Analysis of the B 0 D 0 K* 0 decays at LHCb
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Transcript of Analysis of the B 0 D 0 K* 0 decays at LHCb
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 1 / 19 IOP HEPP Annual Meeting
Analysis of the B0D0K*0 decays at LHCb
Outline:• The LHCb detector• B0 D0K0* event selection• B0 D0K0* sensitivity studies• Conclusion
Jacopo Nardulli RAL
IOP HEPP Annual Meeting
Lancaster 31/3 2/4
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 2 / 19 IOP HEPP Annual Meeting
LHC tunnel
CMSALICE
ATLAS
LHCb CERN
Geneva airport
The Large Hadron Collider (LHC)Start: 2008
LHC LHCb:p-p collisions with 14 TeV L ~ 2 .1032 cm-2s-1 (mostly single interactions)Bunch crossing @ 40MHz (25 ns ) ~ 14 Million collisions per second
1 in 160 collisions is B physicsInelastic pp collisions/crossing
LHCb
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 3 / 19 IOP HEPP Annual Meeting
Physics motivations
B-factories and the Tevatron Winter 2007
LHCbLHCb L=10 fb L=10 fb-1-1
%8.1/)(
%6.3/)(
==
ηησρρσ
Unitarity Triangle prospectsfrom LHCb only (2014)
In this talk I’ll concentrate on a clean mode for γ extraction: B0D0K0*
%7.4/)(
%17/)(
==
ηησρρσ
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 4 / 19 IOP HEPP Annual Meeting
B production
• B hadrons are mostly produced in the forward direction (along the beam)
• Choose a forward spectrometer10–300 mrad
• Both b and b in the acceptance: important to tag the B flavour at production to study CP violation
(PYTHIA)
b–b correlation
Parton 1 Parton 2
p p
Boostb
b-
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 5 / 19 IOP HEPP Annual Meeting
p p
~ 300 mrad
10 mrad
Forward spectrometer (running in pp collider mode)
LHCb Detector
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 6 / 19 IOP HEPP Annual Meeting
Vertex locator around the interaction region
LHCb Detector
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 7 / 19 IOP HEPP Annual Meeting
Tracking system and dipole magnet to measure angles and momenta p/p ~ 0.4 %Magnetic field regularly reversed to reduce experimental systematics
LHCb Detector
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 8 / 19 IOP HEPP Annual Meeting
Two RICH detectors for charged hadron identificationProvide > 3σ \K separation for 3 < p < 100 GeV
LHCb Detector
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 9 / 19 IOP HEPP Annual Meeting
Calorimeter system to identify electrons, hadrons and neutralsImportant for the first level of the trigger
e
h
LHCb Detector
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 10 / 19 IOP HEPP Annual Meeting
Muon system to identify muons, also used in first level of trigger
LHCb Detector
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 11 / 19 IOP HEPP Annual Meeting
Decays of interests are B0 D0K*0 with D0 K± π± and K*0 K+π-
B0 D0K*0 with D0 K±π±
analogously we have B0 D0 K*0 with K*0 K-π+ and B0 D0 K*0
Finally there are also the decays to CP eigenstates: D0 K+K- or D0 π+π-
A bit of theoryDecays of interests
• Extraction of γ through CP modes originally proposed by Gronau - London - Wyler: Phys. Lett. B253, 483 (1991)• Possibility of using not only CP modes proposed by Atwood - Dunietz - Soni Phys.Rev.Lett. 78 3257 (1997)
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 12 / 19 IOP HEPP Annual Meeting
• LHCb cannot easily measure CP odd states GLW alone is not enough
• Combining GLW and ADS solves problem (using also non CP modes)
• We have 6 equations and 5 unknowns: rB, δB, δD, γ and N Kπ
• NCP is determined from NKπ taking in account the different BR and efficiencies
• Method described in LHCb note 2005-066.
A bit of theory
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 13 / 19 IOP HEPP Annual Meeting
D0D0 b u
s
d
c
d
b c
s
d
u
d K(*)0 K(*)0B0 B0
VcbVub
4.01
|)(|
|)(|0*00
0*00
≈≈ →
→=
cb
ubB V
V
KDBA
KDBAr
λ
•Both diagrams colour-suppressed similar magnitude and large interference
• Decays of D0, D0 to same final state gives access to interference
• Modes with K*0→ K+π- are self-tagging: sign of kaon charge distinguishes B0
K*0→ K-π+ from B0
• Branching fractions involved all rather small
A bit of theory
K+u
D0 c ds
uu - D0
-du
u
s
u K+c
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 14 / 19 IOP HEPP Annual Meeting
K
h
h
πK*0
B0dPV
D0
Decay topology and event selection
Analysis described in LHCb public note: 2007-050
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 15 / 19 IOP HEPP Annual Meeting
Mass resolution
B0 K* D0
B0 mass K0* mass D0 mass
μ ~ 5276 MeVσ ~ 14 MeV
μ ~ 892 MeVσ ~ 32 MeV
μ ~ 1864 MeVσ ~ 8 MeV
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 16 / 19 IOP HEPP Annual Meeting
Monte Carlo Selection Results(on 2/fb of data)
Channel Annual yield B/S
B0D0(K+π-)K0* 3350 < 2.1
B0D0(K+π-)K0* 536 < 12.8
B0D0(K+K-)K0* 474 < 4.1
B0D0(+π-)K0* 134 < 14
• Most of the background arises from π/K misidentifications, where we have a ρ0 instead of a K*0. Other background comes from D* resonances•The limits are calculated, assuming Poisson statistics, after none of the original 34 M bbar passes the event selection.
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 17 / 19 IOP HEPP Annual Meeting
TOY MC Results: 1000 experiments (2/fb each)
rB Input : 0.4
δB Input : 10o
γ Input : 60o
δD Input : 12o
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 18 / 19 IOP HEPP Annual Meeting
Scans
δB ScanrB Scan δD Scan
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 19 / 19 IOP HEPP Annual Meeting
Summary
• The B0D0K0* decays offer a “penguin free” way to extract the CKM angle γ• An event selection has been studied on Monte Carlo data, which will allow LHCb to achieve a good S/B for all studied decay channels. It was found that low background levels are crucial in particular for B decays with D0 CP modes. Therefore a tighter event selection has been developed for these rarer decay modes. • Using B0D0(hh)K0*
decays, γ can be determined with a statistical error better than 10 degrees with one year of data at nominal luminosity for rB > 0.3.
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 20 / 19 IOP HEPP Annual Meeting
Back Up Slides
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 21 / 19 IOP HEPP Annual Meeting
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 22 / 19 IOP HEPP Annual Meeting
Particle identification through RICH system p/K/π separation
Invariant mass (no PID)
ππ hypothesis
Clean samples through expected PID performance of RICH system
Invariant mass (with PID)
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 23 / 19 IOP HEPP Annual Meeting
Results : a badly behaved case (2/fb)
rB Input : 0.4
δB Input : 120o
γ Input : 60o
δD Input : 3o
Jacopo Nardulli Lancaster 1/04/2008B0 D0K0* Analysis in LHCb 24 / 19 IOP HEPP Annual Meeting
Sensitivity studies
• A TOY for the extraction of γ in the B0D0K*0 has been developed• In the TOY the following equations are parameterized
• We have 6 equations and 5 unknowns: rB, δB, δD, γ and NKπ
• NCP is determined from NKπ taking in account the different BR and efficiencies