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Matter"],"published-print":{"date-parts":[[2026,6,26]]},"abstract":"<jats:title>Abstract<\/jats:title>\n                  <jats:p>\n                    We extract spin\u2013valley physics in the anomalous Hall and Nernst responses of the\n                    <jats:inline-formula>\n                      <jats:tex-math>\n                        \n                      <\/jats:tex-math>\n                      <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" overflow=\"scroll\">\n                        <mml:mrow>\n                          <mml:mi>\u03b1<\/mml:mi>\n                        <\/mml:mrow>\n                      <\/mml:math>\n                    <\/jats:inline-formula>\n                    -\n                    <jats:inline-formula>\n                      <jats:tex-math>\n                        \n                      <\/jats:tex-math>\n                      <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" overflow=\"scroll\">\n                        <mml:mrow>\n                          <mml:msub>\n                            <mml:mi>T<\/mml:mi>\n                            <mml:mn>3<\/mml:mn>\n                          <\/mml:msub>\n                        <\/mml:mrow>\n                      <\/mml:math>\n                    <\/jats:inline-formula>\n                    system, considering the simultaneous presence of the Kane\u2013Mele type intrinsic spin\u2013orbit interaction (SOI) and a time-reversal symmetry breaking staggered magnetization. Within a full low-energy continuum model, we compute the spin- and valley-resolved anomalous Hall, and anomalous Nernst conductivities. We show that the interplay between the SOI, magnetization, and a model parameter\n                    <jats:inline-formula>\n                      <jats:tex-math>\n                        \n                      <\/jats:tex-math>\n                      <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" overflow=\"scroll\">\n                        <mml:mrow>\n                          <mml:mi>\u03b1<\/mml:mi>\n                        <\/mml:mrow>\n                      <\/mml:math>\n                    <\/jats:inline-formula>\n                    for the\n                    <jats:inline-formula>\n                      <jats:tex-math>\n                        \n                      <\/jats:tex-math>\n                      <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" overflow=\"scroll\">\n                        <mml:mrow>\n                          <mml:mi>\u03b1<\/mml:mi>\n                        <\/mml:mrow>\n                      <\/mml:math>\n                    <\/jats:inline-formula>\n                    -\n                    <jats:inline-formula>\n                      <jats:tex-math>\n                        \n                      <\/jats:tex-math>\n                      <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" overflow=\"scroll\">\n                        <mml:mrow>\n                          <mml:msub>\n                            <mml:mi>T<\/mml:mi>\n                            <mml:mn>3<\/mml:mn>\n                          <\/mml:msub>\n                        <\/mml:mrow>\n                      <\/mml:math>\n                    <\/jats:inline-formula>\n                    lattice enables efficient tuning of spin- and valley-dependent Hall and Nernst signals. The spin\u2013valley physics of the Hall and Nernst responses in the absence and presence of the magnetization are well explained. The peak\u2013dip features of the Nernst responses are also understood from the corresponding Hall responses through the Mott relation. We find that the magnetization introduces highly tunable spin and valley polarizations, which are calculated from the spin- and valley-resolved Nernst conductivities. It is shown that both the spin and valley polarizations can attain nearly complete polarization over extended regions of the parameter space.\n                  <\/jats:p>","DOI":"10.1088\/1361-648x\/ae7c48","type":"journal-article","created":{"date-parts":[[2026,6,11]],"date-time":"2026-06-11T22:53:13Z","timestamp":1781218393000},"page":"255401","update-policy":"https:\/\/doi.org\/10.1088\/crossmark-policy","source":"Crossref","is-referenced-by-count":0,"title":["Spin\u2013valley physics in anomalous thermoelectric responses of the spin\u2013orbit coupled \u03b1\u2010T\n                    <sub>3<\/sub>\n                    system with broken time-reversal symmetry"],"prefix":"10.1088","volume":"38","author":[{"ORCID":"https:\/\/orcid.org\/0000-0001-8322-9561","authenticated-orcid":false,"given":"Lakpa","family":"Tamang","sequence":"first","affiliation":[{"name":"University of North Bengal"}],"role":[{"vocabulary":"crossref","role":"author"}]},{"ORCID":"https:\/\/orcid.org\/0000-0002-7807-905X","authenticated-orcid":true,"given":"Tutul","family":"Biswas","sequence":"additional","affiliation":[{"name":"University of North Bengal"}],"role":[{"vocabulary":"crossref","role":"author"}]}],"member":"266","published-online":{"date-parts":[[2026,6,24]]},"reference":[{"key":"cmae7c48bib1","doi-asserted-by":"publisher","first-page":"1488","DOI":"10.1126\/science.1065389","type":"journal-article","article-title":"Spintronics: a spin- based electronics vision for the future","volume":"294","author":"Wolf","year":"2001","journal-title":"Science"},{"key":"cmae7c48bib2","doi-asserted-by":"publisher","first-page":"323","DOI":"10.1103\/RevModPhys.76.323","type":"journal-article","article-title":"Spintronics: fundamentals and applications","volume":"76","author":"Zutic","year":"2004","journal-title":"Rev. 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