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Spallation Backgrounds in Super-Kamiokande Are Made in Muon-Induced Showers
High Energy Physics - Phenomenology · Submitted 16 Mar 2015
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that almost all spallation decay isotopes are produced by muon-induced showers and that these showers are rare enough and energetic enough to be identifiable.
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The abstract, sentence by sentence
Crucial questions about solar and supernova neutrinos remain unanswered. Super-Kamiokande has the exposure needed for progress, but detector backgrounds are a limiting factor. A leading component is the beta decays of isotopes produced by cosmic-ray muons and their secondaries, which initiate nuclear spallation reactions. Cuts of events after and surrounding muon tracks reduce this spallation decay background by $\simeq 90\%$ (at a cost of $\simeq 20\%$ deadtime), but its rate at 6--18 MeV is still dominant. A better way to cut this background was suggested in a Super-Kamiokande paper [Bays {\it et al.}, Phys.~Rev.~D {\bf 85}, 052007 (2012)] on a search for the diffuse supernova neutrino background. They found that spallation decays above 16 MeV were preceded near the same location by a peak in the apparent Cherenkov light profile from the muon; a more aggressive cut was applied to a limited section of the muon track, leading to decreased background without increased deadtime. We put their empirical discovery on a firm theoretical foundation. We show that almost all spallation decay isotopes are produced by muon-induced showers and that these showers are rare enough and energetic enough to be identifiable. This is the first such demonstration for any detector. We detail how the physics of showers explains the peak in the muon Cherenkov light profile and other Super-K observations. Our results provide a physical basis for practical improvements in background rejection that will benefit multiple studies. For solar neutrinos, in particular, it should be possible to dramatically reduce backgrounds at energies as low as 6 MeV.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Crucial questions about solar and supernova neutrinos remain unanswered. | background 0.79 | 0.03 | 0.02 | asserted 1.00 |
| s1 | Super-Kamiokande has the exposure needed for progress, but detector backgrounds are a limiting factor. | background 0.93 | 0.08 | 0.02 | asserted 1.00 |
| s2 | A leading component is the beta decays of isotopes produced by cosmic-ray muons and their secondaries, which initiate nuclear spallation reactions. | background 1.00 | 0.07 | 0.08 | asserted 0.99 |
| s3 | Cuts of events after and surrounding muon tracks reduce this spallation decay background by $\simeq 90\%$ (at a cost of $\simeq 20\%$ deadtime), but its rate at 6--18 MeV is still dominant. | background 0.94 | 0.28 | 0.05 | asserted 1.00 |
| s4 | A better way to cut this background was suggested in a Super-Kamiokande paper [Bays {\it et al.}, Phys.~Rev.~D {\bf 85}, 052007 (2012)] on a search for the diffuse supernova neutrino background. | background 0.97 | 0.03 | 0.04 | asserted 0.93 |
| s5 | They found that spallation decays above 16 MeV were preceded near the same location by a peak in the apparent Cherenkov light profile from the muon; a more aggressive cut was applied to a limited section of the muon track, leading to decreased background without increased deadtime. | background 0.95 | 0.04 | 0.07 | asserted 1.00 |
| s6 | We put their empirical discovery on a firm theoretical foundation. | contribution 0.96 | 0.78 | 0.10 | asserted 0.98 |
| s7 | We show that almost all spallation decay isotopes are produced by muon-induced showers and that these showers are rare enough and energetic enough to be identifiable. | result 0.92 | 0.94 | 0.81 | asserted 1.00 |
| s8 | This is the first such demonstration for any detector. | contribution 0.66 | 0.80 | 0.14 | asserted 1.00 |
| s9 | We detail how the physics of showers explains the peak in the muon Cherenkov light profile and other Super-K observations. | contribution 0.78 | 0.85 | 0.09 | asserted 1.00 |
| s10 | Our results provide a physical basis for practical improvements in background rejection that will benefit multiple studies. | interpretation 0.93 | 0.64 | 0.19 | asserted 0.94 |
| s11 | For solar neutrinos, in particular, it should be possible to dramatically reduce backgrounds at energies as low as 6 MeV. | interpretation 0.90 | 0.58 | 0.17 | hedged possibility 1.00 |
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The paper
Original abstract
Crucial questions about solar and supernova neutrinos remain unanswered. Super-Kamiokande has the exposure needed for progress, but detector backgrounds are a limiting factor. A leading component is the beta decays of isotopes produced by cosmic-ray muons and their secondaries, which initiate nuclear spallation reactions. Cuts of events after and surrounding muon tracks reduce this spallation decay background by $\simeq 90\%$ (at a cost of $\simeq 20\%$ deadtime), but its rate at 6--18 MeV is still dominant. A better way to cut this background was suggested in a Super-Kamiokande paper [Bays {\it et al.}, Phys.~Rev.~D {\bf 85}, 052007 (2012)] on a search for the diffuse supernova neutrino background. They found that spallation decays above 16 MeV were preceded near the same location by a peak in the apparent Cherenkov light profile from the muon; a more aggressive cut was applied to a limited section of the muon track, leading to decreased background without increased deadtime. We put their empirical discovery on a firm theoretical foundation. We show that almost all spallation decay isotopes are produced by muon-induced showers and that these showers are rare enough and energetic enough to be identifiable. This is the first such demonstration for any detector. We detail how the physics of showers explains the peak in the muon Cherenkov light profile and other Super-K observations. Our results provide a physical basis for practical improvements in background rejection that will benefit multiple studies. For solar neutrinos, in particular, it should be possible to dramatically reduce backgrounds at energies as low as 6 MeV.
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References
How the literature uses it
19 arXiv papers cite this in 37 sentences
Papers citing it · 25 sentences without a confident label
Builds on it 1 paper
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Building on the work of Li and Beacom [ref] , our goals for this paper are to calculate the spallation backgrounds for DUNE in detail, understand their physical mechanisms, and use this understanding to develop cuts to reject backgrounds.
Developing the MeV potential of DUNE: Detailed considerations of muon-induced spallation and other backgrounds · Introduction · 0.99
Uses its data or values 1 paper
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In Super-Kamiokande, there are 3.6, 0.4, 0.04, and 0.003 daughter particles above 0.1, 1, 10, and 100 GeV per vertical muon (of track length 32.2 m) [ref] , showing that shower frequencies are small.
Developing the MeV potential of DUNE: Detailed considerations of muon-induced spallation and other backgrounds · Overview of spallation · 0.99
Compares with it 1 paper
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Compared to the results for Super-K in Ref. [ref] , there are slight differences that arise because of the difference in average muon energy.
New Spallation Background Rejection Techniques to Greatly Improve the Solar Neutrino Sensitivity of JUNO · Secondary particle showers · 0.99
Cites it as background 7 papers
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In this section, we review the physics of spallation isotope production by cosmic-ray muons, which is now understood, due to Refs. [ref] .
Developing the MeV potential of DUNE: Detailed considerations of muon-induced spallation and other backgrounds · Overview of spallation · 0.92
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The longitudinal and lateral profiles of showers have been studied extensively in Refs. [ref] .
New Spallation Background Rejection Techniques to Greatly Improve the Solar Neutrino Sensitivity of JUNO · Spatial distribution of isotopes · 0.89
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The main backgrounds are due to spallation from cosmic-ray muons [ref] , which produces radioactive isotopes, and neutral-current atmospheric neutrino interactions [ref] .
Detectable MeV Neutrino Signals from Neutron-Star Common-Envelope Systems · Introduction · 0.92
What it cites · 2 sentences without a confident label
Uses the method or tool of 1 paper
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We use the particle transport code FLUKA [ref] (version 2011.2b.6) for our calculations, which has been used extensively for simulating muon-induced backgrounds in underground detectors [ref] .
Study of Cosmogenic Neutron Backgrounds at LNGS · Introduction · 1.00
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