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<Article>
<Journal>
<PublisherName>OICC Press</PublisherName>
<JournalTitle>Journal of Theoretical and Applied Physics</JournalTitle>
<Issn>2251-7235</Issn>
<Volume>19</Volume>
<Issue>6</Issue>
<PubDate PubStatus="epublish">
<Year>2025</Year>
<Month>12</Month>
<Day>31</Day>
</PubDate>
</Journal>
<ArticleTitle>Study of the Electric Quadruple Moment of One-‎proton Halo Nucleus 8B by Using the Two-body ‎Model, the Collective Model and the Microscopic ‎Single-particle Shell Model</ArticleTitle>
<VernacularTitle></VernacularTitle>
<FirstPage></FirstPage>
<LastPage></LastPage>
<ELocationID EIdType="doi">10.57647/j.jtap.2025.1906.56</ELocationID>
<Language>EN</Language>
<AuthorList>
<Author>
<FirstName>Md. Mahbub Alam</FirstName>
<LastName>Mamun‎</LastName>
<Affiliation>Department of Physics, Mawlana Bhashani Science and Technology University, Santosh, Tangail, 1902, Bangladesh</Affiliation>
<Identifier Source="ORCID">https://orcid.org/0009-0005-2975-1478</Identifier>
</Author>
<Author>
<FirstName>Md. Sagor</FirstName>
<LastName>Mia‎</LastName>
<Affiliation>Department of Physics, Mawlana Bhashani Science and Technology University, Santosh, Tangail, 1902, Bangladesh</Affiliation>
<Identifier Source="ORCID">https://orcid.org/0009-0003-9737-8631</Identifier>
</Author>
<Author>
<FirstName>Tazul</FirstName>
<LastName>Islam</LastName>
<Affiliation>Department of Physics, Mawlana Bhashani Science and Technology University, Santosh, Tangail, 1902, Bangladesh</Affiliation>
<Identifier Source="ORCID"></Identifier>
</Author>
</AuthorList>
<PublicationType>Journal Article</PublicationType>
<History>
<PubDate PubStatus="received">
<Year>2025</Year>
<Month>12</Month>
<Day>31</Day>
</PubDate>
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<Abstract>The nuclear electric quadruple moment of the proton-rich weakly bound Boron-8 (⁸B) halo nucleus is investigated using three theoretical approaches: the microscopic single-particle shell model, the collective model, and the two-body model. These approaches provide a reasonable prediction of the quadruple deformation that occurred due to the core polarization and many-body effects. These approaches also provide how the extended proton distribution influences the quadruple moment. The experimental value of electric quadruple moment (Q) of 8B is 6.45 efm². While the calculated value using the two-body model is 6.86 efm² and the collective model gives 5.83 efm² and the microscopic single particle shell model gives 4.03 efm². The ⁸B nucleus is a one-proton halo structure with a loosely bound valence proton outside a ⁷Be core, and it is an excellent candidate for studying nuclear deformation and quadruple effects near the proton drip-line. By comparing the predictions of these models with available experimental data, it can be measured their effectiveness in describing ⁸B’s structure. These predictions reveal the structure of the halo configuration that influences the quadruple properties of exotic nuclei.</Abstract>
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<Param Name="value">Nuclear electric quadruple moment</Param>
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<Param Name="value">Proton-rich</Param>
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<Param Name="value">Weakly bound</Param>
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<Param Name="value">Microscopic single-particle shell model</Param>
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<Param Name="value">Collective model</Param>
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<Param Name="value">Two-body model</Param>
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<Param Name="value">Proton drip-line</Param>
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