ViewVC Help
View File | Revision Log | Show Annotations | Root Listing
root/cvsroot/UserCode/codeBS/CMSnote/datasets.tex
Revision: 1.1
Committed: Wed May 5 14:31:43 2010 UTC (14 years, 11 months ago) by cerizza
Content type: application/x-tex
Branch: MAIN
CVS Tags: HEAD
Log Message:
note added

File Contents

# Content
1 \section{Simulated Event Samples}
2
3 Table~\ref{tab:data} lists the sets of fully simulated events
4 used in this study. Based on those samples we optimize
5 the event selection and validate the analysis technique.
6 All samples use PYTHIA~\cite{pythia} for simulation of the $pp$
7 collisions. The signal and the $b \bar{b}$
8 background are studied in the inclusively generated
9 $b\rightarrow J/ \psi X$ sample.
10 The EvtGen~\cite{evtgen} simulation takes care of all $b$ hadron decays.
11 One of the two $b$ hadrons in the event is forced to decay to a final state
12 with a $J/ \psi$ meson, directly or via intermediate excited charmonium states.
13 %in the four inclusive datasets $B^0\rightarrow J/ \psi X$, $B_s\rightarrow J/ \psi X$, $B^+\rightarrow J/ \psi X$ and $\Lambda_b \rightarrow J/ \psi X$
14 %which include EvtGen for the decay of all $b$ hadrons.
15 Events with a $J/ \psi$ decaying into two muons are filtered at the
16 generator level by requiring that the two muons have opposite charge
17 and transverse momentum $p_T > 2.5$~GeV/c and a pseudo-rapidity $|\eta|<2.5$.
18 For detailed studies we also use exclusively generated $B_S\to J/\psi \phi$
19 and $B_d\to J/\psi K^*$ samples.
20 For the prompt $J/ \psi$ background we use a sample of
21 $pp\rightarrow J/ \psi X$-type events produced with the
22 same generator-level muon filter as the $b$ hadrons samples.
23 For the QCD background we study the inclusive
24 $pp\rightarrow \mu \mu X$ sample with the same muon pre-
25 selection requirements on $p_T$ and $\eta$ as for the other sets above.
26
27 In the next iteration we will require that $b$-hadrons are decayed by
28 EventGen~\cite{evtgen}.
29
30 \begin{table}[htbp]
31 \vspace{0.8cm}
32 \centering
33 \begin{tabular}{ccccc}
34 \hline\hline
35 Process & $N_{ev}$ & $\sigma$ (pb) & $\epsilon_{filter}$ $(\%)$ &
36 \cal{L} $(pb^{-1})$ \\
37 \hline
38 %$B^0\rightarrow J/ \psi X$ & & & & \\
39 %$B_s\rightarrow J/ \psi X$ & & & & \\
40 %$B^+\rightarrow J/ \psi X$ & & & & \\
41 %$\Lambda_b\rightarrow J/ \psi X$ & & & & \\
42 $b\rightarrow J/ \psi X$ & $5\times 10^6$& $66.6\times 10^{6}$ &
43 $0.024$ & $31$ \\
44 $pp\rightarrow J/ \psi X$ & $10^7$ & $12.6\times 10^{6}$& $0.074$ & $11$\\
45 $pp\rightarrow \mu \mu X$ & $10^6$ & $48.4$ & $1.12\times 10^{-5}$& $1.87$\\
46 \hline\hline
47 \end{tabular}
48 \label{tab:data}
49 \caption{For each event sample
50 we list the total number of generated events $N_{ev}$,
51 the production cross-section $\sigma$,
52 the filter efficiency $\epsilon_{filter}$, and
53 the integrated luminosity $L$.
54 For the $b\rightarrow J/ \psi X$ sample we
55 derive the integrated luminosity from the
56 $B_s\rightarrow J/ \psi \phi$ sub-set.}
57 \end{table}
58
59 \clearpage