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Adv."],"published-print":{"date-parts":[[2026,10,23]]},"abstract":"<jats:p>\n                    A continuous transition between phases hosting distinct excitations\u2014bosonic magnons versus fermionic spinons\u2014is a long-sought phenomenon in quantum magnetism, analogous to the confinement-deconfinement transition in quantum chromodynamics. We report evidence for such a transition in the triangular-lattice antiferromagnet thallium ytterbium disulfide. Antiferromagnetic order develops below\n                    <jats:italic toggle=\"yes\">T<\/jats:italic>\n                    <jats:sub>N<\/jats:sub>\n                    \u00a0\u2248\u00a00.53\u00a0kelvin. A\n                    <jats:italic toggle=\"yes\">c<\/jats:italic>\n                    -axis field suppresses this order, driving the system into a gapless quantum spin liquid with a spinon Fermi surface above\n                    <jats:inline-formula>\n                      <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\" overflow=\"scroll\">\n                        <mml:mrow>\n                          <mml:msub>\n                            <mml:mi mathvariant=\"normal\">\u03bc<\/mml:mi>\n                            <mml:mn>0<\/mml:mn>\n                          <\/mml:msub>\n                          <mml:msub>\n                            <mml:mi>H<\/mml:mi>\n                            <mml:mi mathvariant=\"normal\">c<\/mml:mi>\n                          <\/mml:msub>\n                          <mml:mo>\u2248<\/mml:mo>\n                          <mml:mn>3<\/mml:mn>\n                          <mml:mo>\u00a0<\/mml:mo>\n                          <mml:mi mathvariant=\"normal\">T<\/mml:mi>\n                        <\/mml:mrow>\n                      <\/mml:math>\n                    <\/jats:inline-formula>\n                    , evidenced by a finite residual linear term in thermal conductivity, a Pauli-like susceptibility, and a temperature-independent nuclear magnetic resonance Knight shift. Approaching\n                    <jats:inline-formula>\n                      <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\" overflow=\"scroll\">\n                        <mml:mrow>\n                          <mml:msub>\n                            <mml:mi>H<\/mml:mi>\n                            <mml:mi mathvariant=\"normal\">c<\/mml:mi>\n                          <\/mml:msub>\n                        <\/mml:mrow>\n                      <\/mml:math>\n                    <\/jats:inline-formula>\n                    from above, the scattering rate of itinerant excitations is strongly enhanced, while their density of states shows no critical enhancement, atypical of conventional magnetic quantum criticality. These results point to a continuous confinement-deconfinement transition governed by fractionalized excitations beyond the Ginzburg-Landau paradigm.\n                  <\/jats:p>","DOI":"10.1126\/sciadv.aej9484","type":"journal-article","created":{"date-parts":[[2026,10,21]],"date-time":"2026-10-21T18:01:42Z","timestamp":1792605702000},"update-policy":"https:\/\/doi.org\/10.34133\/aaas_crossmark","source":"Crossref","is-referenced-by-count":0,"title":["A continuous confinement-deconfinement transition in a triangular quantum magnet"],"prefix":"10.1126","volume":"12","author":[{"ORCID":"https:\/\/orcid.org\/0000-0001-9159-4091","authenticated-orcid":true,"given":"Suguru","family":"Hosoi","sequence":"first","affiliation":[{"name":"Materials Physics and Applications\u2013Quantum, Los Alamos National Laboratory, Los Alamos, NM 87545, 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