Semileptonic and leptonic B and B s decays at Belle
Robin Glattauer
for the Belle Collaboration
B X
Outline and Motivation
●
B→Dlν (exclusive)
●
New analysis
●
Determination of |V
cb|
●
First measurement of the channel with full Belle data sample
●
Inclusive – exclusvie measurements: 3σ discrepancy
●
B
s→D
s(*
)Xlν (semi-inclusive)
●
New analysis
●
Measurement of branching fractions
Worlds largest B meson sample
~772 million BB events
Unique Y(5S) data sample at a lepton collider
Belle luminosity
B→D ν ℓ
●
Differential decay width:
●
Kinematics:
constants electroweak form factor
correction
CKM matrix
Parametrization from Caprini et al (arXiv:hep-ph/9712417)
B→D ν: Tagging ℓ
●
Y(4S) decays into two B mesons
●
Reconstruct one of them in a hadronic mode (B
tag)
●
Reduces background
●
Allows full kinematic
reconstruction
B→D ν: reconstruction ℓ
● 4 samples:
● Tracks and photons from Btag are removed
● Reconstruct D in multiple hadronic channels
● Combine D with a lepton (e,μ) to Bsig
● Determine the missing mass
● If only the neutrino is missing (i.e. genuine reconstruction)
(MC)
B→D ν: Signal yields extraction and final fit ℓ
● Extract signal yield in 10 different w-bins (from 1.0 to 1.6)
● Use MC distribution as template
● Floating: signal, D*- and wrong tag background
● Fixed to MC: other bg (e.g. fake- and non prompt leptons etc.)
● χ² fit of predicted yield (based on differential decay width) to measured yield
Belle preliminary
Belle preliminary
B→D ν: results ℓ (preliminary)
Belle preliminary Belle preliminary
● This results in
● Current HFAG averages:
Belle preliminary Belle preliminary
B s →D s Xlν and B s →D s *Xlν
●
X = feed down from higher D
sstates
●
D
s* and D
s** for B
s→D
sXlν
●
D
s** for B
s→D
s*Xlν
●
D
s→Φ(K
+K
-)π
●
D
s*→D
sγ
●
Combine D
s(*
)with lepton of opposite charge
●
Determining the number of D
s(*
):
●
D
s: fit m(KKπ)
●
D
s*: fit ∆m = m(KKπγ)-m(KKπ)
B s →D s
(*
)Xlν
● Determine number of genuine Bs→Ds(*)Xlnu events with Xmis distribution
● Evis* and pvis*: visible energy and momentum
● EB* and pB*: energy and momentum of Bs meson. Approximated from beam.
● To avoid model dependence of Xmis: use counting experiment with 3 regions:
Wrong side (lepton and Ds(*) from different Bs)
Secondary and fake leptons Signal
B s →D s
(*
)Xlν
●
3 components:
●
Wrong side
(lepton and D
s(*
)from different B
s)
●
Secondary and fake leptons
●
Signal
●
Each region enhances one component
●
Measure D
s(*
)in each region (with m(KKπ) or ∆m fit)
●
3 unknowns and 3 equations
→solve to know N
signalB s →D s
(*
)Xlν: results (preliminary)
●
Theory predictions don't include "X"
→are lower than our results
Theory predictions:
Combined:
Summary
●
B→Dlnu (exclusive)
● Full reconstruction of events using hadronic tag
● Mmiss² allows extraction of B→Dlν signal
● Measure in 10 bins of w and fit differential decay width
●
● Most precise single measurement of
● in agreement with world average, is ~2σ lower.
●
B
s→D
s(*
)Xlν (semi-inclusive)
● Determine yields with fits to m(KKπ) and ∆m
● Using 3 seperate regions for counting experiment separated by Xmis and p*(l)
●
Thank you!
Back Up
1999 – 2010: B factory at KEK (Japan)
Linac KEKB double ring
e+e- collider
e+e- → Y(4S) → BB
B→D ν: e ℓ xtracting |Vcb|G(1)η
EWand ρ²
●
Measured the signal yield in each w-bin
●
Calculate the predicted signal yield for given
|V
cb|G(1)η
ewand ρ²:
(relative to MC)
●
χ² fit of predicted yield to measured yield
Predicted
signal in bin i differential decay width using MC parameters
Belle preliminary
B→D ν: systematic errors ℓ
B s →D s Xeν
B s →D s Xμν
B s →D s *Xeν
B s →D s *Xμν
B s →D s
(*
)Xlν relative systematic
errors