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Vincenzo Vagnoni

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Title: Vincenzo Vagnoni


1
  • Vincenzo Vagnoni
  • Umberto Marconi
  • INFN Bologna
  • Joint Physics Meeting with CERN Theory Group
  • 28th LHCb Week
  • February 28th 2003

2
Overview
  • B0(s) ? h?h? decay selection
  • Selection strategy
  • Determination of the optimal cuts
  • Annual yields and background over signal ratios
  • CP sensitivities
  • Toy Monte Carlo to generate event by event proper
    time distributions
  • Evaluation of ?Adir and ?Amix after one year of
    LHCb data taking
  • Two different approaches
  • ?2 fit of the binned asymmetry
  • Unbinned maximum likelihood estimation
  • Consistency checks
  • Conclusions

3
VELO 21stations (Rmin 8mm) Si 220 mm, strips R
e f
6?5 m2
3 Tracking stations IT Si strips OT straw tubes
TT1.4?1.2 m2 Si microstrips
4
B decay selection strategy
  • MC samples used size (number of events)
  • B0 ? pi pi- 60k
  • Bs ? K K- 65k
  • B0 ? K pi- 62k
  • Bs ? K- pi 24k
  • ?b ? p K- 20k
  • ?b ? p pi- 21k
  • inclusive bb background 1.144M
  • Procedure followed to tune selection
  • Determine offline cuts which maximize the signal
    efficiency but a) reject all the background
    from the (limited) inclusive bb sample b)
    provide good rejection of the specific background
    events
  • Multivariate brute force approach to establish
    the best cut values
  • grid scan over 11-dimension selection parameter
    space
  • reject all the bb background events in 600
    MeV/c2 mass window
  • maximize S / sqrt(SB) with B ? channel specific
    background
  • Determine trigger cuts which maximize the
    efficiency for offline-selected events at fixed
    trigger output rate (determined with min. bias
    sample)
  • only 20 times the signal statistics, but
    BR(signal) ltlt 1/20
  • only 1/2 minute of data-taking at nominal LHCb
    luminosity !

5
B0(s) ? h?h?Selection cuts
  • Charged tracks
  • Each leg identified as a K, or a particle lighter
    than K (using RICH)
  • Cuts on
  • p
  • max. pT
  • min. pT
  • max. IP/?IP
  • min. IP/?IP
  • ?2 of common vertex
  • B candidate
  • Cuts on
  • pT
  • IP/?IP
  • L/?L
  • mass

6
Breakup of the optimal cuts
Parameters used for selection Parameters used for selection Parameters used for selection B0 ? pi pi- B0 ? pi pi- B0 ? K pi- B0 ? K pi- Bs ? K K- Bs ? K K-
pi, K smallest pt (GeV/c) gt 0.65 gt 0.15 gt 0.3
pi, K largest pt (GeV/c) gt 3.1 gt 2.5 gt 2.25
pi, K p (GeV/c) ? 2.5, 100 ? 2.75, 200 ? 2.75, 125
pi, K smallest IP/?IP gt 5.75 gt 7 gt 4
pi, K largest IP/?IP gt 6 gt 7.25 gt 4.5
pi, K vertex fit ?2 lt 6.75 lt 6 lt 20
B pt (GeV/c) gt 1.6 gt 2.25 gt 0.6
B IP/?IP lt 2.5 lt 3.25 lt 2.75
B L/?L gt 7.25 gt 8 gt 7.25
B ?m (MeV/c2) lt 45 lt 55 lt 45
7
Rejection of physics background
B0(s) ? h?h? selections
  • Relying on
  • RICH PID
  • mass resolution (18 MeV/c2 single Gaussian)

B0 ? pi pi-
B0 ? K pi-
BS ? K K-
8
Rejection of combinatorial background (B0? pi
pi-)
incl. bb
signal
  • Assume combinatorial background dominated by bb
    events
  • Can reject all generated bb background
  • also when relaxing B mass cut
  • Preliminary estimate

B/S lt0.7
  • Contribution of ghost tracks to the combinatorial
    background is negligible

9
Inclusive bb background mass spectra
B0 ? pi pi-
B0 ? K pi-
BS ? K K-
Before cuts
After cuts
GeV/c2
GeV/c2
10
Annual yields and B/S ratios
Event type MC sample Efficiency Efficiency B/S B/S Untagged annual yield
Event type MC sample Selection Trigger specific bb inclusive (CL 90) Untagged annual yield
B0 ? pi pi- 60000 0.073 0.31 0.088 lt 0.7 27000
B0 ? pi pi-
B0 ? K pi- 62000 0.084 0.29 0.046 lt 0.2 115000
B0 ? K pi-
Bs ? K K- 65000 0.10 0.27 0.049 lt 0.5 35000
Bs ? K K-
11
Tagging
  • LHCb TP (using only opposite side tagging)
  • ?tag 0.4
  • ?tag 0.3
  • ?tag (1-2?tag )2 6.4
  • Preliminary studies with the current simulation
    indicate a similar result
  • Other methods to be added (analysis on going)
  • Bs tag with Kaon same side
  • Bd tag with Pion same side
  • Jet charge
  • In the following we will assume the TP numbers

12
B0 ? pi pi- BS ? K K- CP sensitivities
  • Two approaches used
  • ?2 fit of the binned asymmetries
  • Unbinned maximum likelihood
  • Tagged event samples generated by means of a toy
    MC taking into account
  • Annual event yield S
  • Background over signal ratio B/S
  • Tagging efficiency ?tag
  • Wrong tag fraction ?tag
  • Proper time resolution function R(?-t)
  • Acceptance ?reco(?)

B0 ? pi pi- BS ? K K-
S (1 year) 27000 35000
B/S 0.8 0.55
xq 0.755 20
?tag 0.4 0.4
?tag 0.3 0.3
Adir 0.19 -0.17
Amix 0.62 -0.27
13
B0 ? pi pi-
Proper time resolution
Proper time acceptance
Single Gaussian fit ?411 fs
ps
14
CP Asymmetryrelevant formulae
15
Example of fitted asymmetries
  • All the following plots correspond to one year of
    data taking

16
Check of fit consistency ?ACP / ?(ACP)
distributions
  • Fit of 500 asymmetries generated with different
    random seeds
  • Distributions consistent with N(0, 1)

17
Adir vs Amix
  • Scatter plots obtained with a multiquadric
    smoothing due to limited statistics (500 trials)

18
Dependence of ?Adir and ?Amix on B/S
Current estimate of B/S
  • Expected error dependence on B/S reproduced

19
Unbinned maximum likelihood approach
  • Maximize log likelihood with respect to Adir and
    Amix

20
log likelihood plots
21
log likelihooderror ellipses and 68.27
confidence regions
22
Check of log likelihood approach consistency
  • 500 event samples generated with different random
    seeds

23
log likelihooddependence of ?Adir and ?Amix on
B/S
24
Dependence of ?Adir and ?Amix on the years of
data taking
25
Conclusions
  • ?Adir and ?Amix after one year of LHCb data
    taking have been estimated
  • Least ?2 fit of the binned asymmetry and unbinned
    maximum likelihood estimation give consistent
    results

B0 ? pi pi-
BS ? K K-
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