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Belle/KEB status & plans +plans for Super-KEKB/Belle
P5 meeting SLAC 10/5/05 S.L. Olsen U. of Hawai’i φ1, φ2, φ3; penguins; new particles;… +plans for Super-KEKB/Belle
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The KEKB Collider (8 x 3.5 GeV, X angle)
L=(1.6 x 1034)/cm2/sec Int(L dt)= 469 fb On- resonance~420fb-1 KEKB Collider
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Status of Asymmetric B Factories
Used this summer KEKB Ldt 2(t/14mo) PEP-II
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Normal injection Continuous injection
661/pb/day 1182 pb/day
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collaboration
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Detector performance Pt resolution (s in %)
M(p0) resolution (s in MeV) (Bp+p-: s(DE)21MeV) (Bp0p0: sM(p0)8MeV) 4.5MeV 0.3% 1 GeV/c 100MeV 1 GeV
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Particle ID in Belle ~80% ~8%
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SVD Occupancy SVD2 L~1.6x1034 → L~5x1034 cm-2s-1 ??? ~10% ~4% ~2%
Present : layer 1 of SVD ~10% occupancy / 200 Krad.yr-1 SVD2 L~1.6x1034 → L~5x1034 cm-2s-1 ???
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DAQ upgrades Faster signal processing with CMS chip in SVD
(Silcon vertex det.) w/o Event Builder Upgrade New pipelined data Acquisition system (COPPER) Present operation
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The B Factory Physics Program
1) Measure of Fundamental SM Params: CKM elements & phases 2) Search for New Physics: look for evidence of new particles in loops 3) Unanticipated new phenomena: large s(e+e-cccc), X(3872),Y(3940),.. 4) + lots of “bread & butter” hc’, cc2’, D**,Sc*, t -physics, spin frag-fcn,… Warning: I can only give a few small tastes from this rich & flavorful menu
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V*2 td sin21 from BfCP + BBfCP interf. J/y B0 KS J/y B0 B0 KS
Sanda, Bigi & Carter: J/y Vcb B0 KS V*2 td J/y V* Vtb td B0 B0 KS Vtb V* td
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Principle of CPV Measurement
(B0 or B0 ?) J/ (r+) fCP KS (r-) z t=0 B - B B + B more B’s more B’s t z/(cβγ) = (1-2w)sin21 = (1-2w)sin21
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_ 2005: B0 J/y K0 w/386 M BB pairs B0 J/y KS B0 J/y KL
B0 J/y KL Nsig = 5264 Purity 98 % CP odd Nsig = 4792 Purity 60 % CP even J/Psi KL Efficiency is improved ~25%
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CP side:s(Dt)0.5ps tag side:s(Dt)0.9ps
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BG subtracted distributions
_ 2005: B0 J/y K0 sin2f1= ±0.039 (stat) ±0.020 (syst) A = ±0.026 (stat) ±0.036 (syst) B0 tag B0 tag _ BG subtracted distributions (good tag region) previous result sin2f1= 0.061 (152 M BB pairs) _ consistent ~1.2s
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f1 measurement f1~70o f1~20o f1 2-fold ambiguity 2f1 p-2f1 ? sin2f1
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B0 D0h0 Belle’s New Method for Direct measurement of f1
_ B0 D0h0 Belle’s New Method for Direct measurement of f1 (D0 KSp+p-) AB0D0h0(Dt) = M(KSp-) M(KSp+) f-+ cos(DMDt/2) M(KSp+) M(KSp-) f+- -ei2f1 hh0 sin(DMDt/2)
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Reconstruction of B0 D[KSp+p-]h0
_ Reconstruction of B0 D[KSp+p-]h0 D0 p0 D0 w D0 h D*0 p0, h Nsig = 157 ±24 purity : 59% Nsig = 67 ±10 purity : 86% Nsig = 58 ±13 purity : 60% Nsig = 27 ±11 purity : 52% D*0 D0 p0 D* D0 pi0 D*pi0 : D*eta : TOTAL Nsig = 309 ±31 purity : 63%
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Time-Dependent Dalitz fit results
Belle preliminary Final state f1 (o) D0 p0 11 ± 26 D0 w, h 28 ± 32 D*0 p0, h 25 ± 35 combined 16 ±21(stat) ±11(syst) -30o < f1 < 62o (95% C.L.)
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Implications of Time-dependent Dalitz analysis
Consistent with B0J/yK* results cos2f1 = 0.87 ±0.75, hep-ex/ f1~70o ? Disfavored >2s sin2f1 (^_^) ? f1~20o f1 2-fold ambiguity resolved !
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Experimental Situation for B+ - in 2004
Belle 152 M BB BABAR 227M BB with 372±32 B0→p+p− events with 467±33 B0→p+p− events hep-ex/ PRL 93, (2004) 5.2s CPV, First evidence for DCPV (3.2σ) Also ~3.2s difference between Belle and BaBar
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DE-Mbc 2D fits to individual time intervals
2005 results: Bkg subtracted B+ - projections B0 tagged B0 tagged 4s signal for Direct CPV p+p− Yield p+p− ACP & DE-Mbc 2D fits to individual time intervals Dt (ps)
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2005: Status of B+ - - App App Spp
Belle 275M Spp BABAR 227M ~2.3s difference between Belle and BABAR - App (Cpp ) Spp
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Belle’s measurement of ACP(B0 0 )
hep-ex/ published in PRL 275M BBbar pairs
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CPV in B0 r+r B(r0r0) << B(r+r), B(r+r0)
Similar to Bp+p, but in principle more complicated … B VV: not a single CP eigenstate r+ p+p0: wide resonance, two 0’s in the final state. Three miracles: fL ~ 100% CP » +1 B()NR and int. small B(r0r0) << B(r+r), B(r+r0) < (26 6 ) x (HFAG Winter05) 2q A+-/ 2 small Penguin pollution (q ) A00 A+0
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B0 r+r signal B = 24.4 2.2 x 10-6 fL= 0.951 275M BB Mpp
continuum b c signal b u B = 24.4 2.2 x 10-6 Mpp 3.8 4.1 Helicity continuum continuum signal r pp fL= 0.033 0.039 0.029 0.031 [Belle-CONF-0545]
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2005: Belle Results on CPV in B+-
Preliminary (274 106 BB pairs) q=1 q=-1 Results: Low quality tag High quality tag No CPV φ2 is near 900
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Belle Constraints on 2 (α)
B only B [hep-ex/ ] & combined at 90% CL at 90% CL
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f3 () measurement + 2(a) 3(g) 1(b) * Vud Vub Simple mixing CPV
Vtd Vtb Vcd Vcb Vud Vub * Simple mixing CPV f3 (with Bd ) + Tree u b s c W B + d D0 K+ Vus Vcb Tree u b c s W B + d K+ D0 Vcs Vub fCOM fCOM _ O(l3) O(l3) Interference of bc and bu diagrams
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Belle method for f3: Dalitz
3) fCOM = D0 KSp+p- B+: r obtain from tagged D0 (D*+ D0p+) sample B-: r |A2| |A1| r = CPV: Asymmetry in Dalitz dist.: m+=m(Ksp+), m-=m(Ksp-)
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BD(*) K(*), DKS +- 275M BB 209 D0K D*0K D0K* 58 36 [D0p0]
signal D0K D*0K D0K* 58 signal 36 signal [D0p0] [hep-ex/ ] [hep-ex/ ]
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f3 Results (Belle and BaBar)
[hep-ex/ , ] f3 = 63 deg. 15 13 [hep-ex/ ] (Non-trivial constraint)
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Current status Simplistic(?) summation: f1+ f2+ f3 182o ~20o
CPV angles only: η=0.321±0.027 =0.193±0.57 consistent with constraints from measmts of lengths of sides only: η=0.342±0.022 =0.216±0.036 Simplistic(?) summation: f1+ f2+ f3 182o ~20o
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SM with KM ansatz works remarkably well for tree-level processes
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SM: sin2f1 = sin2f1 from BJ/y KS (bc c s)
Next step: use bs penguins Example: no KM phase f1 * Vtd , h’, K+K- , h’, K+K- + B B * Vtd f1 _ SM: sin2f1 = sin2f1 from BJ/y KS (bc c s) unless there are other, non-SM particles in the loop eff
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How New Physics contributes to bs
Many new phases are possible in SUSY New physics in loops? “Internal Penguin”
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Belle 2005:
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Significant CP Violation in a bs penguin mode!!
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recent QCD factorization estimates :
>>all systematically below sin(2b) >>QCD corrections : sin2b(penguin)>sin2b(tree) Many bs modes were studied: recent QCD factorization estimates : [Beneke, hep-ph/ ] [Cheng,Chua,Soni, hep-ph/ ] sin2φ1(penguin)-sin2φ1(tree)
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sin2f1(penguin) = 0.50 0.06 (HFAG’s “naïve average”)
0.4-
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B Kl +l - K*l +l - EW penguins (loops with virtual t’s, W’s, & Z’s)
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1st measurement of AFB(BK* l l)
Interference btw and Z AFB (Kl +l -) = 0.09 0.14 (stat) AFB(K*l +l - ) = 0.56 0.13 (stat) already rules out some new physics scenarios
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First Observation of bd
signal qq K*g other B _ Addresses the same physics issue as Bs- Bs mixing (future Tevatron RunII goal).
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Same physics as Bs mixing
Implications of Belle’s observation of bd Same physics as Bs mixing r 68%CL 95%CL Full UT fit New version: purely cosmetic changes
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new mesons, many puzzles! not seen in s(e+e-hadrons)
bonuses: new mesons, many puzzles! Z(3931) cc2’? hc’ X(3872) Y(3940) not seen in s(e+e-hadrons) at Ecm =4.26 GeV e+e-cccc Y(4260) Y(4260) ??? hc”?? M(wJ/y) MeV
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Future
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KEKB near term During the recent summer shutdown (2005)
one more RF station for ARES cavity (a klystron, low level control …) in HER (to be named as D5E) Increase of the HER beam current by about 150mA One RF station costs about 2 Oku-yen. new movable masks in LER: Cu head solenoids for electron cloud Upgrade the 50 power supplies for solenoid coils (3A -> 5A) test of thin coils inside quadrupole magnets 3.5 3.27 (lower?) bucket spacing? Crab cavity (Jan 2006) A crab cavity for the purpose of raising the beam-beam parameters is scheduled to be installed in each ring at the beginning of 2006.
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Comparison of Specific Luminosity
3.5 bucket spacing 3.77 bucket spacing
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Crab crossing in Jan 2006 ξy Head-on (crab) crossing angle 22 mrad
Crab crossing may boost the beam-beam parameter up to 0.19 ! (Strong-weak simulation) ◊ ξy K. Ohmi Head-on (crab) (Strong-strong simulation) crossing angle 22 mrad Superconducting crab cavities are under development, will be installed in KEKB in early 2006. K. Hosoyama, et al
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Lumiinosity projections for KEKB
Lpeak = 1.61034 cm-2s-1 Ltot = 469fb-1 ~1010 BB/year !! & similar number of t+t- world records ! Major upgrade of KEKB & Belle detector (>1yr shutdown) SuperKEKB crab cavities Lpeak (cm-2s-1) Lint 1.6x1034 469 fb-1 5x1034 ~1 ab-1 5x1035 ~10 ab-1
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SuperKEKB: 2010 Interaction Region Crab crossing New Beam pipe
q=30mrad. by*=3mm New QCS New Beam pipe More RF power Ante-chamber & solenoid coils to reduce photo-electron clouds Damping ring Linac upgrade
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Bkg & TRG rate in future x20 Bkg KEKB SuperB Luminosity ~1 50
(1034cm-2sec-1) ~1 50 HER curr. (A) LER curr. (A) vacuum (10-7Pa) 1.2 1.6 ~1.5 4.1 9.4 5 Bkg increase - x 20 TRG rate (kHz) phys. origin Bkg origin 0.4 0.2 14 10 4 x10 Bkg KEKB Bkg SVD CDC PID / ECL KLM Shynchrotoron radiation Beam-gas scattering (inc. intra-beam scattering) Radiative Bhabha
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Belle tracking with 20x background
Bkg x 20 now 4 Higher background ( 20) 4 Higher event rate ( 10) 4 Require special features radiation damage and occupancy fake hits and pile-up noise in the EM Issues: - higher rate trigger, DAQ and computing low p m identification f smm recon. eff. hermeticity f n “reconstruction”
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Belle Upgrade for Super-B
SC solenoid 1.5T New readout and computing systems CsI(Tl) 16X0 g pure CsI (endcap) Aerogel Cherenkov counter + TOF counter “TOP” or DIRC Si vtx. det. 4 lyr. DSSD g 2 pixel/striplet lyrs. + 4 lyr. DSSD Tracking + dE/dx small cell + He/C2H5 remove inner lyrs. fast gas+Si r<20 cm m / KL detection 14/15 lyr. RPC+Fe g tile scintillator
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CKM Unitarity Triangle at
50 ab-1 f1(trees) f1(penguins) (indiv. Modes)
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AFB(BK l+ l-)[q2] at Super Belle
Assume 1 year of running at 5x1035/nb/sec 5/ab integrated luminosity, 10 billion B mesons!! At present, ~0.46/ab DA9/A9~11%, DA10/A10~13% A7 fixed to SM value AFB K*ll with 5/ab Donut : B(BXsll) with140/fb + 100/fb C10NP Belle Toy MC with 5/ab C9NP Determine location of the zero crossing
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Possible schedule for Super B
J-PARC 1 construction ILC construction Construct. fund T2K SuperKEKB const. Operation fund Crab cavity KEKB machine SuperKEKB KEKB >1000fb-1 “Major” upgrade Belle “Minor” upgrade 2004 05 06 07 08 09 10 11 12 Calendar year
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budget for Super B J-PARC construction ends here
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A “balanced” world program for HEP
n experiments, gm-2, mgeg, etc. LHC, ILC Mass spectrum, interactions n mass and mixing, CPV, and LFV Energy frontier Lepton sector New physics Quark sector LFV, t CPV Flavor mixing, CP phases Super B factory, LHCb, K experiments etc.
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Final comment The most important single contributing element to whatever success Belle & KEKB has had to date has been the stimulating & enervating competition with BaBar and PEP-II. Belle & KEKB people sincerely hope this very productive competition will continue.
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Backup Slides
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.“Observation” of Direct CP violation in BK- +
One more nail in the Superweak coffin.
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(hadronic bd s s processes)
Evidence for BK0 K _ (hadronic bd s s processes) fb-1 Measurements of B K0 K0 CPV at Super B will be possible.
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Super KEKB parameters
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