Late-Time Neutrino Emission Impact on DSNB Study

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Impact of late time
neutrino emission on the
DSNB
(Ekanger et al., in prep)
Nick Ekanger
1
Core Collapse Supernovae (CCSNe)
2
Infalling material
bounces off core,
pressure shock
wave
Neutrinos revive
shock, cooling
protoneutron star
[1] Burrows et al. (2021)
[1]
Neutrinos from CCSNe
Early signal:
High luminosity, high mean energy
from accretion
Simulations typically focus on this
Late signal:
After shock revival, PNS cools
Luminosity and mean energy
decrease
SN1987A only case of SN
neutrinos
3
[1] Li et al. (2021)
[1]
Neutrinos from Simulation
Estimate neutrino
emission from
simulations:
Robust, dynamic mass
accretion phase
Few with long term
cooling components
4
[1] Bollig et al. (2021)
[1]
Diffuse Supernova Neutrino Background
(DSNB)
5
[1] https://www.businessinsider.com/super-kamiokande-neutrino-detector-is-unbelievably-beautiful-2018-6
[2] https://www.mpi-hd.mpg.de/WIN2015/talks/neutrino2_ikeda.pdf
[1]
[2]
 
[2]
DSNB Uncertainty
6
DSNB
uncertainty
CC Rate
(from SFR)
Neutrino
emission
Failed
SNe (BH)
PNS
Cooling
[1] Abe et al. (2021)
[2] Li et al. (2021)
 
[1]
Successful
SNe (NS)
Accretion
Phase
First, Set the Stage
7
[1] Burrows et al. (2021)
[2] Yuksel et al. (2008), Horiuchi et al. (2011)
[3] Hudepohl (2014)
[1]
[2]
[3]
Estimate Cooling Phase 5 Ways
8
Constant Mean Energy
Mean energy:
Assume it retains value at end of
simulation
Expected to reduce as PNS cools,
so represents upper limit
Liberated energy:
Assume ~energy liberated =
gravitational binding energy
Determined from PNS
mass/radius and SFHo EOS
9
(‘Const’)
Analytic Solution
10
[1] Suwa et al. (2021)
[1]
(‘Analyt’)
Final Mass-Revival Time Correlation
11
(‘Corr’)
[1] Nakazato et al. (2013)
[1]
Renormalized Correlations
Neutrino emission from ‘Corr’
method systematically lower
than others
Renormalize correlations to
another simulation suite
Re-fit through data well
Depends on EOS:
Mean energy differences are large
12
[1] Hudepohl (2014)
[1]
(‘RenormShen/LS’)
Results
13
Conclusion
Factor of ~3 difference in predicted DSNB rates at SK-Gd
Under current SK flux limits
Comes primarily from uncertainty in cooling phase mean energy
In absence of many long-term, multidimensional
simulations
Among 5 methods, recommend ‘RenormLS’
Recommend ‘Analyt’ if more simulation data is available
14
[1] Abe et al. (2021)
[1]
Thank you!
15
Slide Note

Hello everyone. Today I’m going to be talking about how supernova simulations inform our DSNB predictions. Specifically, I’ll be showing that various reasonable estimates for the uncertain late time neutrino emission leads to a large discrepancy in the predicted DSNB rates at Super Kamiokande.

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Explore the implications of late-time neutrino emission on the Diffuse Supernova Neutrino Background (DSNB) through core collapse supernovae simulations. The research delves into the dynamics of neutrino emission in different phases of supernova events and its relevance to understanding the DSNB.

  • Neutrino emission
  • Core collapse supernovae
  • DSNB study
  • Late-time impact
  • Supernova simulations

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  1. Impact of late time neutrino emission on the DSNB (Ekanger et al., in prep) Nick Ekanger 1

  2. Core Collapse Supernovae (CCSNe) Infalling material bounces off core, pressure shock wave Neutrinos revive shock, cooling protoneutron star [1] 8 ? , Iron fused in core of progenitor, radiation pressure decreases ? ~1.4 ? core collapses, ? + ? ? + ??, neutron degeneracy [1] Burrows et al. (2021) 2 Virginia Tech CNP Research Day 2022 Core collapse supernovae

  3. Neutrinos from CCSNe [1] Early signal: High luminosity, high mean energy from accretion Simulations typically focus on this Late signal: After shock revival, PNS cools Luminosity and mean energy decrease SN1987A only case of SN neutrinos [1] Li et al. (2021) 3 Virginia Tech CNP Research Day 2022 Core collapse supernovae

  4. Neutrinos from Simulation Estimate neutrino emission from simulations: Robust, dynamic mass accretion phase Few with long term cooling components [1] [1] Bollig et al. (2021) 4 Virginia Tech CNP Research Day 2022 Core collapse supernovae

  5. Diffuse Supernova Neutrino Background (DSNB) [1] Sum distribution of CCSNe over cosmological history Individual CCSNe events cannot be detected Detectable at SK through IBD ??+ ? ?++ ? Gadolinium upgrade (SK-Gd) [2] [1] https://www.businessinsider.com/super-kamiokande-neutrino-detector-is-unbelievably-beautiful-2018-6 [2] https://www.mpi-hd.mpg.de/WIN2015/talks/neutrino2_ikeda.pdf 5 Virginia Tech CNP Research Day 2022 Diffuse Supernova Neutrino Background

  6. DSNB Uncertainty [2] CC Rate (from SFR) DSNB uncertainty Failed SNe (BH) Cooling phase Neutrino emission Accretion Phase Successful SNe (NS) PNS Cooling [1] [1] Abe et al. (2021) [2] Li et al. (2021) 6 Virginia Tech CNP Research Day 2022 Diffuse Supernova Neutrino Background

  7. First, Set the Stage [1] Our Model 3D simulations give neutrino emission for accretion phase Assume standard SFR Neutrino emission from BH Choose conservative BH fraction: (M > 40 ? , ~10%) Signal from two 40 ? simulations Need cooling phase neutrino emission [2] [3] [1] Burrows et al. (2021) [2] Yuksel et al. (2008), Horiuchi et al. (2011) [3] Hudepohl (2014) 7 Virginia Tech CNP Research Day 2022 Estimate the Cooling Phase

  8. Estimate Cooling Phase 5 Ways Need mean energy and energy liberated by neutrinos 50% of energy liberation occurs in cooling phase! Without many long-term multi-dimensional simulations, we estimate the cooling phase by: 1. Constant mean energy 2. Analytical solution 3. Correlation method 4. Renormalized correlation methods Shen EOS LS220 EOS 8 Virginia Tech CNP Research Day 2022 Estimate the Cooling Phase

  9. Constant Mean Energy ( Const ) Mean energy: Assume it retains value at end of simulation Expected to reduce as PNS cools, so represents upper limit Liberated energy: Assume ~energy liberated = gravitational binding energy Determined from PNS mass/radius and SFHo EOS 9 Virginia Tech CNP Research Day 2022 Estimate the Cooling Phase

  10. Analytic Solution ( Analyt ) Analytic function to estimate neutrino luminosity and mean energy PNS info: mass, radius, total energy liberated + correction factors for density (g) and scattering off heavy nuclei (?) [1] g, ? adjusted to best fit mean energy Mean energy ~ reasonable, but luminosity fit is poor Despite this, integrating luminosity ~ grav binding energy [1] Suwa et al. (2021) 10 Virginia Tech CNP Research Day 2022 Estimate the Cooling Phase

  11. Final Mass-Revival Time Correlation ( Corr ) Found linear correlation with 1D cooling phase sims Supernova Neutrino Database Both mean energy and log of liberated energy [1] Greater final mass greater neutrino emission Earlier revival time greater neutrino emission [1] Nakazato et al. (2013) 11 Virginia Tech CNP Research Day 2022 Estimate the Cooling Phase

  12. Renormalized Correlations ( RenormShen/LS ) Neutrino emission from Corr method systematically lower than others Renormalize correlations to another simulation suite Re-fit through data well Depends on EOS: Mean energy differences are large [1] [1] Hudepohl (2014) 12 Virginia Tech CNP Research Day 2022 Estimate the Cooling Phase

  13. Results Total ?? energies: early hydro data + late cooling estimations (~0-20s post-bounce) Corr / Const are lower / upper estimates Liberated energies similar Mean energies drive differences in event rates Factor of ~3 difference in event rates (??) and flux (?) 13 Virginia Tech CNP Research Day 2022 Wrapping up

  14. Conclusion Factor of ~3 difference in predicted DSNB rates at SK-Gd Under current SK flux limits Comes primarily from uncertainty in cooling phase mean energy [1] In absence of many long-term, multidimensional simulations Among 5 methods, recommend RenormLS Recommend Analyt if more simulation data is available [1] Abe et al. (2021) 14 Virginia Tech CNP Research Day 2022 Wrapping up

  15. Thank you! 15

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