Time-integrated directional detection of dark matter
The analysis of signals in directional dark matter (DM) detectors typically assumes that the directions of nuclear recoils can be measured in the Galactic rest frame. However, this is not possible with all directional detection technologies. In nuclear emulsions, for example, the recoil events must...
| Main Authors: | , , |
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| Format: | Article |
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American Physical Society
2017
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| Online Access: | https://eprints.nottingham.ac.uk/47357/ |
| _version_ | 1848797525362868224 |
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| author | O'Hare, Ciaran A.J. Kavanagh, Bradley J. Green, Anne M. |
| author_facet | O'Hare, Ciaran A.J. Kavanagh, Bradley J. Green, Anne M. |
| author_sort | O'Hare, Ciaran A.J. |
| building | Nottingham Research Data Repository |
| collection | Online Access |
| description | The analysis of signals in directional dark matter (DM) detectors typically assumes that the directions of nuclear recoils can be measured in the Galactic rest frame. However, this is not possible with all directional detection technologies. In nuclear emulsions, for example, the recoil events must be detected and measured after the exposure time of the experiment. Unless the entire detector is mounted and rotated with the sidereal day, the recoils cannot be reoriented in the Galactic rest frame. We examine the effect of this `time integration' on the primary goals of directional detection, namely: (1) confirming that the recoils are anisotropic; (2) measuring the median recoil direction to confirm their Galactic origin; and (3) probing below the neutrino floor. We show that after time integration the DM recoil distribution retains a preferred direction and is distinct from that of Solar neutrino-induced recoils. Many of the advantages of directional detection are therefore preserved and it is not crucial to mount and rotate the detector. Rejecting isotropic backgrounds requires a factor of 2 more signal events compared with an experiment with event time information, whereas a factor of 1.5-3 more events are needed to measure a median direction in agreement with the expectation for DM. We also find that there is still effectively no neutrino floor in a time-integrated directional experiment. However to reach a cross section an order of magnitude below the floor, a factor of 8 larger exposure is required than with a conventional directional experiment. We also examine how the sensitivity is affected for detectors with only 2D recoil track readout, and/or no head-tail measurement. As for non-time-integrated experiments, 2D readout is not a major disadvantage, though a lack of head-tail sensitivity is. |
| first_indexed | 2025-11-14T20:05:16Z |
| format | Article |
| id | nottingham-47357 |
| institution | University of Nottingham Malaysia Campus |
| institution_category | Local University |
| last_indexed | 2025-11-14T20:05:16Z |
| publishDate | 2017 |
| publisher | American Physical Society |
| recordtype | eprints |
| repository_type | Digital Repository |
| spelling | nottingham-473572020-05-04T19:12:58Z https://eprints.nottingham.ac.uk/47357/ Time-integrated directional detection of dark matter O'Hare, Ciaran A.J. Kavanagh, Bradley J. Green, Anne M. The analysis of signals in directional dark matter (DM) detectors typically assumes that the directions of nuclear recoils can be measured in the Galactic rest frame. However, this is not possible with all directional detection technologies. In nuclear emulsions, for example, the recoil events must be detected and measured after the exposure time of the experiment. Unless the entire detector is mounted and rotated with the sidereal day, the recoils cannot be reoriented in the Galactic rest frame. We examine the effect of this `time integration' on the primary goals of directional detection, namely: (1) confirming that the recoils are anisotropic; (2) measuring the median recoil direction to confirm their Galactic origin; and (3) probing below the neutrino floor. We show that after time integration the DM recoil distribution retains a preferred direction and is distinct from that of Solar neutrino-induced recoils. Many of the advantages of directional detection are therefore preserved and it is not crucial to mount and rotate the detector. Rejecting isotropic backgrounds requires a factor of 2 more signal events compared with an experiment with event time information, whereas a factor of 1.5-3 more events are needed to measure a median direction in agreement with the expectation for DM. We also find that there is still effectively no neutrino floor in a time-integrated directional experiment. However to reach a cross section an order of magnitude below the floor, a factor of 8 larger exposure is required than with a conventional directional experiment. We also examine how the sensitivity is affected for detectors with only 2D recoil track readout, and/or no head-tail measurement. As for non-time-integrated experiments, 2D readout is not a major disadvantage, though a lack of head-tail sensitivity is. American Physical Society 2017-10-16 Article PeerReviewed O'Hare, Ciaran A.J., Kavanagh, Bradley J. and Green, Anne M. (2017) Time-integrated directional detection of dark matter. Physical Review D, 96 . 083011. ISSN 2470-0029 https://journals.aps.org/prd/abstract/10.1103/PhysRevD.96.083011 doi:10.1103/PhysRevD.96.083011 doi:10.1103/PhysRevD.96.083011 |
| spellingShingle | O'Hare, Ciaran A.J. Kavanagh, Bradley J. Green, Anne M. Time-integrated directional detection of dark matter |
| title | Time-integrated directional detection of dark matter |
| title_full | Time-integrated directional detection of dark matter |
| title_fullStr | Time-integrated directional detection of dark matter |
| title_full_unstemmed | Time-integrated directional detection of dark matter |
| title_short | Time-integrated directional detection of dark matter |
| title_sort | time-integrated directional detection of dark matter |
| url | https://eprints.nottingham.ac.uk/47357/ https://eprints.nottingham.ac.uk/47357/ https://eprints.nottingham.ac.uk/47357/ |