Branching Fraction and Direct CP
Violation in
B K
0
0
and B h


Alfio Lazzaro
Dipartimento di Fisica and INFN, Milan
on behalf of the BaBar Collaboration
American Physical Society 2003, Philadelphia
Meeting BaBar Italia,
Capri 10/04/03
Alfio Lazzaro
1
Overview
Physics Motivation
Analysis Strategy: Samples, Event
Selection, ML fits
Results on Branching Fractions and
Charge asymmetries
Conclusion
Meeting BaBar Italia,
Capri 10/04/03
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2
Physics Motivation
• Measurements of Branching Fractions allow constraints on
phenomenological models
• Charge asymmetries (Ach) expected large (>20%) in B K
(Soni, PRL 43, 242 (1979)) and B p (Gronau, PRL 79,
4333 (1997))
Previous Measured Branching Fractions (106):
Need precise measurements
Meeting BaBar Italia,
Capri 10/04/03
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3
Data Samples and Sub-channels
We have used 81.9 fb1 on-resonance
_
(88.9 millions of BB pairs)
We considered 3 channels:
Reconstructed in
(23%)
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Alfio Lazzaro
(39%)
4
Event selection
• Beam energy to constraint B mass and energy:
• Event shapes to distinguish B events from continuum udsc:
Fisher discriminant combining 4 variables:
•direction of B thrust axis wrt beam direction
•direction of B momentum wrt beam direction
•2 Legendre moments of the energy flow of rest of event wrt B thrust axis
|cos (qthrust)| < 0.9
• Loose cuts based on shapes variables, PID and kinematical quantities
of secondary daughters, Cherenkov angle cut for h selection.
We prepare the input to
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Maximum Likelihood Fit
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5
Observables
• Two types of background:
_
 qq (continuum ) dominant
_
 bb (non continuum ) ~ 1% – 2%
• Observables: E, mES , Fisher,  mass
We use Unbinned Extended Maximum
Likelihood (ML) Fit to extract signal
yields and charge asymmetries
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Results for
0
K
and

h
First observation
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Negative logLikelihood
Dashed blue line:
Dotted red line:
Solid black line:
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mES and E projections
Shaded histograms represent   gg
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9
Systematics on BF and Ach
Sources
Error on yields
• Systematics due to ML fit efficiency and bias
• Daughter Branching fractions
• Reconstruction efficiencies
(, p0, KS, charged tracks)
• Other sources: BB Number, MC statistics,
PID, …
0.3 - 0.5
0.03 - 0.4
0.3 - 2.0
0.03 - 0.6
Total systematic error on BF:
7.1% (h +)
7.7% (K 0)
Charge Asymmetries
Systematic on charge dependence bias
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1.1%
10
K0, K
• Branching Fraction for BK larger than initially expected
by theory
• Tree diagrams are Cabibbo suppressed:
• Interference between two penguin diagrams and the known
 –   mixing angle conspire to greatly enhance B K and
suppress B K (Lipkin, Phys. Lett. B 254, 247 (1991))
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Results for K0 and K
BF
Ach
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See also talk by
Fred Blanc,
Session T11
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mES and E Projections
Shaded histograms represent   pp
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Conclusion
We have presented the following preliminary results:
First
observation
Suppressed B K
Enhanced B K
2.5s
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Altre Analisi in Corso
B–> '
• BAD-462 Supporting Document
BAD-605 Physics Note
_
g
_
t
Risultati di CLEO
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d
Alfio Lazzaro
_ 
s
b
B0
s
_
d
W+
d
15

B–> '
• Analisi finita da tempo
• Yields negativi
• Quindi abbiamo fatto una analisi
di tipo Bayesiano
• Si sta ancora discutendo con
i referee (Bob Cahn) ed altri
esperti sul modo piu’ appropriato
di presentare i risultati
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B–> ’KL
• Supporting document : BAD-591
• Scopo : Misura di BR e Time-Dependent CP-Violating
Asymmetries ( analogo a quanto abbiamo fatto con
•Attualmente usiamo il sotto-decadimento 
un prossimo futuro verra’ aggiunto
 °g
KS)
pp
ma in
•Statistica usata : RUN 1 + RUN 2
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B–> ’KL
• Funzioni di likelihood per la
identificazione delle KL (Antimo)
• Constraint su MB e sulle direzioni
per la ricostruzione cinematica
• Analisi ML con le variabili:
Mse , M , M , Fisher
• Forte presenza di fondo comporta
tagli su cos qT  bassa  ( 6 % )
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B–> ’KL
• Ora stiamo cercando di aumentare l’efficienza di ricostruzione
sostituendo alcuni tagli e il discriminante di Fisher con una rete
neurale (NN). Uscita della rete usata come taglio per input ML
• Analisi ML utilizzando le variabili :
• Analisi cut & count nel piano :
E , M , M
( NN ,  )
• Control Sample : e+e-  g (   KS KL )
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B–> ’KS
• Stiamo misurando il BR di questo canale nel sottodecadimento
  p p e  3 p
KS p+ p-
• Stiamo aggiornando l’analisi a tutta la statistica (Run1 + Run2)
• Useremo questi dati nella prossima analisi CP-time dependent
• Supporting Document : BAD-488
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B–> 
,  ,  , 
• Stiamo misurando il BR di B nei sottodecadimenti
con g e   p p ( gg)
• Per i canali , ,   stiamo usando le varie
combinazioni dei sottodecadimenti con gg e 3p,
g e pp . In queste analisi siamo ancora agli
inizi!
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Capri 10/04/03
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21
Scarica

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