Cosmogenic Neutrinos Challenge the Cosmic Ray Proton Dip Model

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Cosmogenic Neutrinos Challenge the Cosmic Ray Proton Dip Model. / Heinze, Jonas; Boncioli, Denise; Bustamante, Mauricio; Winter, Walter.

I: The Astrophysical Journal, Bind 825, Nr. 2, 122, 11.07.2016.

Publikation: Bidrag til tidsskrift › Tidsskriftartikel › Forskning › fagfællebedømt

Harvard

Heinze, J, Boncioli, D, Bustamante, M & Winter, W 2016, 'Cosmogenic Neutrinos Challenge the Cosmic Ray Proton Dip Model', The Astrophysical Journal, bind 825, nr. 2, 122. https://doi.org/10.3847/0004-637X/825/2/122

APA

Heinze, J., Boncioli, D., Bustamante, M., & Winter, W. (2016). Cosmogenic Neutrinos Challenge the Cosmic Ray Proton Dip Model. The Astrophysical Journal, 825(2), [122]. https://doi.org/10.3847/0004-637X/825/2/122

Vancouver

Heinze J, Boncioli D, Bustamante M, Winter W. Cosmogenic Neutrinos Challenge the Cosmic Ray Proton Dip Model. The Astrophysical Journal. 2016 jul. 11;825(2). 122. https://doi.org/10.3847/0004-637X/825/2/122

Author

Heinze, Jonas ; Boncioli, Denise ; Bustamante, Mauricio ; Winter, Walter. / Cosmogenic Neutrinos Challenge the Cosmic Ray Proton Dip Model. I: The Astrophysical Journal. 2016 ; Bind 825, Nr. 2.

Bibtex

@article{32267012c29d4e918f98f8d90f901feb,
title = "Cosmogenic Neutrinos Challenge the Cosmic Ray Proton Dip Model",
abstract = "The origin and composition of ultra-high-energy cosmic rays (UHECRs) remain a mystery. The proton dip model describes their spectral shape in the energy range above $10^9$ GeV by pair production and photohadronic interactions with the cosmic microwave background. The photohadronic interactions also produce cosmogenic neutrinos peaking around $10^9$ GeV. We test whether this model is still viable in light of recent UHECR spectrum measurements from the Telescope Array experiment, and upper limits on the cosmogenic neutrino flux from IceCube. While two-parameter fits have been already presented, we perform a full scan of the three main physical model parameters: source redshift evolution, injected proton maximal energy, and spectral index. We find qualitatively different conclusions compared to earlier two-parameter fits in the literature: a mild preference for a maximal energy cutoff at the sources instead of the Greisen--Zatsepin--Kuzmin (GZK) cutoff, hard injection spectra, and strong source evolution. The predicted cosmogenic neutrino flux exceeds the IceCube limit for any parameter combination. As a result, the proton dip model is challenged at more than 95\% C.L. This is strong evidence against this model independent of mass composition measurements.",
keywords = "astro-ph.HE",
author = "Jonas Heinze and Denise Boncioli and Mauricio Bustamante and Walter Winter",
note = "published in Apj; 15 pages, 12 figures",
year = "2016",
month = jul,
day = "11",
doi = "10.3847/0004-637X/825/2/122",
language = "English",
volume = "825",
journal = "Astrophysical Journal",
issn = "0004-637X",
publisher = "Institute of Physics Publishing, Inc",
number = "2",

}

RIS

TY - JOUR

T1 - Cosmogenic Neutrinos Challenge the Cosmic Ray Proton Dip Model

AU - Heinze, Jonas

AU - Boncioli, Denise

AU - Bustamante, Mauricio

AU - Winter, Walter

N1 - published in Apj; 15 pages, 12 figures

PY - 2016/7/11

Y1 - 2016/7/11

N2 - The origin and composition of ultra-high-energy cosmic rays (UHECRs) remain a mystery. The proton dip model describes their spectral shape in the energy range above $10^9$ GeV by pair production and photohadronic interactions with the cosmic microwave background. The photohadronic interactions also produce cosmogenic neutrinos peaking around $10^9$ GeV. We test whether this model is still viable in light of recent UHECR spectrum measurements from the Telescope Array experiment, and upper limits on the cosmogenic neutrino flux from IceCube. While two-parameter fits have been already presented, we perform a full scan of the three main physical model parameters: source redshift evolution, injected proton maximal energy, and spectral index. We find qualitatively different conclusions compared to earlier two-parameter fits in the literature: a mild preference for a maximal energy cutoff at the sources instead of the Greisen--Zatsepin--Kuzmin (GZK) cutoff, hard injection spectra, and strong source evolution. The predicted cosmogenic neutrino flux exceeds the IceCube limit for any parameter combination. As a result, the proton dip model is challenged at more than 95\% C.L. This is strong evidence against this model independent of mass composition measurements.

AB - The origin and composition of ultra-high-energy cosmic rays (UHECRs) remain a mystery. The proton dip model describes their spectral shape in the energy range above $10^9$ GeV by pair production and photohadronic interactions with the cosmic microwave background. The photohadronic interactions also produce cosmogenic neutrinos peaking around $10^9$ GeV. We test whether this model is still viable in light of recent UHECR spectrum measurements from the Telescope Array experiment, and upper limits on the cosmogenic neutrino flux from IceCube. While two-parameter fits have been already presented, we perform a full scan of the three main physical model parameters: source redshift evolution, injected proton maximal energy, and spectral index. We find qualitatively different conclusions compared to earlier two-parameter fits in the literature: a mild preference for a maximal energy cutoff at the sources instead of the Greisen--Zatsepin--Kuzmin (GZK) cutoff, hard injection spectra, and strong source evolution. The predicted cosmogenic neutrino flux exceeds the IceCube limit for any parameter combination. As a result, the proton dip model is challenged at more than 95\% C.L. This is strong evidence against this model independent of mass composition measurements.

KW - astro-ph.HE

U2 - 10.3847/0004-637X/825/2/122

DO - 10.3847/0004-637X/825/2/122

M3 - Journal article

VL - 825

JO - Astrophysical Journal

JF - Astrophysical Journal

SN - 0004-637X

IS - 2

M1 - 122

ER -

ID: 184745777