250 likes | 257 Views
Overview of JHF-SK experiment measuring neutrino oscillation parameters with various beam options. Detailed construction, operation, and physics sensitivities discussed.
E N D
Neutrino Oscillation Experiment betweenJHF – Super-Kamiokande Yoshihisa OBAYASHI (Kamioka Observatory, ICRR) Yoshihisa OBAYASHI, Oct. 2000 @Seoul
JHF Neutrino Working Group Y. Itow, Y. Obayashi, Y. Totsuka (ICRR) Y. Hayato, H. Ishino, T. Kobayashi, K. Nakamura, M. Sakuda (KEK) T. Hara (Kobe) T. Nakaya, K. Nishikawa (Kyoto) T. Hasegawa, K. Ishihara, A. Suzuki (Tohoku) A. Konaka (TRIUMF) http://neutrino.kek.jp/jhfnu Yoshihisa OBAYASHI, Oct. 2000 @Seoul
Overview of JHF – SK • nm→nx disappearance: • Precise measurement of oscillation parameters: d(Dm232)~ 2x10-4eV2, d(sin22qmx)~ 1% • nm→ne appearance: • Explore down to sin22qme ~ 5x10-3 (sin22q13 ~ 1x10-2) • Oscillation Max @ En=0.5~1.2GeV • P=sin22q・sin2(1.27Dm232L/En) • Dm232=2~5x10-3eV2, L=295km Yoshihisa OBAYASHI, Oct. 2000 @Seoul
JHF (Japan Hadrons Facility) JAERI @ Tokai-mura Construction: 2001 ~ 2006 N 50GeV PS 3GeV PS Neutrino Beam Line 600MeV Linac Front Detector(s) To Super-Kamiokande 1021p.o.t./1year(130day) Yoshihisa OBAYASHI, Oct. 2000 @Seoul
Far Detector • Super-Kamiokande @ Kamioka • Operation Start: 1996 • 295 km from JAERI • 50.0kt Pure Water in the tank • 22.5kt Fiducial Volume as a neutrino target • Energy measurement by total amount of Cherenkov light • e-m separation is performed by ring pattern likelihood Yoshihisa OBAYASHI, Oct. 2000 @Seoul
Neutrino Beam at JHF • Three Possible options: • Wide Band Beam (WBB) • 2 horns, almost same as K2K • Narrow Band Beam (NBB) • Horn(s) + Bending • Off Axis Beam • Another option of NBB • Present Strategy: • First 1(~2) year: • High Statistics Run with WBB • Pin down Dm2 • Next 5 years: • Precise Analysis with (one of) NBB • Measurement of q23,q13 Yoshihisa OBAYASHI, Oct. 2000 @Seoul
Wide Band Beam • High Intensity • Wide sensitivity in Dm2 • Established technique • Backgrounds from HE tail • Spectra diff. btw near&far • Systematic error • Needs Heavy shielding • decay pipe must be short • ~ 4200 nm int./22.5kt/yr • (ne:0.8%) Yoshihisa OBAYASHI, Oct. 2000 @Seoul
Narrow Band Beam • Less systematic error • Less BG from HE tail • Easy to tune En • Less shielding • Low intensity • ~ 830 nm int./22.5kt/yr • (ne:0.3%@peak) Yoshihisa OBAYASHI, Oct. 2000 @Seoul
Off Axis Beam: Another option of NBB q • WBB with intentionally misaligned from detector axis En 10 20 Ep • Quasi Monochromatic Beam Yoshihisa OBAYASHI, Oct. 2000 @Seoul
Off Axis Beam • More intense than NBB • More HE tail than NBB • Hard to tune En • Needs heavy shielding • Not established technique • Beam monitor • Near/Far ratio, … • ~ 2200 nm int./22.5kt/yr • (ne:0.2%@peak) Yoshihisa OBAYASHI, Oct. 2000 @Seoul
Physics Sensitivity Yoshihisa OBAYASHI, Oct. 2000 @Seoul
nm Disappearance • Ratio after BG subtraction: • Fit with 1-sin22q・sin2(1.27Dm2L/E) Yoshihisa OBAYASHI, Oct. 2000 @Seoul
nm Disappearance • Possible systematic errors: • inelastic cross section: 20% • Spectrum @FD: 4%・E • Spectrum diff.(Near/Far): 10% • Energy measurement: 3% • d(sin22q23)~0.01 in 5 years • d(Dm223) ~ 2x10-4eV2 Yoshihisa OBAYASHI, Oct. 2000 @Seoul
nm → ne Appearance m32 Dm2atm m22 Dm2sol m12 • Three flavor oscillation framework: • Dm212 <<Dm223~Dm213≡Dm2 • Dm223= Dm2atm>10-3eV2 • Dm212= Dm2sol<10-4eV2 • Oscillation Probability P : • Present limit: sin22qme < 5x10-2 • sin22qme= sin22q13・ sin2q23 • sin22q13 <0.1(CHOOZ) • sin2q23 ~ 0.5 (Atmospheric n) • Goal: sin22qme ~ 5x10-3 Yoshihisa OBAYASHI, Oct. 2000 @Seoul
Signal & Backgrounds • Signal: ne C.C. interaction • BG 1: nm C.C. interaction • Single fuzzy ring • Cherenkov angle ~ 42deg. ne e+- shower • Sharp ring edge • Cherenkov angle < 42deg. nm m • easy to reject Yoshihisa OBAYASHI, Oct. 2000 @Seoul
Backgrounds (continued) • BG 2: N.C. p0 production n n 2 showers p0→2g • 2 fuzzy rings → hard to separate • Not reproduce En • need effort to reject Yoshihisa OBAYASHI, Oct. 2000 @Seoul
ne Selection by SK Official Cuts • S/N ~ 1/3 (@sin22qme=0.05) • Main Background come from p0 sin22qme=0.05, Dm2=3x10-3eV2 Yoshihisa OBAYASHI, Oct. 2000 @Seoul
p0 rejection • Force to find 2ndg ring • Cut with follow quantities: • Shower direction w.r.t. n (cosqne) • Energy fraction of second g R(g2)=E(g2)/(E(g1)+E(g2)) • Pattern likelihood difference • Invariant mass of 2 g Yoshihisa OBAYASHI, Oct. 2000 @Seoul
p0 cut efficiency PRELIMINARY WBB 1year NBB 1year Off Axis 1year sin22qme=0.05, Dm2=3x10-3eV2 Yoshihisa OBAYASHI, Oct. 2000 @Seoul
nm → ne Oscillation Sensitivity • sin22qme~5(3)x10-3@90%CL by 5year run of NBB(off axis beam) PRELIMINARY 10% systematic in BG rate is considered Yoshihisa OBAYASHI, Oct. 2000 @Seoul
nm → ne Oscillation Sensitivity 10% systematic in BG rate is considered PRELIMINARY Yoshihisa OBAYASHI, Oct. 2000 @Seoul
Comparison to MINOS • JHF neutrino is more sensitive especially in Atmospheric Dm2 region MINOS Ph2he,me,le 2yr exposure (hep-ph0005012) Yoshihisa OBAYASHI, Oct. 2000 @Seoul
nm→ nt? nsterile? • NC p0 production: • n + N → n + N + p0 • In the case of nm→ nsterile oscillation, • Number of p0 also decrease • nt ⇔ nsterile discrimination Yoshihisa OBAYASHI, Oct. 2000 @Seoul
Summary • JHF neutrino experiment • Expected to start in 2006 • Far Detector: Super-K • By 5 years of run: • nm disappearance search • d(Dm223) ~ 2x10-4eV2 • d(sin22q23) ~ 1% • ne appearance search • sin22q13 ~ 10-2 @90%CL • nm⇔nt or nm⇔nsterile • Can be tested Yoshihisa OBAYASHI, Oct. 2000 @Seoul
Test of CP Violation • If sin22q13 ~ 0.01, sin22q12,Dm212~LMA • 1MW(2deg. off axis) → SK : • 2 nm → ne / year • Too few to see CP • 4MW → Mton : • 300 nm → ne / year • 100 nm → ne / year • 1year n + 3year n • 600 total events with asym: 150xsind • d=30deg.(3s), 12deg.(90% CL) Yoshihisa OBAYASHI, Oct. 2000 @Seoul