The Very Long BaselineNeutrino Oscillations

Experiment

Presented toFCP05 Neutrino Session

byTom Kirk

Brookhaven National Laboratory

Nashville, TNMay 23, 2005

likelihood cut (100%signal retained)

Background from

CP+45o

Signal 700 evBkgs 2005 (1878 from +others) ( 127 from

e)

Signal

e backgroundo

CP+45

likelihood cut (~50%signal retained)

Effect of cut on likelihood

Erec Erec

Preliminary Preliminary

Signal/Background

Signal 321 evBkgs 169 (112 from +others) ( 57 from

e)

e CC for signal ; all e NC , e beam for background

Traditional Analysis

Chiaki Yanagisawa – SBUFebruary 28, 2005

Maximum Likelihood Method

Effect of cut on likelihoodCP +45o

Background

All

oCP-45

Erec

Erec

Preliminary Preliminary

S/B

Erec

Erec

Erec Erec

e CC for signal ; all e NC , e beam for backgrounds

100% 50%

40%

50%100%

40%

Chiaki Yanagisawa – SBUFebruary 28, 2005

Maximum Likelihood Method

Effect of cut on likelihood

CP +135o

Background

All

oCP-135

Erec

Erec

Preliminary Preliminary

S/B

Erec

Erec

Erec Erec

100% 100%50% 50%

40% 40%

e CC for signal ; all e NC , e beam for backgrounds

Chiaki Yanagisawa – SBUFebruary 28, 2005

Maximum Likelihood Method

T. Kirk May 3, 2005

Scientific Reach of Future Neutrino Oscillations Exps. Parameter T2K T2K2 Reactor Noa Noa2 VLBNO.

m322 4 4-

221sin2(223) 1.50.4- 0.4%0.20.5sin2(213) a >0.02 >0.01 >0.01 >0.01 >0.01 >0.01

m212 sin(212) b - - - - - 12 %

sign of (m322) c - - - possible yes yes

measure CP d

- ~20 - - ~2013N-decay gain x1 x20 - - - x8

Detector (Ktons) 50 1000 20 30 30+50 400 Beam Power (MW) 0.74 4.0 14000 0.4 2.0 1.5Baseline (km) 295 e 295 e 1 810 e 810 e >2500

Detector Cost ($M) exists ~1000 20 165 +200 400Beam Cost ($M) exists 500 exists 50 1000 400Ops. Cost ($M/10 yrs) 500 700 50 500 600 150/500 f

a detection of e , upper limit on or determination of sin2(213)b detection of e appearance, even if sin2(213) = 0; determine 23 angle ambiguity

c detection of the matter enhancement effect over the entire CP angle ranged measure the CP-violation phase CP in the lepton sector; Noa2 depends on T2K2 e beam is ‘off-axis’ from 0-degree target direction; f with/without RHIC operations

Both results needed toresolve ambiguities!

Best Bets

T. Kirk May 3, 2005

Comments on Neutrino Oscillations Experiments

• All parameters of neutrino oscillations can be measured in one experiment- the Very Long Baseline Neutrino Oscillation (VLBNO) at >2000 km- Use of a broadband Super Neutrino Beam at very long distances is the key- worries about 0 channel background have been successfully addressed- the VLBNO cost is comparable to or lower than less comprehensive methods

• The massive LBNO detector empowers additional forefront physics topics- a powerful next-generation Nucleon Decay search- supernova and relic neutrino searches are also possible- a deep underground detector is required for these searches – NSF’s DUSEL!

• The CP-violation parameter CP is the most difficult parameter to determine

- matter effects interact with CP-violation effects- the CP-violation phase CP has distinct effects over the full 360º range

• Off-axis beam method requires multiple distances and detectors- all experiments will require of order 10 Snomass years of running- each proposed detector will achieve good statistics for most parameters

• All measured oscillation parameters will be limited to ~1% precision by

systematic errors except sin2(223)