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@article{Linehan:2022:10.1016/j.nima.2021.165955,
author = {Linehan, R and Mannino, RL and Fan, A and Ignarra, CM and Luitz, S and Skarpaas, K and Shutt, TA and Akerib, DS and Alsum, SK and Anderson, TJ and Araújo, HM and Arthurs, M and Auyeung, H and Bailey, AJ and Biesiadzinski, TP and Breidenbach, M and Cherwinka, JJ and Conley, RA and Genovesi, J and Gilchriese, MGD and Glaenzer, A and Gonda, TG and Hanzel, K and Hoff, MD and Ji, W and Kaboth, AC and Kravitz, S and Kurita, NR and Lambert, AR and Lesko, KT and Lorenzon, W and Majewski, PA and Miller, EH and Monzani, ME and Palladino, KJ and Ratcliff, BN and Saba, JS and Santone, D and Shutt, GW and Stifter, K and Szydagis, M and Tomás, A and Vavra, J and Waldron, WL and Webb, RC and White, RG and Whitis, TJ and Wilson, K and Wisniewski, WJ},
doi = {10.1016/j.nima.2021.165955},
journal = {Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment},
title = {Design and production of the high voltage electrode grids and electron extraction region for the LZ dual-phase xenon time projection chamber},
url = {http://dx.doi.org/10.1016/j.nima.2021.165955},
volume = {1031},
year = {2022}
}

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TY  - JOUR
AB  - The dual-phase xenon time projection chamber (TPC) is a powerful tool for direct-detection experiments searching for WIMP dark matter, other dark matter models, and neutrinoless double-beta decay. Successful operation of such a TPC is critically dependent on the ability to hold high electric fields in the bulk liquid, across the liquid surface, and in the gas. Careful design and construction of the electrodes used to establish these fields is therefore required. We present the design and production of the LUX-ZEPLIN (LZ) experiment’s high-voltage electrodes, a set of four woven mesh wire grids. Grid design drivers are discussed, with emphasis placed on design of the electron extraction region. We follow this with a description of the grid production process and a discussion of steps taken to validate the LZ grids prior to integration into the TPC.
AU  - Linehan,R
AU  - Mannino,RL
AU  - Fan,A
AU  - Ignarra,CM
AU  - Luitz,S
AU  - Skarpaas,K
AU  - Shutt,TA
AU  - Akerib,DS
AU  - Alsum,SK
AU  - Anderson,TJ
AU  - Araújo,HM
AU  - Arthurs,M
AU  - Auyeung,H
AU  - Bailey,AJ
AU  - Biesiadzinski,TP
AU  - Breidenbach,M
AU  - Cherwinka,JJ
AU  - Conley,RA
AU  - Genovesi,J
AU  - Gilchriese,MGD
AU  - Glaenzer,A
AU  - Gonda,TG
AU  - Hanzel,K
AU  - Hoff,MD
AU  - Ji,W
AU  - Kaboth,AC
AU  - Kravitz,S
AU  - Kurita,NR
AU  - Lambert,AR
AU  - Lesko,KT
AU  - Lorenzon,W
AU  - Majewski,PA
AU  - Miller,EH
AU  - Monzani,ME
AU  - Palladino,KJ
AU  - Ratcliff,BN
AU  - Saba,JS
AU  - Santone,D
AU  - Shutt,GW
AU  - Stifter,K
AU  - Szydagis,M
AU  - Tomás,A
AU  - Vavra,J
AU  - Waldron,WL
AU  - Webb,RC
AU  - White,RG
AU  - Whitis,TJ
AU  - Wilson,K
AU  - Wisniewski,WJ
DO  - 10.1016/j.nima.2021.165955
PY  - 2022///
SN  - 0168-9002
TI  - Design and production of the high voltage electrode grids and electron extraction region for the LZ dual-phase xenon time projection chamber
T2  - Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
UR  - http://dx.doi.org/10.1016/j.nima.2021.165955
UR  - https://www.sciencedirect.com/science/article/pii/S0168900221009062?via%3Dihub
UR  - http://hdl.handle.net/10044/1/95987
VL  - 1031
ER  -

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