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

Post on 20-Jan-2016

24 views 0 download

Tags:

description

Parameter Degeneracy in Neutrino Oscillations (and how to solve it?). INT Program 2010; LBL. Hisakazu Minakata Tokyo Metropolitan University. Purpose of this discussion. To complete n Standard Model (SM + n mass + lepton mixing) measurement of CP phase (KM type) d and q 13 is necessary - PowerPoint PPT Presentation

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

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

Hisakazu Minakata

Tokyo Metropolitan University

INT Program 2010; LBL ..

Purpose of this discussion

• To complete Standard Model (SM + mass + lepton mixing) measurement of CP phase (KM type) and13is necessary

• It seems that is not so easy to determine them, in particular

• If any theoretical issues involved we shall try to remove them

• One of them is P degeneracy

July 27, 2010 INT Program LBL

P degeneracy

• P degeneracy is the fact that measurement of oscillation probability P and -bar oscillation probability bar-P at an energy (which would determine 13 and actually do NOT lead to a unique solution of 13 and

• Experts may say that they know everything

July 27, 2010 INT Program LBL

Is this true? To what extent?

An example; Intrinsic degeneracy

July 27, 2010 INT Program LBL

P degeneracy is simplest to see by bi-P plot (HM-H.Nunokawa 01)

Is P degeneracy necessarily two-fold?

July 27, 2010 INT Program LBL

Intrinsic degeneracy; S. Uchinami for PhD thesis

But, the answer is NO !People suspect

the answer is YES because

July 27, 2010 INT Program LBL

ParameterDegeneracy;

definition

P degeneracy

• Let us assume that all the mixing parameters besides 13 and are known

• measurement of oscillation probability Pe and bar- oscillation probability bar-Pe at an energy E (which would determine 13 and do NOT lead to unique solution of 13 and

• Easy to solve mathematically: measurement at E=E1 and E2 (or adding more channel) solves the degeneracyJuly 27, 2010 INT Program LBL

Intrinsic degeneracy (Burguet-C. et al. 01)

P degeneracy (continued)

• the mixing parameters besides 13 and are not known so precisely

• Mass hierarchy is not known, and may not be known either at the time of measurement of CP phase

• More solutions of 13 and

July 27, 2010 INT Program LBL

Sign m231

degeneracy (HM-Nunokawa 01)

23 octant degeneracy (Fogli-Lisi 96)

July 27, 2010 INT Program LBL

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

A well-defined

framework for P

degeneracy

I use Cervera et al. formula for oscillation probabilities

July 27, 2010 INT Program LBL

You can show 2x2x2=8

P degeneracy; Generalized version

• Similar degeneracy occurs in, in addition to (P, PCP),

• T-conjugate (P=Pe, PT=Pe)

• CPT-conjugate (P, PCPT)

• Golden-silver (PT, PS) channels

July 27, 2010 INT Program LBL

Generally, P degeneracy has simpler structure

July 27, 2010 INT Program LBL

P-degenerac

y as an invariance

of P

P-dege. from symmetry of the probability

July 27, 2010 INT Program LBL

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

How to obtain

degeneracy solutions?

An example; intrinsic degeneracy

July 27, 2010 INT Program LBL

An example; intrinsic degeneracy2

July 27, 2010 INT Program LBL

4th-order eq. of s13!

P degeneracy as a re-parametrization invariance

July 27, 2010 INT Program LBL

Degeneracy solutions form network!

July 27, 2010 INT Program LBL

Degeneracy

solutions; how they look like?

13

July 27, 2010 INT Program LBL

II

III

V

July 27, 2010 INT Program LBL

I focus energy dependence; 13

July 27, 2010 INT Program LBL

I focus energy dependence;

July 27, 2010 INT Program LBL

July 27, 2010 INT Program LBL

How to solve P

degeneracy?

July 27, 2010 INT Program LBL

Varying E at long enough baseline

• 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}GFNea=sqrt{2}GFNe

atmosphericatmospheric

solarsolar

the best way for everything if perfect event reconstruction with 2-3 oscillation periods spanned

the best way for everything if perfect event reconstruction with 2-3 oscillation periods spanned

July 27, 2010 INT Program LBL

Project X: Off-axis NOVA --> VLBL multi-OM type approachProject X: Off-axis NOVA --> VLBL multi-OM type approach

July 27, 2010 INT Program LBL

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

Background at low E for HE beam

Fanny Dufour@3rd T2KK WSFanny Dufour@3rd T2KK WS

July 27, 2010 INT Program LBL

Varying L

• 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)

If a=sqrt{2}GFNe is small If a=sqrt{2}GFNe is small

July 27, 2010 INT Program LBL

Two detector

method is powerful

July 27, 2010 INT Program LBL

Kamioka-Korea 2 detector setting

Why don’t you bring one of the 2 tanks to Korea? (@EPP2010)

Why don’t you bring one of the 2 tanks to Korea? (@EPP2010)

July 27, 2010 INT Program LBL

Original idea: sensitive because dynamism in 2nd oscillation maximum

July 27, 2010 INT Program LBL

Spectral information solves intrinsic degeneracy

from 1000 page Ishitsuka file

from 1000 page Ishitsuka file

SK momentum resolution ~30 MeV at 1 GeVSK momentum resolution ~30 MeV at 1 GeV

T2KT2K T2KKT2KK

2 detector method powerful!2 detector method powerful!

Ishitsuka-Kajita-HM-Nunokawa 05

July 27, 2010 INT Program LBL

Two-detector setting is powerful

• With the same input parameter and Korean detector of 0.54 Mt the sign-m2 degeneracy is NOT completely resolved

T2KKT2KK Korea onlyKorea only

July 27, 2010 INT Program LBL

T2KK vs. T2K II Comparison T2KK vs. T2K II Comparison Total mass of the detectors = 0.54 Mton fid. mass4 years neutrino beam + 4 years anti-neutrino beam

Total mass of the detectors = 0.54 Mton fid. mass4 years neutrino beam + 4 years anti-neutrino beam

3 (thick)3 (thick) 2 (thin)2 (thin)

Mass hierarchyMass hierarchy CP violation (sin≠0)CP violation (sin≠0)

hep-ph/0504026

T2K

T2KK

July 27, 2010 INT Program LBL

Relative cross section error does matter

• Identical 2 detector setting robust to larger systematic error • It gives conservative lower bounds on sensitivity estimate

of mass hierarchy and CP

Barger et al. 07

Barger et al. 07

T2K IIT2K II

T2KKT2KK

July 27, 2010 INT Program LBL

T2KK can solve 23 degeneracy in situ

T2K-II + phase II reactorT2KK=0 assumed

sin

2 2

13

sin2 23

sin

2 2

13

> 32~3

T2KK 2(rough)

T2KK has better sensitivityat sin2 213 < 0.06~0.07 .

hep-ph/0601258

July 27, 2010 INT Program LBL

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-m2 and 23 octant degeneracies are robust against spectrum analysis

• Some ideas are discussed on how to solve P degeneracy

Another example; sign-m2 degeneracy

July 27, 2010 INT Program LBL

Another example; sign-m2 degeneracy2

July 27, 2010 INT Program LBL

Another example; sign-m2 degeneracy3

July 27, 2010 INT Program LBL

July 27, 2010 INT Program LBL

Neutrino factory

July 27, 2010 INT Program LBL

Nufact