Attenuation of acoustic waves in glacial ice and salt domes

Two classes of natural solid media (glacial ice and salt domes) are under consideration as media in which to deploy instruments for detection of neutrinos with energy >1e18 eV. Though insensitive to 1e11 to 1e16 eV neutrinos for which observatories (e.g., AMANDA and IceCube) that utilize optical...

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Main Author: Price, P. B.
Format: Text
Language:unknown
Published: arXiv 2005
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Online Access:https://dx.doi.org/10.48550/arxiv.astro-ph/0506648
https://arxiv.org/abs/astro-ph/0506648
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author Price, P. B.
author_facet Price, P. B.
author_sort Price, P. B.
collection DataCite
description Two classes of natural solid media (glacial ice and salt domes) are under consideration as media in which to deploy instruments for detection of neutrinos with energy >1e18 eV. Though insensitive to 1e11 to 1e16 eV neutrinos for which observatories (e.g., AMANDA and IceCube) that utilize optical Cherenkov radiation detectors are designed, radio and acoustic methods are suited for searches for the very low fluxes of neutrinos with energies >1017 eV. This is because, due to the very long attenuation lengths of radio and acoustic waves in ice and salt, detection modules can be spaced very far apart. In this paper, I calculate the absorption and scattering coefficients as a function of frequency and grain size for acoustic waves in glacial ice and salt domes and show that experimental measurements on laboratory samples and in glacial ice and salt domes are consistent with theory. For South Pole ice with grain size 0.2 cm at -51 degrees C, scattering lengths are calculated to be 2000 km and 25 km at 10 kHz and 30 kHz, respectively, and the absorption length is calculated to be 9 km at frequencies above 100 Hz. For NaCl (rock salt) with grain size 0.75 cm, scattering lengths are calculated to be 120 km and 1.4 km at 10 kHz and 30 kHz, and absorption lengths are calculated to be 30,000 km and 3300 km at 10 kHz and 30 kHz. Existing measurements are consistent with theory. For ice, absorption is the limiting factor; for salt, scattering is the limiting factor. : 16 pages, 7 figures, submitted to Journal of Geophysical Research - Solid Earth
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op_doi https://doi.org/10.48550/arxiv.astro-ph/0506648
https://doi.org/10.1029/2005jb003903
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op_rights Assumed arXiv.org perpetual, non-exclusive license to distribute this article for submissions made before January 2004
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spelling ftdatacite:10.48550/arxiv.astro-ph/0506648 2025-01-17T00:52:46+00:00 Attenuation of acoustic waves in glacial ice and salt domes Price, P. B. 2005 https://dx.doi.org/10.48550/arxiv.astro-ph/0506648 https://arxiv.org/abs/astro-ph/0506648 unknown arXiv https://dx.doi.org/10.1029/2005jb003903 Assumed arXiv.org perpetual, non-exclusive license to distribute this article for submissions made before January 2004 http://arxiv.org/licenses/assumed-1991-2003/ Astrophysics astro-ph FOS Physical sciences article-journal Article ScholarlyArticle Text 2005 ftdatacite https://doi.org/10.48550/arxiv.astro-ph/0506648 https://doi.org/10.1029/2005jb003903 2022-04-01T17:40:14Z Two classes of natural solid media (glacial ice and salt domes) are under consideration as media in which to deploy instruments for detection of neutrinos with energy >1e18 eV. Though insensitive to 1e11 to 1e16 eV neutrinos for which observatories (e.g., AMANDA and IceCube) that utilize optical Cherenkov radiation detectors are designed, radio and acoustic methods are suited for searches for the very low fluxes of neutrinos with energies >1017 eV. This is because, due to the very long attenuation lengths of radio and acoustic waves in ice and salt, detection modules can be spaced very far apart. In this paper, I calculate the absorption and scattering coefficients as a function of frequency and grain size for acoustic waves in glacial ice and salt domes and show that experimental measurements on laboratory samples and in glacial ice and salt domes are consistent with theory. For South Pole ice with grain size 0.2 cm at -51 degrees C, scattering lengths are calculated to be 2000 km and 25 km at 10 kHz and 30 kHz, respectively, and the absorption length is calculated to be 9 km at frequencies above 100 Hz. For NaCl (rock salt) with grain size 0.75 cm, scattering lengths are calculated to be 120 km and 1.4 km at 10 kHz and 30 kHz, and absorption lengths are calculated to be 30,000 km and 3300 km at 10 kHz and 30 kHz. Existing measurements are consistent with theory. For ice, absorption is the limiting factor; for salt, scattering is the limiting factor. : 16 pages, 7 figures, submitted to Journal of Geophysical Research - Solid Earth Text South pole DataCite South Pole
spellingShingle Astrophysics astro-ph
FOS Physical sciences
Price, P. B.
Attenuation of acoustic waves in glacial ice and salt domes
title Attenuation of acoustic waves in glacial ice and salt domes
title_full Attenuation of acoustic waves in glacial ice and salt domes
title_fullStr Attenuation of acoustic waves in glacial ice and salt domes
title_full_unstemmed Attenuation of acoustic waves in glacial ice and salt domes
title_short Attenuation of acoustic waves in glacial ice and salt domes
title_sort attenuation of acoustic waves in glacial ice and salt domes
topic Astrophysics astro-ph
FOS Physical sciences
topic_facet Astrophysics astro-ph
FOS Physical sciences
url https://dx.doi.org/10.48550/arxiv.astro-ph/0506648
https://arxiv.org/abs/astro-ph/0506648