2014
DOI: 10.1088/1748-0221/9/11/p11012
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Measurements of proportional scintillation and electron multiplication in liquid xenon using thin wires

Abstract: Proportional scintillation in liquid xenon has a promising application in the field of direct dark matter detection, potentially allowing for simpler, more sensitive detectors. However, knowledge of the basic properties of the phenomenon as well as guidelines for its practical use are currently limited. We report here on measurements of proportional scintillation light emitted in liquid xenon around thin wires. The maximum proportional scintillation gain of 287 +97 −75 photons per drift electron was obtained u… Show more

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Cited by 38 publications
(91 citation statements)
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“…We note that with a charge gain of ~2, an S2 yield of ~50 photons/electron is consistent with that obtained for thin wires in [17], where an S2 yield of ~290 photons/electron was obtained with a charge gain of ~13. Figure 14: Charge gain as a function of the THGEM voltage at 1.30 bar and 2.05 bar under 'steady state S2' conditions.…”
Section: Additional Observationssupporting
confidence: 89%
See 1 more Smart Citation
“…We note that with a charge gain of ~2, an S2 yield of ~50 photons/electron is consistent with that obtained for thin wires in [17], where an S2 yield of ~290 photons/electron was obtained with a charge gain of ~13. Figure 14: Charge gain as a function of the THGEM voltage at 1.30 bar and 2.05 bar under 'steady state S2' conditions.…”
Section: Additional Observationssupporting
confidence: 89%
“…A possible solution to this problem is to move from a dual-phase TPC configuration to a single-phase liquid-only TPC scheme in which S2 signals would be generated by electrodes immersed within the liquid, rather than in the vapor phase [15,16]. One implementation, suggested in [16] and studied in [17] and [18], relies on thin (Ø5-20 μm) anode wires. In this scheme ionization electrons released at the point of interaction drift towards the immersed wires, where they induce secondary scintillation (accompanied by modest charge multiplication) in the intense field close to the wire surface.…”
Section: Introductionmentioning
confidence: 99%
“…The electrostatic design methodology adopted by previous experiments was thus found to be compromised. This was based on the onsets for electroluminescence and charge multiplication in LXe at 412 +10 −133 kV/cm and 725 +48 −139 kV/cm, respectively [8] (see also [9,10]), while practical LXe-TPC cathodes made from stainless steel wires have been limited to surface fields of 40-65 kV/cm [11][12][13][14][15][16]. A detector with gold-plated stainless steel wires could not operate at the design field either [17].…”
Section: Introductionmentioning
confidence: 99%
“…For example, many researchers considered electron multiplication in the liquid phase unlikely due to the strong scattering effects that are expected for such high density. Yet, electron avalanches have already been observed in liquid argon, [61][62][63] xenon, [64][65][66] nitrogen, 61 sulfur, 67 cyclohexane, 68,69 and propane. 69 For cryogenic liquids, the lower breakdown strength of the liquid phase as compared to the gaseous phase has been explained with the absence of inelastic electron energy losses in liquid.…”
mentioning
confidence: 99%