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Astrophysical Neutrinos Neutrinos as probes HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich
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Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

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Page 1: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

Astrophysical Neutrinos

Neutrinos as probes

HQL, Munich, October 16th-20th, 2006

L. Oberauer, TU Munich

Page 2: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

Energy Spectra of AstrophysicalNeutrinos

thermal sources

Non-thermal sources

Page 3: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

L ≈ 20 km

L ≈ 13000 km

atmosphericneutrinos:Ev ~ GeV

Pion production and subsequent decays (incl. muon)

π −> μ + νμ

μ −> e + νμ + νe

⎟⎟⎠

⎞⎜⎜⎝

⎛ Δ=→

νμ θνν

ELmP atm

atmx

222 27.1sin2sin)(

Oscillations and Atmospheric Neutrinos

Page 4: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

Atmospheric Neutrinos and SuperKamiokande

Charged current reactions

νμ + N −> μ + N` and

νe + N −> e + N`

50 kt WaterCherenkovDetector

Page 5: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

νμνe

Electron events Muon events

Up going Up going Neutrinos

μ

e

No-oscillation

Oscillation

Page 6: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

Result atmospheric Neutrino-Oscillations

Best fit:Δm2

atm = 2.5×10-3 eV2

sin22θatm = 1.0

Best fit:Δm2

atm = 2.5×10-3 eV2

sin22θatm = 1.0

Confirmed by

•MACRO (Gran Sasso)

•Soudan (USA)

•K2K acceleratorlong baseline(250 km) experiment

•MINOS (USA) acc. exp. in 2006

Page 7: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

Oscillations and Solar Neutrinos

Neutrino Energy in MeV

MeV7.2622He4 4 +++→ +eep ν

Page 8: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

Sudbury Neutrino ObservatorySNOcharged current interaction (cc)

νe + D −> p + p + eneutral current interaction (nc)

νx + D −> νx + p + nelastic Neutrino-Electron scattering (cc

+ nc)

νx + e −> νx + e 1kt Cherenkov Detectorwith heavy water

Page 9: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

SNO Result

• Flavour transitiondiscovered: 7 sigma !

• Reasonableagreement with solar model

Neutrinos from the Sun (νe) transform into νμ or ντ !

Page 10: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

Solar Neutrino Oscillation

• Determination of Θ12 ~ 340

νe νμ,τ

Δm2 ~ 8 x 10-5 eV2

• Confirmation by reactorexperiment KamLAND

Page 11: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

The solar matter effect – evidence by GALLEX/GNO

GALLEX/GNO

SNO

• Evidence for matter effect inside the Sun

• m2 > m1

• Why are neutrino masses so small?

• GUT

• Leptogenesis

Survival probability electronneutrino

pp- 7Be

8B

Page 12: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

Future of Solar Neutrino Spectroscopy: low energies

• Monoenergetic 7Be • CNO, pepWhy?• Accurate Measurement of thermo nuclear

fusion processes:7Be ~ 10% => pp ~ 1% !

• CNO important for star development

Page 13: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

The MSW Effect and newPhysics ?

Friedland, Lunardini, Peña-Garay, hep-ph/0402266

The MSW effect as filter

• Θ13

•sterile Neutrinos?

• magnetic Neutrino moment?

• new interactions ?

Page 14: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

16L. Oberauer, TU München

Borexino @ Gran Sasso• 7Be solar neutrino measurement

• neutrino electron scattering

• CNO and pep neutrinos

• Long baseline reactor neutrinos

• Terrestrial neutrinos

• Supernova neutrinos

• Search for neutrino magnetic moment

Page 15: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

Water filling started in August 2006

Page 16: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

BOREXINO sees neutrinos from CERN (August 2006) !

Page 17: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

First neutrino events in BOREXINO

Time of flight (CERN to LNGS) ~ 2.4 ms equivalent to ~ 730 km distance

Page 18: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

Future Neutrino ObservatoriesUnsegmented50 kt liquid scintillatorLENA

HyperKamiokande (1 MtWater Cherenkov)

…Liquid Argon ~100 ktTPC

Page 19: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

LAGUNA

• Large Aparatus for Grand Unification and Neutrino Astronomy

• European initiative (France, Germany, Italy, Switzerland, UK, Poland, Finland)

• Aim: Design studies for all 3 kinds of detectors (water Ch, scintillator, liquid argon) until ~ 2010

Page 20: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

Physics goals of future Neutrino Observatories

• Gravitational collapse• Star formation rate in the early universe• Thermonuclear fusion reactions• Baryon number violation (Proton decay)• Leptonic CP – violation• Geophysics• Indirect search for Dark Matter• Active Galactic Nuclei – UHE Neutrinos

Page 21: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

One example for LENA: Detection of the Diffuse Supernova Neutrino Background

(DSNB) ?

• up to now only limits

• flux and spectral shape depend on

Star formation rate

Gravitational collapse model

Page 22: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

Extremely Large Observatories

Km3 Cherenkov detector in the mediterranian sea

Km3 Cherenkovdetector at the South Pole (Ice Cube)

Page 23: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

Amanda

Frejus

Eν ∝ E-3.8

A change in the slope would indicate a non-atmospheric component

Atmospheric neutrino Waxmann-Bahcall limit: Model-independent upper bound

= 2π = 00-03 combined

Limits from Amanda

Ice-Cube ~ 3 10-9

Page 24: Neutrinos as probes...HQL, Munich, October 16th-20th, 2006 L. Oberauer, TU Munich Energy Spectra of Astrophysical Neutrinos thermal sources Non-thermal sources L ≈20 km L ≈13000

Conclusions

• Neutrino physics very successfull in the last decade

• Neutrino masses and mixing established

• Physics beyond the standard model

• New window to astrophysical observations