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Yoshitaro Takaesu
U. of Tokyo
Determination of mass hierarchy with
medium baseline reactor neutrino
experiments.
Reactor neutrino experiment
νe
Detector
Reactors
6 × 1023
νe/ 3GW/ 15min
2
PMT
Inside Detector (Inverse Beta Decay)
Reactor neutrino experiment
νe
Detector
Reactors
6 × 1023
νe/ 3GW/ 15min
3
Topics on medium baseline reactor ex.
4
• Optimum baselines
• Energy resolution (Energy scale uncertainty)
• Multiple reactor effects
• Geo neutrino
• Synergy with Long Baseline experiments
• Statistical test of hypothesis
• Fourier analysis vs. chi^2 analysis
• Nuclear recoil effect
etc…
survival prob. (Pee)
5
L ~ 1km
MH independent current reactor experiment
[DayaBay: Neutrino2014]
MH
[Minakata,Nunokawa,Parke,
Funchal: hep-ph/0701151]
Sensitivity to the Mass hierarchy
The typical sensitivity curve of this experiment
6
chi^2 analysis
We define
Naively, the significance of this
rejection is , but…(∆ χ2)min σ
NH
IH
Not appropreate
for the MH determination
c.f.) Qian et.al. arXiv: 1210.3651
Evslin et.al. arXiv: 1305.5150
NH is true: tends to be Positive.
IH is true: tends to be Negative.
IH is rejected
NH is rejected
NH is true case
7
Energy Resolution
8
Effect of Energy resolution
16.5GW 18kton 5yrs (RENO-50)
Current value
NH
δE
E
=
a
E/ MeV
2
+ b2
9
[Ge,Hagiwara,Okamura,
Takaesu:1210.8141]
How to achieve better Energy Resolution?
Increase the photo-electron (p.e.)detected by PMT.
p.e.~ 200 pe/MeV ~ 1000 pe/MeV
Ex)
• Increase PMT coverage
• Increase QE of PMT
• More transparent LS
•More Light yield
10
~ 6% ~ 3%
11
[L.Wen: Neutrino 2014]
Multiple Reactor Effect
12
E. Ciuffoli, J. Evslin, X. Zhang: 1302.0624
Y-F. Li, J. Cao, Y. Wang, L. Zhan: 1303.6733
ΔL = L1 – L2
Reactor1
Multiple Reactor Effect
L1 L2
13
Reactor1 + Reactor2
multi-cores
Multiple Reactor Effect: RENO-50 case
16.5GW
18kton 5yrs
a = 3%, b = 0.5%
δE
E
=
a
√
E
2
+ b2
(∆ χ2)min
All Reactors
50 km
14
250m
[Y.Takaesu: International
workshop on RENO-50]
15
[L.Wen: Neutrino 2014]
Geo-neutrino BG
16
KamLAND: 38.3 +- 10 TNU [1/(10^32 proton*yrs)]
Borexino: 38.8 +- 12 TNU
[Gando et.al 2011, Nature Geosci.]
[Ranucci: Neutorino 2014]
36 GW, 20 kton, 5 years, Eres=3% (JUNO)
arXiv:1006.1113
Summary
Future Reactor neutrino Experiment for MH determination
50km is the optimum baseline length
For > 3-sigma determination within 5 years (15GW 20kton)
3% of Energy resolution is required.
(Energy Scale uncertainty should be controlled carefully
arxiv:0901.2976, 1208.1551, 1308.0591)
Multiple reactor effect significantly affects the sensitivity.
Geo-neutrino may also become concern.
17

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Talk at Neutrino conference, Kyoto

  • 1. Yoshitaro Takaesu U. of Tokyo Determination of mass hierarchy with medium baseline reactor neutrino experiments.
  • 2. Reactor neutrino experiment νe Detector Reactors 6 × 1023 νe/ 3GW/ 15min 2 PMT Inside Detector (Inverse Beta Decay)
  • 4. Topics on medium baseline reactor ex. 4 • Optimum baselines • Energy resolution (Energy scale uncertainty) • Multiple reactor effects • Geo neutrino • Synergy with Long Baseline experiments • Statistical test of hypothesis • Fourier analysis vs. chi^2 analysis • Nuclear recoil effect etc…
  • 5. survival prob. (Pee) 5 L ~ 1km MH independent current reactor experiment [DayaBay: Neutrino2014] MH [Minakata,Nunokawa,Parke, Funchal: hep-ph/0701151]
  • 6. Sensitivity to the Mass hierarchy The typical sensitivity curve of this experiment 6
  • 7. chi^2 analysis We define Naively, the significance of this rejection is , but…(∆ χ2)min σ NH IH Not appropreate for the MH determination c.f.) Qian et.al. arXiv: 1210.3651 Evslin et.al. arXiv: 1305.5150 NH is true: tends to be Positive. IH is true: tends to be Negative. IH is rejected NH is rejected NH is true case 7
  • 9. Effect of Energy resolution 16.5GW 18kton 5yrs (RENO-50) Current value NH δE E = a E/ MeV 2 + b2 9 [Ge,Hagiwara,Okamura, Takaesu:1210.8141]
  • 10. How to achieve better Energy Resolution? Increase the photo-electron (p.e.)detected by PMT. p.e.~ 200 pe/MeV ~ 1000 pe/MeV Ex) • Increase PMT coverage • Increase QE of PMT • More transparent LS •More Light yield 10 ~ 6% ~ 3%
  • 13. E. Ciuffoli, J. Evslin, X. Zhang: 1302.0624 Y-F. Li, J. Cao, Y. Wang, L. Zhan: 1303.6733 ΔL = L1 – L2 Reactor1 Multiple Reactor Effect L1 L2 13 Reactor1 + Reactor2
  • 14. multi-cores Multiple Reactor Effect: RENO-50 case 16.5GW 18kton 5yrs a = 3%, b = 0.5% δE E = a √ E 2 + b2 (∆ χ2)min All Reactors 50 km 14 250m [Y.Takaesu: International workshop on RENO-50]
  • 16. Geo-neutrino BG 16 KamLAND: 38.3 +- 10 TNU [1/(10^32 proton*yrs)] Borexino: 38.8 +- 12 TNU [Gando et.al 2011, Nature Geosci.] [Ranucci: Neutorino 2014] 36 GW, 20 kton, 5 years, Eres=3% (JUNO) arXiv:1006.1113
  • 17. Summary Future Reactor neutrino Experiment for MH determination 50km is the optimum baseline length For > 3-sigma determination within 5 years (15GW 20kton) 3% of Energy resolution is required. (Energy Scale uncertainty should be controlled carefully arxiv:0901.2976, 1208.1551, 1308.0591) Multiple reactor effect significantly affects the sensitivity. Geo-neutrino may also become concern. 17