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Rev. Lett."],"accepted":{"date-parts":[[2026,6,11]]},"abstract":"<jats:p>\n                    We report on a blinded search for dark matter (DM) using ionization-only (S2-only) signals in XENONnT with a total exposure of\n                    <a:math xmlns:a=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\">\n                      <a:mrow>\n                        <a:mn>7.83<\/a:mn>\n                        <a:mtext>\u2009<\/a:mtext>\n                        <a:mtext>\u2009<\/a:mtext>\n                        <a:mtext>Tonne-year<\/a:mtext>\n                      <\/a:mrow>\n                    <\/a:math>\n                    over 579\u00a0days in three science runs. Dedicated background suppression techniques and the first complete S2-only background model in XENONnT provide sensitivity to nuclear recoils of\n                    <c:math xmlns:c=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\">\n                      <c:mrow>\n                        <c:mo stretchy=\"false\">[<\/c:mo>\n                        <c:mn>0.5<\/c:mn>\n                        <c:mo>,<\/c:mo>\n                        <c:mn>5.0<\/c:mn>\n                        <c:mo stretchy=\"false\">]<\/c:mo>\n                        <c:mtext>\u2009<\/c:mtext>\n                        <c:mtext>\u2009<\/c:mtext>\n                        <c:msub>\n                          <c:mrow>\n                            <c:mi>keV<\/c:mi>\n                          <\/c:mrow>\n                          <c:mrow>\n                            <c:mi>nr<\/c:mi>\n                          <\/c:mrow>\n                        <\/c:msub>\n                      <\/c:mrow>\n                    <\/c:math>\n                    and electronic recoils of\n                    <g:math xmlns:g=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\">\n                      <g:mrow>\n                        <g:mo stretchy=\"false\">[<\/g:mo>\n                        <g:mn>0.04<\/g:mn>\n                        <g:mo>,<\/g:mo>\n                        <g:mn>0.7<\/g:mn>\n                        <g:mo stretchy=\"false\">]<\/g:mo>\n                        <g:mtext>\u2009<\/g:mtext>\n                        <g:mtext>\u2009<\/g:mtext>\n                        <g:msub>\n                          <g:mrow>\n                            <g:mi>keV<\/g:mi>\n                          <\/g:mrow>\n                          <g:mrow>\n                            <g:mi>ee<\/g:mi>\n                          <\/g:mrow>\n                        <\/g:msub>\n                      <\/g:mrow>\n                    <\/g:math>\n                    . No significant excess over the expected background is observed, and we set 90% confidence level upper limits on spin-independent DM-nucleon and spin-dependent DM-neutron scattering for DM masses between 3 and\n                    <k:math xmlns:k=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\">\n                      <k:mrow>\n                        <k:mn>8<\/k:mn>\n                        <k:mtext>\u2009<\/k:mtext>\n                        <k:mtext>\u2009<\/k:mtext>\n                        <k:mi>GeV<\/k:mi>\n                        <k:mo>\/<\/k:mo>\n                        <k:msup>\n                          <k:mi>c<\/k:mi>\n                          <k:mn>2<\/k:mn>\n                        <\/k:msup>\n                      <\/k:mrow>\n                    <\/k:math>\n                    , as well as on DM-electron scattering, axionlike particles, and dark photons, improving on previous constraints. For spin-independent DM-nucleon scattering, we exclude cross sections above\n                    <m:math xmlns:m=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\">\n                      <m:mn>6.0<\/m:mn>\n                      <m:mo>\u00d7<\/m:mo>\n                      <m:msup>\n                        <m:mn>10<\/m:mn>\n                        <m:mrow>\n                          <m:mo>\u2212<\/m:mo>\n                          <m:mn>45<\/m:mn>\n                        <\/m:mrow>\n                      <\/m:msup>\n                      <m:mtext>\u2009<\/m:mtext>\n                      <m:mtext>\u2009<\/m:mtext>\n                      <m:msup>\n                        <m:mrow>\n                          <m:mi>cm<\/m:mi>\n                        <\/m:mrow>\n                        <m:mrow>\n                          <m:mn>2<\/m:mn>\n                        <\/m:mrow>\n                      <\/m:msup>\n                    <\/m:math>\n                    at a DM mass of\n                    <o:math xmlns:o=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\">\n                      <o:mrow>\n                        <o:mn>5<\/o:mn>\n                        <o:mtext>\u2009<\/o:mtext>\n                        <o:mtext>\u2009<\/o:mtext>\n                        <o:mi>GeV<\/o:mi>\n                        <o:mo>\/<\/o:mo>\n                        <o:msup>\n                          <o:mi>c<\/o:mi>\n                          <o:mn>2<\/o:mn>\n                        <\/o:msup>\n                      <\/o:mrow>\n                    <\/o:math>\n                    , pushing the XENONnT sensitivity closer to the region where coherent elastic neutrino-nucleus scattering becomes an irreducible background.\n                  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