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Menu du jour. Collective Swaps MSW Conversions. www.ps.uci.edu/~tomba/sk/tscan. Neutrino Production. Neutrino Propagation and Flavor Conversion . Neutrino Detection. Neutrino Astronomy Supernova Astrophysics. Neutrino properties and particle physics . - PowerPoint PPT Presentation
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Neutrinos from Supernovae
Basudeb Dasgupta
International Conference in High Energy Physics ICHEP 2010, 22-28 July 2010, Paris, France
Menu du jour
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
www.ps.uci.edu/~tomba/sk/tscan
Neutrino Production
Neutrino Detection
Neutrino Propagation and Flavor Conversion
Neutrino Astronomy Supernova Astrophysics
Neutrino propertiesand particle physics
1. Pointing in advance/SN alerts2. Signatures of stellar dynamics3. Tracking the local SN rate4. Timing/GW-coincidence
1. Neutrino Mass Hierarchy2. Q13 estimate3. QCD phase transition
Collective Swaps
MSW Conversions
Neutrino Production in Supernovae
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
SN Explosion and Neutrino Emission
Main-sequence star
Hydrogen Burning
Helium-burning star
HeliumBurning
HydrogenBurning
Onion structure
Degenerate iron core: r 109 g cm-3
T 1010 K MFe 1.5 Msun
RFe 8000 km
Collapse (implosion)
Adapted from a slide by Georg Raffelt
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
SN Explosion and Neutrino Emission
Collapse (implosion)Bounce (explosion)
neBurst
Prompt Shock StallsNeutrino HeatingNeutrino Driven ExplosionNewborn Neutron Star
~ 50 km
Proto-Neutron Starr rnuc = 3 1014 g cm-3
T 30 MeV
Neutrino Cooling
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Neutrino Luminosities and Energies
Luminosity in 1051erg/s
For ne, anti-ne and nx
Average Energy in MeV
For ne, anti-ne and nx
Raffelt, Keil, Buras, Janka and Rampp, arXiv:astro-ph/0303226
Accretion Phase
Cooling Phase
BurstPhase
Neutrino Propagation and Flavor Conversions
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Free-Streaming Neutrinos
]),)[(cos1(
2qdG2],L[G2,p2
Mi pqqqp33
FpFp2
pt
rrr
rrr
MSW effect depends on ordinary matter density L, i.e. mainly e density
Vacuum oscillations• M is neutrino mass
matrix• minus sign for
antineutrinos
Nonlinear nu-nu effects are important when nu-nu interaction energy exceeds the typical vacuum oscillation frequency
These interactions give rise to “Collective” flavor conversions
Nonlinear Effects depends on the
neutrino density r
Talk by Antonio Marrone, ICHEP-2010
PantaleoneMikheev, Smirnov, WolfensteinPontecorvo
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Status Report at ICHEP 2008
Neutrinos Plenary Talk by Zhi-Zhong Xing, ICHEP-2008
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Spectral Swaps: Accretion Phase
Fogli, Lisi, Marrone and Mirizzi, arXiv: 0707.1998
Nontrivial Evolution only for Inverted Hierarchy
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Collective Flavor Conversion
Swap cannot be complete, because of Total Lepton Number Conservation
Instability in Flavor Space Swap around spectral crossings
Flav
or F
luxe
s
Energy Energy
ne ne nn
Initial
Final
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Spectral Swaps: Cooling Phase
Dasgupta, Dighe, Raffelt and Smirnov, arXiv: 0904.3542 (PRL)
Spectral Splits in Inverted Hierarchy
Spectral Splits in Normal Hierarchy
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
3 Flavor Spectral Swaps: Cooling Phase
Friedland, arXiv:1001.0996 (PRL) Dasgupta, Mirizzi, Tamborra and Tomas, arXiv:1002.2943
NH
IH
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Late-time + Angle-dependent + 3 flavors
Duan and Friedland, arXiv: 1006.2359
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Survey of Flux Models
Fogli, Lisi, Marrone and Tamborra, arXiv:0907.5115 Choubey, Dasgupta, Dighe and Mirizzi, arXiv:1008.xxxx
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
MSW conversions in SN
NH
IH
Spectral Splits in Inverted Hierarchy
L resonance : n1 n2(Dmsol
2 , 12) at 101 – 102 g/cc
Always in neutrinos.
Always adiabatic.
Spectral Splits in
H resonance : n1/n2 n3(Dmatm
2 , 13) at 103 – 104 g/ccIn neutrinos for NH and in
antineutrinos for IH. Adiabaticity ≈ sin213
Dighe and Smirnov, arXiv: hep-ph/9907423
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Regeneration in Earth Matter
Electron flavor flux = cos2 12 n1 + sin2 12 n2
Electron flavor: = (1-P2e) n1 + P2e n2
P2e is the probability of n2 to ne
which depends on Earth density and L
L
Detector LocationMatters!
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Survival Probabilities
B. Dasgupta, arXiv:hep-ph/1005.2681 [Moriond-2010, Proceedings]
<
Neutrino Detection
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Running (soon) SN Neutrino Detectors
Hyper-K/UNO/MEMPHYS/LENA/Km3NET/…
Icecube
Super-K
KamLAND
Mini-BOONE
LVD
Borexino
BaksanIcaru
sHAL
O
SNO+
NOnA
✔
✔
✔
✔=Large (>103 events for 10kpc SN)
Daya-Bay
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Main Detection Channels• SK-like water Cherenkov detector (30 kt, SN at 10kpc)
• Scintillation detector
• Liquid Argon detector Liquid Argon TPC can see neutrinos, others mostly see antineutrinos
Super-Kamiokande and Icecube are at present our largest detectors for SN neutrinos.
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Positron and gamma ray vertices are within ~50cm.[reaction schematic by M. Nakahata]
ne
e+
pn
g
gp
Gd
Gadzooks
ne can be identified by delayed coincidence.
n+Gd → ~8 MeV g (90%)n+p → d + 2.2 MeV g (10%)
Beacom and Vagins, arXiv:hep-ph/0309300 (PRL)
Can identify each antineutrino on an event-by-event basis
Gadolinium Anti-nu Detector Zealously Outperforming Old Kamiokande. Super!
What Can We Learn ?- Astrophysics -
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
SN pointing alerts/SNEWS
Beacom and Vogel, arXiv: astro-ph/9811350
Tomas, Semikoz, Kachelriess, Raffelt and Dighe, arXiv: hep-ph/0307050
Neutrinos reach ~24 hours before the light from SN explosionSN at 10 kpc may be detected within a cone of ∼ 5◦ at SK, factor of 3 better with Gd, and factor of 10 better with a 30xSK
This may be crucial for dust-obscured supernovae!
SNEWShttp://
snews.bnl.gov
Coincidence at multiple detectors will trigger an alert for astronomers
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Stellar Explosion DynamicsStanding Accretion Shock InstabilityLarge scale motion of the stellar material on a millisecond timescaleFluctuations in the neutrino signal, luminosities and energiesLund, Marek,
Lunardini, Janka and Raffelt: astro-ph/1006.1889
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Diffuse Neutrino BackgroundEstimated present-day flux from all SN in our past~ 10 cm-2 s-1en
Beacom and Vagins,hep-ph/0309300 (PRL)
Horiuchi, Beacom and Dwek, arXiv:0812.3157
Guaranteed source of neutrinos from cosmological distances
See also Chakraborty, Choubey, Dasgupta and Kar, arXiv:0805.3131 for effect of collective oscillations on DSNB
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Coincidence with Gravity Wave Expts
SN neutrino-curve is an excellent probe of the
bounce time.This can be used to great advantage for coincidence
measurement with gravitational wave detectors
Pagliaroni, Vissani, Coccia and Fulgione, arXiv:0903:1191 (PRL)Halzen and Raffelt, arXiv:0908.2317
What Can We Learn ? - Particle Physics -
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Can we see the splits? Perhaps…for Cooling.
Choubey, Dasgupta, Dighe and Mirizzi, arXiv:1008.xxxx
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Accretion phase signals…a bit weaker.
Choubey, Dasgupta, Dighe and Mirizzi, arXiv:1008.xxxx
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Earth Matter Effects
Choubey, Dasgupta, Dighe and Mirizzi, arXiv:1008.xxxx
Ratio of events betweenshadowed and
unshadowedWC detectors is an excellent probe of the
Neutrino Mass Hierarchy Fourier analysis of the
event rate reveals earth effect
oscillations for a single Liq.
Argon/Scintillator detector.
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Neutrino Mass Hierarchy
Ratio of events at two 0.4 MT WC detectors, one shadowed and other not. SN taken at 10 kpc.
Dasgupta, Dighe and Mirizzi, arXiv: arXiv:0802.1481 (PRL)
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Q13 Estimate/Shockwave effects
Tomas, Kachelriess, Dighe, Raffelt and Janka,arXiv:astro-ph/0407132
Most of the work on this was done around 2000-2004 After including collective effects …
e.g. Gava, Kneller, Volpe and Mc Laughlin, arXiv:0902.0317 (PRL)
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
QCD anti-nu burst detectable from SN
Sagert, Fischer, Hempel, Pagliara, Schaffner-Bielich, Mezzacappa, Thielemann, and Liebendoerfer, arXiv:0809.4225 (PRL)
Dasgupta, Fischer, Horiuchi, Liebendorfer, Mirizzi, Sagert and Schaffner-Bielich arXiv:0912.2568
2nd Shock Break-out
Width = ~5ms
Summary
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
www.ps.uci.edu/~tomba/sk/tscan
Neutrino Production
Neutrino Detection
Neutrino Propagation and Flavor Conversion
Neutrino Astronomy Supernova Astrophysics
Neutrino propertiesand particle physics
1. Pointing in advance/SN alerts2. Signatures of stellar dynamics3. Tracking the local SN rate4. Timing/GW-coincidence5. …
1. Neutrino Mass Hierarchy2. Q13 estimate3. QCD phase transition4. …
Collective Swaps
MSW Conversions
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Back-up Slide 1: R-process nucleosynthesis
Demanding successful R-process nucleosynthesis puts non-trivial constraints on possible SN fluxes.
Chakraborty, Choubey, Goswami and Kar, arXiv: arXiv:0911.1218
Basudeb Dasgupta, ICHEP-2010 at Paris, France, 22 - 28 July 2010
Back-up Slide 2: Non-Standard effectsNon-Standard Interactions can give rise to a rich set of
possibilities, and make things more complicated.
Esteban-Pretel, Tomas and Valle, arXiv:0909.2196