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Neutrino Oscillation Neutrino Oscillation Physics at a Neutrino Physics at a Neutrino Factory Factory Rob Edgecock RAL/CERN-AB Rob Edgecock RAL/CERN-AB

Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

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Page 1: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

Neutrino Oscillation Physics Neutrino Oscillation Physics at a Neutrino Factoryat a Neutrino Factory

Rob Edgecock RAL/CERN-ABRob Edgecock RAL/CERN-AB

Page 2: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

OutlineOutline

• Neutrino Factory accelerator

• “ “ detector

• Reminder of phenomenology

• Atmospheric parameters

• Sign of m223

• 13 and

• Degeneracies

• Conclusions

Page 3: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

Neutrino Factory AcceleratorNeutrino Factory Accelerator

Important parameters:Important parameters:

Muon energyMuon energy = 20 or 50 GeV Intensity= 20 or 50 GeV Intensity= 10= 102121 muon decays/year

Page 4: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

Neutrino Factory AcceleratorNeutrino Factory Accelerator

Advantages of a Neutrino Factory:Advantages of a Neutrino Factory:

• Muon decay:Muon decay:

• Pure beam of equal numbers of Pure beam of equal numbers of and and ee

• Can look for:Can look for:

• First requires “simple” detectorFirst requires “simple” detector

• High intensity (especially High intensity (especially ee))

• Precisely known intensity and compositionPrecisely known intensity and composition

• Precisely known energy spectraPrecisely known energy spectra

ee

e

e

Page 5: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

Neutrino Factory DetectorsNeutrino Factory Detectors

Magnetised iron calorimeter

20m long 10m radius 40kT

Events in 1 year:Events in 1 year:

1.0x1052.4x1061.2x1063500km

1.1x1055.9x1073.5x107732km

Signalsin213=0.01

Baseline CC CCe

Page 6: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

Neutrino Factory DetectorsNeutrino Factory Detectors

For For ee or or identificationidentification

Liquid argon TPC, etcLiquid argon TPC, etc

e-id up to 5 GeVe-id up to 5 GeV

Page 7: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

Neutrino Factory DetectorsNeutrino Factory Detectors

LANNDDLANNDD

- 70kT70kT

- 61m x 44m61m x 44m

- up to 1Tup to 1T

- 18.5MA18.5MA

- coil: 71kTcoil: 71kT

- yoke: 677kTyoke: 677kT

Page 8: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

PhenomenologyPhenomenology

P(e) to lowest order in the matter effect:

where

To first order, ignoring matter effect and CP:To first order, ignoring matter effect and CP:

Page 9: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

PhenomenologyPhenomenology

20 GeV 20 GeV NF at NF at

3500km3500km

Page 10: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

PhysicsPhysics

• Precise measurement of atmospheric parametersPrecise measurement of atmospheric parameters

• Sign of Sign of mm222323

• 1313

• Solar parametersSolar parameters

• ee

Page 11: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

PhysicsPhysics

From Bueno et al Nucl Phys B589 (2000) 577

Characterise as: - electrons - right-sign muons - wrong-sign muons - others

Plots are for: E = 30 GeV L = 7400 km 1020

decays 10 kT detector

Page 12: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

Atmospheric ParametersAtmospheric Parameters

Fitting to plots, after kinematic cutsFitting to plots, after kinematic cuts

No background Perfect resoln

Background and resoln

Resolutions achieved:Resolutions achieved: 1% in1% in10% in10% in

223m

232sin

Page 13: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

Sign of Sign of mm22

Only Only ee have CC interactions with have CC interactions with electrons in matterelectrons in matter

eeffective massffective mass

Modifies transition probability:Modifies transition probability:

EnGA eF22

E

LmP e 4

sinsin2sin2232

232

132

E

mP m

e 4

27.1sinsin2sin

2232

232

132

wherewhere

21313

213

2

132

2cos2sin

2sin2sin

xm

21313

2 2cos2sin xL

223m

Ax

Page 14: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

Sign of Sign of mm22

Integrated

Energy bins

2x102x102020 muon decays SMA muon decays SMA parametersparameters

Page 15: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

………….in case where one/both solar parameters small!.in case where one/both solar parameters small!

• Determined from a fit to energy spectraDetermined from a fit to energy spectra

• This time, wrong sign muons dominateThis time, wrong sign muons dominate

No background Background

90% CL90% CL

732km

3500km

7332km

Page 16: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

• Probably the most important parameterProbably the most important parameter

• The good newsThe good news

23131223131213 sinsinsinsin2sin2sin2sin2

1~)()( cPP ee

Page 17: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

• The bad news…….matter effect…….The bad news…….matter effect…….

Page 18: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

• ………….and correlations……...and correlations……..

Page 19: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

• ………….and degeneracies.and degeneracies

13=8o, =-90o, 0o, 90o, 180o

Page 20: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

DegeneraciesDegeneracies

Degeneracy: 2 or more parameter sets fit the same data

Three types, all of which can effect measurement of & 13:

1313 ',',

223

223 mm

4,

2 232323

(1)

(2)

(3)

They limit the accuracy of the parameter measurement

,',' 1313 ee

PP

,',' 1313 ee

PP (1)

Page 21: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

DegeneraciesDegeneracies

E

Lm

E

Lm

44cot2sincotcos'

,'212

213

12231313

13

large

NB depends on L/E possible solutions

• Two baselines and E-dependence at NF

• NF + SB combination

• Two off-axis detectors

• e as well as e

Page 22: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

13=8o, =-90o, 0o, 90o, 180o

DegeneraciesDegeneracies

NuFact at 2810km + SB at 130KM

NuFact at 732km + SB at 130KM

large

small

Page 23: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

Silver ChannelSilver Channel

Golden:Golden:

Silver:Silver:

e

e

40kT magnetised iron at 3000km40kT magnetised iron at 3000km

4kT emulsion at 732km4kT emulsion at 732km

Parameters:Parameters: = 90= 90oo

= 5= 5oo

Lines of Lines of equivalent equivalent probabilityprobability

Solve ambiguities for all Solve ambiguities for all and and 11oo

Page 24: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

SensitivitiesSensitivities

Intermediate and long baseline best Intermediate and long baseline best Resolution: Resolution: ~0.1~0.1o o for for 1313

~20~20oo for for

Page 25: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

ComparisonsComparisons

90% CL

JHF-HK = 4MW, 1000kT; 6 years , 2 years

NuFact-II = 5.3 x1020 useful /yr, 50kT; 4 years

Page 26: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

ComparisonsComparisons

Page 27: Neutrino Oscillation Physics at a Neutrino Factory Rob Edgecock RAL/CERN-AB

ConclusionsConclusions

• Neutrino Factory is the ultimate long baseline facilityNeutrino Factory is the ultimate long baseline facility

• In one year……In one year……

atmospheric parameters:atmospheric parameters:

sign of :sign of : 400400sinsin2213 13 :: 4 x 104 x 10-4 -4 at 90% CLat 90% CL ::

9090oo to <2 x 10 to <2 x 10-5 -5

• The only serious competition from combinations of othersThe only serious competition from combinations of others

• Can also do a wide range of other physics:Can also do a wide range of other physics:- short baseline, high intensity neutrino physics- short baseline, high intensity neutrino physics - -

high intensity slow muon physicshigh intensity slow muon physics - test - test bed for other projects: bed for other projects: muon collidermuon collider

proton machines proton machines

1% in 1% in 10% in10% in

223m

232sin

223m