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Toward precision study of atmospheric neutrino oscillations
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Toward precision study of atmospheric neutrino oscillations
Toward precision study of atmospheric neutrino oscillations
Nuclear Physics B (Proc. Suppl.) 159 (2006) 15–20 www.elsevierphysics.com 0920-5632/$ – see front matter © 2006 Elsevier B.V. All rights reserved. do...
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Nuclear Physics B (Proc. Suppl.) 159 (2006) 15–20 www.elsevierphysics.com
0920-5632/$ – see front matter © 2006 Elsevier B.V. All rights reserved. doi:10.1016/j.nuclphysbps.2006.08.022
16
2
(inverted-normal)
T. Kajita / Nuclear Physics B (Proc. Suppl.) 159 (2006) 15–20
40 35 30 25 20 15 10 5 0
0.5
0.5 90% C.L. 99% C.L.
0.3 0.2 0.1 0
90% C.L. 99% C.L.
0.4 sin2θ13
sin2θ13
0.4
0.3 0.2 0.1
0
0.2
0.4
0.6 2
sin θ23
0.8
1
0
0
0.2
0.4
0.6
sin2θ23
0.8
1
0
0.02 0.04 0.06 0.08 0
0.02 0.04 0.06 0.08 0
13
13
sin2
sin2
0.02 0.04 0.06 0.08
sin 2
13
T. Kajita / Nuclear Physics B (Proc. Suppl.) 159 (2006) 15–20
17
18
T. Kajita / Nuclear Physics B (Proc. Suppl.) 159 (2006) 15–20
1
1
2
2 flavor (sin 2θ23=0.96)
0.5
1
w/o 1-2 parameters w/ 1-2 parameters
8 7
-0.5
0 cosθ
0.5
1
2min
0 cosθ
6 5
sin θ23 = 0.4 2 sin θ23 = 0.5 2 sin θ23 = 0.6
1
2
2 flavor (sin 2θ23=0.96)
-0.5
0 cosθ
0.5
1
4
6 5
3
4 3
2
2 1
1
0 0.3
2
0.95 -1
2
-0.5
0.95 -1
χ -χ
2 min
9
2
10
-
0.95 -1
Sub-GeV
1.05
/ (Nμ / Ne)
1.05
osc
1.05
2
sin θ23 = 0.4 2 sin θ23 = 0.5 2 sin θ23 = 0.6
1.1
(Nμ / Ne)
2
sin θ23 = 0.4 2 sin θ23 = 0.5 2 sin θ23 = 0.6
Sub-GeV μ-like
2flavor full-mixing
1.1
Sub-GeV e-like Nμosc / Nμ2flavor full-mixing
Neosc / Ne2flavor full-mixing
1.1
0.4
0.5
0.6
0.7 sin2
23
0
0.3
0.4
0.5
0.6
0.7 2 sin θ23
19
T. Kajita / Nuclear Physics B (Proc. Suppl.) 159 (2006) 15–20 1.2 1.15
Ne/Ne0
1.1 1.05 1 0.95 0.9 -1 -0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 1 1.2
cosΘ
1.15
Ne/Ne0
1.1 1.05 1 0.95 0.9 -1 -0.8 -0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8 1 cosΘ
20 0.18
0.16
0.16
0.14
0.14
0.12
0.12 sin θ13
0.18
0.1
2
sin θ13
2
T. Kajita / Nuclear Physics B (Proc. Suppl.) 159 (2006) 15–20
0.08
0.1
0.08
0.06
0.06
0.04
0.04
0.02 0
0.02 0
50
100 150 200 250 300 350 CP phase
0
0
50
100 150 200 250 300 350 CP phase
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