2013
DOI: 10.1088/1748-0221/8/04/p04024
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Characterization of protonated and deuterated tetra-phenyl butadiene film in a polystyrene matrix

Abstract: We study the effect of deuteration and annealing on the fluorescence spectrum shape and VUV to visible conversion efficiency of TPB films in a polystyrene matrix with input light from 120 to 220 nm. We observed no discernible difference in the fluorescence spectrum shape between any of the films. The deuterated film performed equally well compared to the standard one in terms of conversion efficiency, but annealing seems to degrade this efficiency to roughly 75% of its non annealed value at all wavelengths stu… Show more

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Cited by 17 publications
(32 citation statements)
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“…The PMTs were electrically insulated from the gap by an acrylic box. Three of the four PMTs were made sensitive to the VUV emission of pure Ar by depositing a WLS films (based on TPB in polystyrene matrix [51]) on the inner box surface facing the EL gap in front of these PMTs. Let us designate this readout configuration as 3PMT+WLS.…”
Section: Experimental Setup and Proceduresmentioning
confidence: 99%
See 1 more Smart Citation
“…The PMTs were electrically insulated from the gap by an acrylic box. Three of the four PMTs were made sensitive to the VUV emission of pure Ar by depositing a WLS films (based on TPB in polystyrene matrix [51]) on the inner box surface facing the EL gap in front of these PMTs. Let us designate this readout configuration as 3PMT+WLS.…”
Section: Experimental Setup and Proceduresmentioning
confidence: 99%
“…Regarding the conversion efficiency of the TPB-based WLS, in our previous works [16,18] we used CE = 0.58 around 128 nm [51], CE = 0.40 at 300-400 nm [51,55,57] and CE = 0 above 400 nm. However, the TPB conversion efficiency at 128 nm has recently been significantly revised towards a decrease [58]: the correction factor reached 2.…”
Section: Experimental Setup and Proceduresmentioning
confidence: 99%
“…The first assembly, which will be referred to hereafter as PMT-UV, is comprised of a wavelength shifting plate supported above an 8-inch cryogenic Hamamatsu R5912-02mod PMT [8], which is mounted inside a mu-metal shield. The wavelength shifting plate is a 12-inch disc of clear acrylic upon one side of which is a coating of tetraphenyl butadiene (TPB) suspended in a polystyrene matrix [24][25][26]. The purpose of the plate is to capture the 128 nm argon scintillation light and re-emit at visible wavelengths, with an emission spectrum peaked around 450 nm where PMT quantum efficiency is high [27].…”
Section: Experimental Configuration For This Studymentioning
confidence: 99%
“…Lastly, the larger R11410 has been used in the Panda-X experiment (bottom array) and will be used by next-generation dark matter experiments, such as LZ, XENON1T/NT, and RED, among others. The experimental setup used for all measurements is shown schematically in Figure 1 and is similar to the one used in References [10,11,12]. A Model 632 Deuterium Light source, from McPherson, Inc. [13] created a broad spectrum extending from 110-950 nm with the window facing into a vacuum space pumped down to below 10 −4 Torr.…”
Section: Introductionmentioning
confidence: 99%