2014
DOI: 10.1103/physrevd.89.072013
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The SIMPLE Phase II dark matter search

Abstract: Phase II of SIMPLE (Superheated Instrument for Massive ParticLe Experiments) searched for astroparticle dark matter using superheated liquid C2ClF5 droplet detectors. Each droplet generally requires an energy deposition with linear energy transfer (LET) > ∼ 150 keV/µm for a liquid-to-gas phase transition, providing an intrinsic rejection against minimum ionizing particles of order 10 −10 , and reducing the backgrounds to primarily α and neutron-induced recoil events. The droplet phase transition generates a mi… Show more

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Cited by 53 publications
(46 citation statements)
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“…(ii) When the liquid pressure is slightly below the equilibrium pressure, the deviations in the free energy for bubble formation from the CNT become large. For example, in dark matter detection experiments which use superheated liquids as targets [6][7][8][9], the degree of nonequilibrium is very small. For such a near-equilibrium case, the PCNT should be used instead of CNT.…”
Section: Discussionmentioning
confidence: 99%
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“…(ii) When the liquid pressure is slightly below the equilibrium pressure, the deviations in the free energy for bubble formation from the CNT become large. For example, in dark matter detection experiments which use superheated liquids as targets [6][7][8][9], the degree of nonequilibrium is very small. For such a near-equilibrium case, the PCNT should be used instead of CNT.…”
Section: Discussionmentioning
confidence: 99%
“…Bubble nucleation in liquid is a liquid-to-vapor transition [1] phenomenon, and plays an important role in many areas of science and technology, e.g., degassification of steel [1], bubble jet printers [2], volcanism [3][4][5], the direct detection of dark matter [6][7][8][9], and medicine [10,11]. Bubble nucleation occurs in a metastable liquid under a pressure below its equilibrium vapor pressure.…”
Section: Introductionmentioning
confidence: 99%
“…Underground testing of the standard DM SDD demonstrated an intrinsic background in the order of 10 −4 count/h and 10 −3 count/h for n and , respectively [9] with a detection efficiency of ∼95% [10]. The background signal being the critical parameter to qualify an instrument's ability for low-level measurements, our SDD has an intrinsic -background signal 100 times smaller than that of the ionisation counter, and a comparable detection sensitivity.…”
Section: I-dust 2016mentioning
confidence: 99%
“…At signal amplitudes of ∼100 mV there is a 20 mV gap between the and n-distributions which is clearly resolved by the signal acquisition system (resolution 0.3 mV) [9].…”
Section: Event Localisation and Discriminationmentioning
confidence: 99%
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