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Parameter Degeneracy in Neutrino Oscillations (and how to solve it?)

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Presentation on theme: "Parameter Degeneracy in Neutrino Oscillations (and how to solve it?)"— Presentation transcript:

1 Parameter Degeneracy in Neutrino Oscillations (and how to solve it?)
INT Program 2010; LBL .. Hisakazu Minakata Tokyo Metropolitan University

2 Purpose of this discussion
To complete n Standard Model (SM + n mass + lepton mixing) measurement of CP phase (KM type) d and q13 is necessary It seems that is not so easy to determine them, in particular d If any theoretical issues involved we shall try to remove them One of them is P degeneracy July 27, 2010 INT Program LBL

3 P degeneracy P degeneracy is the fact that measurement of n oscillation probability P and n-bar oscillation probability bar-P at an energy (which would determine q13 and d) actually do NOT lead to a unique solution of q13 and d Experts may say that they know everything Is this true? To what extent? July 27, 2010 INT Program LBL

4 An example; Intrinsic degeneracy
P degeneracy is simplest to see by bi-P plot (HM-H.Nunokawa 01) July 27, 2010 INT Program LBL

5 Is P degeneracy necessarily two-fold?
But, the answer is NO ! People suspect the answer is YES because Intrinsic degeneracy; S. Uchinami for PhD thesis July 27, 2010 INT Program LBL

6 Parameter Degeneracy; definition July 27, 2010 INT Program LBL

7 P degeneracy Let us assume that all the mixing parameters besides q13 and d are known measurement of n oscillation probability Pme and bar-n oscillation probability bar-Pme at an energy E (which would determine q13 and d) do NOT lead to unique solution of q13 and d Easy to solve mathematically: measurement at E=E1 and E2 (or adding more channel) solves the degeneracy Intrinsic degeneracy (Burguet-C. et al. 01) July 27, 2010 INT Program LBL

8 P degeneracy (continued)
the mixing parameters besides q13 and d are not known so precisely Mass hierarchy is not known, and may not be known either at the time of measurement of CP phase d More solutions of q13 and d: Sign Dm231 degeneracy (HM-Nunokawa 01) q23 octant degeneracy (Fogli-Lisi 96) July 27, 2010 INT Program LBL

9 P degeneracy is doubled by unknown mass hierarchy
You can draw two ellipses from a point in P-Pbar space Intrinsic degeneracy Doubled by the unknown sign of m2 4-fold degeneracy July 27, 2010 INT Program LBL

10 A well-defined framework for P degeneracy
July 27, 2010 INT Program LBL

11 I use Cervera et al. formula for n oscillation probabilities
You can show 2x2x2=8 July 27, 2010 INT Program LBL

12 P degeneracy; Generalized version
Similar degeneracy occurs in, in addition to (P, PCP), T-conjugate (P=Pme, PT=Pem) CPT-conjugate (P, PCPT) Golden-silver (PT, PS) channels Generally, P degeneracy has simpler structure July 27, 2010 INT Program LBL

13 P-degeneracy as an invariance of P
July 27, 2010 INT Program LBL

14 P-dege. from symmetry of the probability
are invariant under transf. PT and PS are also invariant under the same transformation (1) P degeneracy obvious (2) Form of the degeneracy solutions are determined by the symmetry July 27, 2010 INT Program LBL

15 How to obtain degeneracy solutions?
July 27, 2010 INT Program LBL

16 An example; intrinsic degeneracy
July 27, 2010 INT Program LBL

17 An example; intrinsic degeneracy2
4th-order eq. of s13! July 27, 2010 INT Program LBL

18 P degeneracy as a re-parametrization invariance
Degeneracy solutions form network! July 27, 2010 INT Program LBL

19 Degeneracy solutions; how they look like?
July 27, 2010 INT Program LBL

20 q13 II III V July 27, 2010 INT Program LBL

21 d July 27, 2010 INT Program LBL

22 I focus energy dependence; q13
July 27, 2010 INT Program LBL

23 I focus energy dependence; d
July 27, 2010 INT Program LBL

24 How to solve P degeneracy?
July 27, 2010 INT Program LBL

25 Varying E at long enough baseline
atmospheric solar Vacuum effect comes in with L/E Matter effect comes in with aL Varying E implies to change relative importance between vacuum and matter effects (varying L not) powerful for mass hierarchy a=sqrt{2}GFNe the best way for everything if perfect event reconstruction with 2-3 oscillation periods spanned July 27, 2010 INT Program LBL

26 Project X: Off-axis NOVA --> VLBL multi-OM type approach
July 27, 2010 INT Program LBL

27 Practical issues in VLBL approach
In water background at low energies for high energy  beam highly nontrivial -> see next page How reliable is the event reconstruction & background rejection algorithm ? Energy resolution Alternative way; ~100 kt scale Liquid Ar detector => feasible when? July 27, 2010 INT Program LBL

28 Background at low E for HE  beam
Fanny T2KK WS July 27, 2010 INT Program LBL

29 Varying L If a=sqrt{2}GFNe is small Matter effect comes in with (aL/2) = ~0.27 and relatively small even at L ~ 1000 km By varying L, the trigonometric nature of the oscillations manifests itself (spectrum analysis helps) Good for CPV search (w. spectrum analysis) July 27, 2010 INT Program LBL

30 Two detector method is powerful
July 27, 2010 INT Program LBL

31 Kamioka-Korea 2 detector setting
Why don’t you bring one of the 2 tanks to Korea? July 27, 2010 INT Program LBL

32 Original idea: sensitive because dynamism in 2nd oscillation maximum
July 27, 2010 INT Program LBL

33 Spectral information solves intrinsic degeneracy
from 1000 page Ishitsuka file T2K T2KK 2 detector method powerful! SK momentum resolution ~30 MeV at 1 GeV Ishitsuka-Kajita-HM-Nunokawa 05 July 27, 2010 INT Program LBL

34 Two-detector setting is powerful
T2KK Korea only With the same input parameter and Korean detector of 0.54 Mt the sign-m2 degeneracy is NOT completely resolved July 27, 2010 INT Program LBL

35 T2KK vs. T2K II Comparison T2KK T2K
hep-ph/ Total mass of the detectors = Mton fid. mass 4 years neutrino beam + 4 years anti-neutrino beam T2KK Mass hierarchy CP violation (sind≠0) T2K 3 s (thick) 2 s (thin) July 27, 2010 INT Program LBL

36 Relative cross section error does matter
T2KK Barger et al. 07 T2K II Identical 2 detector setting robust to larger systematic error It gives conservative lower bounds on sensitivity estimate of mass hierarchy and CP July 27, 2010 INT Program LBL

37 T2KK can solve q23 degeneracy in situ
d=0 assumed T2KK T2K-II + phase II reactor sin2 2q13 T2KK 2s (rough) > 3s 2~3s sin2 2q13 hep-ph/ T2KK has better sensitivity at sin2 2q13 < 0.06~0.07 . July 27, 2010 INT Program LBL sin2 q23

38 Conclusion Global overview of P degeneracy is given
In some cases, P degeneracy can be understood by the symmetry argument More generically it is an invariance under discrete mapping of mixing parameters whose explicit form should be obtained by solving equations Sign-Dm2 and q23 octant degeneracies are robust against spectrum analysis Some ideas are discussed on how to solve P degeneracy July 27, 2010 INT Program LBL

39 Another example; sign-Dm2 degeneracy
July 27, 2010 INT Program LBL

40 Another example; sign-Dm2 degeneracy2
July 27, 2010 INT Program LBL

41 Another example; sign-Dm2 degeneracy3
July 27, 2010 INT Program LBL

42 Neutrino factory July 27, 2010 INT Program LBL

43 Nufact July 27, 2010 INT Program LBL


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