<p>The search for dark matter focuses now on hypothetical light particles with masses ranging from MeV to GeV (refs. <sup><CitationRef AdditionalCitationIDS="CR2 CR3 CR4 CR5 CR6 CR7 CR8 CR9 CR10 CR11" CitationID="CR1">1</CitationRef>–<CitationRef CitationID="CR12">12</CitationRef></sup>). These particles would leave very faint signals experimentally. A potential avenue for enhancing experimental sensitivity to light matter relies on the Migdal effect<sup><CitationRef AdditionalCitationIDS="CR14" CitationID="CR13">13</CitationRef>–<CitationRef CitationID="CR15">15</CitationRef></sup>, which involves the detectable ejection of electrons following the instantaneous accelerations of atoms colliding with neutral dark matter. However, although the Migdal effect could be equally generated in controlled experiments with neutral projectiles, a direct experimental observation of this effect is missing, casting doubt on the reliability of detection experiments relying on this effect. Here we report the direct observation of the Migdal effect in neutron–nucleus collisions, achieving a statistical significance of 5 standard deviations, which rests on 6 candidate events selected out of almost 10<sup>6</sup> recorded events. Our experiments have determined the ratio of the Migdal cross-section to the nuclear recoil cross-section to be <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\({4.9}_{-1.9}^{+2.6}\times {10}^{-5}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mrow> <mn>4.9</mn> </mrow> <mrow> <mo>−</mo> <mn>1.9</mn> </mrow> <mrow> <mo>+</mo> <mn>2.6</mn> </mrow> </msubsup> <mo>×</mo> <msup> <mrow> <mn>10</mn> </mrow> <mrow> <mo>−</mo> <mn>5</mn> </mrow> </msup> </math></EquationSource> </InlineEquation>, in which nuclear recoils exceed 35 keVee and electron recoils span 5–10 keV. These findings are consistent with theoretical predictions. This work resolves a long-standing gap in experimental validation, which not only strengthens the theoretical foundation of the Migdal effect but also paves the way for its application in light dark matter detection.</p>

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Direct observation of the Migdal effect induced by neutron bombardment

  • Difan Yi,
  • Qian Liu,
  • Shi Chen,
  • Chunlai Dong,
  • Huanbo Feng,
  • Chaosong Gao,
  • Wenqian Huang,
  • Xinmei Jing,
  • Lingquan Kong,
  • Jin Li,
  • Peirong Li,
  • Enwei Liang,
  • Ruiting Ma,
  • Chenguang Su,
  • Liangliang Su,
  • Junwei Sun,
  • Dong Wang,
  • Junrun Wang,
  • Zheng Wei,
  • Zeen Yao,
  • Yunlinchen Yu,
  • Yu Zhang,
  • Shiqiang Zhou,
  • Zhuo Zhou,
  • Bin Zhu,
  • Jie Zuo,
  • Hongbang Liu,
  • Xiangming Sun,
  • Lei Wu,
  • Yangheng Zheng

摘要

The search for dark matter focuses now on hypothetical light particles with masses ranging from MeV to GeV (refs. 112). These particles would leave very faint signals experimentally. A potential avenue for enhancing experimental sensitivity to light matter relies on the Migdal effect1315, which involves the detectable ejection of electrons following the instantaneous accelerations of atoms colliding with neutral dark matter. However, although the Migdal effect could be equally generated in controlled experiments with neutral projectiles, a direct experimental observation of this effect is missing, casting doubt on the reliability of detection experiments relying on this effect. Here we report the direct observation of the Migdal effect in neutron–nucleus collisions, achieving a statistical significance of 5 standard deviations, which rests on 6 candidate events selected out of almost 106 recorded events. Our experiments have determined the ratio of the Migdal cross-section to the nuclear recoil cross-section to be \({4.9}_{-1.9}^{+2.6}\times {10}^{-5}\) 4.9 1.9 + 2.6 × 10 5 , in which nuclear recoils exceed 35 keVee and electron recoils span 5–10 keV. These findings are consistent with theoretical predictions. This work resolves a long-standing gap in experimental validation, which not only strengthens the theoretical foundation of the Migdal effect but also paves the way for its application in light dark matter detection.