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Determination of mass hierarchy
with reactor neutrino experiment
Yoshitaro Takaesu
KIAS/KNRC
In collaborationwith S.F. Ge, N. Okamura and K. Hagiwara
arXiv: 1210.8141
Introduction
is observed.
Reactor Experiments
can determine the Neutrino Mass Hierarchy .
The sensitivity is studied
of future Medium Baseline Reactor Experiments
for determining the Neutrino Mass Hierarchy
PMT
Reactor neutrino experiment
Reactor Detector
Inside Detector
Inverse Beta Decay (IBD)
Energy Distribution
@ Detector
near far
How to distinguish Mass Hierarchy ?
Mass Hierarchy difference
Max:
vanish:
MH difference in spectrum
Advantages of Reactor Experiment
• Can determine MH independently from CP phase and matter
effects.
•Need only smaller detector than other experiments (e.g., LBL,
atmospheric).
•Free neutrino source with adjustable baseline length
Analysis methods for MH
determination
• Fourier analysis
• analysis
hep-ph/0612022 J.G. Learned et al.
arXiv: 0807.3203 L. Zhan et al.
arXiv: 0901.2976 L. Zhan et al.
arXiv: 1208.1551 X. Qian et al.
arXiv: 1208.1991 E. Ciuffoli et al.
hep-ph/030601 S. Choubey et.al.
arXiv: 0810.2580 M. Batygov et.al.
arXiv: 1011.1646 P. Ghoshal et.al.
Fourier Analysis
• has sensitivity for small .
• Don’t need accurate knowledge of or flux.
analysis
Data is fitted with the theoretical prediction ,
assuming NH or IH.
Fitting parameters are
Penalty term
analysis – MH determination
MH is determined as the hierarchy which gives smaller .
Ex)
MH is NH.
Sensitivity is estimated by
We claim that MH is determined with
significane.
acc. MH
rej. MH
Sensitivity for MH determination
36 km (Max MH diff.)
Max Sensitivity
Typical sensitivity curve as a function of Baseline length L
Effect of
Baseline Length L should be long enough.
L = 30km
L = 50km
Pull Factor
Effect of Energy Resolution
a = 0 a = 6%
Evergy Resolution
affects the sensitivity
significantly.
How good should the energy resolution be ?
3% ? Not enough for RENO50 class of detector (5kton).
Sensitivity for MH determination
20GW 5kton 5yrs
Current Resolution
NH
Optimal L ~ 50 km
Systematic part of Resolution
20GW 5kton 5yrs
Current Resolution • Sensitivity is reduced by 40%.
• Optimal L is shortened
by a few km.
b = 0 b = 1%
a = 2%
a = 3%
Parameter measurement @ L ~ 50 km
Parametermeasurement is not sensitive to the Energy Resolution.
~ 0.5% accuracy
can be measured accurately @ L ~ 50 km
L = 50km
1%
1%
1%
Fluctuation of Sensitivity
So far, we have discussed on the sensitivity
using the “typical data set”.
In the real experiments, event number in each bin, ,
fluctuates from the “typical event number”, .
Then, follows
Gaussian distribution. a = 3%
a = 2%
0 4 13
20GW 5kton 5yrs
2% level of energy resolution is desired.
Expected Probability
L = 50 km
How to achieve 2% energy resolution ?
Increase the photo-electron (p.e.)detected by PMT.
p.e.~ 200 pe/MeV ~ 2000 pe/MeV
Ex)
• Increase PMT coverage
• Increase QE of PMT
• More transparent LS
By Channgen Yang @ NuMass 2013
Multi-reactor interference
Baseline difference should be < 500m.
0 m
500 m
1 km
1.5 km
2 km
arXiv: 1302.0624
L1 L2
L1
|L1 – L2|
Multi-reactor interference
Because of this effect, DayaBayII has changed its location.
Multi-reactor interference
RENO
50 km
200 km
RENO
1.3 km
RENO50
The angle to RENO50 may
affect the sensitivity.
Reactor site
Summary
We have discussed the sensitivity of
Medium Baseline Reactor Experiments
for MH determination.
For 20GW 5kton 5yrs exposure,
50km optimal Baseline Length
a < 3%
b < 1%
0.5% accuracy is achieved for
of Energy Resolution is required.

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Determining Neutrino Mass Hierarchy with Reactor Experiments

  • 1. Determination of mass hierarchy with reactor neutrino experiment Yoshitaro Takaesu KIAS/KNRC In collaborationwith S.F. Ge, N. Okamura and K. Hagiwara arXiv: 1210.8141
  • 2. Introduction is observed. Reactor Experiments can determine the Neutrino Mass Hierarchy . The sensitivity is studied of future Medium Baseline Reactor Experiments for determining the Neutrino Mass Hierarchy
  • 3. PMT Reactor neutrino experiment Reactor Detector Inside Detector Inverse Beta Decay (IBD)
  • 5. How to distinguish Mass Hierarchy ? Mass Hierarchy difference Max: vanish:
  • 6. MH difference in spectrum
  • 7. Advantages of Reactor Experiment • Can determine MH independently from CP phase and matter effects. •Need only smaller detector than other experiments (e.g., LBL, atmospheric). •Free neutrino source with adjustable baseline length
  • 8. Analysis methods for MH determination • Fourier analysis • analysis hep-ph/0612022 J.G. Learned et al. arXiv: 0807.3203 L. Zhan et al. arXiv: 0901.2976 L. Zhan et al. arXiv: 1208.1551 X. Qian et al. arXiv: 1208.1991 E. Ciuffoli et al. hep-ph/030601 S. Choubey et.al. arXiv: 0810.2580 M. Batygov et.al. arXiv: 1011.1646 P. Ghoshal et.al.
  • 9. Fourier Analysis • has sensitivity for small . • Don’t need accurate knowledge of or flux.
  • 10. analysis Data is fitted with the theoretical prediction , assuming NH or IH. Fitting parameters are Penalty term
  • 11. analysis – MH determination MH is determined as the hierarchy which gives smaller . Ex) MH is NH. Sensitivity is estimated by We claim that MH is determined with significane. acc. MH rej. MH
  • 12. Sensitivity for MH determination 36 km (Max MH diff.) Max Sensitivity Typical sensitivity curve as a function of Baseline length L
  • 13. Effect of Baseline Length L should be long enough. L = 30km L = 50km
  • 15. Effect of Energy Resolution a = 0 a = 6% Evergy Resolution affects the sensitivity significantly. How good should the energy resolution be ? 3% ? Not enough for RENO50 class of detector (5kton).
  • 16. Sensitivity for MH determination 20GW 5kton 5yrs Current Resolution NH Optimal L ~ 50 km
  • 17. Systematic part of Resolution 20GW 5kton 5yrs Current Resolution • Sensitivity is reduced by 40%. • Optimal L is shortened by a few km. b = 0 b = 1% a = 2% a = 3%
  • 18. Parameter measurement @ L ~ 50 km Parametermeasurement is not sensitive to the Energy Resolution. ~ 0.5% accuracy can be measured accurately @ L ~ 50 km L = 50km 1% 1% 1%
  • 19. Fluctuation of Sensitivity So far, we have discussed on the sensitivity using the “typical data set”. In the real experiments, event number in each bin, , fluctuates from the “typical event number”, . Then, follows Gaussian distribution. a = 3% a = 2% 0 4 13 20GW 5kton 5yrs 2% level of energy resolution is desired.
  • 21. How to achieve 2% energy resolution ? Increase the photo-electron (p.e.)detected by PMT. p.e.~ 200 pe/MeV ~ 2000 pe/MeV Ex) • Increase PMT coverage • Increase QE of PMT • More transparent LS
  • 22. By Channgen Yang @ NuMass 2013
  • 23. Multi-reactor interference Baseline difference should be < 500m. 0 m 500 m 1 km 1.5 km 2 km arXiv: 1302.0624 L1 L2 L1 |L1 – L2|
  • 24. Multi-reactor interference Because of this effect, DayaBayII has changed its location.
  • 25. Multi-reactor interference RENO 50 km 200 km RENO 1.3 km RENO50 The angle to RENO50 may affect the sensitivity. Reactor site
  • 26. Summary We have discussed the sensitivity of Medium Baseline Reactor Experiments for MH determination. For 20GW 5kton 5yrs exposure, 50km optimal Baseline Length a < 3% b < 1% 0.5% accuracy is achieved for of Energy Resolution is required.