Track reconstruction and performance of DRIFT directional dark matter detectors using alpha particles
File(s)0707.1758v1.pdf (447.09 KB)
Accepted version
Author(s)
Type
Journal Article
Abstract
First results are presented from an analysis of data from the DRIFT-IIa and DRIFT-IIb directional dark matter detectors at Boulby Mine in which alpha particle tracks were reconstructed and used to characterise detector performance—an important step towards
optimising directional technology. The drift velocity in DRIFT-IIa was 59
:
3
0
:
2 (stat)
7
:
5 (sys) ms
1
based on an analysis of
naturally occurring alpha-emitting background. The drift velocity in DRIFT-IIb was 57
1 (stat)
3 (sys) ms
1
determined by the
analysis of alpha particle tracks from a
210
Po source. Three-dimensional range reconstruction and range spectra were used to identify
alpha particles from the decay of
222
Rn,
218
Po,
220
Rn and
216
Po. This study found that
ð
22
2
Þ
%of
218
Po progeny (from
222
Rn decay)
did not plate out and remained suspended in the 40 Torr CS
2
gas fill until they decayed. A likely explanation for this is that some of the
polonium progeny are produced in an uncharged state. For
216
Po progeny (from
220
Rn decay) the undeposited fraction was apparently
much higher at
ð
100
þ
0
35
Þ
% most likely due to a shorter lifetime, causing a larger fraction of the progeny to decay whilst drifting to the cathode plane. This explanation implies a much slower drift time for positively charged polonium progeny compared to CS2 ions.
optimising directional technology. The drift velocity in DRIFT-IIa was 59
:
3
0
:
2 (stat)
7
:
5 (sys) ms
1
based on an analysis of
naturally occurring alpha-emitting background. The drift velocity in DRIFT-IIb was 57
1 (stat)
3 (sys) ms
1
determined by the
analysis of alpha particle tracks from a
210
Po source. Three-dimensional range reconstruction and range spectra were used to identify
alpha particles from the decay of
222
Rn,
218
Po,
220
Rn and
216
Po. This study found that
ð
22
2
Þ
%of
218
Po progeny (from
222
Rn decay)
did not plate out and remained suspended in the 40 Torr CS
2
gas fill until they decayed. A likely explanation for this is that some of the
polonium progeny are produced in an uncharged state. For
216
Po progeny (from
220
Rn decay) the undeposited fraction was apparently
much higher at
ð
100
þ
0
35
Þ
% most likely due to a shorter lifetime, causing a larger fraction of the progeny to decay whilst drifting to the cathode plane. This explanation implies a much slower drift time for positively charged polonium progeny compared to CS2 ions.
Date Issued
2008-01-01
Date Acceptance
2007-10-08
Citation
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, 2008, 584 (1), pp.114-128
ISSN
0168-9002
Publisher
Elsevier
Start Page
114
End Page
128
Journal / Book Title
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
Volume
584
Issue
1
Copyright Statement
© 2008 Elsevier Ltd. All rights reserved. This manuscript is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 International Licence http://creativecommons.org/licenses/by-nc-nd/4.0/
Identifier
http://gateway.webofknowledge.com/gateway/Gateway.cgi?GWVersion=2&SrcApp=PARTNER_APP&SrcAuth=LinksAMR&KeyUT=WOS:000252559100008&DestLinkType=FullRecord&DestApp=ALL_WOS&UsrCustomerID=1ba7043ffcc86c417c072aa74d649202
Subjects
Science & Technology
Technology
Physical Sciences
Instruments & Instrumentation
Nuclear Science & Technology
Physics, Nuclear
Physics, Particles & Fields
Physics
dark matter
WIMPs
TPC
gas detector
directional detector
negative ion drift
alpha spectrometry
RADON PROGENY
PO-218
POLONIUM-218
DIFFUSION
NEUTRALIZATION
OPERATION
DESIGN
Publication Status
Published
Date Publish Online
2007-10-13