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Search for Light Dark Matter with NA64 at CERN
Thermal dark matter models with particle <math display="inline"><mi>χ</mi></math> masses below the electroweak scale can provide an explanation for the observed relic dark matter density. This would imply the existence of a new feeble interaction between the dark an...
Autores principales: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
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Lenguaje: | eng |
Publicado: |
2023
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1103/PhysRevLett.131.161801 http://cds.cern.ch/record/2864062 |
Sumario: | Thermal dark matter models with particle <math display="inline"><mi>χ</mi></math> masses below the electroweak scale can provide an explanation for the observed relic dark matter density. This would imply the existence of a new feeble interaction between the dark and ordinary matter. We report on a new search for the sub-GeV <math display="inline"><mi>χ</mi></math> production through the interaction mediated by a new vector boson, called the dark photon <math display="inline"><msup><mi>A</mi><mo>′</mo></msup></math>, in collisions of 100 GeV electrons with the active target of the NA64 experiment at the CERN SPS. With <math display="inline"><mn>9.37</mn><mo>×</mo><msup><mn>10</mn><mn>11</mn></msup></math> electrons on target collected during 2016–2022 runs NA64 probes for the first time the well-motivated region of parameter space of benchmark thermal scalar and fermionic dark matter models. No evidence for dark matter production has been found. This allows us to set the most sensitive limits on the <math display="inline"><msup><mi>A</mi><mo>′</mo></msup></math> couplings to photons for masses <math display="inline"><msub><mi>m</mi><msup><mi>A</mi><mo>′</mo></msup></msub><mo>≲</mo><mn>0.35</mn><mtext> </mtext><mtext> </mtext><mi>GeV</mi></math>, and to exclude scalar and Majorana dark matter with the <math display="inline"><mi>χ</mi><mo>-</mo><msup><mi>A</mi><mo>′</mo></msup></math> coupling <math display="inline"><msub><mi>α</mi><mi>D</mi></msub><mo>≤</mo><mn>0.1</mn></math> for masses <math display="inline"><mn>0.001</mn><mo>≲</mo><msub><mi>m</mi><mi>χ</mi></msub><mo>≲</mo><mn>0.1</mn><mtext> </mtext><mtext> </mtext><mi>GeV</mi></math> and <math display="inline"><mn>3</mn><msub><mi>m</mi><mi>χ</mi></msub><mo>≤</mo><msub><mi>m</mi><msup><mi>A</mi><mo>′</mo></msup></msub></math>. |
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