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Learn.: Sci. Technol."],"published-print":{"date-parts":[[2025,9,30]]},"abstract":"<jats:title>Abstract<\/jats:title>\n               <jats:p>We cast the relation between the chemical composition of a solid-state material and its superconducting critical temperature (<jats:inline-formula>\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:mrow>\n                                 <mml:mi mathvariant=\"normal\">c<\/mml:mi>\n                              <\/mml:mrow>\n                           <\/mml:msub>\n                        <\/mml:mrow>\n                     <\/mml:math>\n                  <\/jats:inline-formula>) as a statistical learning problem with reduced complexity. Training of query-aware similarity-based ridge regression models on experimental SuperCon data achieves average <jats:inline-formula>\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:mrow>\n                                 <mml:mi mathvariant=\"normal\">c<\/mml:mi>\n                              <\/mml:mrow>\n                           <\/mml:msub>\n                        <\/mml:mrow>\n                     <\/mml:math>\n                  <\/jats:inline-formula> prediction errors of \u00b15\u2009K for unseen out-of-sample materials. Two models were trained with one excluding high pressure data in training (\u2018ambient\u2019 model) and a second also including high pressure data (\u2018implicit\u2019 model). Subsequent utilization of the approach to scan \u223c153\u2009k materials in the Materials Project enables the ranking of candidates by <jats:inline-formula>\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:mrow>\n                                 <mml:mi mathvariant=\"normal\">c<\/mml:mi>\n                              <\/mml:mrow>\n                           <\/mml:msub>\n                        <\/mml:mrow>\n                     <\/mml:math>\n                  <\/jats:inline-formula> while accounting for thermodynamic stability and small band gap. The ambient model is used to predict stable top three high-<jats:inline-formula>\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:mrow>\n                                 <mml:mi mathvariant=\"normal\">c<\/mml:mi>\n                              <\/mml:mrow>\n                           <\/mml:msub>\n                        <\/mml:mrow>\n                     <\/mml:math>\n                  <\/jats:inline-formula> candidate materials that include those with large band gaps of LiCuF<jats:sub>4<\/jats:sub> (316\u2009K), Ag<jats:sub>2<\/jats:sub>H<jats:sub>12<\/jats:sub>S(NO)<jats:sub>4<\/jats:sub> (316\u2009K), and Na<jats:sub>2<\/jats:sub>H<jats:sub>6<\/jats:sub>PtO<jats:sub>6<\/jats:sub> (315\u2009K). Filtering these candidates for those with small band gaps correspondingly yields LiCuF<jats:sub>4<\/jats:sub> (316\u2009K), Cu<jats:sub>2<\/jats:sub>P<jats:sub>2<\/jats:sub>O<jats:sub>7<\/jats:sub> (311\u2009K), and Cu<jats:sub>3<\/jats:sub>P<jats:sub>2<\/jats:sub>H<jats:sub>2<\/jats:sub>O<jats:sub>9<\/jats:sub> (307\u2009K).<\/jats:p>","DOI":"10.1088\/2632-2153\/ae04c1","type":"journal-article","created":{"date-parts":[[2025,9,8]],"date-time":"2025-09-08T22:53:40Z","timestamp":1757372020000},"page":"035052","update-policy":"https:\/\/doi.org\/10.1088\/crossmark-policy","source":"Crossref","is-referenced-by-count":0,"title":["High-\n\t    \n\t    <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\">\n                     <mml:mrow>\n                        <mml:msub>\n                           <mml:mi>T<\/mml:mi>\n                           <mml:mrow>\n                              <mml:mi>c<\/mml:mi>\n                           <\/mml:mrow>\n                        <\/mml:msub>\n                     <\/mml:mrow>\n                  <\/mml:math>\n\t    \n\t   superconductor candidates proposed by machine learning"],"prefix":"10.1088","volume":"6","author":[{"ORCID":"https:\/\/orcid.org\/0000-0002-4521-389X","authenticated-orcid":true,"given":"Siwoo","family":"Lee","sequence":"first","affiliation":[]},{"given":"Jason","family":"Hattrick-Simpers","sequence":"additional","affiliation":[]},{"ORCID":"https:\/\/orcid.org\/0000-0002-1172-8895","authenticated-orcid":true,"given":"Young-June","family":"Kim","sequence":"additional","affiliation":[]},{"ORCID":"https:\/\/orcid.org\/0000-0001-7419-0466","authenticated-orcid":true,"given":"O","family":"Anatole von Lilienfeld","sequence":"additional","affiliation":[]}],"member":"266","published-online":{"date-parts":[[2025,9,17]]},"reference":[{"key":"mlstae04c1bib1","doi-asserted-by":"publisher","first-page":"103","DOI":"10.1021\/ar00051a003","type":"journal-article","article-title":"Room temperature superconductors","volume":"28","author":"Sleight","year":"1995","journal-title":"Acc. 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