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<!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>6</Volume>
<Issue>1</Issue>
<PubDate PubStatus="epublish">
<Year>2023</Year>
<Month>11</Month>
<Day>17</Day>
</PubDate>
</Journal>
<ArticleTitle>Thermoelectric power of metallic Rb3C60: phonon-drag and carrier diffusion contributions</ArticleTitle>
<VernacularTitle></VernacularTitle>
<FirstPage></FirstPage>
<LastPage></LastPage>
<ELocationID EIdType="doi">10.1186/2251-7235-6-37</ELocationID>
<Language>EN</Language>
<AuthorList>
<Author>
<FirstName>Dinesh</FirstName>
<LastName>Varshney</LastName>
<Affiliation>Materials Science Laboratory, School of Physics, Vigyan Bhawan, Devi Ahilya University</Affiliation>
<Identifier Source="ORCID"></Identifier>
</Author>
<Author>
<FirstName>Namita</FirstName>
<LastName>Singh</LastName>
<Affiliation>Department of Physics, Ranchi College, Ranchi University Ranchi</Affiliation>
<Identifier Source="ORCID"></Identifier>
</Author>
</AuthorList>
<PublicationType>Journal Article</PublicationType>
<History>
<PubDate PubStatus="received">
<Year>2023</Year>
<Month>11</Month>
<Day>17</Day>
</PubDate>
</History>
<Abstract>AbstractThermoelectric power (S) of Rb3C60 fullerides in the metallic phase is theoretically estimated. We first develop a Hamiltonian model that incorporates the scattering rates within the relaxation time approximation to estimate the phonon-drag thermoelectric power (Sphdrag) incorporating the scattering of phonons with defects, electrons as carriers, grain boundaries, and phonon-phonon interactions. As a next step, Mott expression within parabolic band approximation is used to analyze the electron diffusive thermoelectric power (Scdiff) using Fermi energy as electron parameter, and Scdiff shows a linear temperature dependence. The Sphdrag is nonzero in both normal and superconducting states. Its behavior is determined by competition among the several operating scattering rates for heat carriers and a balance between diffusive carrier and phonon-drag contributions. Acoustic phonons are effectively scattered by various scatterers for the thermoelectric power. S infers a change in slope above transition temperature and becomes almost linear above 70 K.</Abstract>
<ObjectList>
<Object Type="keyword">
<Param Name="value">Carrier diffusion</Param>
</Object>
<Object Type="keyword">
<Param Name="value">Intermolecular phonon</Param>
</Object>
<Object Type="keyword">
<Param Name="value">Phonon drag</Param>
</Object>
<Object Type="keyword">
<Param Name="value">RbC</Param>
</Object>
<Object Type="keyword">
<Param Name="value">Thermoelectric power</Param>
</Object>
</ObjectList>
</Article>
</ArticleSet>