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1 Superb prospects: Belle & KEKB upgrades Kay Kinoshita University of Cincinnati Belle Collaboration July 26-31, 2009 motivationplanstatus (CP Violation III)
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2 Superb prospects: Belle & KEKB upgrades Kay Kinoshita University of Cincinnati Belle Collaboration July 26-31, 2009 motivationplanstatus (Detectors II)
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3 Experiments (-2009) CP asymmetry manifested in diverse processes in B decay -> many measurements, (over)constrain CKM B-factories (1999-2009) Primary goal: establish unitarity & complex phase of CKM matrix Kobayashi & Maskawa (1973) proposed 3 rd generation of particles Explain CP violation in K, predict for B found consistent with unitarity 2008 Nobel
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4 B-factories (1999-2009) … + many other successes + more measurements, on B, charm, tau, 2-photon, ϒ (4S), ϒ (10860), B s, ϒ (3S), ϒ (1S),... Addressing CP, CKM, QCD, HQ spectroscopy, LFV, NP, Dark Matter,... Headliners new charmonia, charmonium-like states, ISR, D sJ, new charmonia, charmonium-like states, ISR, D sJ, many B decays many B decays D 0 mixing D 0 mixing limits on/hints of New Physics limits on/hints of New Physics
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5 B pairs world sample KEKB/Belle KEKB + PEP-II ~946/fb (6/09) ~553/fb design luminosity of KEKB L max = 2.1 x 10 34 /cm 2 /sec (design=1.0) PEP-II/BaBar ~ 1.5 billion BB pairs
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6 Why collect more? With 1.5G Bpairs (+similar #’s of c, tau) at Belle+Babar many best measurements: testing CKM unitarity, exploring SM-suppressed/forbidden regions φ 1, φ 2, φ 3 β, α, γ ρ 0 ρ 0 ( φ 2 ), Dalitz ( φ 3 ), b->d γ SM- suppressed B & D processes Lepton universality B-> τν, B->D (*) τν LFV τ->µγ many of these measurements/limits are statistically limited
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7 furthermore... to account for baryon asymmetry of universe... NEED other source(s) of CP violation Why collect more?
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8 complementary to LHC: γ, K L detection; hermeticity -> neutrinos With x10 2 luminosity, in a facility designed for CP studies, a significant new window b->s penguin( φ 1 ) b->s γ, b->d γ, B-> sl + l - RH currents in B->{s} γ CP in D mixing Lepton universality SM-forbidden lepton processes ρ 0 ρ 0 ( φ 2 ), Dalitz ( φ 3 ), b->d γ Higgs in B-> τν, B->D (*) τν LFV τ->µγ
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10 V tb *2 V td 2 V cb V cs * V tb *2 V td 2 V cb V cs * mixing+tree SM: “golden” vs “other” sin2 φ 1 (sin2 β) V cb * V cs V cb * V cs tree (real V ij ) “golden” B -> J/ ψ K s => relative phase = 2 φ 1, CP asymmetry ~ sin 2 φ 1 identical hadronic processes -> same |Amplitude| V cb * V cs V cb * V cs real => zero phase difference well-measured rate mixing V tb *2 V td 2 phase = arg(V tb *2 V td 2 )=2 φ 1
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11 “other” sin2 φ 1 b -> ss ̅ s: identical reasoning “New Physics” w complex phase φ new ---> CP asymmetry ≠ sin (2 φ 1 ) V tb *2 V td 2 V tb V ts * V tb *2 V td 2 V tb V ts * mixing+penguin V tb * V ts V tb * V ts penguin (real V ij ) V tb * V ts V tb * V ts real => zero phase difference => relative phase = 2 φ 1, CP asymmetry ~ sin 2 φ 1
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12 Standard Model: “other” sin2 φ 1 caveat: (small) theory correction -> mostly >0 V tb * V ts V tb * V ts penguin (real V ij ) b -> ss ̅ s: identical reasoning
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13 Heavy Flavor Averaging Group Average “sin2 φ 1 ” from b->s penguins Naïve World Average sin2 φ 1 (b->sqq ̅ )= 0.62 0.04 Compare to cc ̅ s: sin2 φ 1 (b->cc ̅ s) = 0.672 0.024 CL = 0.19 (1.3 σ ) difference is < 0
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14 “sin2 φ 1 ” sensitivity to New Physics Already exploring “New” region: to improve sensitivity, need better statistics systematics theory corrections (Luminosity Projections) ✪ Babar: PRD79, 052003 (2009)
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15 Right-handed currents Atwood, Gronau, Soni (PRL 79, 185 (1997)) Atwood, Gershon, Hazumi, Soni (PRD 71, 076003 (2005)) large asymmetry right-handed current Currently: consistent with no RH currents (but need more data for good sensitivity...) in SM B 0 → X s CP γ is ~flavor-specific ( γ polarization) -> low CP-asymmetry, O(3%)
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16 Right-handed currents CP asymmetry in B → K S π 0 γ precision integrated luminosity
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17 B + -> τ + ν τ : constraints on charged Higgs {WS Hou, PRD 48, 2342 (1993)} (extrapolation) 50 ab -1 allowed (Belle) 0.65 ab –1
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18 Lepton universality: B SM: B(B-> ) = 1.6x10 -4 B(B-> ) = 7.1x10 -7 B(B-> e ) = 1.7x10 -11 B-> B-> deviations from SM sensitive to NP Luminosity (ab -1 ) Significance expect observation with ~4 ab -1 10
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19 Lepton universality: B D (*) c b H/WH/W B(B 0 ->D *- ) = (2.0±0.4±0.4)% [PRL 99, 191807 (2007)] –Ratio ( / ) is sensitive to charged Higgs (similar to B ) M.Tanaka universality via semileptonic decays B X decays probe NP in different ways: B : H-b-u vertex B D : H-b-c vertex
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20 D mixing/CP violation For 75 ab –1 x=0.8 y=0.8 ~4 σ significance on 1-|q/p| |q/p|=0.9 >4 σ significance on x >5 σ significance on y
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21 of B’s => what we need is
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22 Super KEKB Luminosity projection 3 year shutdown for upgrade ~ 2016 10ab -1 L~8x10 35 cm -2 s -1 50ab -1 by ~2020 x50 present
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23 KEKB luminosity upgrade strategy “nano-beam” scheme (proposed by P. Raimondi for Italian Super B factory) 1.8A(LER)/1.45(HER) 3.8A/2.2A 6.5(LER)/5.9(HER) 0.26/0.26
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24 KEKB luminosity upgrade strategy LERHER Emittance xx 2.82.0nm Coupling y/xy/x 0.741.80% Horizontal beta at IP x*x* 17.825.0mm Vertical beta at IP y*y* 0.26 mm Horizontal beam size x*x* 7.067.07 mm Vertical beam size y*y* 0.0730.097 mm Bunch length zz 5mm Half crossing angle 30mrad Beam EnergyE3.58.0 Beam CurrentI3.842.21A Number of bunchesnbnb 2252 Beam-beam parameter yy 0.079 LuminosityL8x10 35 (8.5x10 35 with CW)cm -2 s -1 New lattice: still under study Tentative machine parameters
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25 <100 nanometers Note that KEK Accelerator Test Facility (linear collider damping ring) has achieved 35 nm
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26 Detector: Background projections Issues Radiation damage Occupancy Fake hits, pile-up Event rate Belle detector SuperKEKB (hi-current design) normalized to current rates Design upgrade to tolerate ~20X at full luminosity Year
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27 Detector: Belle II Upgrade of Belle to operate w 20X background, 50X event rate baseline: current performance + improved PID Design Study Report arXiv: 0810.4084 Design Study Report arXiv: 0810.4084 Baseline design – not final Satisfies minimum requirements Many alternatives under study: Design to be finalized in 2009 Physics studies Detector simulations based on Geant 3, fast simulator, Geant 4
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28 Belle II baseline New dead-time-free pipelined readout and high speed computing systems Faster calorimeter with waveform sampling and pure CsI (endcap) New particle identifier with precise Cherenkov device: (i)TOP or fDIRC. Endcap: Aerogel RICH Si vertex detector with high background tolerance (+2 layers, pixels) Background tolerant super small cell tracking detector KL/ detection with scintillator and next generation photon sensors
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29 Baseline design BellesBelle Detector type4-DSSD2-DEPFET pixel + 2- DSSD + 2-DSSD (short strips/angled) chip-on-sensor lyr 5&6 Inner radius15 mm10 mm Outer radius70 mm120 mm DSSD readoutHold 3µs/readout 27µs pipelined Readout time800 ns50 ns Silicon inner tracker improve vertexing -> thin innermost 2 layers, reduce inner radius improve K S acceptance -> increase outer radius background/occupancy -> striplets, pixels, pipelined readout + standalone tracking, dE/dx
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30 Baseline design Silicon inner tracker Layers 5 and 6 shorten strips angle to reduce total area
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31 Baseline design BelleBelle II (t>0) Inner radius77 mm160 mm Outer radius880 mm1140 mm Inner layer cell size 12 mm8 mm # sense wires840015140 Drift chamber improve momentum resolution -> increase outer radius improve dE/dx -> longer radial path background/occupancy -> smaller cells
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32 Baseline design BelleBelle II (t>0) BarrelAerogel TOF dE/dx in CDC Cerenkov time-of- propagation (TOP) Endcap(dE/dx)Aerogel RICH Particle ID improve K/ π for b->s vs b->d, etc. add endcap PID reduce material in front of calorimeter
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33 Baseline design Particle ID Barrel TOP counter with imaging charged particle quartz radiator Cherenkov photon focusing mirror image expansion region Options 2-pc (double readout) 1-pc, time only 1-pc, with standoff, imaging Photon time-of-propagation due to θ c difference; at 3 GeV, 1m path, Δ t ~ 75 ps π /K time-of-flight; at 3 GeV, 1m path, Δ t ~ 50 ps Photon detection Multi-anode Microchannel plate PMT (MCP-PMT) Δ t<40 ps Readout BLAB3 ASIC “oscillioscope on a chip”
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34 Baseline design Particle ID Endcap Proximity focusing Aerogel RICH Multi-index to minimize ring width n = 1.045-1.055 indices TBD Photon detector requirements high QE, >20% high gain 5mm x 5 mm segmentation >70% coverage operate in B=1.5 T Candidates Hybrid APD MCP-PMT (includes TOF)
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35 Baseline design BelleBelle II (t>0) BarrelCsI (Tl) +waveform sampling/fitting Endcap Rise time Photodetector CsI(Tl) 1000 ns Si photodiode Pure CsI 30 ns PMT +waveform sampling/fitting Electromagnetic calorimeter reduce background without loss of resolution Alternatives under study Bismuth silicate (BSO) Lead Tungstate (PbWO 4 )
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36 Baseline design BelleBelle II (t>0) BarrelGlass RPC, streamer mode Same RPC (avalanche mode?) EndcapGlass RPC, streamer mode Plastic scintillator x-y strips K L /muon detector reduce background in endcap
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38 Placement of KEKB upgrade on Roadmap (Jan. 2008) -> official priority of KEK 3-year upgrade: 2010–2 L ∼ 8 × 10 35 cm −2 s −1 Funding: 3.2 x 10 9 ¥ (~$32M) for FY 2009 request for construction (2010-): $350M
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39 Belle II Collaboration New international collaboration (not extension of present Belle) http://superb.kek.jp Belle First meeting December 2008 next meeting Nov. 18-9, 2009 Spokesperson: P. Krizan (Ljubljana) US institutions University of Cincinnati University of Hawaii Virginia Tech Wayne State
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40Summary B-factories 1999-2009, >1.4x10 9 B pairs: firmly established CKM as main source of CP asymmetry at low energy placed multiple constraints on CKM unitarity high precision -> probe for New Physics rare processes as windows to New Physics incl. D mixing, tau decays ~10 2 X luminosity will probe >1 TeV mass scale precision CKM, CP, lepton universality, LFV (complementary to LHC) KEKB upgrade for L=8 x 10 35 included in KEKB Roadmap SuperKEKB/Belle II plans well underway new international collaboration forming
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