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B S Mixing Measurements at the Tevatron. Michael Kirby Radboud University, Nijmegen NIKHEF. New Trends in High Energy Physics, CRIMEA 2006. B Meson Flavor Oscillations. Neutral B mesons can spontaneously transform in the corresponding antiparticle. Mixing involves CKM elements,
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BS Mixing Measurementsat the Tevatron Michael Kirby Radboud University, Nijmegen NIKHEF New Trends in High Energy Physics, CRIMEA 2006
B Meson Flavor Oscillations Neutral B mesons can spontaneously transform in the corresponding antiparticle Mixing involves CKM elements, measuring mq constraints the unitarity triangle New exotic particles may run in the loop mixing sensitive to NP Form factors and B-parameters from Lattice calculations are known at ~15% level
ms and the side of UT md f2BBB [(1-r)2+h2] circle centered in (r,h)=(1,0) f2BBB known at 15% from LQCD • many theoretical uncertainties cancel in the ratio • |Vts|/|Vtd| can be determined at ~4% (hep-lat/0510113) Experimental challenge: |Vts| >> |Vtd| ms >> md needs to resolve > 2.3 THz oscillations Previous Dms measurements: LEP/SLD/CDF-I: ms > 14.4 ps-1 @ 95% CL HFAG Average for PDG 2006
Unitarity Triangle Fit • just for illustration, other fits exist • CKM Fit :Dms: 18.3+6.5 (1s) : +11.4(2) ps-1 -1.5 -2.7 from Dmd Lower limit on Dms from Dmd/Dms
Neutral B Meson system mixture of two mass eigenstates (No CP violation case): BH and BL may have different mass and decay width Dm = MH– ML (>0 by definition) DG = GH - GL The case of DG = 0 B Mixing
Measurement .. In a Perfect World “Right Sign” “Wrong Sign” what about detector effects?
Realistic Effects displacement resolution flavor tagging power, background momentum resolution (L) ~ 50 m mis-tag rate 40% (p)/p = 5%
Real Measurement Layout Data momentum resolution displacement resolution flavor tagging power scan for signal: A(ms=15 ps-1)= ? Unbinned Likelihood Fitter measure frequency: p ~ e-t/[1±AD cosmt] R(t) ms = ?
vertexing (same) side e,,Jet 4 2 4 1 “opposite” side 3 Road map to ms measurement 5 • Collect as many Bs as possible • Tevatron, Trigger, Reconstruction • Extract Signal • Bs flavor at decay inferred from decay products • Measure proper decay time of the Bs meson • Si trackers, per event primary vertex, candidate specific decay time resolution • Determine Bs flavor at production (flavor tagging) • PID (TOF, dE/dx) • Flavor tag quantified by Dilution: D=1-2w, w = mistag probability • Measure asymmetry between unmixed and mixed events • In practice: perform likelihood fit to expected unmixed and mixed distributions
This analysis: Feb 2002 – Jan 2006 1 fb-1 Tevatron Luminosity
SMT H-disks SMT F-disks SMT barrels DZero Detector • Spectrometer : Fiber and Silicon Trackers in 2 T Solenoid • Energy Flow : Fine segmentation liquid Ar Calorimeter and Preshower • Muons : 3 layer system & absorber in Toroidal field • Hermetic : Excellent coverage of Tracking, Calorimeter and Muon Systems
X (e)+ B (e) π- D-S K- K+ Signal Selection Muons were selected by triggers without lifetime bias = no online/offline Impact Parameter cuts Trigger muon can be used as tag muon : gives access to eDs sample with enhanced tagging purity
Signal Selection X Eff=30% + B (e) PV D-S π- LT(DS) K- K+ • Ds lifetime is used to have non-zero selection efficiency at Interaction Point • Bs can decay at IP and be reconstructed
Flavor Tagging and dilution calibration • Identify flavor of reconstructed BS candidate using information from B decay in opposite hemisphere. Ds a)Lepton Tag : Use semileptonic b decay : Charge of electron/muon identifies b flavor n Bs e / m b)Secondary Vertex Tag : Search for secondary vertex on opposite Side and loop over tracks assoc. to SV. m cos f (l, Bs) < 0.8 c) Event charge Tag: All tracks opposide to rec. B Secondary Vertex
Dilution in md measurement • Combine all tagging variables using likelihood ratios • Bd oscillation measurement with combined tagger Dmd= 0.5010.030±0.016ps-1 Input for Bs measurement Combined dilution:D2=2.48±0.21±0.08 %
Cross-check on BdXD±() Amplitude Scan • EXACTLY the same sample & tagger • Amplitude Scan shows Bd oscillations • at correct place no lifetime bias • with correct amplitude correct dilution calibration • Same results for two other modes DØ Run II Preliminary
+ J/ vertex PV - L±σL Measure Resolution Using Data • Ultimately Dms sensitivity is limited by decay length resolution – very important issue • Use J/ sample • Fit pull distribution for J/ Proper Decay Length with 2 Gaussians • Resolution Scale Factor is 1.0 for 72% of the events and 1.8 for the rest • Cross-checked by several other methods DØ Run II Preliminary
Results of the Lifetime Fit • From a fit to signal and background region: BsDs mn X BsDs e n X Ds K*K Ds fp
Bs decay samples after flavor tagging • NBs( fp + m) = 5601 102 • NBs(fp + e) = 1012 62 (Muon tagged) • NBs(K*K + m) = 2997 146 BsDs mn X Ds fp BsDs mn X Ds K*K BsDs e n X Ds fp
Amplitude Scan of BsXDs() • Deviation of the amplitude at 19 ps-1 • 2.5σ from 0 1% probability • 1.6σ from 1 10% probability
Log Likelihood Scan • Resolution • K-factor variation • BR (BsDsX) • VPDL model • BR (BsDsDs) Systematic Have no sensitivity above 22 ps-1 17 < Dms < 21 ps-1 @ 90% CL assuming Gaussian errors Most probable value of Dms = 19 ps-1 “Direct Limits on the Bs Oscillation Frequency” hep-ex/0603029 – published by Physical Review Letters
More Amplitude Scans • New results : Amplitude scans from two additional modes BsDs (fp) e n X BsDs mn X Ds fp Ds K*K
Combined D0 Result • Amplitude is centred at 1 now, smaller errors • Likelihood scan confirms 90% CL Dms limits: 17-21 ps-1 • Data with randomized tagger : 8% probability to have a fluctuation (5% before for mfp mode) • Detailed ensemble tests in progress
The CDFII Detector • multi-purpose detector • excellent momentum resolution (p)/p<0.1% • Yield: • SVT based triggers • Tagging power: • TOF, dE/dX in COT • Proper time resolution: • SVXII, L00
Event Selection: Fully Hadronic Bs used in this analysis • Bs momentum completely reconstructed • Excellent decay time resolution, good S/N • Small BR low statistic • Good sensitivity at high values of ms Cleanest decay mode: BsDs[] [KK]
Event Selection: Semileptonic Bs Ds Mass • Missing momentum () • Poorer decay time resolution • Large BR high statistic • Good sensitivity at low values of ms l+Ds Mass 48000 l+Ds candidates, 75% are from Bs decay • Minv(l+Ds) helps reject BG • BG Sources: • Ds + fake lepton from PV • Bs,dDsDX (DslnX) • cc
Flavor Tagging Performances Two types of flavor tags used in CDF • OST: produce bb pairs: find 2nd b, determine flavor, infer flavor of 1st b • calibrated on large samples of B0 ad B+ decays • SST: use charge correlation between the b flavor and the leading product of b hadronization • performances (D) evaluated in MC, after extensive comparison data VS MC Same-side kaon tag increases effective statistics ~4
Amplitude Scans • example: B0 Mixing signal in hadronic decays • points: A§(A) from likelihood fit for different m • yellow band: A § 1.645 (A) • m values where A+1.645 (A) < 1 are excluded at 95% C.L. • dashed line: 1.645 (A) as function of m • measurement sensitivity: 1.645 (A) = 1 narrow ms range wide ms range
prompt track Ds- vertex “Bs” vertex P.V. Calibrating the Proper Time Resolution • utilize large prompt charm cross section • construct “B0-like” topologies of prompt D- + prompt track • calibrate ct resolution by fitting for “lifetime” of “B0-like” objects period 3 trigger tracks +
p p D decay B decay Lxy RUN 304720 EVENT 109026 Proper decay time reconstruction PV Detector length scale and proper treatment of detector/selection biases controlled by performing lifetime measurements
Lepton Ds- vertex Bs vertex P.V. l+Ds ct* Projections Bs lifetime in 355 pb-1: 1.48 ± 0.03 (stat) ps World Average value: 1.469 ± 0.059 ps
Hadronic Scan: Combined Preliminary Bs! Ds / Ds
Combined Amplitude Scan Preliminary 25.3 ps-1 A/A (17.25 ps-1) = 3.5 How significant is this result?
k k k k = Sst D isolation K-factor ct [cm] pT [GeV/c] Courtesy of J.Kroll Likelihood Data fitted with an unbinned likelihood function to the expected unmixed and mixed distributions Procedure checked on B0 by fitting for md for each event: k=sig,bg k sig pdg (*) H-G.Moser, A.Roussarie, NIM A384 (1997) Amplitude method(*): scan ms space: fix msfit for A: A consistent with 1 mixing detected at the given ms
Measurement of ms ms = 17.33 +0.42 (stat) ± 0.07 (syst) ps-1 -0.21 -0.21 limit ms in [16.94, 17.97] ps-1 at 95% CL “Measurement of the Bs-Bs Oscillation Frequency” hep-ex/0606027 – published by Physical Review Letters
inputs: • m(Bd)/m(Bs) = 0.9830 (PDG 2006) • = 1.21 +0.047 (M. Okamoto, hep-lat/0510113) • md = 0.507 ± 0.005 (PDG 2006) -0.035 |Vtd| / |Vts| = 0.208 +0.008 (stat + syst) -0.007 |Vtd| / |Vts| • compare to Belle bd (hep-ex/0506079): |Vtd| / |Vts| = 0.199 +0.026 (stat) +0.018 (syst) -0.015 -0.025
D0 Outlook • Add Same Side Tagging • Add hadronic modes triggering on tag muon • Add more data (4-8 fb-1 in next 3 years) with improved detector – additional layer of silicon between beampipe and Silicon Tracker (Layer0) – better impact parameter resolution Layer0 has been successfully installed in April 2006 - S/N = 18:1 & no pickup noise - First 50 pb-1 of data on tape, first tracks have been reconstructed, and commissioning advancing quickly
CDF Run II Preliminary L=1 fb-1 CDF Outlook BsDs+-+ (Ds +--) • Collecting new integrated luminosity • Squeezing maximum information from the data • we already have: • Systematic use of Neural Networks in signal extraction: • use decays modes previously discarded cause high BG • more signal in already used modes • Use partially reconstructed BsDs*/K and Ds: • large BR • good momentum resolution • Improve Flavor taggers: • OST: +15% D2 • NN to combine OS taggers • OSKT • SSKT: ~+10% D2 • better use of combined PID and kinematics NBs = 220 BsDs+ (Ds-)
Conclusions • Frequency of Bs mixing successfully measured at the Tevatron! • D0 reported the first two-sided limit on ms • ms [17,21] ps-1 @ 90% C.L. • CDF confirmed result with measurement ms =17.33 +0.42 (stat) ± 0.07 (syst) ps-1 |Vtd / Vts| = 0.208 +0.008 (stat + syst) -0.21 -0.007