<?xml version="1.0" encoding="UTF-8"?>
<!DOCTYPE ArticleSet PUBLIC "-//NLM//DTD PubMed 2.7//EN" "https://dtd.nlm.nih.gov/ncbi/pubmed/in/PubMed.dtd">
<ArticleSet>
<Article>
<Journal>
<PublisherName>OICC Press</PublisherName>
<JournalTitle>Journal of Theoretical and Applied Physics</JournalTitle>
<Issn>2251-7235</Issn>
<Volume>20</Volume>
<Issue>5</Issue>
<PubDate PubStatus="epublish">
<Year>2026</Year>
<Month>10</Month>
<Day>31</Day>
</PubDate>
</Journal>
<ArticleTitle>Analysis of Electromagnetic Scattering from Double Metallic Rods Covered by Anisotropic Inhomogeneous Plasma via FE-BI Method</ArticleTitle>
<VernacularTitle></VernacularTitle>
<FirstPage></FirstPage>
<LastPage></LastPage>
<ELocationID EIdType="doi">10.57647/jtap.2026.2005.01</ELocationID>
<Language>EN</Language>
<AuthorList>
<Author>
<FirstName>Anis</FirstName>
<LastName>Soltani</LastName>
<Affiliation>Department of Laser and Photonics, Faculty of Physics, University of Kashan, Kashan, Iran</Affiliation>
<Identifier Source="ORCID"></Identifier>
</Author>
<Author>
<FirstName>Zeinab</FirstName>
<LastName>Rahmani</LastName>
<Affiliation>Department of Laser and Photonics, Faculty of Physics, University of Kashan, Kashan, Iran</Affiliation>
<Identifier Source="ORCID"></Identifier>
</Author>
<Author>
<FirstName>Ebrahim</FirstName>
<LastName>Heidari Semiromi</LastName>
<Affiliation>Department of Condensed Matter, Faculty of Physics, University of Kashan, Kashan, Iran</Affiliation>
<Identifier Source="ORCID"></Identifier>
</Author>
</AuthorList>
<PublicationType>Journal Article</PublicationType>
<History>
<PubDate PubStatus="received">
<Year>2026</Year>
<Month>10</Month>
<Day>31</Day>
</PubDate>
</History>
<Abstract>We investigate the scattering of linearly polarized plane electromagnetic waves from a system of two metallic cylinders covered by non‑uniform plasma layers, using the Finite Element–Boundary Integral (FE‑BI) method. The structure can be regarded as a plasma antenna. To better reflect practical conditions, we consider inhomogeneous plasma covers, since laboratory and atmospheric plasmas are typically non‑uniform. Introducing anisotropy and inhomogeneity in the plasma coating enhances the tunability and flexibility of the radar cross‑section (RCS). We analyze the total axial magnetic field, the RCS, and the backscattering RCS (BRCS) under variations of incidence angle, wavelength, polarization, external DC magnetic field, and plasma inhomogeneity. For comparison, the system is also examined without plasma coating and without magnetic field, to highlight the role of anisotropic inhomogeneous plasma layers. The validity of the FE‑BI method is confirmed by benchmarking our results against the Perfectly Matched Layer (PML) technique.</Abstract>
<ObjectList>
<Object Type="keyword">
<Param Name="value">Electromagnetic waves</Param>
</Object>
<Object Type="keyword">
<Param Name="value">Inhomogeneous plasma</Param>
</Object>
<Object Type="keyword">
<Param Name="value">Anisotropic plasma</Param>
</Object>
<Object Type="keyword">
<Param Name="value">Radar cross-section</Param>
</Object>
<Object Type="keyword">
<Param Name="value">FE-BI method</Param>
</Object>
<Object Type="keyword">
<Param Name="value">External magnetic field</Param>
</Object>
</ObjectList>
</Article>
</ArticleSet>