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<Article>
<Journal>
<PublisherName>OICC Press</PublisherName>
<JournalTitle>Journal of Theoretical and Applied Physics</JournalTitle>
<Issn>2251-7235</Issn>
<Volume>18</Volume>
<Issue>5</Issue>
<PubDate PubStatus="epublish">
<Year>2024</Year>
<Month>10</Month>
<Day>26</Day>
</PubDate>
</Journal>
<ArticleTitle>Evolution of electromagnetic soliton during laser-plasma interaction in an electron-positron-ion plasma having constant density gradient</ArticleTitle>
<VernacularTitle></VernacularTitle>
<FirstPage>1</FirstPage>
<LastPage>10</LastPage>
<ELocationID EIdType="doi">10.57647/j.jtap.2024.1805.56</ELocationID>
<Language>EN</Language>
<AuthorList>
<Author>
<FirstName>Gaurav</FirstName>
<LastName>Kumar</LastName>
<Affiliation>Plasma Waves and Particle Acceleration Laboratory, Department of Physics, Indian Institute of Technology Delhi, New Delhi, India</Affiliation>
<Identifier Source="ORCID">https://orcid.org/0000-0002-8575-4236</Identifier>
</Author>
<Author>
<FirstName>Hitendra K.</FirstName>
<LastName>Malik</LastName>
<Affiliation>Plasma Waves and Particle Acceleration Laboratory, Department of Physics, Indian Institute of Technology Delhi, New Delhi, India</Affiliation>
<Identifier Source="ORCID">https://orcid.org/0000-0002-9432-8140</Identifier>
</Author>
</AuthorList>
<PublicationType>Journal Article</PublicationType>
<History>
<PubDate PubStatus="received">
<Year>2024</Year>
<Month>10</Month>
<Day>26</Day>
</PubDate>
</History>
<Abstract>Laser propagation in an electron-positron-ion (EPI) plasma medium having a constant densitygradient is studied for the soliton evolution in the presence of a parallelly applied strong magneticfield. In a nonlinear regime, laser-plasma interaction forms an electron density hill that movesbackward due to the density gradient. This hill localizes laser energy by the mechanism ofresonance absorption (ωl =ωpe) and remains stable for a longer period, qualifying for the evolutionof electromagnetic soliton. The position of the soliton from where it starts moving backwarddepends on the slope of the linear density variation. If the slope increases, then the position of thesoliton is closer to the plasma boundary (x = 0). Another interesting property of the soliton is thatits height decreases, and width increases as the temperature of plasma species rises. We simulatethis phenomenon of electromagnetic soliton evolution in 1-D and 2-D by using Particle-In-Cell(PIC) simulation using the EPOCH-4.17.10.</Abstract>
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<Param Name="value">Particle-In-Cell</Param>
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<Object Type="keyword">
<Param Name="value">Electron-Positron-Ion plasma</Param>
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<Object Type="keyword">
<Param Name="value">Resonance absorption</Param>
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<Object Type="keyword">
<Param Name="value">Electromagnetic soliton</Param>
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<Object Type="keyword">
<Param Name="value">Constant density gradient</Param>
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<Object Type="keyword">
<Param Name="value">Plasma species temperature</Param>
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