Sensitivity of the SHiP experiment to dark photons decaying to a pair of charged particles
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...
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Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
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Format: | Journal Article |
Language: | English |
Published: |
01-03-2021
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Subjects: | |
Online Access: | Get full text |
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Summary: | 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 $10^{-17}$. |
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DOI: | 10.48550/arxiv.2011.05115 |