Home > Publications database > Sensitivity of the SHiP experiment to dark photons decaying to a pair of charged particles > print

001     910541
005     20250129092406.0
024 7 _ |a arXiv:2011.05115
|2 arXiv
024 7 _ |a 10.1140/epjc/s10052-021-09224-3
|2 doi
024 7 _ |a 2128/32310
|2 Handle
024 7 _ |a WOS:000680441900002
|2 WOS
037 _ _ |a FZJ-2022-03923
041 _ _ |a English
082 _ _ |a 530
100 1 _ |a SHiP Collaboration
|0 P:(DE-HGF)0
|b 0
|e Corresponding author
245 _ _ |a Sensitivity of the SHiP experiment to dark photons decaying to a pair of charged particles
260 _ _ |a Heidelberg
|c 2021
|b Springer
336 7 _ |a article
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336 7 _ |a Output Types/Journal article
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336 7 _ |a Journal Article
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|m journal
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|s 1667462751_8861
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336 7 _ |a ARTICLE
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336 7 _ |a JOURNAL_ARTICLE
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336 7 _ |a Journal Article
|0 0
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520 _ _ |a Dark photons are hypothetical massive vector particles that could mix with ordinary photons. The simplest theoretical model is fully characterised by only two parameters: the mass of the dark photon m$_{\gamma^{\mathrm{D}}}$ and its mixing parameter with the photon, $\varepsilon$. The sensitivity of the SHiP detector is reviewed for dark photons in the mass range between 0.002 and 10 GeV. Different production mechanisms are simulated, with the dark photons decaying to pairs of visible fermions, including both leptons and quarks. Exclusion contours are presented and compared with those of past experiments. The SHiP detector is expected to have a unique sensitivity for m$_{\gamma^{\mathrm{D}}}$ ranging between 0.8 and 3.3$^{+0.2}_{-0.5}$ GeV, and $\varepsilon^2$ ranging between $10^{-11}$ and $10^{-17}$.
536 _ _ |a 622 - Detector Technologies and Systems (POF4-622)
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650 2 7 |a Particle Physics
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650 1 7 |a Basic research
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650 1 7 |a Nuclei and Particles
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693 _ _ |a LHC
|e LHC: Other
|1 EXP:(DE-588)4398783-7
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700 1 _ |a Ahdida, C.
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700 1 _ |a Akmete, A.
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700 1 _ |a Albanese, R.
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700 1 _ |a Alexandrov, A.
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700 1 _ |a Anokhina, A.
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700 1 _ |a Aoki, S.
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773 _ _ |a 10.1140/epjc/s10052-021-09224-3
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Marc 21