Title: Recent B Physics Results at D
1Recent B Physics Results at DØ
- Bill Lee
- Florida State University
- 18 February 2004
- X(3872)
- B Lifetime and Mixing
- Bs ? mm- Search
2The DØ Run 2 Detector
SMT
3X(3872) at D0
- Using 200 pb-1 of DATA collected April 2002
September 2003, we look for X(3872) ? J/? pp- - Silicon hit gt 1
- num tracks lt 100
- pT(J/?) gt 4 GeV/c
- 2.8 lt M(mm-) lt 3.4 GeV/c2
- pT(?) gt 0.4 GeV/c
- ?s within same cone as J/?
- M(?? -) gt 0.52 GeV/c2
- M(mm- ?? -) -M(mm-) lt 1.0 GeV/c2
- ?2 (mm- ?? - - vertex) lt 16
- zvertex lt 35 cm
4.4s effect
300 ? 61 X(3872) candidates
DM 0.7684 ? 0.0035 (stat) ? 0.0039 (sys) GeV/ c2
4Properties of X(3872)
- Are the production characteristics similar to
the ?(2S)? - To compare, the data was binned for several
different variables decay-length,
isolation, h (pseudo-rapidity), pT, and
helicity of (?? -)
5X(3872) and ?(2S) comparison
Yield per given cut / Total Yield
Within the current statistical uncertainties, the
production of X(3872) has similar behavior as the
?(2S), but an exotic meson could also behave
similarly.
6Is X(3872) charmonia?
- If the charged analog X?J/?pp0 was observed,
then cc hypothesis could be ruled out - While observing radiative decays X???c1 would
favor cc hypothesis - Both of these would require DØ to identify low
energy p0 and ? (work in progress) -
-
-
7Measuring Lifetime using B? J/? X, J/? ???-
- Use J/????- for tagging, vertex constraint, pT
determination - Clean signal
- Large statistics
- Good vertex resolution
- Good momenta resolution
- Large prompt J/? contamination
- Need Pt correction factor from MC
114pb-1
?(2s) Signal 8.22K events Mass 3.668 0.002
GeV/c2 ? 0.071 0.002 GeV/c2
J/? Signal 290.3k events Mass 3.07180.0002
GeV/c2 ? 0.07410.0002 GeV/c2
8B Lifetime from Inclusive B?J/?X
B? J/? X
?Ldt?114 pb-1
F correction factor to use the pT(J/ ?) to
estimate the momentum of the B to find proper
time. Obtained from Monte Carlo
??? 1.564 ? 0.014 ps (PDG)
J/? from Bs 18
??? 1.562 ? 0.013 ? 0.045 ps
Correction factor leads to the major systematic
error
9Bd,s Masses (J/? K0,?,K0s)
For CP and Lifetime studies
10B Lifetime from B?J/?K
?Ldt?114 pb-1
Fully reconstructed?No Correction Factor!
lt?Bgt1.650.083(stat)0.123(syst) ps
lt?Bgt 1.6710.018 ps (PDG)
11Bd,s Lifetimes from B ?J/?K0,?
Similar kinematics?Some systematic errors can be
cancelled in ratio!
Signal 10519
Signal 6913
?Ldt?114 pb-1
?Bd1.510.19 (stat) 0.20(syst) ps
-0.17
PDG ?Bd 1.537 0.015 ps
?Bs1.190.19 (stat) 0.14(syst) ps
-0.16
PDG ?Bs 1.461 0.057 ps
?Bs/ ?Bd0.79 0.14
PDG ?Bs/ ?Bd 0.95 0.038
12Large B Semileptonic Sample
- Charged tracks
- pT gt 0.7-1 GeV/c
- Secondary Vertex
- Lxy / ?L gt 4
- cos(?(L,PD))gt0.95
13B Lifetime from Semileptonic Decays B ? D0?X
We are able to measure Lifetime
?Ldt?12 pb-1
c? LxyMbK/Pt(D?)
K Pt(D?) / PtB (from MC)
?B 1.460 0.083 (stat) ps
?B 1.564 0.014 ps (PDG)
We will use this for mixing studies
14Mixing Flavor tagging
- In order to study Bs mixing we will need
- final state reconstruction
- ability to measure B decay lengths
- the ability to tag the flavor of the B at
production and decay. - We can use flavor-specific decays to get the
flavor of the B at decay. To get the flavor of
the B at production we use three methods - - Soft-lepton tags
- - Jet Charge tag
- - Same Side tagging
- We can test these tools using our B data sample
15Flavour Tagging results
DØ RunII Preliminary
Method Based on B Signal Efficiency Dilution Tagging Power
Soft Muon 5 57
Jet Charge 47 27
Same Side 79 26
Muon DATA, we will also use electrons
Performance with B0/Bs is under study
16Search for Bs ? mm-
SM Br(Bs ? mm- ) 3.7 ? 10-9 Some SUSY
tan(b) models can enhance the signal.
MC
Dimuon spectrum
?Ldt?100 pb-1
No Excess Seen.
Br(Bs ? mm- ) lt 1.6 ? 10-6 at 90 CL
17Summary
- DØ has observed the X(3872) particle in 200 pb-1
data - We have reprocessed ? 200 pb-1 of data to better
improve our analyses. - D0 will be able to study Bs mixing
- Tevatron is performing well.
- D0 recorded 9.4 pb-1 last week.
- Lots of data.
- Many more interesting results coming very soon!