Design and performance of a 35-ton liquid argon time projection chamber as a prototype for future very large detectors

Liquid argon time projection chamber technology is an attractive choice for large neutrino detectors, as it provides a high-resolution active target and it is expected to be scalable to very large masses. Consequently, it has been chosen as the technology for the first module of the DUNE far detecto...

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Veröffentlicht in:Journal of instrumentation 2020-03, Vol.15 (3), p.P03035-P03035, Article P03035
Hauptverfasser: Adams, D.L., Baird, M., Barr, G., Barros, N., Blake, A., Blaufuss, E., Booth, A., Brailsford, D., Buchanan, N., Carls, B., Chen, H., Convery, M., Geronimo, G. De, Dealtry, T., Dharmapalan, R., Djurcic, Z., Fowler, J., Glavin, S., Gomes, R.A., Goodman, M.C., Graham, M., Greenler, L., Hahn, A., Hartnell, J., Herbst, R., Higuera, A., Himmel, A., Insler, J., Jacobsen, J., Junk, T., Kirby, B., Klein, J., Kudryavtsev, V.A., Kutter, T., Li, Y., Li, X., Lin, S., McConkey, N., Moura, C.A., Mufson, S., Nambiar, N., Nowak, J., Nunes, M., Paulos, R., Qian, X., Rodrigues, O., Sands, W., Santucci, G., Sharma, R., Sinev, G., Spooner, N.J.C., Stancu, I., Stefan, D., Stewart, J., Stock, J., Strauss, T., Sulej, R., Sun, Y., Thiesse, M., Thompson, L.F., Tsai, Y.T., Berg, R. Van, Vieira, T., Wallbank, M., Wang, H., Wang, Y., Warburton, T.K., Wenman, D., Whittington, D., Wilson, R.J., Worcester, M., Yang, T., Yu, B., Zhang, C.
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container_issue 3
container_start_page P03035
container_title Journal of instrumentation
container_volume 15
creator Adams, D.L.
Baird, M.
Barr, G.
Barros, N.
Blake, A.
Blaufuss, E.
Booth, A.
Brailsford, D.
Buchanan, N.
Carls, B.
Chen, H.
Convery, M.
Geronimo, G. De
Dealtry, T.
Dharmapalan, R.
Djurcic, Z.
Fowler, J.
Glavin, S.
Gomes, R.A.
Goodman, M.C.
Graham, M.
Greenler, L.
Hahn, A.
Hartnell, J.
Herbst, R.
Higuera, A.
Himmel, A.
Insler, J.
Jacobsen, J.
Junk, T.
Kirby, B.
Klein, J.
Kudryavtsev, V.A.
Kutter, T.
Li, Y.
Li, X.
Lin, S.
McConkey, N.
Moura, C.A.
Mufson, S.
Nambiar, N.
Nowak, J.
Nunes, M.
Paulos, R.
Qian, X.
Rodrigues, O.
Sands, W.
Santucci, G.
Sharma, R.
Sinev, G.
Spooner, N.J.C.
Stancu, I.
Stefan, D.
Stewart, J.
Stock, J.
Strauss, T.
Sulej, R.
Sun, Y.
Thiesse, M.
Thompson, L.F.
Tsai, Y.T.
Berg, R. Van
Vieira, T.
Wallbank, M.
Wang, H.
Wang, Y.
Warburton, T.K.
Wenman, D.
Whittington, D.
Wilson, R.J.
Worcester, M.
Yang, T.
Yu, B.
Zhang, C.
description Liquid argon time projection chamber technology is an attractive choice for large neutrino detectors, as it provides a high-resolution active target and it is expected to be scalable to very large masses. Consequently, it has been chosen as the technology for the first module of the DUNE far detector. However, the fiducial mass required for “far detectors” of the next generation of neutrino oscillation experiments far exceeds what has been demonstrated so far. Scaling to this larger mass, as well as the requirement for underground construction places a number of additional constraints on the design. A prototype 35-ton cryostat was built at Fermi National Acccelerator Laboratory to test the functionality of the components foreseen to be used in a very large far detector. The Phase I run, completed in early 2014, demonstrated that liquid argon could be maintained at sufficient purity in a membrane cryostat. A time projection chamber was installed for the Phase II run, which collected data in February and March of 2016. The Phase II run was a test of the modular anode plane assemblies with wrapped wires, cold readout electronics, and integrated photon detection systems. While the details of the design do not match exactly those chosen for the DUNE far detector, the 35-ton TPC prototype is a demonstration of the functionality of the basic components. Measurements are performed using the Phase II data to extract signal and noise characteristics and to align the detector components. A measurement of the electron lifetime is presented, and a novel technique for measuring a track's position based on pulse properties is described.
doi_str_mv 10.1088/1748-0221/15/03/P03035
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De ; Dealtry, T. ; Dharmapalan, R. ; Djurcic, Z. ; Fowler, J. ; Glavin, S. ; Gomes, R.A. ; Goodman, M.C. ; Graham, M. ; Greenler, L. ; Hahn, A. ; Hartnell, J. ; Herbst, R. ; Higuera, A. ; Himmel, A. ; Insler, J. ; Jacobsen, J. ; Junk, T. ; Kirby, B. ; Klein, J. ; Kudryavtsev, V.A. ; Kutter, T. ; Li, Y. ; Li, X. ; Lin, S. ; McConkey, N. ; Moura, C.A. ; Mufson, S. ; Nambiar, N. ; Nowak, J. ; Nunes, M. ; Paulos, R. ; Qian, X. ; Rodrigues, O. ; Sands, W. ; Santucci, G. ; Sharma, R. ; Sinev, G. ; Spooner, N.J.C. ; Stancu, I. ; Stefan, D. ; Stewart, J. ; Stock, J. ; Strauss, T. ; Sulej, R. ; Sun, Y. ; Thiesse, M. ; Thompson, L.F. ; Tsai, Y.T. ; Berg, R. Van ; Vieira, T. ; Wallbank, M. ; Wang, H. ; Wang, Y. ; Warburton, T.K. ; Wenman, D. ; Whittington, D. ; Wilson, R.J. ; Worcester, M. ; Yang, T. ; Yu, B. ; Zhang, C. ; Argonne National Laboratory (ANL), Argonne, IL (United States) ; SLAC National Accelerator Laboratory (SLAC), Menlo Park, CA (United States) ; Fermi National Accelerator Laboratory (FNAL), Batavia, IL (United States) ; Brookhaven National Laboratory (BNL), Upton, NY (United States)</creatorcontrib><description>Liquid argon time projection chamber technology is an attractive choice for large neutrino detectors, as it provides a high-resolution active target and it is expected to be scalable to very large masses. Consequently, it has been chosen as the technology for the first module of the DUNE far detector. However, the fiducial mass required for “far detectors” of the next generation of neutrino oscillation experiments far exceeds what has been demonstrated so far. Scaling to this larger mass, as well as the requirement for underground construction places a number of additional constraints on the design. A prototype 35-ton cryostat was built at Fermi National Acccelerator Laboratory to test the functionality of the components foreseen to be used in a very large far detector. The Phase I run, completed in early 2014, demonstrated that liquid argon could be maintained at sufficient purity in a membrane cryostat. A time projection chamber was installed for the Phase II run, which collected data in February and March of 2016. The Phase II run was a test of the modular anode plane assemblies with wrapped wires, cold readout electronics, and integrated photon detection systems. While the details of the design do not match exactly those chosen for the DUNE far detector, the 35-ton TPC prototype is a demonstration of the functionality of the basic components. 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Van</creatorcontrib><creatorcontrib>Vieira, T.</creatorcontrib><creatorcontrib>Wallbank, M.</creatorcontrib><creatorcontrib>Wang, H.</creatorcontrib><creatorcontrib>Wang, Y.</creatorcontrib><creatorcontrib>Warburton, T.K.</creatorcontrib><creatorcontrib>Wenman, D.</creatorcontrib><creatorcontrib>Whittington, D.</creatorcontrib><creatorcontrib>Wilson, R.J.</creatorcontrib><creatorcontrib>Worcester, M.</creatorcontrib><creatorcontrib>Yang, T.</creatorcontrib><creatorcontrib>Yu, B.</creatorcontrib><creatorcontrib>Zhang, C.</creatorcontrib><creatorcontrib>Argonne National Laboratory (ANL), Argonne, IL (United States)</creatorcontrib><creatorcontrib>SLAC National Accelerator Laboratory (SLAC), Menlo Park, CA (United States)</creatorcontrib><creatorcontrib>Fermi National Accelerator Laboratory (FNAL), Batavia, IL (United States)</creatorcontrib><creatorcontrib>Brookhaven National Laboratory (BNL), Upton, NY (United States)</creatorcontrib><title>Design and performance of a 35-ton liquid argon time projection chamber as a prototype for future very large detectors</title><title>Journal of instrumentation</title><description>Liquid argon time projection chamber technology is an attractive choice for large neutrino detectors, as it provides a high-resolution active target and it is expected to be scalable to very large masses. Consequently, it has been chosen as the technology for the first module of the DUNE far detector. However, the fiducial mass required for “far detectors” of the next generation of neutrino oscillation experiments far exceeds what has been demonstrated so far. Scaling to this larger mass, as well as the requirement for underground construction places a number of additional constraints on the design. A prototype 35-ton cryostat was built at Fermi National Acccelerator Laboratory to test the functionality of the components foreseen to be used in a very large far detector. The Phase I run, completed in early 2014, demonstrated that liquid argon could be maintained at sufficient purity in a membrane cryostat. A time projection chamber was installed for the Phase II run, which collected data in February and March of 2016. The Phase II run was a test of the modular anode plane assemblies with wrapped wires, cold readout electronics, and integrated photon detection systems. While the details of the design do not match exactly those chosen for the DUNE far detector, the 35-ton TPC prototype is a demonstration of the functionality of the basic components. Measurements are performed using the Phase II data to extract signal and noise characteristics and to align the detector components. A measurement of the electron lifetime is presented, and a novel technique for measuring a track's position based on pulse properties is described.</description><subject>Argon</subject><subject>Data collection</subject><subject>Detectors</subject><subject>INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY</subject><subject>Large detector systems for particle and astroparticle physics</subject><subject>Liquid detectors</subject><subject>Neutrinos</subject><subject>Position measurement</subject><subject>Projection</subject><subject>Prototypes</subject><subject>Radiation counters</subject><subject>Sensors</subject><subject>Time projection chambers</subject><subject>Underground construction</subject><issn>1748-0221</issn><issn>1748-0221</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><recordid>eNqFkUtLAzEUhQdRsFb_ggRdj81zJgNupD6hoAtdh8zMTZsynbRJptB_b2pFxI2r5CbnO_dwb5ZdEnxDsJQTUnKZY0rJhIgJZpM3zDATR9no5-P41_00OwthibGoBMejbHsPwc57pPsWrcEb51e6bwA5gzRiIo-uR53dDLZF2s9TEe0K0Nq7JTTRprpZ6FUNHumQgPQeXdytASUjZIY4eEBb8DvUJRpQCzFhzofz7MToLsDF9znOPh4f3qfP-ez16WV6N8sbXuCY81KWuBatqMBUspKGC0okaWnNjdGFKGVRG8I0FkApByiZYYZ8yXFJq5aNs6uDrwvRqtDY1H_RuL5PMRQpME2uSXR9EKX4mwFCVEs3-D7lUpRJLkpScZlUxUHVeBeCB6PW3q603ymC1X4Raj9jtZ-xIkJhpg6LSODtHzDF0PvhRa9t9x_-CR03jng</recordid><startdate>20200331</startdate><enddate>20200331</enddate><creator>Adams, D.L.</creator><creator>Baird, M.</creator><creator>Barr, G.</creator><creator>Barros, N.</creator><creator>Blake, A.</creator><creator>Blaufuss, E.</creator><creator>Booth, A.</creator><creator>Brailsford, D.</creator><creator>Buchanan, N.</creator><creator>Carls, B.</creator><creator>Chen, H.</creator><creator>Convery, M.</creator><creator>Geronimo, G. 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De ; Dealtry, T. ; Dharmapalan, R. ; Djurcic, Z. ; Fowler, J. ; Glavin, S. ; Gomes, R.A. ; Goodman, M.C. ; Graham, M. ; Greenler, L. ; Hahn, A. ; Hartnell, J. ; Herbst, R. ; Higuera, A. ; Himmel, A. ; Insler, J. ; Jacobsen, J. ; Junk, T. ; Kirby, B. ; Klein, J. ; Kudryavtsev, V.A. ; Kutter, T. ; Li, Y. ; Li, X. ; Lin, S. ; McConkey, N. ; Moura, C.A. ; Mufson, S. ; Nambiar, N. ; Nowak, J. ; Nunes, M. ; Paulos, R. ; Qian, X. ; Rodrigues, O. ; Sands, W. ; Santucci, G. ; Sharma, R. ; Sinev, G. ; Spooner, N.J.C. ; Stancu, I. ; Stefan, D. ; Stewart, J. ; Stock, J. ; Strauss, T. ; Sulej, R. ; Sun, Y. ; Thiesse, M. ; Thompson, L.F. ; Tsai, Y.T. ; Berg, R. Van ; Vieira, T. ; Wallbank, M. ; Wang, H. ; Wang, Y. ; Warburton, T.K. ; Wenman, D. ; Whittington, D. ; Wilson, R.J. ; Worcester, M. ; Yang, T. ; Yu, B. ; Zhang, C.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c460t-47870b5d59ef9898f452181d2b4ffa65786bf13a05e224ee73f3f1d59ef0729d3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>Argon</topic><topic>Data collection</topic><topic>Detectors</topic><topic>INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY</topic><topic>Large detector systems for particle and astroparticle physics</topic><topic>Liquid detectors</topic><topic>Neutrinos</topic><topic>Position measurement</topic><topic>Projection</topic><topic>Prototypes</topic><topic>Radiation counters</topic><topic>Sensors</topic><topic>Time projection chambers</topic><topic>Underground construction</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Adams, D.L.</creatorcontrib><creatorcontrib>Baird, M.</creatorcontrib><creatorcontrib>Barr, G.</creatorcontrib><creatorcontrib>Barros, N.</creatorcontrib><creatorcontrib>Blake, A.</creatorcontrib><creatorcontrib>Blaufuss, E.</creatorcontrib><creatorcontrib>Booth, A.</creatorcontrib><creatorcontrib>Brailsford, D.</creatorcontrib><creatorcontrib>Buchanan, N.</creatorcontrib><creatorcontrib>Carls, B.</creatorcontrib><creatorcontrib>Chen, H.</creatorcontrib><creatorcontrib>Convery, M.</creatorcontrib><creatorcontrib>Geronimo, G. De</creatorcontrib><creatorcontrib>Dealtry, T.</creatorcontrib><creatorcontrib>Dharmapalan, R.</creatorcontrib><creatorcontrib>Djurcic, Z.</creatorcontrib><creatorcontrib>Fowler, J.</creatorcontrib><creatorcontrib>Glavin, S.</creatorcontrib><creatorcontrib>Gomes, R.A.</creatorcontrib><creatorcontrib>Goodman, M.C.</creatorcontrib><creatorcontrib>Graham, M.</creatorcontrib><creatorcontrib>Greenler, L.</creatorcontrib><creatorcontrib>Hahn, A.</creatorcontrib><creatorcontrib>Hartnell, J.</creatorcontrib><creatorcontrib>Herbst, R.</creatorcontrib><creatorcontrib>Higuera, A.</creatorcontrib><creatorcontrib>Himmel, A.</creatorcontrib><creatorcontrib>Insler, J.</creatorcontrib><creatorcontrib>Jacobsen, J.</creatorcontrib><creatorcontrib>Junk, T.</creatorcontrib><creatorcontrib>Kirby, B.</creatorcontrib><creatorcontrib>Klein, J.</creatorcontrib><creatorcontrib>Kudryavtsev, V.A.</creatorcontrib><creatorcontrib>Kutter, T.</creatorcontrib><creatorcontrib>Li, Y.</creatorcontrib><creatorcontrib>Li, X.</creatorcontrib><creatorcontrib>Lin, S.</creatorcontrib><creatorcontrib>McConkey, N.</creatorcontrib><creatorcontrib>Moura, C.A.</creatorcontrib><creatorcontrib>Mufson, S.</creatorcontrib><creatorcontrib>Nambiar, N.</creatorcontrib><creatorcontrib>Nowak, J.</creatorcontrib><creatorcontrib>Nunes, M.</creatorcontrib><creatorcontrib>Paulos, R.</creatorcontrib><creatorcontrib>Qian, X.</creatorcontrib><creatorcontrib>Rodrigues, O.</creatorcontrib><creatorcontrib>Sands, W.</creatorcontrib><creatorcontrib>Santucci, G.</creatorcontrib><creatorcontrib>Sharma, R.</creatorcontrib><creatorcontrib>Sinev, G.</creatorcontrib><creatorcontrib>Spooner, N.J.C.</creatorcontrib><creatorcontrib>Stancu, I.</creatorcontrib><creatorcontrib>Stefan, D.</creatorcontrib><creatorcontrib>Stewart, J.</creatorcontrib><creatorcontrib>Stock, J.</creatorcontrib><creatorcontrib>Strauss, T.</creatorcontrib><creatorcontrib>Sulej, R.</creatorcontrib><creatorcontrib>Sun, Y.</creatorcontrib><creatorcontrib>Thiesse, M.</creatorcontrib><creatorcontrib>Thompson, L.F.</creatorcontrib><creatorcontrib>Tsai, Y.T.</creatorcontrib><creatorcontrib>Berg, R. Van</creatorcontrib><creatorcontrib>Vieira, T.</creatorcontrib><creatorcontrib>Wallbank, M.</creatorcontrib><creatorcontrib>Wang, H.</creatorcontrib><creatorcontrib>Wang, Y.</creatorcontrib><creatorcontrib>Warburton, T.K.</creatorcontrib><creatorcontrib>Wenman, D.</creatorcontrib><creatorcontrib>Whittington, D.</creatorcontrib><creatorcontrib>Wilson, R.J.</creatorcontrib><creatorcontrib>Worcester, M.</creatorcontrib><creatorcontrib>Yang, T.</creatorcontrib><creatorcontrib>Yu, B.</creatorcontrib><creatorcontrib>Zhang, C.</creatorcontrib><creatorcontrib>Argonne National Laboratory (ANL), Argonne, IL (United States)</creatorcontrib><creatorcontrib>SLAC National Accelerator Laboratory (SLAC), Menlo Park, CA (United States)</creatorcontrib><creatorcontrib>Fermi National Accelerator Laboratory (FNAL), Batavia, IL (United States)</creatorcontrib><creatorcontrib>Brookhaven National Laboratory (BNL), Upton, NY (United States)</creatorcontrib><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>OSTI.GOV - Hybrid</collection><collection>OSTI.GOV</collection><jtitle>Journal of instrumentation</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Adams, D.L.</au><au>Baird, M.</au><au>Barr, G.</au><au>Barros, N.</au><au>Blake, A.</au><au>Blaufuss, E.</au><au>Booth, A.</au><au>Brailsford, D.</au><au>Buchanan, N.</au><au>Carls, B.</au><au>Chen, H.</au><au>Convery, M.</au><au>Geronimo, G. De</au><au>Dealtry, T.</au><au>Dharmapalan, R.</au><au>Djurcic, Z.</au><au>Fowler, J.</au><au>Glavin, S.</au><au>Gomes, R.A.</au><au>Goodman, M.C.</au><au>Graham, M.</au><au>Greenler, L.</au><au>Hahn, A.</au><au>Hartnell, J.</au><au>Herbst, R.</au><au>Higuera, A.</au><au>Himmel, A.</au><au>Insler, J.</au><au>Jacobsen, J.</au><au>Junk, T.</au><au>Kirby, B.</au><au>Klein, J.</au><au>Kudryavtsev, V.A.</au><au>Kutter, T.</au><au>Li, Y.</au><au>Li, X.</au><au>Lin, S.</au><au>McConkey, N.</au><au>Moura, C.A.</au><au>Mufson, S.</au><au>Nambiar, N.</au><au>Nowak, J.</au><au>Nunes, M.</au><au>Paulos, R.</au><au>Qian, X.</au><au>Rodrigues, O.</au><au>Sands, W.</au><au>Santucci, G.</au><au>Sharma, R.</au><au>Sinev, G.</au><au>Spooner, N.J.C.</au><au>Stancu, I.</au><au>Stefan, D.</au><au>Stewart, J.</au><au>Stock, J.</au><au>Strauss, T.</au><au>Sulej, R.</au><au>Sun, Y.</au><au>Thiesse, M.</au><au>Thompson, L.F.</au><au>Tsai, Y.T.</au><au>Berg, R. Van</au><au>Vieira, T.</au><au>Wallbank, M.</au><au>Wang, H.</au><au>Wang, Y.</au><au>Warburton, T.K.</au><au>Wenman, D.</au><au>Whittington, D.</au><au>Wilson, R.J.</au><au>Worcester, M.</au><au>Yang, T.</au><au>Yu, B.</au><au>Zhang, C.</au><aucorp>Argonne National Laboratory (ANL), Argonne, IL (United States)</aucorp><aucorp>SLAC National Accelerator Laboratory (SLAC), Menlo Park, CA (United States)</aucorp><aucorp>Fermi National Accelerator Laboratory (FNAL), Batavia, IL (United States)</aucorp><aucorp>Brookhaven National Laboratory (BNL), Upton, NY (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Design and performance of a 35-ton liquid argon time projection chamber as a prototype for future very large detectors</atitle><jtitle>Journal of instrumentation</jtitle><date>2020-03-31</date><risdate>2020</risdate><volume>15</volume><issue>3</issue><spage>P03035</spage><epage>P03035</epage><pages>P03035-P03035</pages><artnum>P03035</artnum><issn>1748-0221</issn><eissn>1748-0221</eissn><abstract>Liquid argon time projection chamber technology is an attractive choice for large neutrino detectors, as it provides a high-resolution active target and it is expected to be scalable to very large masses. Consequently, it has been chosen as the technology for the first module of the DUNE far detector. However, the fiducial mass required for “far detectors” of the next generation of neutrino oscillation experiments far exceeds what has been demonstrated so far. Scaling to this larger mass, as well as the requirement for underground construction places a number of additional constraints on the design. A prototype 35-ton cryostat was built at Fermi National Acccelerator Laboratory to test the functionality of the components foreseen to be used in a very large far detector. The Phase I run, completed in early 2014, demonstrated that liquid argon could be maintained at sufficient purity in a membrane cryostat. A time projection chamber was installed for the Phase II run, which collected data in February and March of 2016. The Phase II run was a test of the modular anode plane assemblies with wrapped wires, cold readout electronics, and integrated photon detection systems. While the details of the design do not match exactly those chosen for the DUNE far detector, the 35-ton TPC prototype is a demonstration of the functionality of the basic components. Measurements are performed using the Phase II data to extract signal and noise characteristics and to align the detector components. A measurement of the electron lifetime is presented, and a novel technique for measuring a track's position based on pulse properties is described.</abstract><cop>Bristol</cop><pub>IOP Publishing</pub><doi>10.1088/1748-0221/15/03/P03035</doi><oa>free_for_read</oa></addata></record>
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identifier ISSN: 1748-0221
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1748-0221
language eng
recordid cdi_osti_scitechconnect_1602989
source Institute of Physics Journals
subjects Argon
Data collection
Detectors
INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY
Large detector systems for particle and astroparticle physics
Liquid detectors
Neutrinos
Position measurement
Projection
Prototypes
Radiation counters
Sensors
Time projection chambers
Underground construction
title Design and performance of a 35-ton liquid argon time projection chamber as a prototype for future very large detectors
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