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Pd<jats:sub>3<\/jats:sub>In<jats:sub>7<\/jats:sub> is characterized by low residual resistivities and high mobilities, which are consistent with Dirac-like quasiparticles. For an applied magnetic field (<jats:italic>\u03bc<\/jats:italic><jats:sub>0<\/jats:sub><jats:italic>H<\/jats:italic>) having a non-zero component along the electrical current, we find a large, positive, and linear in <jats:italic>\u03bc<\/jats:italic><jats:sub>0<\/jats:sub><jats:italic>H<\/jats:italic> longitudinal magnetoresistivity (LMR). The sign of the LMR and its linear dependence deviate from the behavior reported for the chiral-anomaly-driven LMR in Weyl semimetals. Interestingly, such anomalous LMR is consistent with predictions for the role of the anomaly in type-II Weyl semimetals. In contrast, the transverse or conventional magnetoresistivity (CMR for electric fields <jats:bold>E<\/jats:bold>\u22a5<jats:italic>\u03bc<\/jats:italic><jats:sub>0<\/jats:sub><jats:bold>H<\/jats:bold>) is large and positive, increasing by 10<jats:sup>3<\/jats:sup>\u221210<jats:sup>4<\/jats:sup> % as a function of <jats:italic>\u03bc<\/jats:italic><jats:sub>0<\/jats:sub><jats:italic>H<\/jats:italic> while following an anomalous, angle-dependent power law <jats:inline-formula><jats:alternatives><jats:tex-math>$${\\rho }_{{{{\\rm{xx}}}}}\\propto {({\\mu }_{0}H)}^{n}$$<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                  <mml:mrow>\n                    <mml:msub>\n                      <mml:mrow>\n                        <mml:mi>\u03c1<\/mml:mi>\n                      <\/mml:mrow>\n                      <mml:mrow>\n                        <mml:mi>xx<\/mml:mi>\n                      <\/mml:mrow>\n                    <\/mml:msub>\n                    <mml:mo>\u221d<\/mml:mo>\n                    <mml:msup>\n                      <mml:mrow>\n                        <mml:mrow>\n                          <mml:mo>(<\/mml:mo>\n                          <mml:mrow>\n                            <mml:msub>\n                              <mml:mrow>\n                                <mml:mi>\u03bc<\/mml:mi>\n                              <\/mml:mrow>\n                              <mml:mrow>\n                                <mml:mn>0<\/mml:mn>\n                              <\/mml:mrow>\n                            <\/mml:msub>\n                            <mml:mi>H<\/mml:mi>\n                          <\/mml:mrow>\n                          <mml:mo>)<\/mml:mo>\n                        <\/mml:mrow>\n                      <\/mml:mrow>\n                      <mml:mrow>\n                        <mml:mi>n<\/mml:mi>\n                      <\/mml:mrow>\n                    <\/mml:msup>\n                  <\/mml:mrow>\n                <\/mml:math><\/jats:alternatives><\/jats:inline-formula> with <jats:italic>n<\/jats:italic>(<jats:italic>\u03b8<\/jats:italic>)\u2009\u2264\u20091. The order of magnitude of the CMR, and its anomalous power-law, is explained in terms of uncompensated electron and hole-like Fermi surfaces characterized by anisotropic carrier scattering likely due to the lack of Lorentz invariance.<\/jats:p>","DOI":"10.1038\/s41535-023-00601-7","type":"journal-article","created":{"date-parts":[[2023,11,16]],"date-time":"2023-11-16T05:01:52Z","timestamp":1700110912000},"update-policy":"https:\/\/doi.org\/10.1007\/springer_crossmark_policy","source":"Crossref","is-referenced-by-count":8,"title":["Anisotropic positive linear and sub-linear magnetoresistivity in the cubic type-II Dirac metal Pd3In7"],"prefix":"10.1038","volume":"8","author":[{"given":"Aikaterini","family":"Flessa Savvidou","sequence":"first","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"ORCID":"https:\/\/orcid.org\/0000-0002-5566-2656","authenticated-orcid":false,"given":"Andrzej","family":"Ptok","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"G.","family":"Sharma","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Brian","family":"Casas","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Judith K.","family":"Clark","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Victoria M.","family":"Li","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Michael","family":"Shatruk","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"ORCID":"https:\/\/orcid.org\/0000-0002-9979-6306","authenticated-orcid":false,"given":"Sumanta","family":"Tewari","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"ORCID":"https:\/\/orcid.org\/0000-0002-5209-0293","authenticated-orcid":false,"given":"Luis","family":"Balicas","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]}],"member":"297","published-online":{"date-parts":[[2023,11,16]]},"reference":[{"key":"601_CR1","doi-asserted-by":"publisher","first-page":"1057","DOI":"10.1103\/RevModPhys.83.1057","volume":"83","author":"X-L Qi","year":"2011","unstructured":"Qi, X.-L. & Zhang, S.-C. 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