Cryogenic Rare Event Search with Superconducting Thermometers

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The building housing the CRESST cryostat, located in Hall A of the LNGS deep underground laboratory, Gran Sasso, Italy. Laboratori Nazionali del Gran Sasso, CRESSThut.jpg
The building housing the CRESST cryostat, located in Hall A of the LNGS deep underground laboratory, Gran Sasso, Italy.

The Cryogenic Rare Event Search with Superconducting Thermometers (CRESST) is a collaboration of European experimental particle physics groups involved in the construction of cryogenic detectors for direct dark matter searches. The participating institutes are the Max Planck Institute for Physics (Munich), Technical University of Munich, University of Tübingen (Germany), University of Oxford (Great Britain) and the Istituto Nazionale di Fisica Nucleare (INFN, Italy). [1]

The CRESST collaboration currently runs an array of cryogenic detectors in the underground laboratory of the Gran Sasso National Laboratory. The modular detectors used by CRESST facilitate discrimination of background radiation events by the simultaneous measurement of phonon and photon signals from scintillating calcium tungstate crystals. By cooling the detectors to temperatures of a few millikelvin, the excellent discrimination and energy resolution of the detectors allows identification of rare particle events.

CRESST-I took data in 2000 using sapphire detectors with tungsten thermometers. CRESST-II uses CaWO4 crystal scintillating calorimeters. It was prototyped in 2004 and had a 47.9 kg-day commissioning run in 2007 and operated 2009 to 2011. CRESST-II Phase 1 experiment observed excess events above known background that could be understood to constitute a dark matter signal. However, later analysis showed that these excess events were due to a previously uncounted for excess of background from the detector itself and not a true signal from dark matter. [2] The source of the excess background in the detector was removed for Phase 2.

Phase 2 has a new CaWO4 crystal with better radiopurity, improved detectors, and significantly reduced background. It began July 2013 to explore excess signals in the prior run. The results of Phase 2 showed no signal above expected background, proving that the result of Phase 1 had indeed been due to excess background by components of the detector. [2]

CRESST-II first detected the alpha decay of tungsten-180 (180W). [3] CRESST-II phase 1 full results were published in 2012. [4] New phase 2 results have been presented in July 2014 [5] with a limit on spin-independent WIMP-nucleon scattering for WIMP masses below 3 GeV/c2.

In 2015 the CRESST detectors were upgraded by a sensitivity factor of 100 allowing dark-matter particles with a mass around that of a proton to be detected. [6]

In 2019, the team reported results of the first phase of CRESST-III, which ran from 2016 to 2018. CRESST-III used a single 23.6-g CaWO4 detector with a lowered energy threshold of 30.1 eV, about 1/10 that of CRESST-II. This allows the detection of WIMPs as light as 0.16 GeV/c2, slightly heavier than a pion. Despite many events from the electron capture decay of 179Ta, there was an unexplained excess of events imparting less than 200 eV. [7]

The experiment is planning an upgrade to accommodate 100 detector modules. [8]

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The Cryogenic Dark Matter Search (CDMS) is a series of experiments designed to directly detect particle dark matter in the form of Weakly Interacting Massive Particles. Using an array of semiconductor detectors at millikelvin temperatures, CDMS has at times set the most sensitive limits on the interactions of WIMP dark matter with terrestrial materials. The first experiment, CDMS I, was run in a tunnel under the Stanford University campus. It was followed by CDMS II experiment in the Soudan Mine. The most recent experiment, SuperCDMS, was located deep underground in the Soudan Mine in northern Minnesota and collected data from 2011 through 2015. The series of experiments continues with SuperCDMS SNOLAB, an experiment located at the SNOLAB facility near Sudbury, Ontario in Canada that started construction in 2018 and is expected to start data taking in early 2020s.

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<span class="mw-page-title-main">DEAP</span>

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<span class="mw-page-title-main">European Underground Rare Event Calorimeter Array</span> Planned dark matter search experiment

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<span class="mw-page-title-main">EDELWEISS</span>

EDELWEISS is a dark matter search experiment located at the Modane Underground Laboratory in France. The experiment uses cryogenic detectors, measuring both the phonon and ionization signals produced by particle interactions in germanium crystals. This technique allows nuclear recoils events to be distinguished from electron recoil events.

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Ar
, which makes up one in every 1015 (quadrillion) atoms in atmospheric argon. The Darkside-10 (DS-10) prototype was tested in 2012, and the Darkside-50 (DS-50) experiment has been operating since 2013. Darkside-20k (DS-20k) with 20 tonnes of liquid argon is being planned as of 2019.

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<span class="mw-page-title-main">CUORE</span>

The Cryogenic Underground Observatory for Rare Events (CUORE[ˈkwɔːre], also Italian for 'heart') is a particle physics facility located underground at the Laboratori Nazionali del Gran Sasso in Assergi, Italy. CUORE was designed primarily as a search for neutrinoless double beta decay in 130Te, a process that has never been observed. It uses tellurium dioxide (TeO2) crystals as both the source of the decay and as bolometers to detect the resulting electrons. CUORE searches for the characteristic signal of neutrinoless double beta decay, a small peak in the observed energy spectrum around the known decay energy; for 130Te, this is Q = 2527.518 ± 0.013 keV. CUORE can also search for signals from dark matter candidates, such as axions and WIMPs.

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<span class="mw-page-title-main">ANAIS-112</span>

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References

  1. "CRESST: Home".
  2. 1 2 Davis, Jonathan (2015). "The Past and Future of Light Dark Matter Direct Detection". Int. J. Mod. Phys. A. 30 (15): 1530038. arXiv: 1506.03924 . Bibcode:2015IJMPA..3030038D. doi:10.1142/S0217751X15300380. S2CID   119269304.
  3. Lang, Rafael; Seidel, Wolfgang (2009). "Search for dark matter with CRESST". New Journal of Physics. 11 (10): 105017. arXiv: 0906.3290 . Bibcode:2009NJPh...11j5017L. doi: 10.1088/1367-2630/11/10/105017 .
  4. Angloher, G; Bauer, M; Bavykina, I; Bento, A; Bucci, C; Ciemniak, C; Deuter, G; von Feilitzsch, F; Hauff, D; Huff, P; Isaila, C; Jochum, J; Kiefer, M; Kimmerle, M; Lanfranchi, J. -C; Petricca, F; Pfister, S; Potzel, W; Pröbst, F; Reindl, F; Roth, S; Rottler, K; Sailer, C; Schäffner, K; Schmaler, J; Scholl, S; Seidel, W; Sivers, M. v; Stodolsky, L; et al. (Apr 12, 2012). "Results from 730 kg days of the CRESST-II Dark Matter search". European Physical Journal C. 72 (4): 1971. arXiv: 1109.0702 . Bibcode:2012EPJC...72.1971A. doi:10.1140/epjc/s10052-012-1971-8. S2CID   119283621.
  5. The CRESST Collaboration, Results on low mass WIMPs using an upgraded CRESST-II detector, https://arxiv.org/abs/1407.3146
  6. "New detectors allow search for lightweight dark matter particles". PhyOrg. September 2015. Retrieved 14 September 2015.
  7. A. H. Abdelhameed et al. (CRESST Collab.) (31 March 2019). "First results from the CRESST-III low-mass dark matter program". Physical Review D. 100 (10): 102002. arXiv: 1904.00498 . Bibcode:2019PhRvD.100j2002A. doi:10.1103/PhysRevD.100.102002. S2CID   90261775.
  8. "Searches for Dark Matter with the CRESST-III Experiment" (PDF). Indico.cern. 28 July 2020. Retrieved 20 January 2022.