Kazumi Tolich Stanford University 2/6/2007
Outline KamLAND Previous Reactor Neutrino Result Previous Geoneutrino Result Future Possibilities - Full Energy Analysis
- Solar Neutrinos
- Supernova
KamLAND
KamLAND Location KamLAND was designed to measure reactor anti-neutrinos. KamLAND is surrounded by nuclear reactors in Japan.
KamLAND Detector
Detecting Anti-neutrinos with KamLAND KamLAND (Kamioka Liquid scintillator Anti-Neutrino Detector)
Major Background Events for Antineutrino Detection Accidentals: uncorrelated events due to the radioactivity in the detector mimicking the inverse beta decay signature.
Neutrino Oscillation Results Phys. Rev. Lett. 90, 021802 (2003) “First Results from KamLAND: Evidence for Reactor Anti-Neutrino Disappearance” 1269 citations as of last week! The most cited paper in physics in 2003 The 2nd most cited paper in all sciences in 2003
Neutrino Oscillations in Vacuum The weak interaction neutrino eigenstates may be expressed as superpositions of definite mass eigenstates The electron neutrino survival probability can be estimated as a two flavor oscillations:
Selecting Reactor Anti-neutrino Events Δr < 2m 0.5μs < ΔT < 1000μs 2.6MeV < Ee+, p < 8.5MeV 1.8MeV < E, d < 2.6MeV Veto after muons Rp, Rd < 5.5m
Dataset and Rate Analysis From March 9 2002 to January 11 2004. 365.2 ± 23.7 expected reactor antineutrinos with no oscillation. 17.8 ± 7.3 expected background events. 258 candidate events. The average survival probability is 0.658 ± 0.044(stat) ± 0.047(syst). We confirmed antineutrino disappearance at 99.998% C.L. (~4).
Prompt Energy Distribution KamLAND saw an antineutrino energy spectral distortion at 99.6% significance.
Oscillation Analysis Shape distortion is the key factor in determining m2.
Average Distance, L0
L0/E
Geoneutrino Result Nature 436, 499-503 (28 July 2005) geologically produced antineutrinos with KamLAND”
Convection in the Earth The mantle convection is responsible for the plate tectonics and earthquakes. The mantle convection is driven by the heat production in the Earth.
Heat from the Earth Heat production rate from U, Th, and K decays is estimated from chondritic meteorites to be 19TW. Heat flow is estimated from bore-hole measurements to be 44 or 31TW. Models of mantle convection suggest that the radiogenic heat production rate should be a large fraction of the total heat flow. Problem with - Mantle convection model?
- Total heat flow measured?
- Estimated radiogenic heat production rate?
Geoneutrino Signal decays in U and Th decay chains produce antineutrinos. Geoneutrinos can serve as a cross-check of the radiogenic heat production rate. KamLAND is only sensitive to antineutrinos above 1.8MeV Geoneutrinos from K decay cannot be detected with KamLAND.
Selecting Geoneutrino Events Δr < 1m* 0.5μs < ΔT < 500μs* 1.7MeV < E,p< 3.4MeV 1.8MeV < E,d< 2.6MeV Veto after muons Rp, Rd < 5m* ρd>1.2m*
How Many Geoneutrinos?
Future Possibility I Full Energy Analysis
Combined Analysis Combined analysis probes lower energy reactor anti-neutrinos and should improve m2 measurement. We will possibly observe the re-reappearance of reactor antineutrinos. Better understanding of reactor spectrum might improve the geoneutrino measurement.
Previous and Planned Cuts Geoneutrino event selection cuts are tighter due to the low energy accidental background. Combined analysis requires consolidation of the difference in the event selection cuts.
Real and Visible Energies Ereal is the particle’s real energy. Evisible is determined from the amount of optical photons detected, including quenching and Cerenkov radiation effects. The model of Evisible/Ereal as a function of Ereal fits calibration data very well. Previous analyses were done in positron real energy, having to convert background energies (such as ’s) into effective positron real energies.
Expected Delayed Energy Spectra
Expected t Spectra
Time Variation of Reactor Neutrino Flux Shika reactor ~90km (half of L0) away turned on from May 26 2005 to July 4 2006. Shika contributed 14% of total flux. May help distinguish LMA I and LMA II.
Probability Density Functions Expected prompt energy spectra and time variation of reactor neutrino flux were used in the previous analyses. Expected delayed energy and t spectra will be added to distinguish accidental background.
Solar Neutrinos from the p-p Chain Reactions
Solar Neutrino Spectrum
7Be Solar Neutrino Detection Solar scatters off e-. The electron recoil energy is
Current Radioactivity in KamLAND
Test Removal of Reducible Background Distillation removed 222Rn by a factor of 104 to 105. Heating and distillation reduced the 212Pb activity by a factor of 104 to 105. Distillation reduced the 40K concentration in PPO by a factor of 102. Distillation reduced natKr by a factor of 105 to 106.
Expected Energy Spectra after the Purification
Purification System Constructed The purification system is being commissioned right now. We have done some testing and are fixing bugs. We should be able to start the full purification operations soon.
Future Possibility III Supernova Detection
Expected Signals For a “standard supernova” (d = 10 kpc, E=3x1053 ergs, equal luminosity in all neutrino flavors), we expect to see (no neutrino oscillations): - ~310 events
- ~20 events
- ~60 events
- ~45 events
- ~20 events
- ~10 events
- ~300 events
- (0.2 MeV threshold)
There should be 300 e+ events above 10 MeV, with an initial rate of 100 Hz (exponential decay with ~3s time constant). The proton scattering events (low visible energy) provide a determination of both luminosity of all neutrino flavors and temperature.
Supernova Trigger 8 high energy inverse beta decay events (>~9MeV) within ~0.8s causes a supernova trigger. With the supernova trigger, the trigger switches to a pre-determined supernova mode. The supernova mode has a lower energy threshold (~0.6MeV) in order to detect low energy events (especially ν + p → ν + p.) The energy threshold could be lowered after the purification.
Conclusions KamLAND has been producing some impressive results. I am analyzing the full energy range, reactor neutrinos and geoneutrinos simultaneously, to improve sensitivity. The planned purification of scintillator will be followed by the solar neutrino phase. If there is a supernova explosion, KamLAND is the only detector that can possibly detect the proton scattering events.
Questions?
Total Heat Flow from the Earth Conductive heat flow measured from bore-hole temperature gradient and conductivity Deepest bore-hole (12km) is only ~1/500 of the Earth’s radius. Total heat flow 44.21.0TW (87mW/m2), or 311TW (61mW/m2) according to more recent evaluation of same data despite the small quoted errors.
Radiogenic Heat Earth are based on measurement of chondritic meteorites. Chondritic meteorites consist of elements similar to those in the solar photosphere. The predicted radiogenic total heat production is 19TW. Th/U ratio of 3.9 is known better than the absolute concentrations of Th and U.
Reference Earth Model Flux ~20% from nearby crust (within ~30km). ~20% from outside of a ~4000km radius. ~25% from the mantle.
MSW Effect in the Sun e’s experience MSW effect in the Sun.
Irreducible Radioactivity ’s (1.46MeV) and ’s from 40K in the balloon ’s (2.6MeV) from 208Tl decay in the surrounding rocks 14C throughout the detector (less than ~200keV) 11C from cosmic muons (more than 700keV) Most of the 40K and 208Tl background is removed with fiducial volume cut. Most of the 14C and 11C background is removed with energy cut.
Detector Capability The electronics’ buffers can hold ~10k high energy events (all PMTs hit). KamLAND handled a simulated supernova with 400 Hz high energy events (all PMTs hit) for 10 seconds with ~0.6MeV detector threshold.
Do'stlaringiz bilan baham: |