2010
DOI: 10.1103/physrevd.82.033011
|View full text |Cite
|
Sign up to set email alerts
|

Acquiring information about neutrino parameters by detecting supernova neutrinos

Abstract: We consider the supernova shock effects, the Mikheyev-Smirnov-Wolfenstein effects, the collective effects, and the Earth matter effects in the detection of type II supernova neutrinos on the Earth. It is found that the event number of supernova neutrinos depends on the neutrino mass hierarchy, the neutrino mixing angle 13 , and neutrino masses. Therefore, we propose possible methods to identify the mass hierarchy and acquire information about 13 and neutrino masses by detecting supernova neutrinos. We apply th… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

0
20
1

Year Published

2012
2012
2016
2016

Publication Types

Select...
5

Relationship

4
1

Authors

Journals

citations
Cited by 7 publications
(21 citation statements)
references
References 111 publications
0
20
1
Order By: Relevance
“…2 shows the path of SN neutrinos reaching the detector on the Earth. When all effects, including the SN shock effects, the MSW effects, the neutrino collective effects, and the Earth matter effects, are taken into account, the SN neutrino fluxes at the detector can be written as [26]…”
Section: Sn Neutrino Detection At Csnsmentioning
confidence: 99%
See 2 more Smart Citations
“…2 shows the path of SN neutrinos reaching the detector on the Earth. When all effects, including the SN shock effects, the MSW effects, the neutrino collective effects, and the Earth matter effects, are taken into account, the SN neutrino fluxes at the detector can be written as [26]…”
Section: Sn Neutrino Detection At Csnsmentioning
confidence: 99%
“…In Eqs. ( 2) and (3), P 2e ( P2e ) is the probability that a (anti)neutrino mass eigenstate ν 2 (ν 2 ) enters the surface of the Earth and arrives at the detector as an electron (anti)neutrino ν e (ν e ), P νν ( Pνν ) is the probability that the (anti)neutrino ν(ν) remains as ν(ν) after the collective effects, and P H ( PH ) is the crossing probability for (anti)neutrinos to jump from one eigenstate to another at the high resonance layer [26]. We assume a "standard" SN explosion at a distance D = 10 kpc from the Earth, releasing a total energy E B = 3 × 10 53 erg (similar to SN1987A [4,5]).…”
Section: Sn Neutrino Detection At Csnsmentioning
confidence: 99%
See 1 more Smart Citation
“…A summary for neutrino flavor conversions due to the neutrino shock wave effects and the MSW effects in various density regions is given in Table II [10].…”
Section: B Sn Shock Wave Effects and Phmentioning
confidence: 99%
“…In addition, the shock wave effects may change the density distribution of SN and the position of the high resonance. The expression of P H for large θ 13 needs to be developed [10][19] [25]. When studying the Earth matter effects, the realistic density distribution of the Earth needs to be considered [26][27].…”
Section: Introductionmentioning
confidence: 99%