Title: L.Lista INFN Sezione di Napoli
1L.Lista INFN Sezione di Napoli
Results of BABAR experiment on CP violation and B
physics
2Outline
- Experimental set-up
- CP asymmetries
- sin2b
- sin2?eff
- B Mixing and lifetime
- Rare B decays
- Conclusions
- (Many topics will be skipped)
?(4S)
3The PEP-II B-Factory
4Integrated Luminosity
32 Million Y(4S) decays recorded
- BaBar recorded
- 37.7fb-1
- 4.05 fb-1 off peak
- Top luminosity
- 3.4x1033 cm-2s-1
- Design
- 3x1033 cm-2s-1
5The BaBar detector
6The Unitarity Triangle
- Quark mixing is described by the CKM matrix
- Unitarity relations on matrix elements lead to a
triangle in the complex plane
?
?
?
1
7CP violation at asymmetric B factory
CP violation via mixing interference
fCP eigenvalue
? e-2ib
For golden b?ccs modes
8sin2b Improvements w.r.t. run I
- More data!
- Added new modes
- ?c1KS, J/?K0
- Improved reconstruction efficiency
- Improved tracking
- 30 KS reconstruction eff.
- Improved vertex resolution
- New alignments
- More elaborated vertex algorithm
- Optimized KL selection taking into account the
background CP asymmetry - Maximize (SAB/ASB)2/(SB), not S2/(SB)
9All sin2b CP modes
hCP 1
IFR
B0?J/?K0L
KL momentum not measured DE determined from B
mass and beam energy constraints
N129 (65 pur.)
hCP -1
B0?J/?K0S B0??(2S)K0S B0??cK0S
N724
EMC
N128 (56 pur.)
Golden modes 30 higher efficiency than run 1
KS efficiency improved
10Fully reconstructed B flavor modes
- Cabibbo favored decays
- B0?D()-p/r/a1
- B? D()0 ? , J/??K, ?(2S)K
11Mixing and CP asymmetry of B0/B0
CP modes FCP?(Dt) ? e-Dt/tB ( 1 ? hCP sin2b .
sin Dmd Dt )
Flavour specific modes
Fflav?(Dt) ? e-Dt/tB ( 1 ? cos Dmd Dt )
mixed B0B0 or B0B0
12Imperfect tagging and resolution
D 1-2w dilution, w wrong tag fraction R(Dt)
resolution function
Imperfect tagging
Imperfect resolution
B0 B0
e-Dt/tB (1? hCP sin2b ? sin Dmd Dt)
e-Dt/tB (1? hCP D sin2b ?sin Dmd
Dt)
e-Dt/tB (1? hCP D sin2b ? sin Dmd Dt) ?
R(Dt)
unmixed mixed
e-Dt/tB (1? cos DmdDt)
e-Dt/tB (1? D cos Dmd Dt)
e-Dt/tB (1? D cos DmdDt) ? R(Dt)
13Fitting Procedure
- Unbinned maximum likelihood fit
- Mistag and resolution empirical distribution
- fitted from data
- fixed in the fit
- ?md 0.472 ps-1 (was extracted from the same fit
in Run-I analysis) - tB 1.548 ps
Parameter sample
sin2? 1 CP
w and ?w 8 Flavor
?t resolution 16 Flavor, CP
Bkgd w 8 Sidebands
Bkgd ?t 12 Sidebands
Separate for Run I II
Largest correlation With sin2b 13
14Flavor misid. measurement
e
w
D1-2w Qe(1-w)2 s(sin2b) ? 1/?(Q)
Neural network mainly to recover unidentified
leptons and use soft pions from D
15sin2b result
sin2b 0.59 0.14stat 0.05syst
16Comparison of different samples
Submitted to Phys. Rev. Lett. On July 5 2001
17Unitarity triangle
sin2b 0.59 0.14stat 0.05syst
18Search for direct CP violation
- Assuming more than one amplitude dominate the
decay - ? may be ?1
- Only ?CP -1 used
- High purity, no assumption needed on CP of the
background - No evidence found (none expected from SM)
?0.93 0.09 0.03
19Systematic errors
- 0.03 from vertexing
- 0.03 from tagging
- 0.02 from background
- Total 0.05
20Dmd measurement
preliminary
Dmd 0.519 0.020stat
0.016syst ps-1
Run I only
21Lifetime results
B?
B0/B0
background
Dt (ps)
Dt (ps)
t0 1.546 ? 0.032(stat) ? 0.022(syst) ps t ?
1.673 ? 0.032(stat) ? 0.022(syst) ps t0 /t?
1.082 ? 0.026(stat) ? 0.011(syst)
common resolution
22Charmless Hadronic Decays
- Significant penguin contribution
- Direct CP violation studies
- Measurement of ? from time-dependent asymmetry
isospin analysis - Possible field for new physics
p-(K-)
Vud(s)
d(s)
W-
Vub
b
p
u
B0
Cabibbo suppressed tree diagram
p-(K-)
Vtd(s)
W-
d(s)
Vtb
p
b
u
t
B0
Penguin diagram
23Two body Branching fractions
control sample D??D0, D0?K-?
gt 3 sigma
Run I only
p (GeV/c)
24CP violation in B0???- sin2aeff
- Neglecting penguin pollution
- ? ?f e-2i(???) ?f e2i? ? C??0, S?? sin2?
- Considering penguin diagrams
- ? ? 1
- C?? ? 0, S?? sin2?eff sin2? ? f (Penguin /
Tree) - Extraction of sin2? requires the study of B0??0?0
and B0??0?0 - Fitted simultaneously with branching fractions
- Dilutions and time resolutions taken from sin2b
fit
Run I II
expected 0.3
preliminary
S?? 0.03 0.53-0.56 ? 0.11 C ?? 0.25
0.45-0.47 ? 0.14
ACP(Kp-) -0.07 ? 0.08 ? 0.02
25Radiative Penguin B ? K?
Signal B0 ? K0?, K0 ?
K?- Backgrounds ee- ? qq ? ee- ? qq ? X
?0
- Sensitive to top quark couplings
- CKM matrix elements Vtd,Vts
- Sensitive to New Physics
- SUSY, Charged Higgs
- No CP asymmetry in the Standard Model (lt 1)
- Possible sources beyond SM
26B0 ? K0? yield and branching ratio
B0 ? K0? K0 ? Kp-
- Nsignal 139.2 ? 13.1 events
- Br(B0 ? K0?) (43.9 ? 4.1 ? 2.7) ? 10-6
- Br(B ? Kll-) lt 0.6 ? 10-6 (90 C.L.)
- Br(B ? Kll-) lt 25.7 ? 10-6 (90 C.L.)
27B??K, B??K
Max Lik. Fit projections
- B??K (7.7 1.6-1.4 ? 0.8) ? 10-6
- B ??p lt 1.4 ? 10-6 (90 C.L.)
- B ??K (9.7 4.2-3.4 ? 1.7) ? 10-6
- Possible measure of sin2b
- B0 ??K0 (8.6 2.8-2.4 ? 1.1) ? 10-6
- B0 ??K0 (8.1 3.1-2.5 ? 0.8) ? 10-6
28Quasi 2-body and 3-body decays
- B??p ( 6.6 2.1-1.8 ? 0.7 ) ? 10-6
- B0??K0 lt 12 ? 10-6
- B???K ( 70 ? 8 ? 5 ) ? 10-6
- B0???K0 ( 42 13-11 ? 4 ) ? 10-6
- B??K ( 22.1 11.1-9.2 ? 3.3 ) ? 10-6
- B0??K0 ( 19.8 6.5-5.6 ? 1.7 ) ? 10-6
- B0?K0 p lt 28 ? 10-6
- B??0K lt 39 ? 10-6
- B??0p lt 39 ? 10-6
- B?Kpp- lt 54 ? 10-6
- B?ppp- lt 22 ? 10-6
- B0???p ( 49 ? 13 6-5 ) ? 10-6
- B0?a0(980)?p
- ?Br(a0 ??p) ( 6.7 3.2-2.7 ? 1.3 ) ? 10-6
Potential for sin2a
?
First Observation
?
29Search for direct CP violation
30B ? DD()K
- Study of the b?ccs transition
- Experimental inclusive estimate from from B?DSX,
(cc)X, ?CX, ?CX (ALEPH, CLEO) - Br(b?ccs) 15.8?2.8
- Theoretical calculation cant determine this low
value together with inclusive s.l. branching
ratio (b?cW) - Three-body B ? DDK can contribute
- Study of color suppressed modes (B? DD-K)
Color allowed
Color suppressed
31B ? DD()K
- Reconstructed decays
- D? D0p
- D0? D0p0
- D0? D0g
- D0? K-p
- D0? K-pp0
- D0? K-pp-p
- D? K-pp
- Br(B0? DD0K) (0.28?0.07?0.05)?10-2
- Br(B0? DD0K) (0.68?0.17?0.17)?10-2
- Br(B? DD-K) (0.34?0.16?0.11)?10-2
- First observation of color suppressed mode other
than B ? (charmonium)X
B0 (all modes) NS 180?21
B (all modes)NS 117?15
B? DD-K NS 8.2?3.5
32Conclusions
- sin2? extracted from 37.7 millions of BB events
- sin2b 0.59 0.14stat 0.05syst
- CP violation established at 4.1? level
- First measurement of CP violation in B0?????
- High precision measurements of mixing parameter
and lifetimes - High precision measurements of B decays branching
fractions - Many newly observed decays
- Most of the results are still statistically
limited
33Backup slides
34J/? K angular analysis
J/? rest frame K decay plane
Channels without p0
Channels with p0
- L0,1,2 waves
- Both CP even and odd amplitudes are present
- Measurement of sin2b is possible from angular
analysis
- f ( cos?tr, cos?K, ?tr )
- f1 A02 f2 A2 f3A?2
- f4 Im(A A?) f5 Re (A0 A)
- f6 Im (A0 A?)
A?2 0.160?0.032 ? 0.014 CP odd, P wave
A2 0.243?0.034 ? 0.017 CP even, SD wave
A02 0.597?0.028 ? 0.024 CP even, SD wave
?? arg(A?/A0)-0.17?0.16 ?0.07
? arg(A /A0)2.50?0.20 ?0.08
Time dependent CP asymmetry dilution factor D
1 2 A?2 0.68?0.10
35B0 ? DD-
- Cabibbo suppressed decay
- A measurement in b?ccd of CP violating
time-dependent asymmetry can be performed from
angular analysis - Possible penguin contamination
- Measurement of sin2b independent from B0?J/?K0S
- Significant deviations from B0?J/?K0S measurement
of sin2b may be indication of new physics
Tree diagram
Penguin contribution
- Branching ration measurement of B ? D()D()-
36B0 ? DD-
Br(B0?DD-) (8.0 ? 1.6 ? 1.2)?10-4
37Inclusive Charmonium decays
c
J/?, ?(2S), ?c
b
c
W-
B0, B-
s, d
X
d,
u
- Inclusive J/? branching ratio
- Br(B?J/?X) (1.044?0.013 ?0.028) ? 10-2
- Br(B?J/?X dir.) (0.789?0.010 ?0.034) ? 10-2
- Inclusive ?(2S) branching ratio
- Br(B? ?(2S) X) (0.275?0.020 ?0.029) ?10-2
- ?(2S)?ll- branching ratio
- ?(2S) ? ee- (7.8 ? 0.9 ? 0.8)?10-3
- ?(2S) ? ??- (6.7 ? 0.8 ? 0.7)?10-3
- Inclusive ?c branching ratios
- Br(B? ?c1 X) ( 0.378 ? 0.034 ? 0.026 ) ?
10-2 - Br(B? ?c1 X dir.) ( 0.353 ? 0.034 ? 0.024 ) ?
10-2 - Br(B? ?c2 X) lt 0.21?10-2 _at_ 90 C.L.
( 0.137 ? 0.058 ? 0.012 ) ? 10-2
Br(?(2S) ? J/?pp-) assumed from PDG
38Exclusive B decays
- Main motivation
- Channels are used for CP violation measurements
- Kinematics selection
- Energy substituted mass
- Independent on particle mass hypotheses
- Energy difference in the center of mass
B0?J/? ?0
First observation B0??c1 K0
39J/? production in continuum
- First observation of J/? production in continuum
- ? (4S) events with pJ/?gt2 GeV/c
- Off-resonance events
Angular distribution ?1A cos2q
- A (all E) 0.25 ? 0.19
- A (pgt3.5 GeV) l 0.62 ? 0.39
- Color singles prediction ? ? 0.8 pb A ?
0.8, - NRQCD (c.o.) prediction ? ? 2.8 pb 0.6ltAlt1.0
40Branching ratios results
Mode Br (?10-4)
B0 ? J/? ?0 0.20 ? 0.06 ? 0.02
B0 ? J/? K0 12.4 ? 0.5 ? 0.9
B ? J/? K 13.7 ? 0.9 ? 1.1
B ? J/? K 10.1 ? 0.3 ? 0.5
B0 ? J/? K0 (KL) 6.8 ? 0.8 ? 0.8
B0 ? J/? K0 (KS??0?0) 9.6 ? 1.5 ? 0.7
B0 ? J/? K0 (KS???-) 8.5 ? 0.5 ? 0.6
B0 ? J/? K0 (All) 8.3 ? 0.4 ? 0.5
B0 ? ?c1 K0 4.8 ? 1.4 ? 0.9
B0 ? ?c1 K0 5.4 ? 1.4 ? 1.1
B ? ?c1 K 7.5 ? 0.8 ? 0.8
B ? ?(2S) K 6.3 ? 0.5 ? 0.8
B0 ? ?(2S) K0 6.8 ? 1.0 ? 1.1
Br(B?J/??)/ Br(B?J/?K ) (3.91?0.78 ?0.19)?10-2
RUN 1 22.7 MBB
41Dmd measurement the di-lepton analysis
Dmd 0.499 0.010 0.012 ps-1
42Semileptonic B decays
- Determine the sign of the B from a sample of
14000 fully reconstructed B - B0?D()-?, D()-?, D()-a1, J/?K0
- B- ?D()0?, J/?K, ?(2S)K
- Lepton identified in the decay of the other B
B
B0
Mixing corrected
43b?s?, B0 ? ??
mES for 0.6 ltmhad lt 2.0 GeV
- Semi-exclusive study
- Sum of exclusive modesKnp (n1,2,3)
Branching ratio measurementcoming soon
B0 ? ??
- Theoretical exp. 10-8
- Br(B0???) lt 1.7 x 10-6 90 C.L.
- PDG Br(B0 ???) lt 3.9 x 10-5 90 C.L. (L3)