Neutrinos: Ghostparticles of the UniverseGeorg Raffelt, MPI Physics, Munich Physics Colloquium,...
Transcript of Neutrinos: Ghostparticles of the UniverseGeorg Raffelt, MPI Physics, Munich Physics Colloquium,...
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Neutrinos – Ghost Particles of the Universe
Neutrinos Ghost Particles of the Universe
Georg G. Raffelt
Max-Planck-Institut für Physik, München, Germany
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Neutron
Proton
Periodic System of Elementary Particles
Quarks Leptons
Charge -1/3
Down
Charge -1
Electron
Charge 0
e-Neutrino ne e d
Charge +2/3
Up u
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Neutron
Proton
Gravitation (Gravitons?)
Weak Interaction (W and Z Bosons)
Periodic System of Elementary Particles
Electromagnetic Interaction (Photon)
Strong Interaction (8 Gluons)
Down
Strange
Bottom
Electron
Muon
Tau
e-Neutrino
m-Neutrino
t-Neutrino nt
nm
ne e
m
t
d
s
b
1st Family
2nd Family
3rd Family
Up
Charm
Top
u
c
t
Quarks Leptons
Charge -1/3
Down
Charge -1
Electron
Charge 0
e-Neutrino ne e d
Charge +2/3
Up u
Higgs
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Georg Raffelt, MPI Physics, Munich Colloquium, UNSW, Sydney, 4 March 2014
Where do Neutrinos Appear in Nature?
Nuclear Reactors
Particle Accelerators
Earth Atmosphere (Cosmic Rays)
Earth Crust (Natural Radioactivity)
Sun
Supernovae (Stellar Collapse) SN 1987A
Cosmic Big Bang (Today 330 n/cm3) Indirect Evidence
Astrophysical Accelerators
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Neutrinos from the Sun
Reaction- chains
Energy 26.7 MeV
Helium
Solar radiation: 98 % light 2 % neutrinos At Earth 66 billion neutrinos/cm2 sec
Hans Bethe (1906-2005, Nobel prize 1967)
Thermonuclear reaction chains (1938)
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Sun Glasses for Neutrinos?
8.3 light minutes
Several light years of lead needed to shield solar neutrinos
Bethe & Peierls 1934: … this evidently means that one will never be able to observe a neutrino.
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
First Detection (1954 – 1956)
Fred Reines (1918 – 1998) Nobel prize 1995
Clyde Cowan (1919 – 1974) Detector prototype
Anti-Electron
Neutrinos
from
Hanford
Nuclear Reactor
3 Gammas
in coincidence 𝝂𝐞 p
n Cd
e+ e−
g
g
g
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
First Measurement of Solar Neutrinos
600 tons of Perchloroethylene
Homestake solar neutrino observatory (1967–2002)
Inverse beta decay of chlorine
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
2002 Physics Nobel Prize for Neutrino Astronomy
Ray Davis Jr. (1914–2006)
Masatoshi Koshiba (*1926)
“for pioneering contributions to astrophysics, in particular for the detection of cosmic neutrinos”
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Georg Raffelt, MPI Physics, Munich Colloquium, UNSW, Sydney, 4 March 2014
Cherenkov Effect
Water
Elastic scattering or CC reaction
Light
Light
Cherenkov Ring
Electron or Muon (Charged Particle)
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Super-Kamiokande Neutrino Detector (Since 1996)
42 m
39.3 m
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Super-Kamiokande: Sun in the Light of Neutrinos
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Super-Kamiokande: Sun in the Light of Neutrinos
ca. 60,000 solar neutrinos measured in Super-K (1996–2012)
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Average (1970-1994) 2.56 0.16stat 0.16sys SNU (SNU = Solar Neutrino Unit = 1 Absorption / sec / 1036 Atoms)
Theoretical Prediction 6-9 SNU “Solar Neutrino Problem” since 1968
Results of Chlorine Experiment (Homestake)
ApJ 496:505, 1998
Average Rate
Theoretical Expectation
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Neutrino Flavor Oscillations
Bruno Pontecorvo (1913–1993)
Invented nu oscillations
Two-flavor mixing
Each mass eigenstate propagates as 𝑒i𝑝𝑧
with 𝑝 = 𝐸2 −𝑚2 ≈ 𝐸 −𝑚2 2𝐸
Phase difference 𝛿𝑚2
2𝐸𝑧 implies flavor oscillations
Oscillation Length
sin2(2𝜃)
Probability 𝜈𝑒 → 𝜈𝜇
z
𝜈𝑒𝜈𝜇=cos 𝜃 sin 𝜃−sin 𝜃 cos 𝜃
𝜈1𝜈2
4𝜋𝐸
𝛿𝑚2= 2.5 m
𝐸
MeV eV
𝛿𝑚
2
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Oscillation of Reactor Neutrinos at KamLAND (Japan)
Oscillation pattern for anti-electron neutrinos from Japanese power reactors as a function of L/E
KamLAND Scintillator detector (1000 t)
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Atmospheric Neutrino Oscillations
Atmospheric neutrino oscillations show characteristic L/E variation
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Long-Baseline (LBL) Experiments
K2K Experiment (KEK to Kamiokande) and then other LBL experiments measure precise neutrino oscillation parameters.
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Q13 from Reactor Experiments (2012)
4MeV ͞ne
sin22θ13 = 0.089 ± 0.010 (stat) ± 0.005 (syst)
0.113 ± 0.013 (stat) ± 0.019 (syst)
Daya Bay (China)
Reno (Korea)
0.086 ± 0.041 (stat) ± 0.030 (syst) Double Chooz (Europe)
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
v
Three-Flavor Neutrino Parameters
𝜈𝑒𝜈𝜇𝜈𝜏=1 0 00 𝑐23 𝑠230 −𝑠23 𝑐23
𝑐13 0 𝑒−𝑖𝛿𝑠130 1 0−𝑒𝑖𝛿𝑠13 0 𝑐13
𝑐12 𝑠12 0−𝑠12 𝑐12 00 0 1
1 0 0
0 𝑒𝑖𝛼22 0
0 0 𝑒𝑖𝛼32
𝜈1𝜈2𝜈3
Three mixing angles 𝜃12, 𝜃13, 𝜃23 (Euler angles for 3D rotation), 𝑐𝑖𝑗 = cos 𝜃𝑖𝑗,
a CP-violating “Dirac phase” 𝛿, and two “Majorana phases” 𝛼2 and 𝛼3
39∘ < 𝜃23 < 53∘ 7∘ < 𝜃13 < 11
∘ 33∘ < 𝜃12 < 37∘ Relevant for
0n2b decay Atmospheric/LBL-Beams Reactor Solar/KamLAND
m e t
m e t
m t
1 Sun
Normal
2
3
Atmosphere
m e t
m e t
m t
1 Sun
Inverted
2
3
Atmosphere
Δ𝑚2 72–80 meV2
2180–2640 meV2
Tasks and Open Questions • Precision for all angles
• CP-violating phase d ? • Mass ordering ? (normal vs inverted) • Absolute masses ? (hierarchical vs degenerate) • Dirac or Majorana ?
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Antineutrino Oscillations Different from Neutrinos?
Dirac phase causes different 3-flavor oscillations for neutrinos and antineutrinos
Distance [1000 km] for E = 1 GeV
𝜈𝑒 → 𝜈𝑒 same as 𝜈𝑒 → 𝜈𝑒
𝜈𝑒 → 𝜈𝜇
𝜈𝑒 → 𝜈𝜇
𝝂𝐞 = 𝑐12𝑐13 𝝂𝟏 + 𝑠12𝑐13 𝝂𝟐 + 𝑠13𝑒−𝑖 𝛿 𝝂𝟑
𝝂𝐞 = 𝑐12𝑐13 𝝂𝟏 + 𝑠12𝑐13 𝝂𝟐 + 𝑠13𝑒+𝑖 𝛿 𝝂𝟑
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Neutrino Carabiner Named for a subatomic particle with almost zero mass, …
Greek “nu”
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Neutrino Carabiner Named for a subatomic particle with almost zero mass, …
Greek “nu” Now also in color
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
“Weighing” Neutrinos with KATRIN
• Sensitive to common mass scale m for all flavors because of small mass differences from oscillations
• Best limit from Mainz und Troitsk m < 2.2 eV (95% CL)
• KATRIN can reach 0.2 eV
• Under construction
• Data taking to begin 2015/16
• http://www.katrin.kit.edu
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
KATRIN Ante Portas (25 Nov 2006)
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Weighing Neutrinos with the Universe
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Cosmological Limit on Neutrino Masses
JETP Lett. 4 (1966) 120
Cosmic neutrino “sea” ~112 cm-3 neutrinos + anti-neutrinos per flavor
Ω𝜈ℎ2 =
𝑚𝜈93 eV< 0.23
For all
stable flavors ∑𝑚𝜈 ≲ 20 eV
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
What is wrong with neutrino dark matter?
Galactic Phase Space (“Tremaine-Gunn-Limit”)
Maximum mass density of a degenerate Fermi gas
𝜌max = 𝑚𝜈𝑝max3
3𝜋2 𝑛max
=𝑚𝜈 𝑚𝜈𝑣escape
3
3𝜋2
Spiral galaxies mn > 20–40 eV Dwarf galaxies mn > 100–200 eV
Neutrino Free Streaming (Collisionless Phase Mixing)
Neutrinos Neutrinos
Over-density
• At T < 1 MeV neutrino scattering in early universe is ineffective • Stream freely until non-relativistic • Wash out density contrasts on small scales
• Neutrinos are “Hot Dark Matter” • Ruled out by structure formation
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Sky Map of Galaxies (XMASS XSC)
http://spider.ipac.caltech.edu/staff/jarrett/2mass/XSC/jarrett_allsky.html
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Georg Raffelt, MPI Physics, Munich Colloquium, UNSW, Sydney, 4 March 2014
Structure Formation with Hot Dark Matter
Neutrinos with Smn = 6.9 eV Standard LCDM Model
Structure fromation simulated with Gadget code Cube size 256 Mpc at zero redshift
Troels Haugbølle, http://users-phys.au.dk/haugboel
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Neutrino Mass Limits Post Planck (2013)
Ade et al. (Planck Collaboration), arXiv:1303.5076
CMB alone constraining Smn CMB + BAO constraining Smn + Neff
CMB + BAO limit: Smn < 0.23 eV (95% CL)
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Future Cosmological Neutrino Mass Sensitivity
Basse, Bjælde, Hamann, Hannestad & Wong, arXiv:1304.2321: Dark energy and neutrino constraints from a future EUCLID-like survey
ESA’s Euclid satellite to be launched in 2020 Precision measurement of the universe out to redshift of 2
Pin down the neutrino mass in the sky!
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Georg Raffelt, MPI Physics, Munich Colloquium, UNSW, Sydney, 4 March 2014
Neutrinos as Astrophysical Messengers
Nuclear Reactors
Particle Accelerators
Earth Atmosphere (Cosmic Rays)
Earth Crust (Natural Radioactivity)
Sun
Supernovae (Stellar Collapse) SN 1987A
Cosmic Big Bang (Today 330 n/cm3) Indirect Evidence
Astrophysical Accelerators
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Geo Neutrinos: What is it all about?
We know surprisingly little about the Earth’s interior
• Deepest drill hole ~ 12 km
• Samples of crust for chemical analysis available (e.g. vulcanoes)
• Reconstructed density profile from seismic measurements
• Heat flux from measured temperature gradient 30-44 TW (Expectation from canonical BSE model ~ 19 TW from crust and mantle, nothing from core)
• Neutrinos escape unscathed
• Carry information about chemical composition, radioactive energy production or even a hypothetical reactor in the Earth’s core
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Geo Neutrinos Expected Geoneutrino Flux
Reactor Background
KamLAND Scintillator-Detector (1000 t)
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Reactor On-Off KamLAND Data
KamLAND Collaboration, arXiv:1303.4667 (2013)
Scintillator Purification
KamLAND-Zen Construction
2011 Earthquake Reactors shut down
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
KamLAND Geo-Neutrino Flux
KamLAND Collaboration, arXiv:1303.4667 (2013)
116−27+28 Geoneutrino events
(U/Th = 3.9 fixed) Separately free fitting: U 116 events Th 8 events
Beginning of neutrino geophysics!
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Applied Anti-Neutrino Physics (AAP)
Applied Anti-Neutrino Physics (AAP) Annual Conference Series since 2004 • Neutrino geophysics • Reactor monitoring (“Neutrinos for Peace”)
• Relatively small detectors can measure nuclear activity without intrusion
• Of interest for monitoring by International Atomic Energy Agency (Monitors fissile material in civil nuclear cycles)
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Cosmic Rays
Air Shower: 1019 eV primary particle 100 billion secondary particles at sea level
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Cosmic Rays
Air Shower: 1019 eV primary particle 100 billion secondary particles at sea level Victor Hess (1911/12)
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Cosmic Rays
Air Shower: 1019 eV primary particle 100 billion secondary particles at sea level Victor Hess (1911/12)
100 years later we are still asking
What are the sources for the primary
cosmic rays?
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Neutrino Beams: Heaven and Earth
Target: Protons or Photons
Approx. equal fluxes of photons & neutrinos
Equal neutrino fluxes in all flavors due to oscillations
F. Halzen (2002)
𝜋0
𝜸
𝜋±
𝝁 𝝂𝝁
𝒆 𝝂𝒆𝝂𝝁
𝝂𝒆𝝂𝝁𝝂𝝉
p
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Georg Raffelt, MPI Physics, Munich Colloquium, UNSW, Sydney, 4 March 2014
Nucleus of the Active Galaxy NGC 4261
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Georg Raffelt, MPI Physics, Munich Colloquium, UNSW, Sydney, 4 March 2014
Nucleus of the Active Galaxy NGC 4261
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
IceCube Neutrino Telescope at the South Pole Instrumentation of 1 km3 antarctic ice with ~ 5000 photo multipliers completed December 2010
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Georg Raffelt, MPI Physics, Munich Colloquium, UNSW, Sydney, 4 March 2014
Two High-Energy Events in IceCube
Ernie ~ 1.1 PeV Bert ~ 1.3 PeV
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Ernie & Bert and 26 Additional Events in IceCube
Significance of all 28 events: 4.1s, Background 10.6−3.6+5.0
Ernie & Bert
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
SN 1006 over Sydney
Supernova Neutrinos
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
SN 1006 over Sydney
Supernova Neutrinos
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Crab Nebula
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Georg Raffelt, MPI Physics, Munich Colloquium, UNSW, Sydney, 4 March 2014
Stellar Collapse and Supernova Explosion
Hydrogen Burning
Main-sequence star Helium-burning star
Helium Burning
Hydrogen Burning
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Georg Raffelt, MPI Physics, Munich Colloquium, UNSW, Sydney, 4 March 2014
Stellar Collapse and Supernova Explosion
Hydrogen Burning
Main-sequence star Helium-burning star
Helium Burning
Hydrogen Burning
Onion structure
Degenerate iron core: r 109 g cm-3
T 1010 K MFe 1.5 Msun RFe 3000 km
Collapse (implosion)
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Georg Raffelt, MPI Physics, Munich Colloquium, UNSW, Sydney, 4 March 2014
Stellar Collapse and Supernova Explosion
Collapse (implosion)
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Georg Raffelt, MPI Physics, Munich Colloquium, UNSW, Sydney, 4 March 2014
Stellar Collapse and Supernova Explosion
Collapse (implosion) Explosion Newborn Neutron Star
~ 50 km
Proto-Neutron Star
r ~ rnuc = 3 1014 g cm-3
T ~ 30 MeV
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Georg Raffelt, MPI Physics, Munich Colloquium, UNSW, Sydney, 4 March 2014
Stellar Collapse and Supernova Explosion
Newborn Neutron Star
~ 50 km
Proto-Neutron Star
r ~ rnuc = 3 1014 g cm-3
T ~ 30 MeV
Neutrino
cooling by
diffusion
Gravitational binding energy
Eb 3 1053 erg 17% MSUN c2
This shows up as 99% Neutrinos 1% Kinetic energy of explosion 0.01% Photons, outshine host galaxy
Neutrino luminosity
Ln ~ 3 1053 erg / 3 sec ~ 3 1019 LSUN
While it lasts, outshines the entire visible universe
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Diffuse Supernova Neutrino Background (DSNB)
• Approx. 10 core collapses/sec in the visible universe
• Emitted 𝜈 energy density ~ extra galactic background light ~ 10% of CMB density
• Detectable 𝜈𝑒 flux at Earth ∼ 10 cm−2 s−1 mostly from redshift 𝑧 ∼ 1
• Confirm star-formation rate
• Nu emission from average core collapse & black-hole formation
• Pushing frontiers of neutrino astronomy to cosmic distances!
Beacom & Vagins, PRL 93:171101,2004
Window of opportunity between reactor 𝜈𝑒 and atmospheric 𝜈 bkg
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Sanduleak -69 202 Sanduleak -69 202
Large Magellanic Cloud Distance 50 kpc (160.000 light years)
Tarantula Nebula
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Sanduleak -69 202 Sanduleak -69 202
Large Magellanic Cloud Distance 50 kpc (160.000 light years)
Tarantula Nebula
Supernova 1987A 23 February 1987
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Neutrino Signal of Supernova 1987A
Kamiokande-II (Japan) Water Cherenkov detector 2140 tons Clock uncertainty 1 min
Irvine-Michigan-Brookhaven (US) Water Cherenkov detector 6800 tons Clock uncertainty 50 ms
Baksan Scintillator Telescope (Soviet Union), 200 tons Random event cluster ~ 0.7/day Clock uncertainty +2/-54 s
Within clock uncertainties, all signals are contemporaneous
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Do Neutrinos Gravitate?
Early light curve of SN 1987A
• Neutrinos arrived several hours before photons as expected • Transit time for 𝜈 and 𝛾 same (160.000 yr) within a few hours
Shapiro time delay for particles moving in a gravitational potential
Δ𝑡 = −2 𝑑𝑡𝐵
𝐴Φ 𝑟 𝑡
For trip from LMC to us, depending on galactic model,
Δ𝑡 ≈ 1–5 months
Neutrinos and photons respond to gravity the same to within
1–4 × 10−3
Longo, PRL 60:173, 1988 Krauss & Tremaine, PRL 60:176, 1988
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Supernova 1987A Energy-Loss Argument
SN 1987A neutrino signal
Late-time signal most sensitive observable
Emission of very weakly interacting particles would “steal” energy from the neutrino burst and shorten it. (Early neutrino burst powered by accretion, not sensitive to volume energy loss.)
Neutrino diffusion
Neutrino sphere
Volume emission of new particles
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Flavor Oscillations in Core-Collapse Supernovae
Neutrino sphere
MSW region
Neutrino flux
Flavor eigenstates are propagation eigenstates
Neutrino-neutrino refraction causes a flavor instability, flavor exchange between different parts of spectrum
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Neutrino Oscillations in Matter
Lincoln Wolfenstein
Neutrinos in a medium suffer flavor-dependent refraction
f
Z n n n n
W
f
Typical density of Earth: 5 g/cm3
𝑉weak = 2𝐺F × 𝑁e − 𝑁n 2
−𝑁n 2 for 𝜈efor 𝜈μ
Δ𝑉weak ≈ 2 × 10−13 eV = 0.2 peV
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Flavor-Off-Diagonal Refractive Index
2-flavor neutrino evolution as an effective 2-level problem
i𝜕
𝜕𝑡
𝜈𝑒𝜈𝜇= 𝐻𝜈𝑒𝜈𝜇
𝐻 =𝑀2
2𝐸+ 2𝐺F
𝑁𝑒 −𝑁𝑛20
0 −𝑁𝑛2
+ 2𝐺F𝑁𝜈𝑒 𝑁⟨𝜈𝑒 𝜈𝜇𝑁⟨𝜈𝜇 𝜈𝑒 𝑁𝜈𝜇
Effective mixing Hamiltonian
Mass term in flavor basis: causes vacuum oscillations
Wolfenstein’s weak potential, causes MSW “resonant” conversion together with vacuum term
Flavor-off-diagonal potential, caused by flavor oscillations.
(J.Pantaleone, PLB 287:128,1992)
Flavor oscillations feed back on the Hamiltonian: Nonlinear effects!
𝝂
Z n n
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Collective Supernova Nu Oscillations since 2006 Two seminal papers in 2006 triggered a torrent of activities Duan, Fuller, Qian, astro-ph/0511275, Duan et al. astro-ph/0606616 Balantekin, Gava & Volpe [0710.3112]. Balantekin & Pehlivan [astro-ph/0607527]. Blennow, Mirizzi & Serpico
[0810.2297]. Cherry, Fuller, Carlson, Duan & Qian [1006.2175, 1108.4064]. Cherry, Wu, Fuller, Carlson, Duan & Qian
[1109.5195]. Cherry, Carlson, Friedland, Fuller & Vlasenko [1203.1607]. Chakraborty, Choubey, Dasgupta & Kar
[0805.3131]. Chakraborty, Fischer, Mirizzi, Saviano, Tomàs [1104.4031, 1105.1130]. Choubey, Dasgupta, Dighe &
Mirizzi [1008.0308]. Dasgupta & Dighe [0712.3798]. Dasgupta, Dighe & Mirizzi [0802.1481]. Dasgupta, Dighe, Raffelt
& Smirnov [0904.3542]. Dasgupta, Dighe, Mirizzi & Raffelt [0801.1660, 0805.3300]. Dasgupta, Mirizzi, Tamborra &
Tomàs [1002.2943]. Dasgupta, Raffelt & Tamborra [1001.5396]. Dasgupta, O'Connor & Ott [1106.1167]. Duan
[1309.7377]. Duan, Fuller, Carlson & Qian [astro-ph/0608050, 0703776, 0707.0290, 0710.1271]. Duan, Fuller & Qian
[0706.4293, 0801.1363, 0808.2046, 1001.2799]. Duan, Fuller & Carlson [0803.3650]. Duan & Kneller [0904.0974].
Duan & Friedland [1006.2359]. Duan, Friedland, McLaughlin & Surman [1012.0532]. Esteban-Pretel, Mirizzi, Pastor,
Tomàs, Raffelt, Serpico & Sigl [0807.0659]. Esteban-Pretel, Pastor, Tomàs, Raffelt & Sigl [0706.2498, 0712.1137].
Fogli, Lisi, Marrone & Mirizzi [0707.1998]. Fogli, Lisi, Marrone & Tamborra [0812.3031]. Friedland [1001.0996]. Gava
& Jean-Louis [0907.3947]. Gava & Volpe [0807.3418]. Galais, Kneller & Volpe [1102.1471]. Galais & Volpe
[1103.5302]. Gava, Kneller, Volpe & McLaughlin [0902.0317]. Hannestad, Raffelt, Sigl & Wong [astro-ph/0608695].
Wei Liao [0904.0075, 0904.2855]. Lunardini, Müller & Janka [0712.3000]. Mirizzi [1308.5255, 1308.1402]. Mirizzi,
Pozzorini, Raffelt & Serpico [0907.3674]. Mirizzi & Serpico [1111.4483]. Mirizzi & Tomàs [1012.1339]. Pehlivan,
Balantekin, Kajino & Yoshida [1105.1182]. Pejcha, Dasgupta & Thompson [1106.5718]. Raffelt [0810.1407,
1103.2891]. Raffelt, Sarikas & Seixas [1305.7140]. Raffelt & Seixas [1307.7625]. Raffelt & Sigl [hep-ph/0701182].
Raffelt & Smirnov [0705.1830, 0709.4641]. Raffelt & Tamborra [1006.0002]. Sawyer [hep-ph/0408265, 0503013,
0803.4319, 1011.4585]. Sarikas, Raffelt, Hüdepohl & Janka [1109.3601]. Sarikas, Tamborra, Raffelt, Hüdepohl &
Janka [1204.0971]. Saviano, Chakraborty, Fischer, Mirizzi [1203.1484]. Väänänen & Volpe [1306.6372]. Volpe,
Väänänen & Espinoza [1302.2374]. Vlasenko, Fuller Cirigliano [1309.2628]. Wu & Qian [1105.2068].
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Operational Detectors for Supernova Neutrinos
Super-K (104) KamLAND (400)
MiniBooNE (200)
In brackets events for a “fiducial SN” at distance 10 kpc
LVD (400) Borexino (100)
IceCube (106)
Baksan (100)
HALO (tens)
Daya Bay (100)
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
SuperNova Early Warning System (SNEWS)
http://snews.bnl.gov
Early light curve of SN 1987A
Coincidence Server @ BNL
Super-K
Alert
Borexino
LVD
IceCube • Neutrinos arrive several hours before photons • Can alert astronomers several hours in advance
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Local Group of Galaxies
Current best neutrino detectors sensitive out to few 100 kpc
With megatonne class (30 x SK) 60 events from Andromeda
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Georg Raffelt, MPI Physics, Munich Colloquium, UNSW, Sydney, 4 March 2014
The Red Supergiant Betelgeuse (Alpha Orionis) First resolved image of a star other than Sun
Distance (Hipparcos) 130 pc (425 lyr)
If Betelgeuse goes Supernova: • 6 107 neutrino events in Super-Kamiokande • 2.4 103 neutrons /day from Si burning phase (few days warning!), need neutron tagging [Odrzywolek, Misiaszek & Kutschera, astro-ph/0311012]
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
IceCube as a Supernova Neutrino Detector
Pryor, Roos & Webster, ApJ 329:355, 1988. Halzen, Jacobsen & Zas, astro-ph/9512080. Demirörs, Ribordy & Salathe, arXiv:1106.1937.
• Each optical module (OM) picks up Cherenkov light from its neighborhood
• ~ 300 Cherenkov photons per OM from SN at 10 kpc, bkgd rate in one OM < 300 Hz
• SN appears as “correlated noise” in ~ 5000 OMs
• Significant energy information from time-correlated hits
SN signal at 10 kpc 10.8 Msun simulation of Basel group [arXiv:0908.1871]
Accretion
Cooling
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Georg Raffelt, MPI Physics, Munich Colloquium, UNSW, Sydney, 4 March 2014
First Realistic 3D Simulation (27 M⊙ Garching Group)
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Variability seen in Neutrinos (3D Model)
Tamborra, Hanke, Müller, Janka & Raffelt, arXiv:1307.7936 See also Lund, Marek, Lunardini, Janka & Raffelt, arXiv:1006.1889
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Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Next Generation Large-Scale Detector Concepts
Memphys
Hyper-K
DUSEL LBNE
Megaton-scale water Cherenkov
5-100 kton liquid Argon
100 kton scale scintillator
LENA HanoHano
![Page 74: Neutrinos: Ghostparticles of the UniverseGeorg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014 Neutrinos –Neutrinos Ghost Particles of the Universe Ghost](https://reader034.fdocuments.us/reader034/viewer/2022043006/5f908673eebc8727153e39da/html5/thumbnails/74.jpg)
Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
LENA: From Dream to Reality
50 kt Scintillator
![Page 75: Neutrinos: Ghostparticles of the UniverseGeorg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014 Neutrinos –Neutrinos Ghost Particles of the Universe Ghost](https://reader034.fdocuments.us/reader034/viewer/2022043006/5f908673eebc8727153e39da/html5/thumbnails/75.jpg)
Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
LENA: From Dream to Reality
50 kt Scintillator
Juno (formerly Daya Bay II), Collaboration formed (2014) 20 kt scintillator detector Hierarchy determination with reactor neutrinos Also good for low-energy neutrino astronomy
![Page 76: Neutrinos: Ghostparticles of the UniverseGeorg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014 Neutrinos –Neutrinos Ghost Particles of the Universe Ghost](https://reader034.fdocuments.us/reader034/viewer/2022043006/5f908673eebc8727153e39da/html5/thumbnails/76.jpg)
Georg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014
Summary
Understanding neutrino internal properties — a mature field • Neutrino mixing parameters: Matrix well known from astro and lab evidence • New experiments for missing parameters in the making • Absolute masses yet to be determined (KATRIN, cosmology) • Majorana nature yet to be found (neutrino-less double beta expts) Neutrinos as astrophysical messengers — a field in its infancy • Detailed measurement of solar nus (ca 60,000 events in Super-K) • First geo-neutrinos (ca 116 events in KamLAND) • SN 1987A (ca 20 events) • First high-E events in IceCube (Ernie, Bert, and 26 others)
- More statistics needed in all of these areas: bigger/better detectors planned or discussed - Waiting for next nearby supernova
![Page 77: Neutrinos: Ghostparticles of the UniverseGeorg Raffelt, MPI Physics, Munich Physics Colloquium, UNSW, Sydney, 4 March 2014 Neutrinos –Neutrinos Ghost Particles of the Universe Ghost](https://reader034.fdocuments.us/reader034/viewer/2022043006/5f908673eebc8727153e39da/html5/thumbnails/77.jpg)
Neutrinos at the center