple"/></disp-formula><p>Proof. Define the function <img src="6-7401010\369074c2-ad96-4e60-8e4f-d75354611ba0.jpg" /> for<img src="6-7401010\1c71a505-a1f1-4eab-8031-71fa4cf7e672.jpg" />. A very easy computation provides the following equation, for the function<img src="6-7401010\a6881994-46b1-42de-8d6f-05e5ae1fed67.jpg" />,</p><disp-formula id="scirp.25441-formula125019"><label>(4)</label><graphic position="anchor" xlink:href="6-7401010\87cfb02d-ae69-444c-9092-043f71434685.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="6-7401010\0cddc818-0ef4-46da-bed0-72a3240beaa8.jpg" /> The weak maximum principle applies [<xref ref-type="bibr" rid="scirp.25441-ref5">5</xref>] and thus</p><disp-formula id="scirp.25441-formula125020"><label>(5)</label><graphic position="anchor" xlink:href="6-7401010\da77eb8d-fb52-4978-8944-1b1d4539e626.jpg"  xlink:type="simple"/></disp-formula></sec><sec id="s3"><title>3. Existence of a Solution</title><p>Existence of solution to (1) will be obtained using some classical arguments. Define the unbounded linear operator</p><disp-formula id="scirp.25441-formula125021"><label>(6)</label><graphic position="anchor" xlink:href="6-7401010\3df84a3c-9cd2-4b5d-99f6-0c46942e0f82.jpg"  xlink:type="simple"/></disp-formula><p>with homogeneous Neumann boundary conditions and where<img src="6-7401010\96ce8f13-38c0-42fc-ab76-13daa5725fa8.jpg" />.</p><p>It is well known that <img src="6-7401010\b48e648e-ea9f-4348-a4bf-00e05b03c791.jpg" /> is strongly elliptic and invertible [6,7]. Define the function</p><p><img src="6-7401010\49cb2354-5cac-4d88-a7fb-dcec0b6dc573.jpg" /></p><p>Lemma 3.1. Let</p><p><img src="6-7401010\d5a66b8f-7a66-41ff-abb3-31f9661af286.jpg" />be given. The operator</p><p><img src="6-7401010\7dfa2b59-e532-47fd-8dd5-94d180462484.jpg" /></p><p>which associates <img src="6-7401010\d58d5266-96e9-44c2-bca0-95fc1a687cf7.jpg" /> to <img src="6-7401010\75c2567e-6af6-4788-9f90-9de01a88c790.jpg" /> is Lipschitzian with a Lipschitz constant<img src="6-7401010\bc32ae9b-bc68-49a1-bbec-9fd759df3a26.jpg" />.</p><p>Proof. Since the function <img src="6-7401010\b1d7f50c-c6bd-405c-b6ab-ae03d5e6affe.jpg" /> is continuously differentiable, its derivative is bounded on<img src="6-7401010\20592419-fb9f-44df-b8ab-55a2f8fde64f.jpg" />. We then obtain the estimate by using the fundamental theorem of calculus.</p><p>Theorem 3.2. Assume that the assumptions on the functions<img src="6-7401010\bd7f7404-8b78-4305-82c3-06f5bb95dcab.jpg" />;<img src="6-7401010\c5c4f6f2-cde3-4be5-8d88-7c3b9f668a3c.jpg" />; <img src="6-7401010\259d4a73-a9a8-414b-8ea4-880409cb863c.jpg" />and <img src="6-7401010\6dc2f1d7-f15c-45d0-a637-fee6560ad851.jpg" /> hold. Then for all<img src="6-7401010\9c95ac28-acd6-4757-bbae-42f50746ccbb.jpg" />, the problem (1) has a unique solution<img src="6-7401010\216dbbb3-4a1f-4847-914b-54c6d4816247.jpg" />.</p><p>Proof. Problem (1) is rewritten in the following way:</p><disp-formula id="scirp.25441-formula125022"><label>(7)</label><graphic position="anchor" xlink:href="6-7401010\bb4c7d2b-8948-4237-8a3a-00b903babd0b.jpg"  xlink:type="simple"/></disp-formula><p>The operator <img src="6-7401010\0b631b8a-e332-47ad-9569-1f4e350832c3.jpg" /> generates an analytical semigroup. According to Lemma 2.2 we consider Problem (7) on a bounded subset of<img src="6-7401010\708626f2-fab2-4a39-ba76-3d3e8ba94b3b.jpg" />. From Lemma 3.1 we know that <img src="6-7401010\2f1f0538-1441-44ed-82d3-b8f0988f30d4.jpg" /> is Lipschitzian. Therefore, one obtains the existence and uniqueness of a solution by using Theorem 3.1 and 3.3 in [<xref ref-type="bibr" rid="scirp.25441-ref7">7</xref>].</p></sec><sec id="s4"><title>4. Controllability of Problem (1) with the Functions α and β</title><p>Problem (1) is expressed in <img src="6-7401010\fe412a9a-25bf-4e18-acb5-e24406ba6755.jpg" /> as:</p><disp-formula id="scirp.25441-formula125023"><label>(8)</label><graphic position="anchor" xlink:href="6-7401010\5cfd5cc2-2ff9-4d2d-adab-4b4afb3a9d45.jpg"  xlink:type="simple"/></disp-formula><p>Theorem 4.1. Assume that the assumptions on the functions<img src="6-7401010\7ec02244-ed12-4d4c-8c72-3d44517135f7.jpg" />;<img src="6-7401010\40056026-44bf-49b3-a7af-409e64caf669.jpg" />; <img src="6-7401010\f2aa1b4b-059f-4031-8c36-4c0ea4b0d943.jpg" />and <img src="6-7401010\a701c550-5686-4866-8f2c-edaf1533bb19.jpg" /> hold and that <img src="6-7401010\91f7eca5-950b-4581-8e58-59c1b305bd25.jpg" /> has <img src="6-7401010\16a8e2e3-61b8-463b-985c-6be30f4c8314.jpg" /> regularity. Let <img src="6-7401010\9ec09205-a821-4686-a798-f3deda4443ae.jpg" /> be given and let <img src="6-7401010\ab7848b7-f71d-401d-867c-8c1be7063850.jpg" /> be an open subset and let <img src="6-7401010\5e29c0d5-0ddf-468c-8a1a-3ee050b9cc15.jpg" /> be fixed. For <img src="6-7401010\665f17a7-9d51-420a-afc0-654fe54a5948.jpg" /> the solution to Problem (1) there is a real <img src="6-7401010\7c519c62-3c6f-4240-8071-c4e4263e9d19.jpg" /> such that, if the functions<img src="6-7401010\3c5706c9-33f2-4549-a3a0-f7dece5f01eb.jpg" />, <img src="6-7401010\1a7793f7-2347-4e72-97ee-54ee0d6b69cb.jpg" />satisfy the following condition:</p><disp-formula id="scirp.25441-formula125024"><label>(9)</label><graphic position="anchor" xlink:href="6-7401010\8e66b6d2-9017-4f14-a482-11d7791bff98.jpg"  xlink:type="simple"/></disp-formula><p>then<img src="6-7401010\4ba8f524-1266-4142-a863-a20c9380c0d2.jpg" />.</p><p>Proof. The solution to Problem (1) is a classical solution. Since the boundary of the domain <img src="6-7401010\ed64106f-4f30-452b-9e08-9fe4d5e0746d.jpg" /> is regular, from the theory of analytical semigroup, we know that</p><p><img src="6-7401010\4f3dbd5e-0ad1-4758-895d-ef1d326ca8d8.jpg" /></p><p>because the time derivative of <img src="6-7401010\d788257e-093d-4078-8e3f-94e79e3aaab3.jpg" /> is bounded in the graph norm of a fractional power of the generator <img src="6-7401010\9e19253a-1736-4735-9eca-6042f0996389.jpg" /> ([<xref ref-type="bibr" rid="scirp.25441-ref7">7</xref>] Chapter 2 Section 2.6 and Theorem 8.4.3). The strong maximum principle applies. Assume the maximum <img src="6-7401010\e57f6d2f-14e3-4a83-83da-1b47fa1588ad.jpg" /> of the function <img src="6-7401010\67475e83-7420-49db-ac93-096607089b6f.jpg" /> is reached at the point<img src="6-7401010\0004e81f-c45c-4720-840b-ab9bc0483f41.jpg" />, from Equation (8) we deduce that</p><disp-formula id="scirp.25441-formula125025"><label>(10)</label><graphic position="anchor" xlink:href="6-7401010\7618e4c9-7cf3-488b-bfa9-94057422224f.jpg"  xlink:type="simple"/></disp-formula><p>Since <img src="6-7401010\6a925fef-8302-4b0e-853e-3ec329dffcbb.jpg" /> is uniformly continuous, there is <img src="6-7401010\25d396ff-067e-4489-ae46-b68338091fa7.jpg" /> independent of <img src="6-7401010\7974483e-1577-4e0e-98e9-f7dfbc93bcfc.jpg" /> such that</p><p><img src="6-7401010\85b9006c-b3db-40ab-b5e5-c5a4f617084e.jpg" /></p><p>We have:</p><p><img src="6-7401010\28c703d3-19c9-453b-8ee6-e09e12df7362.jpg" /></p><p>and we get a contradiction.</p></sec><sec id="s5"><title>5. Numerical Applications and Discussions</title><p>In the following figures we give the isovalues of the infection in a two dimensional environment.</p><p><xref ref-type="fig" rid="fig1">Figure 1</xref> corresponds to the case in which the diffusion is isotropic.</p><p><xref ref-type="fig" rid="fig2">Figure 2</xref> corresponds to the unisotropic case. We can see in the two cases the spread of the infection.</p><p>Now we give some numerical results in order to show the effect of the medical care effort on the intensity of the epidemic in two different areas: site 1 and site 2, representing two cities with two different incidence rates.</p><p>In <xref ref-type="fig" rid="fig3">Figure 3</xref> we suppose that no effort for medical care is made.</p><p>In <xref ref-type="fig" rid="fig4">Figure 4</xref> we consider that the rates of medical care effort are <img src="6-7401010\c0dce1af-a75f-4bb6-aaad-669b544c0d8e.jpg" /> in the site 1 and <img src="6-7401010\d19eb264-2afd-413e-b666-5960aefd9074.jpg" /> in the site 2. Then we note a decrease of the intensity of the infection in all the two sites.</p><p>In <xref ref-type="fig" rid="fig5">Figure 5</xref> we consider a medical care effort rate <img src="6-7401010\7bb490b8-df46-4d5e-82fe-516411443c7e.jpg" /> in site 1 and <img src="6-7401010\bf91ab9c-898d-4184-aca4-1722369a188f.jpg" /> in the site 2. Then we note a decrease of the intensity of the infection in all the two sites. These results mean that all medical care effort in one of the regions contributes to the decrease of the epidemic in the other one.</p><p>In <xref ref-type="fig" rid="fig6">Figure 6</xref> we use simultaneously the same medical care effort rate in the two sites:<img src="6-7401010\7fa0b044-3375-454a-98ad-b5e6b32dde75.jpg" />, then we can see that the intensity of the infection decreases more.</p><p>These results show that we can control the spread of the epidemic if we augment the medical care effort. A best result can be obtained, in the two sites, if efficient actions are done simultaneously in the two sites.</p><p>Therefore, by a policy of education we can operate on</p><p>the incidence rate in the two sites and well control the spread of the infection (<xref ref-type="fig" rid="fig6">Figure 6</xref>(b) where <img src="6-7401010\c9a87234-a342-4fae-9fa5-0ea8bdd96905.jpg" />).</p><p>In this way, it will be important that the leaders in the countries of the same area define together their policies in the fight against HIV spread.</p><p>In conclusion, we can say that, in addition to the medical treatment, if in the two sites, we reduce the incidence rate by more sensitization, then we can expect that the epidemic is controllable. That must be an operational aim for the deciders to fight against the spread of VIH/AIDS.</p></sec><sec id="s6"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.25441-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">E. Maisse, “Analyse et Simulation Numérique de Phénomènes de Diffusion-Dissolution/Précipitation en Milieu Poreux, Appliquuées au Stockage de Déchets,” Thèse de doctorat, Université Claude Bernard-Lyon1, Lyon, 1998.</mixed-citation></ref><ref id="scirp.25441-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">G. F. Webb, “A Reaction-Difusion Model for a Deterministic Diffusive Epidemic,” Journal of Mathematical Analysis and Applications, Vol. 84, No. 1, 1981, pp. 150-161. doi:10.1016/0022-247X(81)90156-6</mixed-citation></ref><ref id="scirp.25441-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">L. Melkemi, A. Z. Mokrane and A. Youkana, “On the Uniform Boundedness of the Solutions of Systems of Reaction-Diffusion Equations,” Electronic Journal of Qualitative Theory of Differential Equations, Vol. 2005, No. 24, 2005, pp. 1-10. </mixed-citation></ref><ref id="scirp.25441-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">F. A. Milner and R. Zhao, “Analysis of an S-I-R Model of Epidemics with Directed Spatial Diffusion,” 2011. 
http://biblioteca.universia.net/html_bura/ficha/params/title/analysis-of-an-s-i-r-model-of-epidemics-with/id/46036797.html</mixed-citation></ref><ref id="scirp.25441-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">H. Brezis, “Analyse fonctionnelle,” Théorie et applications, Dunod, 2002. </mixed-citation></ref><ref id="scirp.25441-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">R. Dautray and J. L. Lions, “Analyse Mathématique et Calcul Numérique Pour les Sciences et les Techniques,” Vol. 3, Masson, Paris, 1985.</mixed-citation></ref><ref id="scirp.25441-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">A. Pazy, “Semigroup of Linear Operators and Applications to Partial Differential Equations,” Springer-Verlag, New York, 1983. doi:10.1007/978-1-4612-5561-1</mixed-citation></ref></ref-list></back></article>