Measurement of the Amplitude Ratio of B 0 J/ K *0 to B 0 J/ K *0 (K + - ) decays
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Transcript of Measurement of the Amplitude Ratio of B 0 J/ K *0 to B 0 J/ K *0 (K + - ) decays
Max Baak 1
Measurement of the Amplitude Ratio of Measurement of the Amplitude Ratio of B B0 0 J/J/ K K*0*0 to B to B0 0 J/J/ K K*0*0 (K (K++--) decays) decays
Max BaakNIKHEF, Amsterdam
For the BaBar Collaboration
APS MeetingPhiladelphia, 8 April 2003
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Two simple conceptsTwo simple concepts
cs
c /J
0B d
b(*)0K
Wrong-flavor decay
d?
- B0 J/ K * 0
- B0 J/ K * 0
( )
( )
cs
c /J
0B d d
b(*)0K
Right-flavor decay
- B0 J/ K * 0
- B0 J/ K * 0( )
( )
s
s
d duu
0*K
K
s
s
d duu
0*K
K
To tag a K*, use charge of kaon and pion
1
2
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Can sin2ßCan sin2ßSS and sin2ßand sin2ßL L be different?be different?
• Time-dependent asymmetry for B0 J/ KS,L normally given by-
sin2ßS = sin2ßL
• Can sin2ßS and sin2ßL be different?
- SM corrections: (sin2ßS - sin2ßL) ~ 0.01
- Experimental limit: 0.02 ± 0.17
• How to find wrong-flavor decays if K0 and K0 mix into CP states? Use B0 J/ K*0 sample! Same quark-level process. Tag with
K*0 K+-.
S,L
S,L S,L/ ψ
S L SS,L
, ,L
( ( ) ) ( ( ) )( ) sin( )
( ( ) ) ( ( )sin(2β)
)B J K d
B t K B t Ka t m t
B t K B t K
sin2L = 0.723 0.158
sin2S = 0.741 0.067 Ob
serv
ed a
sym
met
ry
Grossman, Ligeti, KaganPhys.Lett.B538:327
BaBar
data
0 0 0 0/ , /B J K B J K
For different sin2ßS and sin2ßL, need non-zero wrong-flavor decay amplitudes (New Physics)
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B B J/ J/ K K*0*0 time dependent analysis time dependent analysis
B0(t) J/K*0
B0
Initialstate
Flavor eigenstate
No wrong- flavor
decays
B0(t)B0
Initialstate
Flavor eigenstate J/K*0
a) unmixed b) mixed
B0
B0
With wrong- flavor
decays
J/K*0
Standard ModelWrong-flavor
2
2
1 | λ |1 | λ |
C
2
2Im λ1 | λ |
S
0 *
0 *
/
/
A B J Kqλp A B J K
0 *
0 *
/
/
A B J Kpλq A B J K
For final state J/ K*0
replace C -C , S -S .
Extract wrong-flavor to right-flavor amplitude-ratios and from time-dependent fit to B0/B0 J/ K*0 and B0/B0 J/ K*0
=0 C=1, S=0 (standard B0B0 mixing)
*04( / , ) e c [1 + )]os(t
unmix dedf J K m tt *0
4( / , ) e cos( ) [1 - ]dt
mixedf J m tK t b)
a) *04( / , ) e [1 cos( ) + sin ( )+ ]t
unmi de dx df J S mt tmK Ct *0
4( / , ) e [1 cos sin( )( ) -- ]tmixe dd dS mf J t tCt mK b)
a)
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BaBar DetectorBaBar Detector
Cerenkov Detector (DIRC)144 quartz bars
11000 PMs
1.5 T solenoid
Electromagnetic Calorimeter 6580 CsI(Tl) crystals
Drift Chamber40 stereo
layers
Silicon Vertex Tracker5 layers, double sided
strips
e+ (3.1 GeV)
e- (9 GeV)
SVT: 97% efficiency, 15 m z hit resolution (inner layers, perp. tracks)
SVT+DCH: (pT)/pT = 0.13 % pT + 0.45 % DIRC: K- separation 4.2 @ 3.0 GeV/c 2.5 @ 4.0 GeV/c EMC: E/E = 2.3 %E-1/4 1.9 %
z
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K-K- separation with Cerenkov Detector (DIRC) separation with Cerenkov Detector (DIRC)• Good kaon-pion separation essential to distinguish
between K*0K+- and K*0 K-+ • BaBar uses DIRC: Čerenkov light in quartz angle c handle on
particle ID
(c) 2.2 mrad
K/ separation
>9
Momentum range of K and from K* < 3 GeV
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Analysis TechniqueAnalysis Technique
Fully reconstruct B mesonin state J/K*0 or J/K*0
Determine flavor of other B meson BTAG (“tagging”)
Reconstruct vertex of BTAG and compute proper time difference t
(4s)
Tag Bz ~ 110 m Reco B
z ~ 65 mJ/
K*0zcB 260 m
K+
t z/c = 0.55
At time of BTAG decay,the 2 B’s are in opposite
flavor states
z
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t distribution of mixed and unmixed eventst distribution of mixed and unmixed events
Decay Time Difference (reco-tag) (ps)
UnMixedMixed
0
10
20
30
40
50
60
-8 -6 -4 -2 0 2 4 6 8
perfect flavor tagging & time
resolution
x
UnmixMi
1 cos( ) sin( )4
f (Δ t)Bd
d
| Δ t |
d
/τ
dB
e C ΔtΔm S Δtmτ
Δ
Decay Time Difference (reco-tag) (ps)
UnMixedMixed
0
10
20
30
40
50
60
-8 -6 -4 -2 0 2 4 6 8
realistic mis-tagging & finite time
resolution
UnmixMix
cos( ) sin( )f (Δ t) 1 1 2 Resolution4 d d
Bd
d
| Δ t |/τ
BΔC Δt S Δtm Δme
τ w
w
J/ K* pdf (similar for J/ K*)Bflav Mixing pdf
D(*) , , a1 sample (Bflav) determines mistag fraction w and resolution function
tmetf dB
t
mixingd
dB
cos211τ4
)(τ
||
, Resw
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Data Sample [1999-2002]: 82 fbData Sample [1999-2002]: 82 fb-1-1 on on (4s) (4s) ResonanceResonance
Sample Ntagged PurityJ/ K*0 860 96%J/ K*0 856 96%
3 cut on E applied
‘tight’ kaon selection
* *B beamE E E
2 2* *ES beam Bm = E - p
signal region
mES [GeV/c2]
E [M
eV]
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Likelihood FitLikelihood Fit• Combined unbinned maximum likelihood fit to t spectra
of B-flavor and J/K*0 and J/K*0 samples.• Analysis performed blind.
Fit ParametersC,S,C,S 4Mistag fractions for B0 and B0 tags 12Signal resolution function 8Empirical description of background t 24B lifetime fixed (PDG 2002 value) B = 1.542 psMixing Frequency fixed (PDG) md = 0.489 ps-1
48 total free parameters
All t parameters extracted from data Correct estimate of the error and correlations
tagged flavor sample
tagged J/K*
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]sin[]cos[1),(
]sin[]cos[1),(
]sin[]cos[1),(
]sin[]cos[1),(
0*
0*
0*
0*
tmStmCtKR
tmStmCtKR
tmStmCtKR
tmStmCtKR
mix
unmix
mix
unmix
(assuming C, C and S, S are of equal size)
mixed upon wrec
occasions
• Doubly mis-IDing both K+ and - for each other fakes a K*0 for a K*0 - From MC: double mis-ID rate wrec = 0.3 %
K-K- swapping swapping
]sin[]cos[)21(1),(
]sin[]cos[)21(1),(
]sin[]cos[)21(1),(
]sin[]cos[)21(1),(
0*
0*
0*
0*
tmStmCwtKR
tmStmCwtKR
tmStmCwtKR
tmStmCwtKR
recmix
recunmix
recmix
recunmix
• To lowest order sine terms not affected, but cosine terms are.
Coefficient C S C SSyst. Error 0.004 0.001 0.003 0.001
Determined using MC
WARNING! Fake wrong-flavor decays! Need to minimize this
effect• Effect of K- swapping on time-dependent decay distributions?
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ResultResult
Source Error C/C
Error S/S
Background description 0.019 0.017t resolution and detector effects
0.016 0.021
Signal mistag fractions 0.013 0.000md and B (PDG 2002) 0.004 0.006Monte Carlo statistics 0.015 0.016K swapping 0.004 0.001Tag-side DCKM decays 0.006 0.019Total 0.034 0.039
C = 1.045 ± 0.058 (stat) ± 0.034 (syst)S = -0.024 ± 0.094 (stat) ± 0.039 (syst)C = 0.966 ± 0.051 (stat) ± 0.034 (syst)S = 0.004 ± 0.090 (stat) ± 0.039 (syst)
See my next talk!t (ps)
a) unmixed
b) mixed
c) asymmetry
Asym
met
ryEn
tries
/ 0.
6 ps
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ConclusionConclusion
• To be submitted to PRL.Assuming common wrong-flavor decay amplitudes for B0 J/ K*0 and B0 J/
K*0
2 2
2 2
1 | λ | 1 | λ |;1 | λ | 1 | λ |
C C
0 *0
0 *0
2
/
/
0.041 (90% )
0.20 (90% )
B J K
B J K
CL
CL
0 *0
0 *0
2
/
/
0.063 (90% )
0.25 (90% )
B J K
B J K
CL
CL
• No sign for wrong-flavor decays B0 J/ K*0 and B0 J/ K*0
• Using the relations:
1
2
3
Measured values Standard Model
0.17 (90% )CL
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Backup SlidesBackup Slides
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Cerenkov Particle Identification System (DIRC)Cerenkov Particle Identification System (DIRC)• Good kaon-pion separation essential to
distinguish between K*0K+- and K*0
K-+ • DIRC: Čerenkov light in quartz
Transmitted by internal reflectionRings projected in standoff boxDetected by PMTsEssential for Kaon ID >2 GeV
K- separation > 4
for this analysis
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B Flavor Tagging MethodsB Flavor Tagging Methods• In BaBar tagging is handled with Neural
Nets• Information used:Primary leptonSecondary leptonKaon(s)Soft pions from D* decaysFast charged tracks
0
0 *
0
0 0
,,
, s
B D lB D D K lB DX D K XB D X D D
l ,
K b c s
W W
l
Tagging category
Fraction of tagged events(%)
Wrong tag fraction w (%)
Q = (1-2w)2 (%)
Lepton 9.1 0.2 3.3 0.6 7.9 0.3
Kaon+Kpi 16.7 0.2 9.9 0.7 10.7 0.4
Kaon+Spi 19.8 0.3 20.9 0.8 6.7 0.4
Inclusive 20.0 0.3 31.6 0.9 0.9 0.2
ALL 65.6 0.5 28.1 0.7
Smallest mistag fraction
The errors on C,S,C,S
scale with quality Q
1Q
Mistag fraction w determined with flavor eigen-states sample Bflav (23.7k events,
purity 82%)