Exploiting stellar explosion induced by the QCD phase transition in large-scale neutrino detectors

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Exploiting stellar explosion induced by the QCD phase transition in large-scale neutrino detectors. / Pitik, Tetyana; Heimsoth, Daniel J.; Suliga, Anna M.; Balantekin, A. Baha.

In: Physical Review D, Vol. 106, No. 10, 103007, 04.11.2022.

Research output: Contribution to journalJournal articleResearchpeer-review

Harvard

Pitik, T, Heimsoth, DJ, Suliga, AM & Balantekin, AB 2022, 'Exploiting stellar explosion induced by the QCD phase transition in large-scale neutrino detectors', Physical Review D, vol. 106, no. 10, 103007. https://doi.org/10.1103/PhysRevD.106.103007

APA

Pitik, T., Heimsoth, D. J., Suliga, A. M., & Balantekin, A. B. (2022). Exploiting stellar explosion induced by the QCD phase transition in large-scale neutrino detectors. Physical Review D, 106(10), [103007]. https://doi.org/10.1103/PhysRevD.106.103007

Vancouver

Pitik T, Heimsoth DJ, Suliga AM, Balantekin AB. Exploiting stellar explosion induced by the QCD phase transition in large-scale neutrino detectors. Physical Review D. 2022 Nov 4;106(10). 103007. https://doi.org/10.1103/PhysRevD.106.103007

Author

Pitik, Tetyana ; Heimsoth, Daniel J. ; Suliga, Anna M. ; Balantekin, A. Baha. / Exploiting stellar explosion induced by the QCD phase transition in large-scale neutrino detectors. In: Physical Review D. 2022 ; Vol. 106, No. 10.

Bibtex

@article{982d06be3e414704bf2a185794a7da99,
title = "Exploiting stellar explosion induced by the QCD phase transition in large-scale neutrino detectors",
abstract = "The centers of the core-collapse supernovae are one of the densest environments in the Universe. Under such conditions, it is conceivable that a first-order phase transition from ordinary nuclear matter to the quark-gluon plasma occurs. This transition releases a large amount of latent heat that can drive a supernova explosion and may imprint a sharp signature in the neutrino signal. We show how this snap feature, if observed at large-scale neutrino detectors, can set competitive limits on the neutrino masses and assist the localization of the supernova via triangulation. The 95% C.L. limit on the neutrino mass can reach 0.16 eV in Ice-Cube, 0.22 eV in Hyper-Kamiokande, and 0.58 eV in DUNE, for a supernova at a distance of 10 kpc. For the same distance and in the most optimistic neutrino conversion case, the triangulation method can constrain the 1 sigma angular uncertainty of the supernova localization within similar to 0.3 degrees-9.0 degrees in the considered pairs of the detectors, leading to an improvement up to an order of magnitude with respect to the often considered in the literature rise time of the neutronization burst.",
keywords = "LARGE BINOCULAR TELESCOPE, GAMMA-RAY BURST, CORE-COLLAPSE, SUPERNOVA EXPLOSION, FAILED SUPERNOVAE, SEARCH, CONSTRAINTS, EQUATION, STARS, OSCILLATIONS",
author = "Tetyana Pitik and Heimsoth, {Daniel J.} and Suliga, {Anna M.} and Balantekin, {A. Baha}",
year = "2022",
month = nov,
day = "4",
doi = "10.1103/PhysRevD.106.103007",
language = "English",
volume = "106",
journal = "Physical Review D",
issn = "2470-0010",
publisher = "American Physical Society",
number = "10",

}

RIS

TY - JOUR

T1 - Exploiting stellar explosion induced by the QCD phase transition in large-scale neutrino detectors

AU - Pitik, Tetyana

AU - Heimsoth, Daniel J.

AU - Suliga, Anna M.

AU - Balantekin, A. Baha

PY - 2022/11/4

Y1 - 2022/11/4

N2 - The centers of the core-collapse supernovae are one of the densest environments in the Universe. Under such conditions, it is conceivable that a first-order phase transition from ordinary nuclear matter to the quark-gluon plasma occurs. This transition releases a large amount of latent heat that can drive a supernova explosion and may imprint a sharp signature in the neutrino signal. We show how this snap feature, if observed at large-scale neutrino detectors, can set competitive limits on the neutrino masses and assist the localization of the supernova via triangulation. The 95% C.L. limit on the neutrino mass can reach 0.16 eV in Ice-Cube, 0.22 eV in Hyper-Kamiokande, and 0.58 eV in DUNE, for a supernova at a distance of 10 kpc. For the same distance and in the most optimistic neutrino conversion case, the triangulation method can constrain the 1 sigma angular uncertainty of the supernova localization within similar to 0.3 degrees-9.0 degrees in the considered pairs of the detectors, leading to an improvement up to an order of magnitude with respect to the often considered in the literature rise time of the neutronization burst.

AB - The centers of the core-collapse supernovae are one of the densest environments in the Universe. Under such conditions, it is conceivable that a first-order phase transition from ordinary nuclear matter to the quark-gluon plasma occurs. This transition releases a large amount of latent heat that can drive a supernova explosion and may imprint a sharp signature in the neutrino signal. We show how this snap feature, if observed at large-scale neutrino detectors, can set competitive limits on the neutrino masses and assist the localization of the supernova via triangulation. The 95% C.L. limit on the neutrino mass can reach 0.16 eV in Ice-Cube, 0.22 eV in Hyper-Kamiokande, and 0.58 eV in DUNE, for a supernova at a distance of 10 kpc. For the same distance and in the most optimistic neutrino conversion case, the triangulation method can constrain the 1 sigma angular uncertainty of the supernova localization within similar to 0.3 degrees-9.0 degrees in the considered pairs of the detectors, leading to an improvement up to an order of magnitude with respect to the often considered in the literature rise time of the neutronization burst.

KW - LARGE BINOCULAR TELESCOPE

KW - GAMMA-RAY BURST

KW - CORE-COLLAPSE

KW - SUPERNOVA EXPLOSION

KW - FAILED SUPERNOVAE

KW - SEARCH

KW - CONSTRAINTS

KW - EQUATION

KW - STARS

KW - OSCILLATIONS

U2 - 10.1103/PhysRevD.106.103007

DO - 10.1103/PhysRevD.106.103007

M3 - Journal article

VL - 106

JO - Physical Review D

JF - Physical Review D

SN - 2470-0010

IS - 10

M1 - 103007

ER -

ID: 327056801