study of the b c meson properties using b c g j/ y e n decay at cdf ii
DESCRIPTION
Study of the B c Meson Properties using B c g J/ y e n Decay at CDF II. Masato Aoki University of Tsukuba, Japan. “ Periodic Table ”. B c meson is the last meson experimentally observed. The B c meson. Only meson state with differently flavored heavy quarks - PowerPoint PPT PresentationTRANSCRIPT
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Study of the Bc Meson Properties using BcJ/e Decay at CDF II
Masato Aoki
University of Tsukuba, Japan
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“Periodic Table”
Bc meson is the last meson experimentally observed
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q
q’
The Bc meson
Only meson state with differently flavored heavy quarks
(bottom and charm quark)Both quarks are heavySimilar binding interaction to heavy quarkonia families
(J/, etc.)Other quarkonia decay via strong interaction
The two quarks have different flavorOnly weak decay is possible
Comparable timescales for decay of two heavy constituents
Measurable lifetime but shorter than other B mesons (~0.5 ps)
J/
Bu, Bd, Bs
q
q
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The Bc properties
Quarkonia described by Quark Potential modelsOpportunity to test with Bc
Expect:•Tightly bound: f(Bc) eV
•Ground state mass predictions : 6.1<M(Bc )<6.5 GeV/c2
•Rich spectroscopy of narrow states below B-D threshold
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Decay properties
Three dominant processes: b decay:
• J/ p+, J/Ds+, J/ l+
c decay: • Bs
0+, Bs0 l+
Annihilation: • , DK, multi-
Large f(Bc) and Vcb vertex 400x larger annihilation width than for B+
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Decay properties
Naïvely expect factorization to applyb+c+ ann.
• Expect - psHowever, bound-state effects may be large
• Eichten and Quigg predict ps
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Theoretical calculations
V. V. Kiselev, hep-ph/0308214 (2003) : Review paper
(Bc) [ps] Author
0.357 ~ 0.362 C. H. Chang et al. (Commun. Theor. Phys. 35, 57 (2001))
0.480.05 V. V. Kiselev et al. (Nucl. Phys. B 585, 353 (2000))
0.630.02 A. Yu. Anisimov et al. (Phys. Atom. Nucl. 62, 1739 (1999))
0.590.06 A. Yu. Anisimov et al. (Phys. Lett. B 452, 129 (1999))
0.46 ~ 0.47 A. El-Hady et al. (Phys. Rev. D 59, 094001 (1999))
0.380.03 L. P. Fulcher (Phys. Rev. D 60, 074006 (1999))
0.4 ~ 0.7 M. Beneke et al. (Phys. Rev. D 53, 4991 (1996))
0.550.1 V. V. Kiselev (Phys. Lett. B 372, 326 (1996))
< 1.0 I. I. Bigi (Phys. Lett. B 371, 105 (1996))
0.40 C. H. Chang et al. (Phys. Rev. D 49, 3399 (1994))
1.1 ~ 1.2 C. Quigg (FERMILAB-CONF-93/265-T (1993))
0.50 M. Lusignoli et al. (Z. Phys. C 51, 549 (1991))
Bc
obse
rvat
ion
by C
DF
(199
8)
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Rich decay modes
Decay BR
bcBcJ/e ~1.9%
BcJ/ ~0.13%
csBcBs ~16.4%
BcBs* ~20.2%
ann.Bc ~1.6%
Bccs ~4.9%hep-ph/0308214(2003)
Large J/ rate provides experimental signature
( For example, BR(BuJ/K) =0.1% )
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Hadronic productionDominant process is
ggBc+bc
Calculation requires 36 diagrams O(s
4)Contributions from color
singlet / octet
Chang et al, PRD, 71 (2005) 074012
curves representdifferent singlet/octet contributions
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Bc production rate
Much smaller production rate than other b-hadrons
Species Prod. Fraction
B+ 40%
B0 40%
Bs 10%
b-baryons 10%
Bc ~0.05%Theoretical calculation : 7.4nbPhys. Lett. B605, 311(2005)
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Heavy Flavor Physics at CDFHuge production cross sections
at Tevatron b~30 b
Currently only Tevatron can produce the Bc mesonB-factories cannot produce the Bc meson because the beam energy is not enough for the Bc generation
Large backgrounds as well B triggers are necessary lepton trigger displaced track trigger and combined trigger
quark annihilation gluon fusion
flavor excitation gluon splitting
Typical bb pair production diagrams
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Bc discovery in CDF Run I (’91~’96)
Bc signal search using BcJ/l(l=e,) channel ~20 Bc signal events were observed in 110 pb-1 of
J/ trigger data [PRL 81, 2432 (1998) and PRD 58, 112004 (1998)]
M=6.4±0.39±0.13 GeV/c2 =0.46 ±0.03 ps+0.18–0.16
=0.132 ±0.031+0.041–0.037
+0.032–0.020
(Bc)B(BcJ/l)(Bu)B(BuJ/K)
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The CDF II detector @Tevatron
Silicon Detector ||<2.0 vertex~30m
Central Outer Tracker ||<1.0 pT/pT=0.15% pT
Muon Chamber ||<0.6 (1.0)
EM, HAD Calorimeter ||<1.1(EM), <0.9(HAD) E/E=√ (13.52/ET +32) % (EM)
=√ (502/ET +32) % (HAD)
HAD CalorimeterHAD CalorimeterMuon ChamberMuon Chamber
Central Outer TrackerCentral Outer Tracker
Silicon DetectorSilicon Detector
EM CalorimeterEM Calorimeter
All of the tracking system are replacedfor Run II
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Bc signature in this analysis
Use semileptonic decay BcJ/e Larger BR than other triggerable decay modes
statistical advantage
Improved J/ trigger• pT()>1.5 GeV/c (was 2 GeV/c)• Factor ~5 J/ yield (factor ~2 BJ/ yield)
No narrow mass peak due to missing neutrino…• Bc signal = excess above estimated backgrounds
More photon conversion background due to new tracking system (more material than Run I)
Establishing the Bc again and precise measurements (Bc)B(BcJ/e) / (Bu)B(BuJ/K) and lifetime
(Mass to be measured in exclusive channel)
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J/ trigger data
Lint ~ 360 pb-1
pT() > 3 GeV/c Reduce fake Reduce prompt
~2.2M J/Signal window |M()-M(PDG:J/)| < 50 MeV/c2
Sideband : for fake J/ study
J/ signal region
Additional requirements in this analysis…
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Electron reconstructionpT(e) > 2 GeV/c, ||<1.0Track-seeded reconstruction : Inside-Out algorithm
High reconstruction efficiency for low pT electrons Calorimeter-seeded algorithm is used for high pT physics
Electron ID using both calorimeter and dE/dx measured by COT
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Calorimeter 10 variables
— Red : electrons from e+e
— Blue : pions from Ks
E/p EHad/EEm E/p(shower max)
Ewire/Estrip
(shower max)
2wire
(shower max)
2strip
(shower max)
Z/(shower max)
Q·X/(shower max)
E(preradiator)
X(preradiator)
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Electron ID using calorimeter10 variables from
calorimeterForm a Joint Likelihood
Function
L cut position is varied not to have any dependences for electron efficiency (isolation,pT,charge)
~70% efficiency
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Isolation
Isolation is defined by pT/pT
pT in the denominator is the pT of the track of interestpT in the numerator is the scalar sum of pT of all other tracks in the same calorimeter tower
Calorimeter variables strongly depend on the isolationIsolation correction is
necessaryBcJ/e decay is expected to
have similar isolation to that for BuJ/K
CDF Preliminary
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Electron ID using dE/dxEnergy deposit in COT
Ze/Z–1.3
Ze=Log((dE/dx)measured/(dE/dx)pred. for e)
~90% efficiency
22GeVGeV
e
p K
ep
K
e
pK22GeVGeV
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(Bc)B(BcJ/e) / (Bu)B(BuJ/K) Measurement
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(Bc)B(BcJ/e) / (Bu)B(BuJ/K) measurement strategy
1. Reconstruct mass of J/-e pair
2. Estimate all the backgrounds
3. Event counting above the backgrounds
4. Estimate the acceptance and efficiency Use BuJ/K as the normalization mode
BuJ/K has similar topology to BcJ/e
Cancel out most of uncertainties
Bu+
J/ +
-
K+
Bc+
J/ +
-
e+
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J/e pair reconstruction
One displaced decay vertexLxy/Lxy > 3
Prompt background becomes negligible
pT(J/-e) > 5 GeV/c Reduce non-B tracks
Search window Wide mass region due to
missing neutrino 4 < M(J/e) < 6 GeV/c2
Primary Vertex
Secondary VertexpT
Lxy
Rx
y
signal region
Bc+
J/+
-
e+
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Background Estimates
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Backgrounds and control samples
fake J/ J/ mass sideband events
fake electron J/ + track
bb (beX, bJ/X) PYTHIA Monte Carlo
electron from photon conversion J/ + electron tagged as photon conversion
prompt J/ No control sample. There is no reliable Monte Carlo Zero lifetime killed by Lxy/Lxy>3 requirement
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Fake J/ background
Fake J/ background can be estimated by J/ mass sideband events
J/+electron, J/+track, J/+conv.-e have fake J/ part each other
To avoid double counting, fake J/ events (sideband events) will be subtracted in the following background estimations
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Fake electron background
Control sample : J/ + track
(after dE/dx requirement)Fake rate after eID by calorimeter
1.Fake rates for K//p• Control samples from high statistics
Two displaced Tracks Trigger (TTT) data
2.Combine them with proper fraction obtained from PYTHIA Monte Carlo
Nfake = N(J/+track) x fake
primary vertex
secondary vertex
d0
Long lived particle
Displaced track trigger
particle composition around J/
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Fake rate estimates for K//p
Control samples in TTT data D0K for K p for protonFit the mass distribution to obtain # of events before and after eID by calorimeterFake rate = N after eID / N before eID
after eID
after eID
p p
after eID
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Particle composition in J/+track sample
PYTHIA Monte Carlo simulation
Dominant fake source : pion
after dE/dx requirement
Kaon
Pion
Proton
Kaon
Pion
Proton
pion fraction from dE/dx fitting max difference ~0.09
Data
PYTHIA
~0.09
CDF Preliminary
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Average fake rate
The average fake rate is applied to J/+track after dE/dx cut
KK
pp
positive chargenegative charge
average fake rate
< 0.8%
CDF Preliminary
CombinePPKKππaverage fεfεfεε
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Systematic uncertainties
Isolation dependence on fake rate ~14.5%
Difference between TTT data and J/ trigger data (tight requirement on # of silicon hits for TTT) ~7.2%
Particle fraction in PYTHIA ~1.9%
Sample statistics J/+track : ~2.0% Fake rate : ~0.9%
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Estimated fake electron background
From J/+track data with fake rate convolution15.43 2.54 events in the signal region
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Photon conversion electrons
Control sample : J/+e tagged as ee Find collinear partner track
These candidates are removed from the J/e candidate list
Miss-tracking due to very low pT partner track
Not 100% finding efficiency
Residual photon conversion electronsNeed to understand the finding efficiency
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Conversion finding efficiency
Monte Carlo sample : B0J/0
98% 0, 2% 0eetag = ~50% efficiency
Residual ee events
Systematics study Another MC : use pT(tracks) in J/+track as pT(0)
tag
tagtaggedresidual ε
ε1NN
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Systematic uncertainties
pT spectrum~43.7%
Lifetime of B0
~2.0%Dalitz decay
~1.0%Sample statistics
Finding efficiency : ~3.8% J/+conv. e : ~30.1%
CDF Monte Carlo
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Estimated residual photon conversion
From J/+conv-e data and conversion finding efficiency
14.54 7.75 events in the signal region
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bb background
It is possible to make a common vertex with J/ from one B decay and e from another B decay
bb background
quark annihilation gluon fusion
flavor excitation gluon splitting
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bb background estimatePYTHIA Monte Carlo simulationValidated using bb azimuthal correlation information [PRD71,092001 (2005) ] Reasonable agreement with data
Normalization with data : N(BuJ/K)
Azimuthal angle distribution between J/ and electron with all kinematical requirements
Bc signal MC
Additional requirement : J/-e< 90deg.
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Systematic uncertainties
Monte Carlo setting (PDF/ISR) ~31.4%
Isolation dependence on eID efficiency ~2.9%
Branching ratio of normalization mode BuJ/K ~0.9%
Calorimeter fiducial coverage ~0.9%
Statistics MC sample : ~6.5% N(BuJ/K) in MC : ~1.9% N(BuJ/K) in data : ~1.8% (eID by cal) : ~1.4% (eID by dE/dx) : ~1.0%
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Estimated bb background From PYTHIA Monte Carlo BuJ/K for normalization to data
33.63 11.38 events in the signal region
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Summary table
Fake e 15.430.312.52
Conversion 14.544.386.39
bb 33.632.2011.17
Total bkg 63.594.9113.59
Data 178.5014.67*J/ sideband events are subtracted
*before the subtraction, data has 203 events and the fake J/ is 24.5±3.5
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M(J/+electron) data and excess
Total background : 63.6±14.4 eventsExcess : ~115 eventsSignificance : 5.9
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Cross check : e-track IP w.r.t. J/ vertex
Lxy(J/)/Lxy> 3 Bc decay vertex position is the same as
that for J/ (J/ immediately decays) Bc should make a peak around IP=0
CDF Preliminary
CDF Preliminary
electron
Lxy(J/)
IP
PV
Peak exists!
J/-eBuJ/K
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(Bc)B(BcJ/e) / (Bu)B(BuJ/K) calculation
Have established the signal !!Let’s calculate (Bc)B(BcJ/e) / (Bu)B(BuJ/K)
• acceptance ratio • efficiency ratio
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Similar reconstruction criteria as J/eN(Bu)=287259 was found in the same data
Normalization mode : BuJ/K
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Kinematical acceptance ratioRK = Akin(Bu)/Akin(Bc) = 4.42±1.02
MC parameters RK RK
Central value (M=6.271GeV/c2,=0.55ps) 4.4160.082
0
M(Bc)=6.291 GeV/c2 4.4030.082
0.013
M(Bc)=2.251 GeV/c2 4.3940.082
0.022
(Bc)=0.7 ps 4.0760.074
-0.34
(Bc)=0.4 ps 5.0060.096
+0.59
pT(Bc) spectrum 3.5780.062
0.838
Lxy 4.5760.086
0.16
BcJ/eX other decays 4.7690.090
+0.353
Trigger 4.2990.079
-0.117
e/K tracking 2%
Systematic uncertainties
Lar
ge
st
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Reconstruction efficiency ratio
)/()()()/()()(
)()/()()(
dXdEcaleJvertextrigger
KJvertextriggerR
trkcccc
trkuuuu
%90~%70~
1
)/()(
1
dXdEcalR
Most of the efficiencies are expected to
be same for Bc and Bu
electron ID with calorimeter and dE/dx
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Kinematical limits
Choose pT(B) > 4GeV/c, |y(B)| < 1 as our cross section definition
(Run1 : pT(B) > 6GeV/c, |y(B)| < 1)
4GeV -1 < y(Bc) < 1
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Result of B ratio measurement(Bc)B(BcJ/e) / (Bu)B(BuJ/K)= 0.282 0.038(stat.) 0.035(yield) 0.065(acc.) (pT(B)>4GeV/c, |(B)|<1)
Most of the difference to the Run I measurement is from the treatment of input pT(Bc) spectrum
Still consistent with Run I
Consistent with result from muon channel 0.245 ± 0.045(stat.) ± 0.066(syst.) +0.080/-0.032(life.)
The result is consistent with recent QCD calculation
0.132 ±0.031+0.041–0.037
+0.032–0.020
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Lifetime Measurement
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Lifetime measurement strategy
1. Release Lxy(J/e)/Lxy > 3 requirement
2. Cut on Lxy error (Lxy < 70 m)3. Use J/e events in the signal region(4-6 GeV/c2)4. Estimate # of background events using same way
as B ratio measurement5. Un-binned maximum likelihood fit with J/e data
1. Input : pseudo-proper decay length and its error2. Background shapes from each control sample3. Prompt background shape is assumed to be a
resolution function (Gaussian)4. Signal shape with neutrino effect correction
5. Fit J/e data to extract Bc lifetime
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Fit input value and neutrino effect correction
ct : proper decay length
X : pseudo-proper decay length
K : correction factor
KX
Bp
BM
eJM
eJp
eJp
eJML
)(Bp
)M(BL)ct(B
cT
cT
Txy
cT
cxyc
)(
)(
)/(
)/(
)/(
)/(
K-distributions for 4 M(J/e) binsInput value for the lifetime fitting
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Background estimates (w/o decay length cut) Background events are estimated using same way as B ratio measurement
Prompt background and Bc signal are from the lifetime fitting directly
M(J/e) [GeV/c2] 4-6
fake J/ 164.0±9.1
fake electron 110.2±19.0
photon conversion
67.4±34.8
bb 63.0±18.4
prompt ??
Bc ??
data 783*systematic uncertainties are included
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Background distributionsFake J/
Fake electron Photon conversion
bb
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J/e data fit result
c=142 +22/-20 mN(Bc)237 events (N(prompt bkg) 127)
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Systematic uncertainties on c(Bc)
Total systematic uncertainty is order of ~7% (10m)
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Bc lifetime result
CDF Run2 (360pb-1, J/+e) c = 142 +22/-20 ±10 m = 0.474 +0.073/-0.066 ±0.033 ps
Operator Product Expansion 0.55 0.15 ps
Bethe-Salpeter Model 0.46~0.47 ps
Light-Front Constituent Quark Model
0.59 0.06 ps
Light-Front ISGW Model 0.63 0.02 ps
Hard-Soft Factorization 0.55 0.1 ps
QCD Sum Rules 0.48 0.05 ps
Recent theoretical calculations in which 3 major decay diagrams play important roles
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Experimental results of the Bc meson lifetime measurement
This analysis
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Summary of the Bc analysis
Have established the Bc signal in J/e final state with 5.9 significance
Measurements with good precision (world’s best) (Bc)B(BcJ/e) / (Bu)B(BuJ/K) = 0.282 0.038(stat.) 0.035(yield) 0.065(acc.) Lifetime = 0.474+0.073/-0.066(stat.) 0.033(syst.) ps
The results are consistent with CDF Run I measurements
Lifetime result agrees with theoretical models in which all the three major decay diagrams play important roles in the Bc decays
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FIN
Thank you•This lifetime result with minor update was accepted for publication in Physical Review Letters [PRL 97, 012002 (2006)]
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Backup slides
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Introduction
Three major decay diagramsLifetime should be Bc 1/(0.6+1.2+0.1) 0.5 ps
if all the three diagrams contribute to the decay
*Others : – Pauli interference) + penguin) + …
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PDF and likelihood functionSignal PDF :
Background PDF for fake J/,fake e, conv. e, bb :
Event PDF :
Log likelihood :
signal term
backgrounds term
Background shapes and the numbers are constrained
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Fitter check before J/e data fitting
Toy MC
BuJ/K data
c=504.1 ± 9.3(stat.) mgood agreement with CDF Run II result : 498.8 ± 8(stat.) ± 4(syst.) m
Fitter returns reasonable lifetime result and error
CDF Preliminary
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Cross check : J/+e mass distribution
Normalization : 4~6 GeV/c2 using lifetime fit result Prompt shape : Assume to be J/+track with Lxy < –3Good agreement
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Determination of the angle from nonleptonic BcDsD0 decays
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CP-even factors
CP-eigenstates for the oscillation D0D0
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Branching ratio of BcDD
Several billion Bc events are expected at LHC 104~105 decays of Bc
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CDF Run-II
M(J/)
M(J/)M(J/e)
ct*(J/e)0.460.08 ps62875GeV
Pub. Pub.
Pre. Pub.
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D0 Run-II
Pre.
Pre.
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Bc mass measurement
CDF Run-II~1.1pb-1
Bc+J/+
~50 signals>7.5sigma
6276.5 ± 4.0 ± 2.7 MeV/c2
Latest
Clo
se u
p