Identification and reconstruction of low-energy electrons in the ProtoDUNE-SP detector
Phys. Rev. D 107, 092012 (2023) Measurements of electrons from $\nu_e$ interactions are crucial for the Deep Underground Neutrino Experiment (DUNE) neutrino oscillation program, as well as searches for physics beyond the standard model, supernova neutrino detection, and solar neutrino measurements....
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creator | Acciarri, R Adamowski, M Aduszkiewicz, A Aimard, B Akbar, F Alrashed, M Asquith, L Aushev, V Back, J. J Barros, A Bevan, A Boran, F Boyden, D Brice, S. J Bross, A Calabrese, R Castillo, A Chatterjee, A Cicero, V Collot, J Cremaldi, L da Motta, H De, S De Almeida, P Decowski, M. P De Souza, G Ezeribe, A. C Fajt, L Filip, P Filkins, A Fiorillo, G Freestone, J Gibin, D Granados, E Granger, P Grenard, J Hamacher-Baumann, P Hamilton, P Morquecho, M. A. Hernandez Howell, R Hristova, I Huang, J Hulcher, Z Illingworth, R Oliveira, M. Ismerio Jediny, F Jiang, L Kearns, E King, B Kose, U Kurita, N Marinho, F Martynenko, S Matichard, F Mendez, P Meng, G Meyer, H Mohanta, R Molina, J Mote, M Papaleo, R Papanestis, A Parsa, S Patton, S. J Pershey, D Pickering, L Radeka, V Rameika, R Rigamonti, A Rigaut, Y Rivera, D Rossi, M Rout, J Sala, P Sharma, R Shrock, R Skarpaas, K Soleti, S. R Surdo, A Talukdar, N Tomassetti, L Touramanis, C Trilov, S Tsang, K. V Utaegbulam, H Valentim, R Oliva, D. Vargas Vaughan, N Verzocchi, M Vicenzi, M Vrba, T Wang, H Wetstein, M Williams, Z Worcester, M Wu, S Yandel, E Yankelevich, A Yuan, W Zuklin, J |
description | Phys. Rev. D 107, 092012 (2023) Measurements of electrons from $\nu_e$ interactions are crucial for the Deep
Underground Neutrino Experiment (DUNE) neutrino oscillation program, as well as
searches for physics beyond the standard model, supernova neutrino detection,
and solar neutrino measurements. This article describes the selection and
reconstruction of low-energy (Michel) electrons in the ProtoDUNE-SP detector.
ProtoDUNE-SP is one of the prototypes for the DUNE far detector, built and
operated at CERN as a charged particle test beam experiment. A sample of
low-energy electrons produced by the decay of cosmic muons is selected with a
purity of 95%. This sample is used to calibrate the low-energy electron energy
scale with two techniques. An electron energy calibration based on a cosmic ray
muon sample uses calibration constants derived from measured and simulated
cosmic ray muon events. Another calibration technique makes use of the
theoretically well-understood Michel electron energy spectrum to convert
reconstructed charge to electron energy. In addition, the effects of detector
response to low-energy electron energy scale and its resolution including
readout electronics threshold effects are quantified. Finally, the relation
between the theoretical and reconstructed low-energy electron energy spectrum
is derived and the energy resolution is characterized. The low-energy electron
selection presented here accounts for about 75% of the total electron deposited
energy. After the addition of lost energy using a Monte Carlo simulation, the
energy resolution improves from about 40% to 25% at 50~MeV. These results are
used to validate the expected capabilities of the DUNE far detector to
reconstruct low-energy electrons. |
doi_str_mv | 10.48550/arxiv.2211.01166 |
format | Article |
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Underground Neutrino Experiment (DUNE) neutrino oscillation program, as well as
searches for physics beyond the standard model, supernova neutrino detection,
and solar neutrino measurements. This article describes the selection and
reconstruction of low-energy (Michel) electrons in the ProtoDUNE-SP detector.
ProtoDUNE-SP is one of the prototypes for the DUNE far detector, built and
operated at CERN as a charged particle test beam experiment. A sample of
low-energy electrons produced by the decay of cosmic muons is selected with a
purity of 95%. This sample is used to calibrate the low-energy electron energy
scale with two techniques. An electron energy calibration based on a cosmic ray
muon sample uses calibration constants derived from measured and simulated
cosmic ray muon events. Another calibration technique makes use of the
theoretically well-understood Michel electron energy spectrum to convert
reconstructed charge to electron energy. In addition, the effects of detector
response to low-energy electron energy scale and its resolution including
readout electronics threshold effects are quantified. Finally, the relation
between the theoretical and reconstructed low-energy electron energy spectrum
is derived and the energy resolution is characterized. The low-energy electron
selection presented here accounts for about 75% of the total electron deposited
energy. After the addition of lost energy using a Monte Carlo simulation, the
energy resolution improves from about 40% to 25% at 50~MeV. These results are
used to validate the expected capabilities of the DUNE far detector to
reconstruct low-energy electrons.</description><identifier>DOI: 10.48550/arxiv.2211.01166</identifier><language>eng</language><subject>Physics - High Energy Physics - Experiment ; Physics - Instrumentation and Detectors</subject><creationdate>2022-11</creationdate><rights>http://creativecommons.org/licenses/by/4.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,781,886</link.rule.ids><linktorsrc>$$Uhttps://arxiv.org/abs/2211.01166$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.48550/arXiv.2211.01166$$DView paper in arXiv$$Hfree_for_read</backlink></links><search><creatorcontrib>Acciarri, R</creatorcontrib><creatorcontrib>Adamowski, M</creatorcontrib><creatorcontrib>Aduszkiewicz, A</creatorcontrib><creatorcontrib>Aimard, B</creatorcontrib><creatorcontrib>Akbar, F</creatorcontrib><creatorcontrib>Alrashed, M</creatorcontrib><creatorcontrib>Asquith, L</creatorcontrib><creatorcontrib>Aushev, V</creatorcontrib><creatorcontrib>Back, J. J</creatorcontrib><creatorcontrib>Barros, A</creatorcontrib><creatorcontrib>Bevan, A</creatorcontrib><creatorcontrib>Boran, F</creatorcontrib><creatorcontrib>Boyden, D</creatorcontrib><creatorcontrib>Brice, S. J</creatorcontrib><creatorcontrib>Bross, A</creatorcontrib><creatorcontrib>Calabrese, R</creatorcontrib><creatorcontrib>Castillo, A</creatorcontrib><creatorcontrib>Chatterjee, A</creatorcontrib><creatorcontrib>Cicero, V</creatorcontrib><creatorcontrib>Collot, J</creatorcontrib><creatorcontrib>Cremaldi, L</creatorcontrib><creatorcontrib>da Motta, H</creatorcontrib><creatorcontrib>De, S</creatorcontrib><creatorcontrib>De Almeida, P</creatorcontrib><creatorcontrib>Decowski, M. P</creatorcontrib><creatorcontrib>De Souza, G</creatorcontrib><creatorcontrib>Ezeribe, A. C</creatorcontrib><creatorcontrib>Fajt, L</creatorcontrib><creatorcontrib>Filip, P</creatorcontrib><creatorcontrib>Filkins, A</creatorcontrib><creatorcontrib>Fiorillo, G</creatorcontrib><creatorcontrib>Freestone, J</creatorcontrib><creatorcontrib>Gibin, D</creatorcontrib><creatorcontrib>Granados, E</creatorcontrib><creatorcontrib>Granger, P</creatorcontrib><creatorcontrib>Grenard, J</creatorcontrib><creatorcontrib>Hamacher-Baumann, P</creatorcontrib><creatorcontrib>Hamilton, P</creatorcontrib><creatorcontrib>Morquecho, M. A. Hernandez</creatorcontrib><creatorcontrib>Howell, R</creatorcontrib><creatorcontrib>Hristova, I</creatorcontrib><creatorcontrib>Huang, J</creatorcontrib><creatorcontrib>Hulcher, Z</creatorcontrib><creatorcontrib>Illingworth, R</creatorcontrib><creatorcontrib>Oliveira, M. Ismerio</creatorcontrib><creatorcontrib>Jediny, F</creatorcontrib><creatorcontrib>Jiang, L</creatorcontrib><creatorcontrib>Kearns, E</creatorcontrib><creatorcontrib>King, B</creatorcontrib><creatorcontrib>Kose, U</creatorcontrib><creatorcontrib>Kurita, N</creatorcontrib><creatorcontrib>Marinho, F</creatorcontrib><creatorcontrib>Martynenko, S</creatorcontrib><creatorcontrib>Matichard, F</creatorcontrib><creatorcontrib>Mendez, P</creatorcontrib><creatorcontrib>Meng, G</creatorcontrib><creatorcontrib>Meyer, H</creatorcontrib><creatorcontrib>Mohanta, R</creatorcontrib><creatorcontrib>Molina, J</creatorcontrib><creatorcontrib>Mote, M</creatorcontrib><creatorcontrib>Papaleo, R</creatorcontrib><creatorcontrib>Papanestis, A</creatorcontrib><creatorcontrib>Parsa, S</creatorcontrib><creatorcontrib>Patton, S. J</creatorcontrib><creatorcontrib>Pershey, D</creatorcontrib><creatorcontrib>Pickering, L</creatorcontrib><creatorcontrib>Radeka, V</creatorcontrib><creatorcontrib>Rameika, R</creatorcontrib><creatorcontrib>Rigamonti, A</creatorcontrib><creatorcontrib>Rigaut, Y</creatorcontrib><creatorcontrib>Rivera, D</creatorcontrib><creatorcontrib>Rossi, M</creatorcontrib><creatorcontrib>Rout, J</creatorcontrib><creatorcontrib>Sala, P</creatorcontrib><creatorcontrib>Sharma, R</creatorcontrib><creatorcontrib>Shrock, R</creatorcontrib><creatorcontrib>Skarpaas, K</creatorcontrib><creatorcontrib>Soleti, S. R</creatorcontrib><creatorcontrib>Surdo, A</creatorcontrib><creatorcontrib>Talukdar, N</creatorcontrib><creatorcontrib>Tomassetti, L</creatorcontrib><creatorcontrib>Touramanis, C</creatorcontrib><creatorcontrib>Trilov, S</creatorcontrib><creatorcontrib>Tsang, K. V</creatorcontrib><creatorcontrib>Utaegbulam, H</creatorcontrib><creatorcontrib>Valentim, R</creatorcontrib><creatorcontrib>Oliva, D. Vargas</creatorcontrib><creatorcontrib>Vaughan, N</creatorcontrib><creatorcontrib>Verzocchi, M</creatorcontrib><creatorcontrib>Vicenzi, M</creatorcontrib><creatorcontrib>Vrba, T</creatorcontrib><creatorcontrib>Wang, H</creatorcontrib><creatorcontrib>Wetstein, M</creatorcontrib><creatorcontrib>Williams, Z</creatorcontrib><creatorcontrib>Worcester, M</creatorcontrib><creatorcontrib>Wu, S</creatorcontrib><creatorcontrib>Yandel, E</creatorcontrib><creatorcontrib>Yankelevich, A</creatorcontrib><creatorcontrib>Yuan, W</creatorcontrib><creatorcontrib>Zuklin, J</creatorcontrib><title>Identification and reconstruction of low-energy electrons in the ProtoDUNE-SP detector</title><description>Phys. Rev. D 107, 092012 (2023) Measurements of electrons from $\nu_e$ interactions are crucial for the Deep
Underground Neutrino Experiment (DUNE) neutrino oscillation program, as well as
searches for physics beyond the standard model, supernova neutrino detection,
and solar neutrino measurements. This article describes the selection and
reconstruction of low-energy (Michel) electrons in the ProtoDUNE-SP detector.
ProtoDUNE-SP is one of the prototypes for the DUNE far detector, built and
operated at CERN as a charged particle test beam experiment. A sample of
low-energy electrons produced by the decay of cosmic muons is selected with a
purity of 95%. This sample is used to calibrate the low-energy electron energy
scale with two techniques. An electron energy calibration based on a cosmic ray
muon sample uses calibration constants derived from measured and simulated
cosmic ray muon events. Another calibration technique makes use of the
theoretically well-understood Michel electron energy spectrum to convert
reconstructed charge to electron energy. In addition, the effects of detector
response to low-energy electron energy scale and its resolution including
readout electronics threshold effects are quantified. Finally, the relation
between the theoretical and reconstructed low-energy electron energy spectrum
is derived and the energy resolution is characterized. The low-energy electron
selection presented here accounts for about 75% of the total electron deposited
energy. After the addition of lost energy using a Monte Carlo simulation, the
energy resolution improves from about 40% to 25% at 50~MeV. These results are
used to validate the expected capabilities of the DUNE far detector to
reconstruct low-energy electrons.</description><subject>Physics - High Energy Physics - Experiment</subject><subject>Physics - Instrumentation and Detectors</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2022</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNotj81KAzEUhbNxIdUHcGVeIGNuMpOZWUqtWihasLod0uRGA2Mit_Gnb287CgcOnA8OfIxdgKzqrmnklaWf-FUpBVBJAGNO2cvSYyoxRGdLzInb5Dmhy2lX6NNNUw58zN8CE9LrnuOIrtCB85h4eUO-plzyzfPDQjytucdywJnO2Emw4w7P_3vGNreLzfxerB7vlvPrlbCmNcKD7L0KaBTqLmw7bMFtO6WcqdUx3mtQsg2u71EbByjRSV03XloMTQA9Y5d_t5PY8EHx3dJ-OAoOk6D-BaN6TCA</recordid><startdate>20221102</startdate><enddate>20221102</enddate><creator>Acciarri, R</creator><creator>Adamowski, M</creator><creator>Aduszkiewicz, A</creator><creator>Aimard, B</creator><creator>Akbar, F</creator><creator>Alrashed, M</creator><creator>Asquith, L</creator><creator>Aushev, V</creator><creator>Back, J. J</creator><creator>Barros, A</creator><creator>Bevan, A</creator><creator>Boran, F</creator><creator>Boyden, D</creator><creator>Brice, S. J</creator><creator>Bross, A</creator><creator>Calabrese, R</creator><creator>Castillo, A</creator><creator>Chatterjee, A</creator><creator>Cicero, V</creator><creator>Collot, J</creator><creator>Cremaldi, L</creator><creator>da Motta, H</creator><creator>De, S</creator><creator>De Almeida, P</creator><creator>Decowski, M. P</creator><creator>De Souza, G</creator><creator>Ezeribe, A. C</creator><creator>Fajt, L</creator><creator>Filip, P</creator><creator>Filkins, A</creator><creator>Fiorillo, G</creator><creator>Freestone, J</creator><creator>Gibin, D</creator><creator>Granados, E</creator><creator>Granger, P</creator><creator>Grenard, J</creator><creator>Hamacher-Baumann, P</creator><creator>Hamilton, P</creator><creator>Morquecho, M. A. 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C ; Fajt, L ; Filip, P ; Filkins, A ; Fiorillo, G ; Freestone, J ; Gibin, D ; Granados, E ; Granger, P ; Grenard, J ; Hamacher-Baumann, P ; Hamilton, P ; Morquecho, M. A. Hernandez ; Howell, R ; Hristova, I ; Huang, J ; Hulcher, Z ; Illingworth, R ; Oliveira, M. Ismerio ; Jediny, F ; Jiang, L ; Kearns, E ; King, B ; Kose, U ; Kurita, N ; Marinho, F ; Martynenko, S ; Matichard, F ; Mendez, P ; Meng, G ; Meyer, H ; Mohanta, R ; Molina, J ; Mote, M ; Papaleo, R ; Papanestis, A ; Parsa, S ; Patton, S. J ; Pershey, D ; Pickering, L ; Radeka, V ; Rameika, R ; Rigamonti, A ; Rigaut, Y ; Rivera, D ; Rossi, M ; Rout, J ; Sala, P ; Sharma, R ; Shrock, R ; Skarpaas, K ; Soleti, S. R ; Surdo, A ; Talukdar, N ; Tomassetti, L ; Touramanis, C ; Trilov, S ; Tsang, K. V ; Utaegbulam, H ; Valentim, R ; Oliva, D. 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Ismerio</creatorcontrib><creatorcontrib>Jediny, F</creatorcontrib><creatorcontrib>Jiang, L</creatorcontrib><creatorcontrib>Kearns, E</creatorcontrib><creatorcontrib>King, B</creatorcontrib><creatorcontrib>Kose, U</creatorcontrib><creatorcontrib>Kurita, N</creatorcontrib><creatorcontrib>Marinho, F</creatorcontrib><creatorcontrib>Martynenko, S</creatorcontrib><creatorcontrib>Matichard, F</creatorcontrib><creatorcontrib>Mendez, P</creatorcontrib><creatorcontrib>Meng, G</creatorcontrib><creatorcontrib>Meyer, H</creatorcontrib><creatorcontrib>Mohanta, R</creatorcontrib><creatorcontrib>Molina, J</creatorcontrib><creatorcontrib>Mote, M</creatorcontrib><creatorcontrib>Papaleo, R</creatorcontrib><creatorcontrib>Papanestis, A</creatorcontrib><creatorcontrib>Parsa, S</creatorcontrib><creatorcontrib>Patton, S. J</creatorcontrib><creatorcontrib>Pershey, D</creatorcontrib><creatorcontrib>Pickering, L</creatorcontrib><creatorcontrib>Radeka, V</creatorcontrib><creatorcontrib>Rameika, R</creatorcontrib><creatorcontrib>Rigamonti, A</creatorcontrib><creatorcontrib>Rigaut, Y</creatorcontrib><creatorcontrib>Rivera, D</creatorcontrib><creatorcontrib>Rossi, M</creatorcontrib><creatorcontrib>Rout, J</creatorcontrib><creatorcontrib>Sala, P</creatorcontrib><creatorcontrib>Sharma, R</creatorcontrib><creatorcontrib>Shrock, R</creatorcontrib><creatorcontrib>Skarpaas, K</creatorcontrib><creatorcontrib>Soleti, S. R</creatorcontrib><creatorcontrib>Surdo, A</creatorcontrib><creatorcontrib>Talukdar, N</creatorcontrib><creatorcontrib>Tomassetti, L</creatorcontrib><creatorcontrib>Touramanis, C</creatorcontrib><creatorcontrib>Trilov, S</creatorcontrib><creatorcontrib>Tsang, K. V</creatorcontrib><creatorcontrib>Utaegbulam, H</creatorcontrib><creatorcontrib>Valentim, R</creatorcontrib><creatorcontrib>Oliva, D. Vargas</creatorcontrib><creatorcontrib>Vaughan, N</creatorcontrib><creatorcontrib>Verzocchi, M</creatorcontrib><creatorcontrib>Vicenzi, M</creatorcontrib><creatorcontrib>Vrba, T</creatorcontrib><creatorcontrib>Wang, H</creatorcontrib><creatorcontrib>Wetstein, M</creatorcontrib><creatorcontrib>Williams, Z</creatorcontrib><creatorcontrib>Worcester, M</creatorcontrib><creatorcontrib>Wu, S</creatorcontrib><creatorcontrib>Yandel, E</creatorcontrib><creatorcontrib>Yankelevich, A</creatorcontrib><creatorcontrib>Yuan, W</creatorcontrib><creatorcontrib>Zuklin, J</creatorcontrib><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Acciarri, R</au><au>Adamowski, M</au><au>Aduszkiewicz, A</au><au>Aimard, B</au><au>Akbar, F</au><au>Alrashed, M</au><au>Asquith, L</au><au>Aushev, V</au><au>Back, J. J</au><au>Barros, A</au><au>Bevan, A</au><au>Boran, F</au><au>Boyden, D</au><au>Brice, S. J</au><au>Bross, A</au><au>Calabrese, R</au><au>Castillo, A</au><au>Chatterjee, A</au><au>Cicero, V</au><au>Collot, J</au><au>Cremaldi, L</au><au>da Motta, H</au><au>De, S</au><au>De Almeida, P</au><au>Decowski, M. P</au><au>De Souza, G</au><au>Ezeribe, A. C</au><au>Fajt, L</au><au>Filip, P</au><au>Filkins, A</au><au>Fiorillo, G</au><au>Freestone, J</au><au>Gibin, D</au><au>Granados, E</au><au>Granger, P</au><au>Grenard, J</au><au>Hamacher-Baumann, P</au><au>Hamilton, P</au><au>Morquecho, M. A. Hernandez</au><au>Howell, R</au><au>Hristova, I</au><au>Huang, J</au><au>Hulcher, Z</au><au>Illingworth, R</au><au>Oliveira, M. Ismerio</au><au>Jediny, F</au><au>Jiang, L</au><au>Kearns, E</au><au>King, B</au><au>Kose, U</au><au>Kurita, N</au><au>Marinho, F</au><au>Martynenko, S</au><au>Matichard, F</au><au>Mendez, P</au><au>Meng, G</au><au>Meyer, H</au><au>Mohanta, R</au><au>Molina, J</au><au>Mote, M</au><au>Papaleo, R</au><au>Papanestis, A</au><au>Parsa, S</au><au>Patton, S. J</au><au>Pershey, D</au><au>Pickering, L</au><au>Radeka, V</au><au>Rameika, R</au><au>Rigamonti, A</au><au>Rigaut, Y</au><au>Rivera, D</au><au>Rossi, M</au><au>Rout, J</au><au>Sala, P</au><au>Sharma, R</au><au>Shrock, R</au><au>Skarpaas, K</au><au>Soleti, S. R</au><au>Surdo, A</au><au>Talukdar, N</au><au>Tomassetti, L</au><au>Touramanis, C</au><au>Trilov, S</au><au>Tsang, K. V</au><au>Utaegbulam, H</au><au>Valentim, R</au><au>Oliva, D. Vargas</au><au>Vaughan, N</au><au>Verzocchi, M</au><au>Vicenzi, M</au><au>Vrba, T</au><au>Wang, H</au><au>Wetstein, M</au><au>Williams, Z</au><au>Worcester, M</au><au>Wu, S</au><au>Yandel, E</au><au>Yankelevich, A</au><au>Yuan, W</au><au>Zuklin, J</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Identification and reconstruction of low-energy electrons in the ProtoDUNE-SP detector</atitle><date>2022-11-02</date><risdate>2022</risdate><abstract>Phys. Rev. D 107, 092012 (2023) Measurements of electrons from $\nu_e$ interactions are crucial for the Deep
Underground Neutrino Experiment (DUNE) neutrino oscillation program, as well as
searches for physics beyond the standard model, supernova neutrino detection,
and solar neutrino measurements. This article describes the selection and
reconstruction of low-energy (Michel) electrons in the ProtoDUNE-SP detector.
ProtoDUNE-SP is one of the prototypes for the DUNE far detector, built and
operated at CERN as a charged particle test beam experiment. A sample of
low-energy electrons produced by the decay of cosmic muons is selected with a
purity of 95%. This sample is used to calibrate the low-energy electron energy
scale with two techniques. An electron energy calibration based on a cosmic ray
muon sample uses calibration constants derived from measured and simulated
cosmic ray muon events. Another calibration technique makes use of the
theoretically well-understood Michel electron energy spectrum to convert
reconstructed charge to electron energy. In addition, the effects of detector
response to low-energy electron energy scale and its resolution including
readout electronics threshold effects are quantified. Finally, the relation
between the theoretical and reconstructed low-energy electron energy spectrum
is derived and the energy resolution is characterized. The low-energy electron
selection presented here accounts for about 75% of the total electron deposited
energy. After the addition of lost energy using a Monte Carlo simulation, the
energy resolution improves from about 40% to 25% at 50~MeV. These results are
used to validate the expected capabilities of the DUNE far detector to
reconstruct low-energy electrons.</abstract><doi>10.48550/arxiv.2211.01166</doi><oa>free_for_read</oa></addata></record> |
fulltext | fulltext_linktorsrc |
identifier | DOI: 10.48550/arxiv.2211.01166 |
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language | eng |
recordid | cdi_arxiv_primary_2211_01166 |
source | arXiv.org |
subjects | Physics - High Energy Physics - Experiment Physics - Instrumentation and Detectors |
title | Identification and reconstruction of low-energy electrons in the ProtoDUNE-SP detector |
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