Measurements of a and future projections
description
Transcript of Measurements of a and future projections
Measurements of and future projections
Fabrizio BianchiUniversity of Torino and INFN-Torino
Beauty 2006 The XI International Conference on B-Physics at
Hadron Machines
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Outline Introduction to the measurement of
Results from the B-factories: B ±
±
Summary and outlook
Will not cover expectations at LHC and Super B-Factories
See talks of P. Robbe and A. Bevan
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Measuring
)(cos)(sin))(())((
))(())(()(
00
00
tmCtmSftBftB
ftBftBtA
dd BBCP
0
)2sin(
222
C
S
eeeA
A
p
q iii
Access to from the interference of a b→u decay () with B0B0 mixing ()
sin
)2sin(1 2
C
CS eff
ii
iii
eePT
eePTe
2
Inc. penguin contribution
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From eff to : Isospin Analysis
0hhB
)(~
)(
)(~
)(
)(~
)(
00000
00000
00
00
0
0
hhBAA
hhBAA
hhBAA
hhBAA
hhBAA
hhBAA
Gronau and London, Phys. Rev. Lett. 65, 3381 (1990)
Neglecting EW Penguins: is a pure tree mode.The triangles share a common side.
Assume SU(2) symmetry among amplitudes
00 ~ AA0hhB
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Time Dependent Analysis Outline
Fully reconstruct the B decaying to a CP eigenstate.
Tag the flavor of the other B. Mis-tag probability measured in Bflav sample.
Measure t.
Extract S and C with a ML fit on a signal enriched sample. Signal PDF from MC. Background PDF from MC or sidebands
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Variables used in the ML fit
2*2*BbeamES pEm **
beamB EEE
signal signal
background background
Event TopologyCombine variables in F or N
PID info: DIRC + dE/dX (BaBar) Aerogel + dE/dX (Belle)
t
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:results (preliminary)
0B
Background Signal
mE
S
mE
S
E
E
347 million BB
0B
sPlotN = 675±42
hep-ex/0607106
B0tag
B0tag
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:results (preliminary)
535 million BB
0B
N = 1464±65
hep-ex/0608035
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:results (preliminary) 0B
C = - 0.55 ± 0.08 ± 0.05S= - 0.61 ± 0.10 ± 0.04
C = - 0.16 ± 0.11 ± 0.03S = - 0.53 ± 0.14 ± 0.02
(S, C) = (0.0, 0.0) excluded at 3.6
Observation of Direct CPV at 5.5 Observation of mixing-induced CPV at 5.6
347 million BB
535 million BB
2.3 discrepancy
C =−A
Belle
BaBar
Average
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(preliminary)0000 , B
347 million BB
hep-ex/0607106
N = 140 ± 25N± = 572 ± 53
0 B
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constraint from B
No stringent constraintfrom system alone need and
|| < 41o at 90% C.L.
Frequentist interpretation: use only the B→branching fractions and isospin-triangle relations.
eff
1-
C.L
.1-
C.L
.
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The analysis
Worse than at first sight: V V final state. Mixture of CP = +1 and 1: need to
know each fraction
However: ~100% longitudinally polarized (~pure CP-even
state) no need for elaborate angular analysis
Branching fraction for B0 is larger than
Branching fraction for B0 is small (~1.1x10-6) small penguin pollution
0B
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results (preliminary)
0B
347 million BB
hep-ex/0607098
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results
0B
09.041.008.0
09.030.000.0
long
long
S
C68.2
6.2 10)8.38.22( BR
275 million BB
PRL 96, 171801 (2006)
030.0941.0 034.0040.0
Lf
0B
N = 194±32
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results (preliminary)
0B
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results (preliminary)
0 B
232 million BB
hep-ex/0607092
N =390 ± 49
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results (preliminary)
000 B
347 million BB
hep-ex/0607097
N = 98 ± 32 ± 22
3.0 evidence
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constraint from B[71, 105]o
at 68.3% C.L.
Frequentist interpretation: use only the B→ρρbranching fractions, polarization fractions and isospin-triangle relations.
First evidence of B→00
Constraint on is less stringent
PRL 96, 171801 (2006)hep-ex/0607098
Use BR(B->00)<1.1 X 10-6
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The Dalitz analysis00 )(B
A. Snyder and H. Quinn, Phys. Rev. D, 48, 2139 (1993)
B0
B0
Monte Carlo
(1450) and (1700) are included
Interference provides information on strong phase difference
Time-dependent Dalitz-plot analysis assuming isospin simmetry.
26 coefficients of the bilinear form factor terms occurring in the decay rate are measured with a UML fit. Physically relevant quantities are derived from subsequent fits to these coefficients.
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analysis (preliminary) 00 )(B
hep-ex/0608002347 million BB
m’ and ’ are thetransformed Dalitz variables
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analysis (preliminary)00 )(B
hep-ex/0609003449 million BB
mass
helicity
Dalitz + Isospin (pentagon) analysis 26(Dalitz) + 5(Br(), Br(+0), Br(0+), A(+0), and A(0+))
SignalSCFBB bkgcontinuum
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constraint from (preliminary)
00 )(B
[0,8]o U [60,95]o U[129,180]o
at 68.3% C.L.
(deg) (deg)
1-
C.L
.
1-
C.L
.
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constraints
B-Factories = [ 93 ] º +11-9
Global Fit = [ 98 ] º +5-19
Belle result is not included.It will weakens the suppressionof solutions around 0o and 180o.
Nice agreement B-Factories = [92 ± 7]o (SM Solution)
Global Fit = [93 ± 6]o
CKMfitter http://ckmfitter.in2p3.fr/UTfit http://utfit.dreamhosters.com/
B-Factories
Global Fit
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Pending Issues
Discrepancy on C
Solutions at 0o and 180o should be (more) suppressed. Using nice suppression from BaBar, not from Belle.
Background modeling.
Interference with other resonances or non-resonant component in , modes.
Subtleties on statistical analysis with small statistics.
C = - 0.16 ± 0.11 ± 0.03
C = - 0.55 ± 0.08 ± 0.05
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Uncertainties on extraction Possible contribution of EW penguin and isospin
breaking effect. EW penguin effect seems to be small (~2°). Other isospin breaking effect ~ O(1°).
[M.Gronau and J.Zupan PRD 71, 074017(2005)]
I=1 contribution due to finite width of mass ( mode).[A.Falk et al. PRD 69, 011502(R)]
Too small to be an issue at B-factories
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Summary and Outlook The three modes are complementary.
Need to study them all.
Good agreement between the CKM fit ( determined by others) and direct measurements.
Still a lot to do. Refine previous analysis and exploit new ideas:
from B->a1 ? Constraint on from B0->+- and B+->K*0+
[M. Beneke et al., Phys. Lett. B638, 68(2006)] Doubling of statistics at the B-factories is much needed.
Looking forward to LHC and to a Super B-Factory.
Backup Slides
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)(cos)(sin
))(())((
))(())(()(
00
00
tmCtmS
ftBftB
ftBftBtA
dCPdCP
CP
BfBf
CPphysCPphys
CPphysCPphysf
0B
0B
CPfCP
mixin
g
decay
0t
tCPfA
CPfA
CP
CP
CPCP
f
fff
A
A
pq
ηλ
CP eigenvalue i2e
Amplituderatio2
f
2f
f||1
||1C
CP
CPCP
2f
ff
||1
Im2S
CP
CPCP
Time Dependent CP Asymmetry
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BABAR Detector
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DIRC: Control samples for and
K
K
Projection for 2.5 < p < 3 GeV/c
* 0From ( )D KD
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:results (preliminary) 0B
C = - 0.16 ± 0.11 ± 0.03S = - 0.53 ± 0.14 ± 0.02
(S, C) = (0.0, 0.0) excluded at 3.6
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:results (preliminary) 0B
A = + 0.55 ± 0.08 ± 0.05S= - 0.61 ± 0.10 ± 0.04Observation of Direct CPV at 5.5
Observation of mixing-induced CPV at 5.6
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constraint from B
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constraint from B
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formalism
)]cos(()()sin()(1[8
))(1())((/||
tmCCQtmSSQ
eAtB
tagtag
t
CP
CAC
CACAA
CAC
CACAA
CP
CPCP
CP
CPCP
)(1
)()()(
)(1
)()()(
S
Direct CP Violation
CP violation in the interference with and without B mixing.
00 )(B
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parameters (prelim)00 )(B
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Direct CP violation in 00 )(B
Significance for non-zero DCPV:BaBar: 3.0 Belle: 2.4