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The CKM matrix
u
d
s
b
1-l2/2
l
A l3(r-ih)
b
c,u
Vub,Vcb
c
-l
1-l2/2
Al2
t
A l3(1-r-ih)
-Al2
1
B decays
Vtb
Vtd ,Vts
B Oscillations
b
d, s
Theory
d, s
b
Wolfenstein parametrization
4 parameters : l ,A, r, h
2
Experiments at the Z / (4S)
~ 150 M
BABAR
(4S) BB
pB ~ 30 GeV
BELLE
DELPHI
pB ~ 1 GeV
OPAL
CLEO
ALEPH
~ 3.4 M
pB ~ 0.3 GeV
The DELPHI experiment
Z  bb
~ 0.8 M
3
Event Selection
Lifetime probability
Analysed data samples
4
Event Reconstruction
Decay distances
D mass resolution
Analysed data samples
5
Discriminant variables
~80%
~80%
~80%
~46%
QX< 0
Analysed data samples
2
3
QX= 0
1
3
6
q2 measurement
|Vcb| from
7
q2 measurement
|Vcb| from
8
Fit

Event by event likelihood:
Nsignal 
d
dq2
dq2
dN
|Vcb|2 F2(w) K(w) 


eff(q2)  res(q2)
dq2
meas.
+ Constraints on Nj
(except for combinatorial
and D** backgrounds)
P(q2)
|Vcb| from
P(m)
F(w) as function of
the f.f. r2, R1 and R2.
Fit F(1)|Vcb| and r2
P(d+)
P(d-)
9
Results on simulated events
Generator level
|Vcb| from
Reconstruction level
10
Results on individual samples
|Vcb| from
11
Results on individual samples
Fixing the BR
|Vcb| from
= (0.67 ± 0.08 ± 0.11)%
12
DELPHI average
Increased statistics ( 4)
Results:
New channel (K- +(0))
Improvements in the
reconstruction (Eb, mD*)
Control on background
New observables
New measurements
DELPHI average:
|Vcb| from
13
Results on Real Data
|Vcb| from
14
Systematic uncertainties
External parameters
K-+X rates:
|Vcb| from
b fragmentation:
15
Systematic uncertainties
Detector performance
Resolution function:
Syst. due to the
parameterization:
F(1)|Vcb|
r2
Including/excluding
K-+
(0)
|Vcb| from
F(1)|Vcb|
r2
2.0%
5%
1.0%
3.5%
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Systematic uncertainties
Detector performance
d± distributions:
|Vcb| from
17
Systematic uncertainties
Signal and background modelling
Signal:
|Vcb| from
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Systematic uncertainties
Background modelling
Model 1
Model 2
D*1
D*2
D1
q2sim
|Vcb| from
q2sim
19
Comparison with other measurements
|Vcb| from
20
Systematics
|Vcb| from
21
Probability distributions
D** properties
22
Probability distributions
D** properties
23
RD/MC
D** properties
24
Discriminat variables
D** properties
25
Discriminat variables
D** properties
26
Discriminat variables
D** properties
27
Cascade correction factors
D** properties
28
Systematics
R*
D** properties
29
Backgr. mass distribution RD/MC
 = 0.5  0.2
i = 3, 5
D** properties
30
Non-resonant contribution
D** properties
31
Non-resonant contribution
= 0.42%
H.-Y. Cheng et al. PRD48 (‘93) 3204
D** properties
32
D contribution
D** properties
33
Efficiencies
D** properties
34
Fit m wrong sign candidates
D** properties
35
Fit m RS cand. for 0.25 < R < 0.70
D** properties
36
Ds spectroscopy
D** properties
37
OPE formalisms
Pole mass expansion
Kinetic mass (=1GeV)
l 1, l 2
2, 2G
Can be measured
|Vcb| from inclusive decays
r1, r2, i (i=1,4)
3
rD3 , rLS
  Energy of light quarks and gluons (related
with mb, mc )
l1 (2 )  Kinetic energy of the b quark inside
the meson
l2 (2G) = chromo-magnetic coupling
 (MB*-MB)
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Spectral moments
Expressed in terms of
the same theoretical
parameters
PRL 87 251807 ’01
PRL 87 251808 ’01

Inclusive observables  O 
b
Photon and lepton energy (E, El),
Mass hadronic distribution (Mx), ...
s
l
CLEO
nl
q2
CLEO CONF 98-21
b
c
= (0.35 ±0.07±0.10) GeV
l1=(-0.236 ±0.071±0.078) GeV2
|Vcb| from inclusive decays
PDG2000
|Vcb|=(40.8  0.5  2.5)  10-3
PDG2002
|Vcb|=(40.4  0.5  0.5  0.8)  10-3
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Moments of the D** distribution
Inclusive b semileptonic decays
Exclusive
processes
 22% D
Known
 50% D*
Study of D** properties
 28% D**
@ LEP
 78% Bd , B 22% Bs , b
Moments of the total hadronic
mass distribution in bc l- nl
Inclusive decay width determination
|Vcb| from inclusive decays
40
Systematics on moments
|Vcb| from inclusive decays
41
Combining information on moments
Moments of the lepton energy spectrum by DELPHI
(DELPHI 2002-070-CONF-604)
2 fit to 6 moments
Two formalisms
Combined fit to the
3 first moments
of hadronic and
leptonic moments
mqpole
mqkin (q)
Constraints from external results
Included s and (1/mb)3 corrections
s = 0.22 ± 0.01
Moments
42
Pole mass formalism
Fixing
Constraints from
and
BABAR
 = 0.53 ± 0.09 GeV
l1 = - 0.36 ± 0.09 GeV2
CLEO
 = 0.35 ± 0.07 ± 0.10 GeV
l1 = - 0.238 ± 0.071 ± 0.078 GeV2
Moments
43
Comparison with other measurements
Well defined scheme
Control on non-perturbative
3
corrections up to O(1/mb)
Remaining perturbative
corrections ~ 1 %
Error of |Vcb| ~ 2%
|Vcb| (inclusive)
Moments
44
Updated results
New moment expressions by P. Gambino :
Using the numerical expression of the sl
advised by N. Uraltsev :
|Vcb| from moments
45
BPS limit
N. Uraltsev
Allows an accurate extraction of
(Bogolmo’nyi-Prasad-Sommerfeld)
|Vcb| from moments
46
The b quark mass
Ph.D. M.J. Costa
Ph.D. P. Tortosa
This result
Moments
47
Summary and conclusions
|Vcb| from
Improves the previous result from DELPHI
Competitive with LEP, CLEO and b-factories
Measurement of b s.l. decays to higher mass states
Large dispersion between results from several
experiments  Need for more measurements
Errors of |Vcb| dominated by the theory
Need measurements of form factors, production rates, BR’s…
Summary and conclusions
48
Summary and conclusions
D** properties
Measurement of the production rates of D**
Increased stat., improved syst.
D** D production limits
Study of the D** mass distribution
First determination of D1* properties in B s.l. decays
Compatible results of D0* properties
Measurement of the 3 first moments of the hadronic mass
distribution
First measurements at low pl
Compatible result with CLEO and BABAR  check OPE consistency
Summary and conclusions
49
Summary and conclusions
|Vcb| from the inclusive decay width
Development of the kinetic mass scheme
Combined fit to 6 DELPHI moments
Quark masses determination
Control of non-perturbative parameters
Proximity to the BPS limit
Accurate determination of |Vcb|
Summary and conclusions
50