Properties of B c Meson On behalf of DØ Collaboration Dmitri Tsybychev, SUNY at Stony Brook, PANIC05, Santa Fe, New Mexico B c is ground state of bc system.

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Properties of B c Meson On behalf of DØ Collaboration Dmitri Tsybychev, SUNY at Stony Brook, PANIC05, Santa Fe, New Mexico B c is ground state of bc system o Unique system with two heavy quarks of different flavor o Probes heavy-quark theories in the region between the cc and bb o m exp = 6400 ± 390 ± 130 MeV/c 2 (first observation Bc →J/  X CDF Run I, PRD 58, ) o m exp = ± 4.8 Mev/c 2 (CDF Run II, B c →J/  X)   exp = ± 0.03ps o m theor = 6304 ± Mev/c 2 (lattice QCD, PRL 94, )   theor =0.4~1.4 ps

B c Production at Tevatron Phys. Rev. D 71, B c production cross section: o qq, gg → B c + b + c o Sum of production cross sections of ground and excited states o Contribution from color-singlet and color octet states o  ( B c )/  inel ~ o Trigger is important

D. Tsybychev, PANIC05, Santa Fe NM3 Decays of B c B c decays through weak interactions  b-quark decay with a spectator c quark B c →J/   X, B c →J/   X Observed at Tevatron J/  final state is distinctive signature, useful for trigger and reconstruction  c-quark decay with a spectator b  The annihilation decays bc → l,cs,us  Charge conjugation assumed Searched for B c in 210 pb -1 inclusive J/  data sample collected by DØ b b BsBs s c BcBc c c J/  cb BcBc +, u+, u,d +, u+, u

D. Tsybychev, PANIC05, Santa Fe NM4 SMT DØ Detector Excellent coverage of Tracking and Muon Systems  Forward muon system with |  |<2 and good shielding 60% pure at L1 trigger  4-layer Silicon and 16-layer Fiber Trackers in 2 T magnetic field

Bc signal Use tri-muon final state  J/  →  and tight third muon form a vertex  231 J/  X events selected Include contributions to signal from  Feed-down from B c →  (2S)  X  B c → J/   X B c not fully reconstructed (neutrino)  Estimate from control J/  + track sample  Prompt J/  + random or fake muon (prompt background)  J/  from B decay + random or fake muon (heavy flavor background) BcBc J/  Primary Vertex Secondary Vertex    

DØ Observation of Bc→J/  X Plot invariant mass of three muons and pseudo-proper time  Not exclusive reconstruction  Use MC to get mass template shapes Background probability density is obtained from control sample  T < 0 – prompt background  Symmetric distribution about 0 subtracted off to get  T > 0, 2 – heavy flavor background Clear excess at higher mass Do likelihood fit to pseudo- proper time distribution in invariant mass bins Number of B c candidates: 95 ± 12 (stat.) ± 11 (sys.)

D. Tsybychev, PANIC05, Santa Fe NM7 Fit Results Mass: (stat.) ± 0.34 (syst.) GeV/c 2 Lifetime: (stat.) ± 0.12 (syst.) ps Main systematics  Mass: signal sample composition, MC signal modeling, fraction of prompt background  Lifetime: Bias from vertexing algorithm, fraction of prompt background Mass log likelihood Mass Hypothesis, GeV

D. Tsybychev, PANIC05, Santa Fe NM8 Heavy Flavor Background Check Expect B c →  (2S)  X be dominated by background B c →  (2S)  X ~ 5 to 100 times smaller than B c → J/  (2S)  X  Compare B c →  (2S)  sample to B c →  (2S)  track sample  Test of heavy flavor background B c →  (2S)  X B c →  (2S) track X Heavy flavor component

D. Tsybychev, PANIC05, Santa Fe NM9 Counting Analysis Perform a simple counting experiment  Normalize background from the control sample Use region with pseudo-proper time > 2 ps  183 candidate events in heavy flavor component  65 ± 26 signal events

D. Tsybychev, PANIC05, Santa Fe NM10 Systematic Uncertainties

D. Tsybychev, PANIC05, Santa Fe NM11 Fragmentation process b →B c + c dominates production  Charm quark should form weakly decaying charmed hadron in vicinity of B c Measured probability to have muon within  ± 90 o of B c candidate  5 ± 2 % for signal sample  1% for background sample Other Properties b b c c Bc

D. Tsybychev, PANIC05, Santa Fe NM12 Conclusions Observed B c  J/  X  at DØ Preliminary results  Number of candidates: 95 ± 12 (stat.) ± 11 (syst.)  Mass: (stat.) ± 0.34 (syst.) GeV/c 2  Lifetime: (stat.) ± 0.12 (syst.) ps Analysis is repeated with much bigger dataset Significant progress in B c → J/  channel