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Semileptonic and leptonic B and Bs decays at Belle

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(1)

Semileptonic and leptonic B and B s decays at Belle

Robin Glattauer

for the Belle Collaboration

B X

(2)

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

(3)

Worlds largest B meson sample

~772 million BB events

Unique Y(5S) data sample at a lepton collider

Belle luminosity

(4)

B→D ν ℓ

Differential decay width:

Kinematics:

constants electroweak form factor

correction

CKM matrix

Parametrization from Caprini et al (arXiv:hep-ph/9712417)

(5)

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

(6)

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)

(7)

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

(8)

B→D ν: results ℓ (preliminary)

Belle preliminary Belle preliminary

This results in

Current HFAG averages:

Belle preliminary Belle preliminary

(9)

B s →D s Xlν and B s →D s *Xlν

X = feed down from higher D

s

states

D

s

* and D

s

** for B

s

→D

s

Xlν

D

s

** for B

s

→D

s

*Xlν

D

s

→Φ(K

+

K

-

D

s

*→D

s

γ

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)

(10)

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

(11)

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

signal
(12)

B s →D s

(

*

)

Xlν: results (preliminary)

Theory predictions don't include "X"

→are lower than our results

Theory predictions:

Combined:

(13)

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)

(14)

Thank you!

(15)

Back Up

(16)

1999 – 2010: B factory at KEK (Japan)

Linac KEKB double ring

e+e- collider

e+e- → Y(4S) → BB

(17)

B→D ν: e ℓ xtracting |Vcb|G(1)η

EW

and ρ²

Measured the signal yield in each w-bin

Calculate the predicted signal yield for given

|V

cb

|G(1)η

ew

and 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

(18)

B→D ν: systematic errors ℓ

(19)

B s →D s Xeν

(20)

B s →D s Xμν

(21)

B s →D s *Xeν

(22)

B s →D s *Xμν

(23)

B s →D s

(

*

)

Xlν relative systematic

errors

Referencias

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