scholarly journals Design of Low-energy Calibration Sources for Liquid Xenon Dark Matter Detectors

2015 ◽  
Vol 61 ◽  
pp. 714-718
Author(s):  
K. Hosokawa
2007 ◽  
Vol 173 ◽  
pp. 160-163 ◽  
Author(s):  
T. Shutt ◽  
C.E. Dahl ◽  
J. Kwong ◽  
A. Bolozdynya ◽  
P. Brusov

2011 ◽  
Vol 26 (13) ◽  
pp. 925-935 ◽  
Author(s):  
DAVID B. CLINE

We briefly review the constraints on the search for low mass WIMPs (<15 GeV) and the various experimental methods. These experiments depend on the response of detectors to low energy signals (less than 15 keV equivalent energy). We then describe recent fits to the data and attempt to determine L eff , the energy response at low energy. We find that the use of a liquid Xenon two-phase detector that employs the S2 data near threshold is the most sensitive current study of the low mass region. We rely on some talks at Dark Matter 2010.


1987 ◽  
Vol 117 ◽  
pp. 490-490
Author(s):  
A. K. Drukier ◽  
K. Freese ◽  
D. N. Spergel

We consider the use of superheated superconducting colloids as detectors of weakly interacting galactic halo candidate particles (e.g. photinos, massive neutrinos, and scalar neutrinos). These low temperature detectors are sensitive to the deposition of a few hundreds of eV's. The recoil of a dark matter particle off of a superheated superconducting grain in the detector causes the grain to make a transition to the normal state. Their low energy threshold makes this class of detectors ideal for detecting massive weakly interacting halo particles.We discuss realistic models for the detector and for the galactic halo. We show that the expected count rate (≈103 count/day for scalar and massive neutrinos) exceeds the expected background by several orders of magnitude. For photinos, we expect ≈1 count/day, more than 100 times the predicted background rate. We find that if the detector temperature is maintained at 50 mK and the system noise is reduced below 5 × 10−4 flux quanta, particles with mass as low as 2 GeV can be detected. We show that the earth's motion around the Sun can produce a significant annual modulation in the signal.


Instruments ◽  
2021 ◽  
Vol 5 (1) ◽  
pp. 13
Author(s):  
Matthew Szydagis ◽  
Grant A. Block ◽  
Collin Farquhar ◽  
Alexander J. Flesher ◽  
Ekaterina S. Kozlova ◽  
...  

Detectors based upon the noble elements, especially liquid xenon as well as liquid argon, as both single- and dual-phase types, require reconstruction of the energies of interacting particles, both in the field of direct detection of dark matter (weakly interacting massive particles WIMPs, axions, etc.) and in neutrino physics. Experimentalists, as well as theorists who reanalyze/reinterpret experimental data, have used a few different techniques over the past few decades. In this paper, we review techniques based on solely the primary scintillation channel, the ionization or secondary channel available at non-zero drift electric fields, and combined techniques that include a simple linear combination and weighted averages, with a brief discussion of the application of profile likelihood, maximum likelihood, and machine learning. Comparing results for electron recoils (beta and gamma interactions) and nuclear recoils (primarily from neutrons) from the Noble Element Simulation Technique (NEST) simulation to available data, we confirm that combining all available information generates higher-precision means, lower widths (energy resolution), and more symmetric shapes (approximately Gaussian) especially at keV-scale energies, with the symmetry even greater when thresholding is addressed. Near thresholds, bias from upward fluctuations matters. For MeV-GeV scales, if only one channel is utilized, an ionization-only-based energy scale outperforms scintillation; channel combination remains beneficial. We discuss here what major collaborations use.


2002 ◽  
Vol 524 (3-4) ◽  
pp. 245-251 ◽  
Author(s):  
D Akimov ◽  
A Bewick ◽  
D Davidge ◽  
J Dawson ◽  
A.S Howard ◽  
...  

2017 ◽  
Vol 96 (10) ◽  
Author(s):  
L. W. Goetzke ◽  
E. Aprile ◽  
M. Anthony ◽  
G. Plante ◽  
M. Weber
Keyword(s):  

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