TY - JOUR
T1 - Detectability of collective neutrino oscillation signatures in the supernova explosion of a 8.8 M ⊙ star
AU - Sasaki, Hirokazu
AU - Takiwaki, Tomoya
AU - Kawagoe, Shio
AU - Horiuchi, Shunsaku
AU - Ishidoshiro, Koji
N1 - Funding Information:
This study was supported in part by the Grants-in-Aid for the Scientific Research of Japan Society for the Promotion of Science (JSPS, No. JP17H01130, No. JP17K14306, No. JP17K17655, No. JP19J13632, and No. JP18H01212), the Ministry of Education, Science and Culture of Japan (MEXT, No. JP15H01039, No. JP17H06357, No. JP17H06364, No. JP17H05206, No. JP26104001, No. JP26104007, and No. JP19H05803), and JICFuS as a priority issue to be tackled by using the Post ‘K’ Computer. This work is also supported by the NINS program for cross-disciplinary study (Grants No. 01321802 and No. 01311904) on Turbulence, Transport, and Heating Dynamics in Laboratory and Solar/Astrophysical Plasmas: “SoLaBo-X.” The work of S. H. is supported by the US Department of Energy Office of Science under Award No. DE-SC0020262, NSF Grant No. AST-1908960, and NSF Grant No. PHY-1914409.
Publisher Copyright:
© 2020 American Physical Society.
PY - 2020/3/15
Y1 - 2020/3/15
N2 - In order to investigate the impact of collective neutrino oscillations (CNOs) on the neutrino signal from a nearby supernova, we perform three-flavor neutrino oscillation simulations employing the multiangle effect. The background hydrodynamic model is based on the neutrino hydrodynamic simulation of a 8.8 M⊙ progenitor star. We find that CNO commences after some 100 ms post bounce. Before this, CNO is suppressed by matter-induced decoherence. In the inverted mass hierarchy, the spectrum of νe becomes softer after the onset of CNO. To evaluate the detectability of this modification, we define a hardness ratio between the number of high energy neutrino events and low energy neutrino events adopting a fixed critical energy. We show that Hyper-Kamiokande (HK) can distinguish the effect of CNO for supernova distances out to ∼10 kpc. On the other hand, for the normal mass hierarchy, the spectrum of νe becomes softer after the onset of CNO, and we show that DUNE can distinguish this feature for supernova distances out to ∼10 kpc. More work is necessary to optimize the best value of critical energy for maximum sensitivity. We also show that if the spectrum of νe in HK becomes softer due to CNO, the spectrum of νe in DUNE becomes harder, and vice versa. These synergistic observations in νe and νe, by HK and DUNE, respectively, will be an intriguing opportunity to test the occurrence of CNO.
AB - In order to investigate the impact of collective neutrino oscillations (CNOs) on the neutrino signal from a nearby supernova, we perform three-flavor neutrino oscillation simulations employing the multiangle effect. The background hydrodynamic model is based on the neutrino hydrodynamic simulation of a 8.8 M⊙ progenitor star. We find that CNO commences after some 100 ms post bounce. Before this, CNO is suppressed by matter-induced decoherence. In the inverted mass hierarchy, the spectrum of νe becomes softer after the onset of CNO. To evaluate the detectability of this modification, we define a hardness ratio between the number of high energy neutrino events and low energy neutrino events adopting a fixed critical energy. We show that Hyper-Kamiokande (HK) can distinguish the effect of CNO for supernova distances out to ∼10 kpc. On the other hand, for the normal mass hierarchy, the spectrum of νe becomes softer after the onset of CNO, and we show that DUNE can distinguish this feature for supernova distances out to ∼10 kpc. More work is necessary to optimize the best value of critical energy for maximum sensitivity. We also show that if the spectrum of νe in HK becomes softer due to CNO, the spectrum of νe in DUNE becomes harder, and vice versa. These synergistic observations in νe and νe, by HK and DUNE, respectively, will be an intriguing opportunity to test the occurrence of CNO.
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U2 - 10.1103/PhysRevD.101.063027
DO - 10.1103/PhysRevD.101.063027
M3 - Article
AN - SCOPUS:85083502622
SN - 2470-0010
VL - 101
JO - Physical Review D
JF - Physical Review D
IS - 6
M1 - 063027
ER -