1 / 49

Superbeam long baseline experiments

100830 Neutrino Summer School @Tokai. Superbeam long baseline experiments. Takashi Kobayashi KEK. n e. n m. n t. 3 flavor mixing of neutrino. Flavor eigenstates. Mass eigenstates. m 1. Unitary matrix. m 2. m 3. 6 parameters q 12 , q 23 , q 13 , d

walt
Download Presentation

Superbeam long baseline experiments

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. 100830 Neutrino Summer School @Tokai Superbeam long baseline experiments Takashi Kobayashi KEK

  2. ne nm nt 3 flavor mixing of neutrino Flavor eigenstates Mass eigenstates m1 Unitary matrix m2 m3 6 parameters q12, q23, q13, d Dm122, Dm232, Dm132 Dmij=mi2-mj2 2

  3. Known and Unknowns • Solar & Reactor • q12~33o • Dm122~0.00008eV2 • Atomspheric + Acc • q23~45o • Dm232~0.0025eV2 • Unknown! • q13<10o • (Dm132~Dm232)? • d ??? ne?? n3 n2 OR n1 Mass hierarchy

  4. Unknown properties of neutrino q13? Last unknown mixing angle T2K, NOvA, Double Chooz, RENO, DayaBay CP invariance ? Mass hierarchy ? Absolute mass Tritium beta decay, double-beta Majorana or Dirac? Double-beta Next generation accelerator based expriemtns 4

  5. Toward unraveling the mystery of matter dominated universe

  6. Sakharov’s 3 conditions To generate Baryon asymmetry in the unverse • There is a fundamental process that violates Baryon number • C and CP invariance is violated at the same time • There is a deviation from thermal equilibrium acting on B violating process

  7. Toward origin of matter dominated universe • Quark sector CPV is found to be not sufficient for reproducing present baryon content • Scenario for baryogenesis through lepton CP violation: Leptogenesis • CPV in lepton sector is responsible for B genesis • CPV in neutrino oscillation could provide a key to unravel mystery of origin of matter

  8. Let’s find CPV in lepton sector Let’s design an experiment to search for CPV in lepton sector • I give you • 1000億円 or • 1.2 Billion USD • 755M GBP • 55 Billion INR • 1,401 Billion Won • 2,130 Billion Peso • 7.9 Billion 元 • 918 Million Euro • 35 Billion Ruble • 1.2 Billion CHF If you find any good idea, let’s write a paper! One condition: Within 10years

  9. How? …. : Q1 • Do we really need oscillation phenomena to probe CPV?? • Can’t we attack CPV in an experiment which fit in an experimental hall like such as Kaon CPV or B CPV • Why??

  10. Measuring CPV in quark sector • Through loop diagram • Amplitude ∝ (mu,c,t/MW)2 • Please calculate • Since quark is heavy (especially top), this process becomes measureable VCKM u,c,t VCKM s,b W W W u,c,t d s,b VCKM VCKM VCKM u,c,t VCKM

  11. How about lepton sector? g Example: meg • Amplitude ∝ (mn/MW)2 • Standard model process STRONGLY suppressed • Thus, good field to search for physics beyond standard model W ne,nm,nt m e VMNS VMNS

  12. Oscillation n1 nl n2 nl’ n3

  13. Oscillation (cont) If Ei are same for all mass eigenstates E Ei’s are same, no oscillation, in other word, Ei’s are different, we can probe mixing matrix through oscillation Difference of Ei, ie, phase advance difference is essential For Dm2~10-3eV2

  14. B.Kyser, in this SS

  15. Q2: What oscillation process is best? • OK, now, we somehow understand we need (long baseline) oscillation phenomena to probe matrix elements and attack CPV. • What type of oscillation is best? • Fundamental physics reason • Experimental feasibility

  16. Disappearance ? Appearance? Oscillation probability Disappearance case There is no place for complex phase d in UMNS to appear Disappearance has no sensitivity on (standard) CPV

  17. Appearance • Conventional nm beam (~GeV) • nm ne • Not yet discovered • nm  nt • Dominant oscillation mode • Neutrino factory/Beta beam (~10GeV) • ne  nm • ne  nt Next talks

  18. ne vsnt appearance Oscillation probability (w/ CPV) • nm ntcase, • probability A∝sin22q23, is known to be large, relative effect of CPV becomes small • Also experimentally, identification of nt (out of lots of nm interactions ) is not easy • For nue appearance, A∝sin22q13 is known to be small •  Large CPV effect expected CP conserved part CPV part Relative effect of CPV

  19. Matter effect Interactions through propagation in matter nt ne nm e- nt nm ne ne NC W Z Z Z X X X ne e- X X X CC

  20. Relative size of effect ∝ E Change sign when Dm2 sign change: Can probe sign Change sign when n⇔nbar: Fake CPV effect Matter effect

  21. Oscillation probabilities 3 Dm232 2 1 when contribution from Dm12 is small (No CPV & matter eff. approx.) nm disappearance (LBL/Atm) q23 and Dm232 ~1 ne appearance (LBL/Atm) q13 and Dm132 ~0.5 Pure q13 and Dm132 ne disappearance (Reactor) ≪1

  22. d-d, a-a for nmne appearance & CPV Main CP-odd Solar Matter Matter eff.: Sensitivity indep. from q13 (if no BG & no syst. err) # of signal ∝ sin2q13 (Stat err∝sinq13), CP-odd term ∝ sinq13

  23. All mixing angle need to be non-zero Leading CP-odd d-d, a-a for + other terms.. Matter eff.: CPV effect (where sinq12~0.5, sinq23~0.7, sinq13<0.2) Same as Kobayashi-Maskawa model which require 3x3 to incorporate CPV 23 Takashi Kobayashi (KEK), PAC07

  24. CPV vs matter effect nmne osc. probability w/ CPV/matter 295km 730km @sin22q13=0.01 Smaller distance/lower energy  small matter effect Pure CPV & Less sensitivity on sign of Dm2 Combination of diff. E&L help to solve.

  25. Lepton Sector CP Violation Effect of CP Phase δ appear as • νe Appearance Energy Spectrum Shape *Peak position and height for 1st, 2nd maximum and minimum *Sensitive to all the non-vanishing δincluding 180° *Could investigate CP phase with νrun only • Difference between νe and νeBehavior

  26. How to do experiment? OK, we now understand • Importance of CPV in lepton sector • Necessity of oscillation to probe CPV • What process is suited for CPV measurement • Behavior of oscillation probabilities and relevant physics So, now, let’s consider more on experimentation!

  27. Decay Pipe Focusing Devices Proton Beam Target m nm p,K Beam Dump Super Beam Conventional neutrino beam with (Multi-)MW proton beam (nFact) • Pure nm beam (≳99%) • ne (≲1%) from pme chain and K decay(Ke3) • nm/nm can be switched by flipping polarity of focusing device Strongly motivated by high precision LBL n osc. exp.

  28. Far Det. q Decay Pipe Horns Target En(GeV) En(GeV) Ep(GeV) High intensity narrow band beam-- Off-axis (OA) beam -- (ref.: BNL-E889 Proposal) nm flux Decay Kinematics 1 2 5 1/gp~q • Increase statistics @ osc. max. • Decrease background from HE tail

  29. nm -15%@peak nm 1021POT/yr nm/nm flux for CPV meas. Example Sign flip by just changing horn plarity 50GeV proton At 295km

  30. Cross section ∝ E Higher energy  higher statistics Anti-neutrino cross section smaller than neutrino by ~1/3 Why? Take ~3 times more time for anti-neutrino measurements to acquire same statistics as neutrino Cross sections

  31. ne appearance search m e p0 • Back ground for ne appearance search • Intrinsic ne component in initial beam • Merged p0 ring from nm interactions 31

  32. “Available” technologies for huge detector Good at low E (<1GeV) narrow band beam LiqAr TPC • Aim O(100kton) • Electronic “bubble chamber” • Can track every charged particle • Down to very low energy • Neutrino energy reconstruction by eg. total energy • No need to assume process type • Capable upto high energy • Good PID w/ dE/dx, pi0 rejection • Realized O(1kton) Water Cherenkov • Aim O(1000kton) • Energy reconstruction assuming Ccqe • Effective < 1GeV • Good PID (m/e) at low energy • Cherenkov threshold • Realized 50kton Good at Wideband beam

  33. m- m- nm+ n→ m+ p+ p nm+n→m + p (Em, pm) (Em, pm) ql qm n n p p inelastic QE Neutrino Energy En reconstruction in Water Cherenkov CC quasi elastic reaction  p

  34. 2 approaches for CPV (and sign(Dm2) ) • Energy spectrum measurement of appeared ne • Only w/ numu beam (at least early part) • Measure term ∝ cosd (and sind) • Assume standard source of CPV (d in MNS) • Cover 2nd oscillation maximum (higher sensitivity on CPV) • Higher energy = longer baseline favorable • Wideband beam suited • LiqAr TPC is better suited • Difference between P(numunue) and P(numubar nuebar) • Measure term ∝ sind • Not rely on the standard scenario

  35. Angle and Baseline • Off-axis angle • On-Axis: Wide Energy Coverage, ○Energy Spectrum Measurement ×Control of π0 Background • Off-Axis: Narrow Energy Coverage, ○Control of π0 Background ×Energy Spectrum Measurement 　　　　　　　　　→ Counting Experiment • Baseline • Long: ○ 2ndOsc. Max. at Measurable Energy × Less Statistics ? Large Matter Effect • Short: ○ High Statistics × 2ndOsc.Max.Too Low Energy to Measure ? Less Matter Effect dCP=0 OA0° dCP=90 nm flux OA2° dCP=270 OA2.5° OA3° νμ νeoscillation probability Oscillation probability Dm312 = 2.5x10-3 eV2 sin22q13 = 0.1 No matter effects (E/L)

  36. “Available” beams

  37. FNAL possible future Plan

  38. CERN future possibilities Present accelerator complex Various POSSIBLE scenarios • Under discussion

  39. CERN possibilities

  40. Possible scenarios in Japan Okinoshima Kamioka Korea 295km 2.5deg. Off-axis 658km 0.8deg. Off-axis 1000km 1deg. Off-axis

  41. Scenario 1 νeSpectrum sin22θ13=0.03,Normal Hierarchy • Cover 1st and 2nd Maximum • Neutrino Run Only 5Years×1.66MW • 100kt Liq. Ar TPC • -Good Energy Resolution • -Good e/π０discrimination • Keeping Reasonable Statistics δ=0° δ=90° δ=180° δ=270° CP Measurement Potential Okinoshima Beam νe Background 3s 658km 0.8deg. Off-axis NP08, arXiv:0804.2111

  42. Scenario 2 • Cover 1st Maximum Only • 2.2Years Neutrino+7.8Years anti-Neutrino Run 1.66MW • 540kt Water Cherenkov Detector 295km 2.5deg. Off-axis <En>~0.6GeV Kamioka Tokai sin22θ13=0.03,Normal Hierarchy d=0 d=p/2 CP sensitivity signal+BG 3s nm+nm+ne+neBG nm sin22q13 nm+nmBG deg. Enrec Enrec 3s Fraction of d nm sin22θ13 Enrec Enrec K.Kaneyuki @NP08

  43. Site studies in Europe

  44. FNAL possibilities NOvA 700kW 15kt Liquid Scintillator Under construction NSF’s proposed Underground Lab. DUSEL 735 km 2.5 msec 810 km MiniBooNE SciBooNE MINOS NOvA MINERvA MicroBooNE 1300 km ~300 kton Water Cerenkov ~50 kton Liquid Ar TPC Project X: ~2 MW Combination of WC and LAr US Superbeam Strategy: Young-Kee Kim, Oct. 1-3, 2009

  45. FNAL-DUSEL potential

  46. To realize the experiments Need • Finite (reasonable) q13 T2K, NOvA, Reactors! • High power (>MW) neutrino beam • Huge high-sensitivity detector •  YOUR CHALLENGE • OR YOUR NEW IDEA!

  47. Summary • Properties of neutrino are gradually being revealed • However still yet far unknown than quarks • CPV, mass hierarchy, etc. • Especially, CP symmetry could be a critical key to answer the fundamental question: What is the origin of matter in the universe • Future superbeam long baseline oscillation experiments have chance to discover CPV effect (if q13 is large enough to be detected in present on-going experiments) • Already many studies and developments (beam, detectors) are being made around the world to realize the experiments • Lot’s of challenges and funs forseen • Let’s enjoy!

More Related