The Design and Performance of IceCube DeepCore

The IceCube neutrino observatory in operation at the South Pole, Antarctica, comprises three distinct components: a large buried array for ultrahigh energy neutrino detection, a surface air shower array, and a new buried component called DeepCore. DeepCore was designed to lower the IceCube neutrino...

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Main Author: The IceCube Collaboration
Format: Text
Language:unknown
Published: arXiv 2011
Subjects:
Online Access:https://dx.doi.org/10.48550/arxiv.1109.6096
https://arxiv.org/abs/1109.6096
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spelling ftdatacite:10.48550/arxiv.1109.6096 2023-05-15T13:54:43+02:00 The Design and Performance of IceCube DeepCore The IceCube Collaboration 2011 https://dx.doi.org/10.48550/arxiv.1109.6096 https://arxiv.org/abs/1109.6096 unknown arXiv https://dx.doi.org/10.1016/j.astropartphys.2012.01.004 arXiv.org perpetual, non-exclusive license http://arxiv.org/licenses/nonexclusive-distrib/1.0/ Instrumentation and Methods for Astrophysics astro-ph.IM Cosmology and Nongalactic Astrophysics astro-ph.CO High Energy Physics - Experiment hep-ex Instrumentation and Detectors physics.ins-det FOS Physical sciences article-journal Article ScholarlyArticle Text 2011 ftdatacite https://doi.org/10.48550/arxiv.1109.6096 https://doi.org/10.1016/j.astropartphys.2012.01.004 2022-04-01T14:00:42Z The IceCube neutrino observatory in operation at the South Pole, Antarctica, comprises three distinct components: a large buried array for ultrahigh energy neutrino detection, a surface air shower array, and a new buried component called DeepCore. DeepCore was designed to lower the IceCube neutrino energy threshold by over an order of magnitude, to energies as low as about 10 GeV. DeepCore is situated primarily 2100 m below the surface of the icecap at the South Pole, at the bottom center of the existing IceCube array, and began taking physics data in May 2010. Its location takes advantage of the exceptionally clear ice at those depths and allows it to use the surrounding IceCube detector as a highly efficient active veto against the principal background of downward-going muons produced in cosmic-ray air showers. DeepCore has a module density roughly five times higher than that of the standard IceCube array, and uses photomultiplier tubes with a new photocathode featuring a quantum efficiency about 35% higher than standard IceCube PMTs. Taken together, these features of DeepCore will increase IceCube's sensitivity to neutrinos from WIMP dark matter annihilations, atmospheric neutrino oscillations, galactic supernova neutrinos, and point sources of neutrinos in the northern and southern skies. In this paper we describe the design and initial performance of DeepCore. : 22 pages, 13 figures Text Antarc* Antarctica South pole South pole DataCite Metadata Store (German National Library of Science and Technology) South Pole
institution Open Polar
collection DataCite Metadata Store (German National Library of Science and Technology)
op_collection_id ftdatacite
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topic Instrumentation and Methods for Astrophysics astro-ph.IM
Cosmology and Nongalactic Astrophysics astro-ph.CO
High Energy Physics - Experiment hep-ex
Instrumentation and Detectors physics.ins-det
FOS Physical sciences
spellingShingle Instrumentation and Methods for Astrophysics astro-ph.IM
Cosmology and Nongalactic Astrophysics astro-ph.CO
High Energy Physics - Experiment hep-ex
Instrumentation and Detectors physics.ins-det
FOS Physical sciences
The IceCube Collaboration
The Design and Performance of IceCube DeepCore
topic_facet Instrumentation and Methods for Astrophysics astro-ph.IM
Cosmology and Nongalactic Astrophysics astro-ph.CO
High Energy Physics - Experiment hep-ex
Instrumentation and Detectors physics.ins-det
FOS Physical sciences
description The IceCube neutrino observatory in operation at the South Pole, Antarctica, comprises three distinct components: a large buried array for ultrahigh energy neutrino detection, a surface air shower array, and a new buried component called DeepCore. DeepCore was designed to lower the IceCube neutrino energy threshold by over an order of magnitude, to energies as low as about 10 GeV. DeepCore is situated primarily 2100 m below the surface of the icecap at the South Pole, at the bottom center of the existing IceCube array, and began taking physics data in May 2010. Its location takes advantage of the exceptionally clear ice at those depths and allows it to use the surrounding IceCube detector as a highly efficient active veto against the principal background of downward-going muons produced in cosmic-ray air showers. DeepCore has a module density roughly five times higher than that of the standard IceCube array, and uses photomultiplier tubes with a new photocathode featuring a quantum efficiency about 35% higher than standard IceCube PMTs. Taken together, these features of DeepCore will increase IceCube's sensitivity to neutrinos from WIMP dark matter annihilations, atmospheric neutrino oscillations, galactic supernova neutrinos, and point sources of neutrinos in the northern and southern skies. In this paper we describe the design and initial performance of DeepCore. : 22 pages, 13 figures
format Text
author The IceCube Collaboration
author_facet The IceCube Collaboration
author_sort The IceCube Collaboration
title The Design and Performance of IceCube DeepCore
title_short The Design and Performance of IceCube DeepCore
title_full The Design and Performance of IceCube DeepCore
title_fullStr The Design and Performance of IceCube DeepCore
title_full_unstemmed The Design and Performance of IceCube DeepCore
title_sort design and performance of icecube deepcore
publisher arXiv
publishDate 2011
url https://dx.doi.org/10.48550/arxiv.1109.6096
https://arxiv.org/abs/1109.6096
geographic South Pole
geographic_facet South Pole
genre Antarc*
Antarctica
South pole
South pole
genre_facet Antarc*
Antarctica
South pole
South pole
op_relation https://dx.doi.org/10.1016/j.astropartphys.2012.01.004
op_rights arXiv.org perpetual, non-exclusive license
http://arxiv.org/licenses/nonexclusive-distrib/1.0/
op_doi https://doi.org/10.48550/arxiv.1109.6096
https://doi.org/10.1016/j.astropartphys.2012.01.004
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