Neutrinos in Core Collapse Supernovae
Evan O’Connor, Stockholm University
Outline:
- SN theory & status
- Neutrino Signal
Neutrinos in Core Collapse Supernovae Evan OConnor, Stockholm - - PowerPoint PPT Presentation
Neutrinos in Core Collapse Supernovae Evan OConnor, Stockholm University Outline: SN theory & status Neutrino Signal Supernovae have a broad connection to the Universe Neutrinos & Gravitational Waves Nucleosynthesis Stellar
Cosmology High-Z & SCP
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Stellar Evolution ESO Long gamma-ray burst Science/MacFadyen LIGO/VIRGO Neutron Star & Black Holes Hubble Galaxy Evolution Neutrinos & Gravitational Waves Nucleosynthesis Wikimedia/Jennifer Johnson Extreme Nuclear Physics
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Volumetric Supernova Survey: Li et al. (2010)
Core Collapse Thermonuclear
HST HST
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red supergiant phase
core (~1000km, or 1/106 of the star’s radius)
pressure can no longer support the core against gravity
1000 Rsun
Iron Core 1000 km M ~ 1.4Msun
Protoneutron Star ~30km HST
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Iron core collapse
sonic point
t = -5ms
r~1012 g cm-3
|---200 km---|
bounce
shock n n n n
r~1014 g cm-3
n
t = 0ms
|---20 km---|
shock stagnation
stalled shock
n n n
|---200 km---|
t = ~100ms
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Iron core collapse
sonic point
t = -5ms
r~1012 g cm-3
|---200 km---|
bounce
shock n n n n
r~1014 g cm-3
n
t = 0ms
|---20 km---|
shock stagnation
stalled shock
n n n
|---200 km---|
t = ~100ms
t > ~200ms
n ne e- p n
|---150 km---|
n
Explosion
Require some mechanism to drive explosion
turbulence-aided neutrino mechanism
and drives explosion
successful explosions
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Understanding the transition from an imploding iron core to an exploding star has been a persistent and difficult problem in astrophysics.
EO & Couch (2018b)
General Relativity Neutrino Transport & Interactions Nuclear Reactions 3D - (Magneto)hydrodynamics Nuclear Equation
Progenitors
Computational Physics
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Burrows et al. (2019)
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Burrows et al. (2019) Lentz et al. (2015)
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Burrows et al. (2019) Lentz et al. (2015) Melson et al. (2015b)
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Burrows et al. (2019) Lentz et al. (2015) Melson et al. (2015b) Ott et al. (2018)
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e- n p ne
from 3ms before bounce to 6 ms after (animation)
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2 4 6 8 10 12 14 16 18 20
t - tbounce [ms]
1 2 3 4 5 6
Luminosity [1053 erg/s] Iron core mass increasing -> Matter temperature increasing ->
_
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x3-4
Warren et al. (in prep) Compactness
Luminosity (1051 erg/s)
Couch et al. (2019) & 200 1D models from
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Warren et al. (in prep) Couch et al. (2019) & 200 1D models from
Compactness
Luminosity (1051 erg/s)
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ensure fair comparison
Journal of Physics: G 45 10 2018
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EO+ 2018 Si/O interface Si/O interface
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Malmenbeck, O’Sullivan (2019) PoS- ICRC2019-975; arXiv:1909.00886 Implementation of detailed IceCube detector into SNOwGLoBES
detector efficiency, deadtime, … *Normal Hierarchy: only adiabatic MSW
https://github.com/SNOwGLoBES/
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Hyper-K design report (arXiv:1805.04163)
EO & Couch (2018b)
data: Tamborra et al. (2013)
see also TAUP talk by T. Takiwaki
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Westernacher-Schneider, O’Connor, O’Sullivan+ (arXiv:1907.01138) see also TAUP talk by T. Takiwaki
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Westernacher-Schneider, O’Connor, O’Sullivan+ (arXiv:1907.01138) see also TAUP talk by T. Takiwaki
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*Realizations take into account statistical noise and detector background noise Westernacher-Schneider, O’Connor, O’Sullivan+ (arXiv:1907.01138)
(animation) (animation) (animation)
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(but also others) shows simultaneous accretion & ejection Luminosity 1052 erg/s
post bounce time [s]
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info about the EOS
talkby Y. Suwa)
important and can impact nucleosynthesis
Horowitz et al. (2016) Super-K like
x=
*Here x characterizes additional opacity due to nuclear pasta formation
x=5 x=5 x= x=
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LIGO
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with SNOwGLoBES 10kpc
O’Connor (2015)
MSW only
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TAUP talks by: A. Harada, K. Nakazato, S. Abbar, N. Yamamoto,