Study of the B+ ->J/Psi K decay at LHCb - High Energy Physics
Study of the B+ ->J/Psi K decay at LHCb - High Energy Physics
Study of the B+ ->J/Psi K decay at LHCb - High Energy Physics
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<strong>Study</strong> <strong>of</strong> <strong>the</strong> B + ->J/<strong>Psi</strong> K<br />
<strong>decay</strong> <strong>at</strong> <strong>LHCb</strong> <br />
Ross Young<br />
University <strong>of</strong> Edinburgh<br />
Mar-30-10<br />
R. Young<br />
1
Introduction<br />
• With <strong>the</strong> start-up <strong>of</strong> collisions <strong>at</strong> <strong>the</strong> LHC <strong>the</strong> priority is for<br />
early physics and calibr<strong>at</strong>ion <strong>of</strong> our detector. <br />
• Measuring <strong>the</strong> cross-sections for particles is vital in<br />
understanding <strong>the</strong> processes involved in pp interactions, and<br />
how we can use this understanding to simul<strong>at</strong>e our d<strong>at</strong>a better.<br />
• This talk covers <strong>the</strong> first steps involved in making a<br />
measurement <strong>of</strong> B + production cross-sections (in regions <strong>of</strong><br />
transverse momentum p T and rapidity y) <strong>at</strong> <strong>LHCb</strong>. It includes:<br />
– Plan <strong>of</strong> action<br />
– Preliminary results<br />
Mar-30-10<br />
R. Young 2
Cross-section studies <strong>at</strong> <strong>LHCb</strong><br />
Λ 0 production cross section<br />
measured in 2009 d<strong>at</strong>a <strong>at</strong><br />
E cm =900GeV/c 2 (Vanya Belyaev)<br />
K S production cross section<br />
measured in 2009 d<strong>at</strong>a <strong>at</strong><br />
E cm =900GeV/c 2 (Manuel Shiller)<br />
3/30/10 R. Young 3
Analysis Outline<br />
• This study uses <strong>the</strong> flavour-specific B + ->J/<br />
ΨK + , due to its high production r<strong>at</strong>e and<br />
clean signal.<br />
• Measure cross-section σ in bins <strong>of</strong> p T and y,<br />
– L INT . σ <strong>B+</strong> = BR(B + ->J/ΨK + ) -1 . ε -1 sel(p T, y). ε -1 trig<br />
(p T, y) -1 . N(p T ,y)<br />
• ε sel (p T, y), ε trig (p T, y) from Monte Carlo<br />
• N(p T ,y) from d<strong>at</strong>a.<br />
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B + ->J/<strong>Psi</strong> K + selection <br />
• We analysed 277k MC signal events (<strong>at</strong> E cm = 10TeV).<br />
• Loose cuts were applied to <strong>the</strong> d<strong>at</strong>aset to discern true candid<strong>at</strong>es from<br />
mis-reconstructed candid<strong>at</strong>es.<br />
• ε sel = 33.8%<br />
Signal d<strong>at</strong>a was fitted with a single<br />
Gaussian; background with a Chebychev.<br />
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Yields in bins <strong>of</strong> p T and y (1)<br />
We split <strong>the</strong> d<strong>at</strong>a fur<strong>the</strong>r into bins <strong>of</strong> transverse momentum p T and rapidity y <strong>of</strong> <strong>the</strong> B +<br />
candid<strong>at</strong>e and refit (below – 3
Yields in bins <strong>of</strong> p T and y (2)<br />
The table below gives <strong>the</strong> total number <strong>of</strong> selected events per region <strong>of</strong> y<br />
and pT…<br />
…or histogrammed per<br />
unit p T – one can see a<br />
clear peak in <strong>the</strong><br />
regions 2
-production <strong>at</strong> <strong>LHCb</strong><br />
• The MC d<strong>at</strong>a used for this analysis<br />
is based on beam collisions <strong>of</strong> E cm =<br />
10TeV. The corresponding bb crosssection<br />
is approxim<strong>at</strong>ely 300μb. <br />
• There is an error on this, as bb cross<br />
sections <strong>at</strong> <strong>the</strong> LHC is not yet fully<br />
understood.<br />
• In 0.1fb -1 , we expect:<br />
• 3e+10 bb events<br />
• 1.2e+10 B + <br />
Cross-section as a function <strong>of</strong><br />
beam energy<br />
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Integr<strong>at</strong>ed luminosity and annual<br />
yield<br />
• Let us make a quick calcul<strong>at</strong>ion <strong>of</strong> <strong>the</strong> B + cross section.<br />
• For <strong>the</strong> process B u ->J/<strong>Psi</strong> K:<br />
– Visible branching fraction BR = 6x10 -5<br />
– Gener<strong>at</strong>or-level efficiency ε gen = 0.1630<br />
– Average selection efficiency ε sel = 0.330<br />
• The MC d<strong>at</strong>aset (277k gener<strong>at</strong>ed events) corresponds an<br />
integr<strong>at</strong>ed luminosity <strong>of</strong> L int = 0.12 fb -1 .<br />
• Taking bin 3
B + /B - production r<strong>at</strong>ios<br />
• The r<strong>at</strong>io <strong>of</strong> selected B + to B - candid<strong>at</strong>es was also<br />
investig<strong>at</strong>ed on <strong>the</strong> MC signal d<strong>at</strong>a.<br />
• An asymmetry here may indic<strong>at</strong>e differences in <strong>the</strong><br />
production r<strong>at</strong>es <strong>at</strong> <strong>the</strong> gener<strong>at</strong>or level, or in <strong>the</strong><br />
reconstruction efficiencies.<br />
• No significant devi<strong>at</strong>ion from an equal r<strong>at</strong>io is observed.<br />
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Future Work<br />
• This is a work in progress.<br />
• A background study is being run on various samples to<br />
<strong>at</strong>tain a full selection <strong>of</strong> <strong>the</strong> channel<br />
• At first glance, prompt modes and ghost tracks look to be<br />
<strong>the</strong> main contributions – tighter cuts on <strong>the</strong> track χ 2 and a<br />
cut on <strong>the</strong> Kaon ID may need to be imposed.<br />
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Summary<br />
• A Monte Carlo study on <strong>the</strong> B + production crosssection<br />
has been carried out using a selection <strong>of</strong><br />
<strong>the</strong> <strong>decay</strong> B u ->J/Ψ K.<br />
• The cross-section peaks in <strong>the</strong> 3