1 |
benhoob |
1.1 |
\clearpage
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2 |
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\section{Results for the ``edge analysis'' SUS-12-019}
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3 |
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\label{sec:edge}
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4 |
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5 |
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The Aachen and ETH groups have reported an excess of low-mass, opposite-sign same-flavor events (see AN 2012/200 and AN 2012/231).
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In App.~\ref{sec:edge_templates} we derive predictions for the Z background in the Z mass regions for the two signal regions used for this analysis,
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and use these predictions to derive an estimate of the low-mass $\gamma^*$/Z contributions using an extrapolation technique
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commonly referred to as the ``$R_{out/in}$'' technique.
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%In App.~\ref{sec:edge_triggers} we provide a cross-check using single lepton triggers.
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\subsection{Z Background Predictions for the ``Edge Analysis''}
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\label{sec:edge_templates}
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15 |
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The two signal regions of the edge analysis are defined as:
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\begin{itemize}
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\item Low-\MET signal region (ETH)
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\begin{itemize}
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\item 2 \pt $>$ 20 GeV leptons with $|\eta|<2.4$
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\item At least 3 jets (\pt\ $>$ 40 GeV, $|\eta|<3$)
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\item \MET\ $>$ 100 GeV
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\end{itemize}
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\item High-\MET signal region (Aachen)
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\begin{itemize}
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\item leading lepton \pt $>$ 20 GeV, trailing lepton \pt\ $>$ 10 GeV, both with $|\eta|<2.4$
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\item At least 2 jets (\pt\ $>$ 40 GeV, $|\eta|<3$) with scalar sum $H_{T}>100$~GeV
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\item \MET\ $>$ 150 GeV
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\end{itemize}
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\end{itemize}
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32 |
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We begin with a synchronization exercise to make sure that we can reproduce the ETH/Aachen results. In Table~\ref{tab:edgesync} we
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display the yields in the Z mass regions of the 2 signal regions and compare these to results from the ETH group.
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In general we are synchronized to 3\% or better in all channels. Note that for the purposes of this exercise we include an additional
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dimuon trigger (HLT\_Mu17\_TkMu8) which is not yet included in the results that follow. The inclusion of this trigger adds 3 $\mu\mu$
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events in both the low \MET\ and high \MET\ signal regions.
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38 |
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\begin{table}[htb]
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\begin{center}
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41 |
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\footnotesize
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\caption{\label{tab:edgesync} Summary of the synchronization exercise with the ETH group with 9.2 fb$^{-1}$.
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The yields in the Z mass region ($81<m_{\ell\ell}<101$~GeV) are displayed for the low \MET\ and high \MET\ signal regions.}
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\begin{tabular}{l|c|c}
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\hline
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\hline
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48 |
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49 |
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low \MET\ signal region & UCSB-UCSD-FNAL & ETH \\
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\hline
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ee & 125 & 123 \\
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$\mu\mu$ & 166 & 164 \\
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e$\mu$ & 186 & 186 \\
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\hline
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\hline
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57 |
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58 |
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high \MET\ signal region & UCSB-UCSD-FNAL & ETH \\
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\hline
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ee & 75 & 72 \\
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$\mu\mu$ & 95 & 94 \\
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e$\mu$ & 113 & 113 \\
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\hline
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\hline
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66 |
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\end{tabular}
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\end{center}
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\end{table}
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71 |
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In order to adapt the \MET\ templates method to predict the Z background in these regions, we make minor modifications
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to the flavor-symmetric (FS) scaling factor $K$ and to the binning used for the \MET\ templates. The FS background
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is estimated using e$\mu$ events in data.
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To improve the precision of this background estimate, the dilepton mass requirement is not applied, and we apply a scaling
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factor $K$, which is the efficiency for e$\mu$ events to fall in the Z mass window, extracted from MC.
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The values of $K$ for various \MET\ intervals for the high-\MET\ region (using \pt\ $>$ (20,10) GeV leptons and at least 2 jets)
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are shown in Fig.~\ref{fig:K_incl_highmet}.
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Based on this plot we choose $K=0.13\pm0.02$ for \MET\ signal regions up to 200 GeV; for \MET\ 200-300 GeV and \MET\ $>$ 300 GeV
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we inflate the uncertainty to $K=0.13\pm0.04$ and $K=0.13\pm0.05$, respectively, due to the limited statistical precision.
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The values of $K$ for the low-\MET\ region (using \pt\ $>$ (20,20) GeV leptons and at least 3 jets) are shown in
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Fig.~\ref{fig:K_incl_lowmet}.
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Based on this plot we choose $K=0.14\pm0.02$ for \MET\ signal regions up to 200 GeV; for \MET\ 200-300 GeV and \MET\ $>$ 300 GeV
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we inflate the uncertainty to $K=0.14\pm0.03$ and $K=0.14\pm0.07$, respectively. In addition, we change the
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jet \pt\ threshold for the \MET\ templates jet multiplicity binning from 30 to 40 GeV, and change the $H_T$ bins to
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(0,80,100,150,200,250,300,5000) GeV.
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\clearpage
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90 |
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\begin{figure}[!ht]
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\begin{center}
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\begin{tabular}{cc}
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\includegraphics[width=0.4\textwidth]{plots/extractK_inclusive_pt2010_92fb.pdf} &
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\includegraphics[width=0.4\textwidth]{plots/extractK_exclusive_pt2010_92fb.pdf} \\
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\end{tabular}
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\caption{\label{fig:K_incl_highmet}
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The efficiency for e$\mu$ events to satisfy the dilepton mass requirement, $K$, in data and simulation for inclusive \MET\ intervals
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(left) and exclusive \MET\ intervals (right) for the dilepton \pt\ $>$ (20,10) GeV selection with at least 2 \pt\ $>$ 40 GeV jets
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(used for the high \MET\ signal region).
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}
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101 |
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\end{center}
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102 |
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\end{figure}
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103 |
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104 |
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\begin{comment}
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105 |
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|
106 |
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Using selection : ((((leptype==2)&&(csc==0 && hbhe==1 && hcallaser==1 && ecaltp==1 && trkfail==1 && eebadsc==1 && hbhenew==1))&&(isdata==0 || (run<197556 || run>198913)))&&(njets40>=2))&&(lep1.pt()>20 && lep2.pt()>10)
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107 |
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Using weight : vtxweight * weight
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108 |
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OF entries (total) 23031
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109 |
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OF entries (Z mass) 2791
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110 |
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K 0.121184
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111 |
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Warning in <TROOT::Append>: Replacing existing TH1: htot (Potential memory leak).
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112 |
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Warning in <TROOT::Append>: Replacing existing TH1: hZ (Potential memory leak).
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113 |
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|
114 |
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--------------------------------------------------------------
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115 |
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pfmet>0 && pfmet<30
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116 |
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|
117 |
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data :
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118 |
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total : 3835
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119 |
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Z : 413
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120 |
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K : 0.11 +/- 0.005
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121 |
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|
122 |
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MC :
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123 |
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total : 378.922
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124 |
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Z : 47.9593
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125 |
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K : 0.13 +/- 0.008
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126 |
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--------------------------------------------------------------
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127 |
|
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|
128 |
|
|
|
129 |
|
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--------------------------------------------------------------
|
130 |
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pfmet>30 && pfmet<60
|
131 |
|
|
|
132 |
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data :
|
133 |
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total : 7090
|
134 |
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Z : 849
|
135 |
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K : 0.12 +/- 0.004
|
136 |
|
|
|
137 |
|
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MC :
|
138 |
|
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total : 775.198
|
139 |
|
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Z : 104.129
|
140 |
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K : 0.13 +/- 0.003
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141 |
|
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--------------------------------------------------------------
|
142 |
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|
143 |
|
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|
144 |
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--------------------------------------------------------------
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145 |
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pfmet>60 && pfmet<100
|
146 |
|
|
|
147 |
|
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data :
|
148 |
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total : 7598
|
149 |
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Z : 1000
|
150 |
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K : 0.13 +/- 0.004
|
151 |
|
|
|
152 |
|
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MC :
|
153 |
|
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total : 886.062
|
154 |
|
|
Z : 118.721
|
155 |
|
|
K : 0.13 +/- 0.003
|
156 |
|
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--------------------------------------------------------------
|
157 |
|
|
|
158 |
|
|
|
159 |
|
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--------------------------------------------------------------
|
160 |
|
|
pfmet>100 && pfmet<200
|
161 |
|
|
|
162 |
|
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data :
|
163 |
|
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total : 4258
|
164 |
|
|
Z : 506
|
165 |
|
|
K : 0.12 +/- 0.005
|
166 |
|
|
|
167 |
|
|
MC :
|
168 |
|
|
total : 538.442
|
169 |
|
|
Z : 71.0424
|
170 |
|
|
K : 0.13 +/- 0.003
|
171 |
|
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--------------------------------------------------------------
|
172 |
|
|
|
173 |
|
|
|
174 |
|
|
--------------------------------------------------------------
|
175 |
|
|
pfmet>200 && pfmet<300
|
176 |
|
|
|
177 |
|
|
data :
|
178 |
|
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total : 221
|
179 |
|
|
Z : 19
|
180 |
|
|
K : 0.09 +/- 0.020
|
181 |
|
|
|
182 |
|
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MC :
|
183 |
|
|
total : 29.8247
|
184 |
|
|
Z : 3.46834
|
185 |
|
|
K : 0.12 +/- 0.012
|
186 |
|
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--------------------------------------------------------------
|
187 |
|
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|
188 |
|
|
|
189 |
|
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--------------------------------------------------------------
|
190 |
|
|
pfmet>300
|
191 |
|
|
|
192 |
|
|
data :
|
193 |
|
|
total : 29
|
194 |
|
|
Z : 4
|
195 |
|
|
K : 0.14 +/- 0.069
|
196 |
|
|
|
197 |
|
|
MC :
|
198 |
|
|
total : 5.45734
|
199 |
|
|
Z : 0.438259
|
200 |
|
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K : 0.08 +/- 0.028
|
201 |
|
|
--------------------------------------------------------------
|
202 |
|
|
|
203 |
|
|
root [1] extractK(false,false,false)
|
204 |
|
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Using selection : ((((leptype==2)&&(csc==0 && hbhe==1 && hcallaser==1 && ecaltp==1 && trkfail==1 && eebadsc==1 && hbhenew==1))&&(isdata==0 || (run<197556 || run>198913)))&&(njets40>=2))&&(lep1.pt()>20 && lep2.pt()>10)
|
205 |
|
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Using weight : vtxweight * weight
|
206 |
|
|
OF entries (total) 23031
|
207 |
|
|
OF entries (Z mass) 2791
|
208 |
|
|
K 0.121184
|
209 |
|
|
Info in <TCanvas::MakeDefCanvas>: created default TCanvas with name c1
|
210 |
|
|
|
211 |
|
|
--------------------------------------------------------------
|
212 |
|
|
pfmet>0
|
213 |
|
|
|
214 |
|
|
data :
|
215 |
|
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total : 23031
|
216 |
|
|
Z : 2791
|
217 |
|
|
K : 0.12 +/- 0.002
|
218 |
|
|
|
219 |
|
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MC :
|
220 |
|
|
total : 2613.71
|
221 |
|
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Z : 345.768
|
222 |
|
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K : 0.13 +/- 0.002
|
223 |
|
|
--------------------------------------------------------------
|
224 |
|
|
|
225 |
|
|
|
226 |
|
|
--------------------------------------------------------------
|
227 |
|
|
pfmet>30
|
228 |
|
|
|
229 |
|
|
data :
|
230 |
|
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total : 19196
|
231 |
|
|
Z : 2378
|
232 |
|
|
K : 0.12 +/- 0.003
|
233 |
|
|
|
234 |
|
|
MC :
|
235 |
|
|
total : 2234.8
|
236 |
|
|
Z : 297.807
|
237 |
|
|
K : 0.13 +/- 0.002
|
238 |
|
|
--------------------------------------------------------------
|
239 |
|
|
|
240 |
|
|
|
241 |
|
|
--------------------------------------------------------------
|
242 |
|
|
pfmet>60
|
243 |
|
|
|
244 |
|
|
data :
|
245 |
|
|
total : 12106
|
246 |
|
|
Z : 1529
|
247 |
|
|
K : 0.13 +/- 0.003
|
248 |
|
|
|
249 |
|
|
MC :
|
250 |
|
|
total : 1459.78
|
251 |
|
|
Z : 193.67
|
252 |
|
|
K : 0.13 +/- 0.002
|
253 |
|
|
--------------------------------------------------------------
|
254 |
|
|
|
255 |
|
|
|
256 |
|
|
--------------------------------------------------------------
|
257 |
|
|
pfmet>100
|
258 |
|
|
|
259 |
|
|
data :
|
260 |
|
|
total : 4508
|
261 |
|
|
Z : 529
|
262 |
|
|
K : 0.12 +/- 0.005
|
263 |
|
|
|
264 |
|
|
MC :
|
265 |
|
|
total : 573.708
|
266 |
|
|
Z : 74.9489
|
267 |
|
|
K : 0.13 +/- 0.003
|
268 |
|
|
--------------------------------------------------------------
|
269 |
|
|
|
270 |
|
|
|
271 |
|
|
--------------------------------------------------------------
|
272 |
|
|
pfmet>200
|
273 |
|
|
|
274 |
|
|
data :
|
275 |
|
|
total : 250
|
276 |
|
|
Z : 23
|
277 |
|
|
K : 0.09 +/- 0.019
|
278 |
|
|
|
279 |
|
|
MC :
|
280 |
|
|
total : 35.2821
|
281 |
|
|
Z : 3.90659
|
282 |
|
|
K : 0.11 +/- 0.011
|
283 |
|
|
--------------------------------------------------------------
|
284 |
|
|
|
285 |
|
|
|
286 |
|
|
--------------------------------------------------------------
|
287 |
|
|
pfmet>300
|
288 |
|
|
|
289 |
|
|
data :
|
290 |
|
|
total : 29
|
291 |
|
|
Z : 4
|
292 |
|
|
K : 0.14 +/- 0.069
|
293 |
|
|
|
294 |
|
|
MC :
|
295 |
|
|
total : 5.45734
|
296 |
|
|
Z : 0.438259
|
297 |
|
|
K : 0.08 +/- 0.028
|
298 |
|
|
--------------------------------------------------------------
|
299 |
|
|
|
300 |
|
|
\end{comment}
|
301 |
|
|
|
302 |
|
|
|
303 |
|
|
\begin{figure}[!ht]
|
304 |
|
|
\begin{center}
|
305 |
|
|
\begin{tabular}{cc}
|
306 |
|
|
\includegraphics[width=0.4\textwidth]{plots/extractK_inclusive_lowmet.pdf} &
|
307 |
|
|
\includegraphics[width=0.4\textwidth]{plots/extractK_exclusive_lowmet.pdf} \\
|
308 |
|
|
\end{tabular}
|
309 |
|
|
\caption{\label{fig:K_incl_lowmet}
|
310 |
|
|
The efficiency for e$\mu$ events to satisfy the dilepton mass requirement, $K$, in data and simulation for inclusive \MET\ intervals
|
311 |
|
|
(left) and exclusive \MET\ intervals (right) for the dilepton \pt\ $>$ (20,20) GeV selection with at least 3 \pt\ $>$ 40 GeV jets
|
312 |
|
|
(used for the low \MET\ signal region).
|
313 |
|
|
}
|
314 |
|
|
\end{center}
|
315 |
|
|
\end{figure}
|
316 |
|
|
|
317 |
|
|
\begin{comment}
|
318 |
|
|
|
319 |
|
|
Using selection : ((((leptype==2)&&(csc==0 && hbhe==1 && hcallaser==1 && ecaltp==1 && trkfail==1 && eebadsc==1 && hbhenew==1))&&(isdata==0 || (run<197556 || run>198913)))&&(njets40>=3))&&(lep1.pt()>20 && lep2.pt()>20)
|
320 |
|
|
Using weight : vtxweight * weight
|
321 |
|
|
OF entries (total) 5934
|
322 |
|
|
OF entries (Z mass) 827
|
323 |
|
|
K 0.139366
|
324 |
|
|
|
325 |
|
|
--------------------------------------------------------------
|
326 |
|
|
pfmet>0
|
327 |
|
|
|
328 |
|
|
data :
|
329 |
|
|
total : 5934
|
330 |
|
|
Z : 827
|
331 |
|
|
K : 0.14 +/- 0.005
|
332 |
|
|
|
333 |
|
|
MC :
|
334 |
|
|
total : 725.106
|
335 |
|
|
Z : 103.443
|
336 |
|
|
K : 0.14 +/- 0.004
|
337 |
|
|
--------------------------------------------------------------
|
338 |
|
|
|
339 |
|
|
|
340 |
|
|
--------------------------------------------------------------
|
341 |
|
|
pfmet>30
|
342 |
|
|
|
343 |
|
|
data :
|
344 |
|
|
total : 5110
|
345 |
|
|
Z : 722
|
346 |
|
|
K : 0.14 +/- 0.005
|
347 |
|
|
|
348 |
|
|
MC :
|
349 |
|
|
total : 625.723
|
350 |
|
|
Z : 89.0789
|
351 |
|
|
K : 0.14 +/- 0.003
|
352 |
|
|
--------------------------------------------------------------
|
353 |
|
|
|
354 |
|
|
|
355 |
|
|
--------------------------------------------------------------
|
356 |
|
|
pfmet>60
|
357 |
|
|
|
358 |
|
|
data :
|
359 |
|
|
total : 3362
|
360 |
|
|
Z : 475
|
361 |
|
|
K : 0.14 +/- 0.006
|
362 |
|
|
|
363 |
|
|
MC :
|
364 |
|
|
total : 418.375
|
365 |
|
|
Z : 59.5404
|
366 |
|
|
K : 0.14 +/- 0.004
|
367 |
|
|
--------------------------------------------------------------
|
368 |
|
|
|
369 |
|
|
|
370 |
|
|
--------------------------------------------------------------
|
371 |
|
|
pfmet>100
|
372 |
|
|
|
373 |
|
|
data :
|
374 |
|
|
total : 1347
|
375 |
|
|
Z : 184
|
376 |
|
|
K : 0.14 +/- 0.010
|
377 |
|
|
|
378 |
|
|
MC :
|
379 |
|
|
total : 177.754
|
380 |
|
|
Z : 26.7455
|
381 |
|
|
K : 0.15 +/- 0.006
|
382 |
|
|
--------------------------------------------------------------
|
383 |
|
|
|
384 |
|
|
|
385 |
|
|
--------------------------------------------------------------
|
386 |
|
|
pfmet>200
|
387 |
|
|
|
388 |
|
|
data :
|
389 |
|
|
total : 104
|
390 |
|
|
Z : 12
|
391 |
|
|
K : 0.12 +/- 0.033
|
392 |
|
|
|
393 |
|
|
MC :
|
394 |
|
|
total : 14.1212
|
395 |
|
|
Z : 1.59283
|
396 |
|
|
K : 0.11 +/- 0.018
|
397 |
|
|
--------------------------------------------------------------
|
398 |
|
|
|
399 |
|
|
|
400 |
|
|
--------------------------------------------------------------
|
401 |
|
|
pfmet>300
|
402 |
|
|
|
403 |
|
|
data :
|
404 |
|
|
total : 11
|
405 |
|
|
Z : 1
|
406 |
|
|
K : 0.09 +/- 0.091
|
407 |
|
|
|
408 |
|
|
MC :
|
409 |
|
|
total : 2.00086
|
410 |
|
|
Z : 0.142752
|
411 |
|
|
K : 0.07 +/- 0.034
|
412 |
|
|
--------------------------------------------------------------
|
413 |
|
|
|
414 |
|
|
root [3] Info in <TCanvas::Print>: pdf file /home/users/benhoob/ZMet2012/plots/extractK_inclusive_lowmet.pdf has been created
|
415 |
|
|
|
416 |
|
|
root [3]
|
417 |
|
|
root [3] extractK(true,false,false)
|
418 |
|
|
Using selection : ((((leptype==2)&&(csc==0 && hbhe==1 && hcallaser==1 && ecaltp==1 && trkfail==1 && eebadsc==1 && hbhenew==1))&&(isdata==0 || (run<197556 || run>198913)))&&(njets40>=3))&&(lep1.pt()>20 && lep2.pt()>20)
|
419 |
|
|
Using weight : vtxweight * weight
|
420 |
|
|
OF entries (total) 5934
|
421 |
|
|
OF entries (Z mass) 827
|
422 |
|
|
K 0.139366
|
423 |
|
|
Warning in <TFile::Append>: Replacing existing TH1: htot (Potential memory leak).
|
424 |
|
|
Warning in <TFile::Append>: Replacing existing TH1: hZ (Potential memory leak).
|
425 |
|
|
|
426 |
|
|
--------------------------------------------------------------
|
427 |
|
|
pfmet>0 && pfmet<30
|
428 |
|
|
|
429 |
|
|
data :
|
430 |
|
|
total : 824
|
431 |
|
|
Z : 105
|
432 |
|
|
K : 0.13 +/- 0.012
|
433 |
|
|
|
434 |
|
|
MC :
|
435 |
|
|
total : 99.3853
|
436 |
|
|
Z : 14.3649
|
437 |
|
|
K : 0.14 +/- 0.017
|
438 |
|
|
--------------------------------------------------------------
|
439 |
|
|
|
440 |
|
|
|
441 |
|
|
--------------------------------------------------------------
|
442 |
|
|
pfmet>30 && pfmet<60
|
443 |
|
|
|
444 |
|
|
data :
|
445 |
|
|
total : 1748
|
446 |
|
|
Z : 247
|
447 |
|
|
K : 0.14 +/- 0.009
|
448 |
|
|
|
449 |
|
|
MC :
|
450 |
|
|
total : 207.368
|
451 |
|
|
Z : 29.5391
|
452 |
|
|
K : 0.14 +/- 0.006
|
453 |
|
|
--------------------------------------------------------------
|
454 |
|
|
|
455 |
|
|
|
456 |
|
|
--------------------------------------------------------------
|
457 |
|
|
pfmet>60 && pfmet<100
|
458 |
|
|
|
459 |
|
|
data :
|
460 |
|
|
total : 2015
|
461 |
|
|
Z : 291
|
462 |
|
|
K : 0.14 +/- 0.008
|
463 |
|
|
|
464 |
|
|
MC :
|
465 |
|
|
total : 240.615
|
466 |
|
|
Z : 32.7949
|
467 |
|
|
K : 0.14 +/- 0.005
|
468 |
|
|
--------------------------------------------------------------
|
469 |
|
|
|
470 |
|
|
|
471 |
|
|
--------------------------------------------------------------
|
472 |
|
|
pfmet>100 && pfmet<200
|
473 |
|
|
|
474 |
|
|
data :
|
475 |
|
|
total : 1243
|
476 |
|
|
Z : 172
|
477 |
|
|
K : 0.14 +/- 0.011
|
478 |
|
|
|
479 |
|
|
MC :
|
480 |
|
|
total : 163.632
|
481 |
|
|
Z : 25.1526
|
482 |
|
|
K : 0.15 +/- 0.007
|
483 |
|
|
--------------------------------------------------------------
|
484 |
|
|
|
485 |
|
|
|
486 |
|
|
--------------------------------------------------------------
|
487 |
|
|
pfmet>200 && pfmet<300
|
488 |
|
|
|
489 |
|
|
data :
|
490 |
|
|
total : 93
|
491 |
|
|
Z : 11
|
492 |
|
|
K : 0.12 +/- 0.036
|
493 |
|
|
|
494 |
|
|
MC :
|
495 |
|
|
total : 12.1203
|
496 |
|
|
Z : 1.45008
|
497 |
|
|
K : 0.12 +/- 0.020
|
498 |
|
|
--------------------------------------------------------------
|
499 |
|
|
|
500 |
|
|
|
501 |
|
|
--------------------------------------------------------------
|
502 |
|
|
pfmet>300
|
503 |
|
|
|
504 |
|
|
data :
|
505 |
|
|
total : 11
|
506 |
|
|
Z : 1
|
507 |
|
|
K : 0.09 +/- 0.091
|
508 |
|
|
|
509 |
|
|
MC :
|
510 |
|
|
total : 2.00086
|
511 |
|
|
Z : 0.142752
|
512 |
|
|
K : 0.07 +/- 0.034
|
513 |
|
|
--------------------------------------------------------------
|
514 |
|
|
|
515 |
|
|
|
516 |
|
|
\end{comment}
|
517 |
|
|
|
518 |
|
|
The strategy is to select Z$\to\ell\ell$ candidates ($81<m_{\ell\ell}<101$ GeV) with jet requirements corresponding to the
|
519 |
|
|
low-\MET\ and high-\MET\ signal regions, and compare the observed \MET\ distribution to the sum of the predictions from the
|
520 |
|
|
\zjets\ background (from the \MET\ templates method based on the \gjets\ data control sample), the flavor-symmetric background predicted
|
521 |
|
|
from e$\mu$ data events, and MC contributions from WZ/ZZ, as well as the rare SM processes with Z bosons ($t\bar{t}\rm{Z}$ and ZZZ, ZZW, ZWW).
|
522 |
|
|
|
523 |
|
|
The results of the low \MET\ signal region are displayed in Fig.~\ref{fig:results_lowmet} and summarized in Table~\ref{tab:results_lowmet},
|
524 |
|
|
separately for the Run2012A+B data (5.1 fb$^{-1}$) and Run2012C data (4.1 fb$^{-1}$).
|
525 |
|
|
In the Run2012A+B data, we observed a 1.6$\sigma$ excess for \MET\ $>$ 100 GeV, corresponding to the low \MET\ signal region.
|
526 |
|
|
However, this excess does not persist in Run2012C data, where we observe good agreement between the data and the predicted background.
|
527 |
|
|
In the combined Run2012A+B+C data (Fig.~\ref{fig:results_fulledge} and Table~\ref{tab:results_edgefull}) we observe reasonable
|
528 |
|
|
agreement over the full \MET\ range. In the \MET\ $>$ 100 GeV region we observe 288 events with a predicted background of $251\pm33$,
|
529 |
|
|
representing an excess of 1.0$\sigma$.
|
530 |
|
|
|
531 |
|
|
The results of the high \MET\ signal region are displayed in Fig.~\ref{fig:results_highmet} and summarized in Table~\ref{tab:results_highmet},
|
532 |
|
|
separately for the Run2012A+B data (5.1 fb$^{-1}$) and Run2012C data (4.1 fb$^{-1}$).
|
533 |
|
|
In both periods we observe good agreement between the data and predicted background over the full \MET\ range.
|
534 |
|
|
In the \MET\ $>$ 150 GeV region corresponding to the high \MET\ signal region in the full sample, we observe 167 events with a predicted
|
535 |
|
|
background of $177\pm25$ events, representing a deficit of -0.4$\sigma$.
|
536 |
|
|
|
537 |
|
|
\clearpage
|
538 |
|
|
|
539 |
|
|
\begin{figure}[!h]
|
540 |
|
|
\begin{center}
|
541 |
|
|
\begin{tabular}{cc}
|
542 |
|
|
\includegraphics[width=0.45\textwidth]{plots/pfmet_pt40_2012AB_lowMet_all.pdf}
|
543 |
|
|
\includegraphics[width=0.45\textwidth]{plots/pfmet_pt40_2012C_lowMet_all.pdf}
|
544 |
|
|
%\includegraphics[width=0.48\textwidth]{plots/pfmet_pt40_2012AB_lowMet_all_linear.pdf}
|
545 |
|
|
\end{tabular}
|
546 |
|
|
\caption{\footnotesize Results for the low \MET\ signal region.
|
547 |
|
|
The results for 5.1 fb$^{-1}$ 2012A+B data are displayed on the left, the results for 4.1 fb$^{-1}$ 2012C data are displayed on the right.
|
548 |
|
|
%The left plot shows the full \MET\ range, the right plot is zoomed in on the \MET\ $>$ 100 GeV region.
|
549 |
|
|
The observed \MET\ distribution (black points) is compared with the sum of the predicted \MET\
|
550 |
|
|
distributions from \zjets, flavor-symmetric backgrounds, WZ+ZZ backgrounds, and rare SM backgrounds.
|
551 |
|
|
The ratio of observed to predicted yields in each bin is
|
552 |
|
|
indicated. The error bars indicate the statistical uncertainty in the data and the shaded band indicates the total background uncertainty.
|
553 |
|
|
\label{fig:results_lowmet}
|
554 |
|
|
}
|
555 |
|
|
\end{center}
|
556 |
|
|
\end{figure}
|
557 |
|
|
|
558 |
|
|
\begin{table}[htb]
|
559 |
|
|
\begin{center}
|
560 |
|
|
\footnotesize
|
561 |
|
|
\caption{\label{tab:results_lowmet} \footnotesize Results for the low \MET\ signal region.
|
562 |
|
|
The results for 5.1 fb$^{-1}$ 2012A+B data are displayed in the top table, the results for 4.1 fb$^{-1}$ 2012C data are displayed in the bottom table.
|
563 |
|
|
The total background is the sum of the \zjets\ background predicted from
|
564 |
|
|
the \MET\ templates method (\zjets\ bkg), the flavor-symmetric background predicted from e$\mu$ events (FS bkg), the WZ and ZZ backgrounds predicted from MC
|
565 |
|
|
(WZ bkg and ZZ bkg) and the rare SM backgrounds. All uncertainties include both the statistical and systematic components. The Gaussian significance of the deviation between the data
|
566 |
|
|
and total background is indicated for signal regions with at least 20 observed events. }
|
567 |
|
|
\begin{tabular}{l|c|c|c|c|c|c}
|
568 |
|
|
|
569 |
|
|
\hline
|
570 |
|
|
\hline
|
571 |
|
|
|
572 |
|
|
\begin{comment}
|
573 |
|
|
Using pfmet out-of-the-box
|
574 |
|
|
Using pT > 40 GeV jets, low MET signal region
|
575 |
|
|
WZ/ZZ selection : ((((((leptype==0 && (ee==1 || isdata==0))||(leptype==1 && (mm==1 || isdata==0)))&&(ngennu>0))&&(csc==0 && hbhe==1 && hcallaser==1 && ecaltp==1 && trkfail==1 && eebadsc==1 && hbhenew==1))&&(dilmass>81 && dilmass<101))&&(lep1.pt()>20.0 && lep2.pt()>20.0))&&(njets40>=3)
|
576 |
|
|
WZ/ZZ weight : weight * 5.1 * vtxweight * trgeff
|
577 |
|
|
Opening ../output/V00-01-04/babylooper_data_ALL_53X_PhotonStitchedTemplate_pfmet_pt40_2012AB_lowMet.root
|
578 |
|
|
B-veto? 0
|
579 |
|
|
K 0.14
|
580 |
|
|
ee+mm channels: scale em yield by 0.99
|
581 |
|
|
Yields in 0-60 GeV region
|
582 |
|
|
data : 12728
|
583 |
|
|
gjets : 13041.3
|
584 |
|
|
OF : 194.733
|
585 |
|
|
WZ : 12.3421
|
586 |
|
|
ZZ : 1.31265
|
587 |
|
|
Rare : 5.32478
|
588 |
|
|
Scaling gjets by : 0.959591
|
589 |
|
|
SF events 13412
|
590 |
|
|
OF events 3254
|
591 |
|
|
|
592 |
|
|
ee/#mu#mu events
|
593 |
|
|
\end{comment}
|
594 |
|
|
|
595 |
|
|
|
596 |
|
|
& \MET\ $>$ 0 GeV & \MET\ $>$ 30 GeV & \MET\ $>$ 60 GeV & \MET\ $>$ 100 GeV & \MET\ $>$ 200 GeV & \MET\ $>$ 300 GeV \\
|
597 |
|
|
\hline
|
598 |
|
|
\zjets\ bkg & 12870 $\pm$ 3862 & 4118 $\pm$ 1236 & 356 $\pm$ 107 & 27.5 $\pm$ 8.5 & 2.6 $\pm$ 1.1 & 0.3 $\pm$ 0.3 \\
|
599 |
|
|
FS bkg & 451 $\pm$ 70 & 389 $\pm$ 61 & 256 $\pm$ 40 & 99.1 $\pm$ 15.8 & 6.9 $\pm$ 1.8 & 1.0 $\pm$ 0.6 \\
|
600 |
|
|
WZ bkg & 24.1 $\pm$ 16.9 & 19.5 $\pm$ 13.7 & 11.8 $\pm$ 8.3 & 5.6 $\pm$ 3.9 & 1.1 $\pm$ 1.0 & 0.2 $\pm$ 0.2 \\
|
601 |
|
|
ZZ bkg & 4.3 $\pm$ 2.2 & 3.9 $\pm$ 2.0 & 3.0 $\pm$ 1.5 & 1.9 $\pm$ 1.0 & 0.5 $\pm$ 0.4 & 0.1 $\pm$ 0.1 \\
|
602 |
|
|
rare SM bkg & 12.2 $\pm$ 6.1 & 10.5 $\pm$ 5.3 & 6.9 $\pm$ 3.5 & 3.5 $\pm$ 1.8 & 0.7 $\pm$ 0.6 & 0.2 $\pm$ 0.2 \\
|
603 |
|
|
\hline
|
604 |
|
|
total bkg & 13362 $\pm$ 3862 & 4541 $\pm$ 1238 & 634 $\pm$ 115 & {\bf 138 $\pm$ 18} & 11.8 $\pm$ 2.5 & 1.8 $\pm$ 0.8 \\
|
605 |
|
|
data & 13412 & 4461 & 684 & {\bf 175 } & 14 & 3 \\
|
606 |
|
|
significance & 0.0$\sigma$ & -0.1$\sigma$ & 0.4$\sigma$ & {\bf 1.6$\sigma$ } & 0.5$\sigma$ & \\
|
607 |
|
|
|
608 |
|
|
\hline
|
609 |
|
|
\hline
|
610 |
|
|
|
611 |
|
|
|
612 |
|
|
\begin{comment}
|
613 |
|
|
Using pfmet out-of-the-box
|
614 |
|
|
Using pT > 40 GeV jets, low MET signal region
|
615 |
|
|
WZ/ZZ selection : ((((((leptype==0 && (ee==1 || isdata==0))||(leptype==1 && (mm==1 || isdata==0)))&&(ngennu>0))&&(csc==0 && hbhe==1 && hcallaser==1 && ecaltp==1 && trkfail==1 && eebadsc==1 && hbhenew==1))&&(dilmass>81 && dilmass<101))&&(lep1.pt()>20.0 && lep2.pt()>20.0))&&(njets40>=3)
|
616 |
|
|
WZ/ZZ weight : weight * 4.1 * vtxweight * trgeff
|
617 |
|
|
Opening ../output/V00-01-04/babylooper_data_ALL_53X_PhotonStitchedTemplate_pfmet_pt40_2012C_lowMet.root
|
618 |
|
|
B-veto? 0
|
619 |
|
|
K 0.14
|
620 |
|
|
ee+mm channels: scale em yield by 0.99
|
621 |
|
|
Yields in 0-60 GeV region
|
622 |
|
|
data : 10054
|
623 |
|
|
gjets : 10255.2
|
624 |
|
|
OF : 155.509
|
625 |
|
|
WZ : 9.92205
|
626 |
|
|
ZZ : 1.05527
|
627 |
|
|
Rare : 4.2807
|
628 |
|
|
Scaling gjets by : 0.963729
|
629 |
|
|
SF events 10587
|
630 |
|
|
OF events 2572
|
631 |
|
|
|
632 |
|
|
ee/#mu#mu events
|
633 |
|
|
\end{comment}
|
634 |
|
|
|
635 |
|
|
& \MET\ $>$ 0 GeV & \MET\ $>$ 30 GeV & \MET\ $>$ 60 GeV & \MET\ $>$ 100 GeV & \MET\ $>$ 200 GeV & \MET\ $>$ 300 GeV \\
|
636 |
|
|
\hline
|
637 |
|
|
\zjets\ bkg & 10203 $\pm$ 3061 & 3449 $\pm$ 1035 & 320 $\pm$ 97 & 20.5 $\pm$ 6.3 & 2.1 $\pm$ 0.6 & 0.8 $\pm$ 0.2 \\
|
638 |
|
|
FS bkg & 356 $\pm$ 56 & 307 $\pm$ 48 & 201 $\pm$ 32 & 84.5 $\pm$ 13.5 & 7.2 $\pm$ 1.9 & 0.6 $\pm$ 0.4 \\
|
639 |
|
|
WZ bkg & 19.4 $\pm$ 13.6 & 15.7 $\pm$ 11.0 & 9.5 $\pm$ 6.6 & 4.5 $\pm$ 3.2 & 0.9 $\pm$ 0.8 & 0.2 $\pm$ 0.2 \\
|
640 |
|
|
ZZ bkg & 3.5 $\pm$ 1.8 & 3.1 $\pm$ 1.6 & 2.4 $\pm$ 1.2 & 1.5 $\pm$ 0.8 & 0.4 $\pm$ 0.4 & 0.1 $\pm$ 0.1 \\
|
641 |
|
|
rare SM bkg & 9.8 $\pm$ 4.9 & 8.5 $\pm$ 4.3 & 5.5 $\pm$ 2.8 & 2.8 $\pm$ 1.5 & 0.6 $\pm$ 0.5 & 0.1 $\pm$ 0.1 \\
|
642 |
|
|
\hline
|
643 |
|
|
total bkg & 10592 $\pm$ 3062 & 3783 $\pm$ 1036 & 538 $\pm$ 102 &{\bf 114 $\pm$ 15} & 11.2 $\pm$ 2.2 & 1.8 $\pm$ 0.5 \\
|
644 |
|
|
data & 10587 & 3673 & 533 & {\bf 113 } & 12 & 1 \\
|
645 |
|
|
significance & -0.0$\sigma$ & -0.1$\sigma$ & -0.0$\sigma$ & {\bf-0.0$\sigma$ } & & \\
|
646 |
|
|
\hline
|
647 |
|
|
\hline
|
648 |
|
|
|
649 |
|
|
|
650 |
|
|
|
651 |
|
|
\end{tabular}
|
652 |
|
|
\end{center}
|
653 |
|
|
\end{table}
|
654 |
|
|
|
655 |
|
|
\clearpage
|
656 |
|
|
|
657 |
|
|
|
658 |
|
|
\begin{figure}[!h]
|
659 |
|
|
\begin{center}
|
660 |
|
|
\begin{tabular}{cc}
|
661 |
|
|
\includegraphics[width=0.45\textwidth]{plots/pfmet_pt40_2012AB_highMet_all.pdf}
|
662 |
|
|
\includegraphics[width=0.45\textwidth]{plots/pfmet_pt40_2012C_highMet_all.pdf}
|
663 |
|
|
%\includegraphics[width=0.48\textwidth]{plots/pfmet_pt40_2012AB_highMet_all_linear.pdf}
|
664 |
|
|
\end{tabular}
|
665 |
|
|
\caption{\footnotesize Results of for the high \MET\ signal region.
|
666 |
|
|
The results for 5.1 fb$^{-1}$ 2012A+B data are displayed on the left, the results for 4.1 fb$^{-1}$ 2012C data are displayed on the right.
|
667 |
|
|
The observed \MET\ distribution (black points) is compared with the sum of the predicted \MET\
|
668 |
|
|
distributions from \zjets, flavor-symmetric backgrounds, WZ+ZZ backgrounds, and rare SM backgrounds.
|
669 |
|
|
The ratio of observed to predicted yields in each bin is
|
670 |
|
|
indicated. The error bars indicate the statistical uncertainty in the data and the shaded band indicates the total background uncertainty.
|
671 |
|
|
\label{fig:results_highmet}
|
672 |
|
|
}
|
673 |
|
|
\end{center}
|
674 |
|
|
\end{figure}
|
675 |
|
|
|
676 |
|
|
\begin{table}[htb]
|
677 |
|
|
\begin{center}
|
678 |
|
|
\footnotesize
|
679 |
|
|
\caption{\label{tab:results_highmet}\footnotesize Results for the high \MET\ signal region.
|
680 |
|
|
The results for 5.1 fb$^{-1}$ 2012A+B data are displayed in the top table, the results for 4.1 fb$^{-1}$ 2012C data are displayed in the bottom table.
|
681 |
|
|
The total background is the sum of the \zjets\ background predicted from
|
682 |
|
|
the \MET\ templates method (\zjets\ bkg), the flavor-symmetric background predicted from e$\mu$ events (FS bkg), the WZ and ZZ backgrounds predicted from MC
|
683 |
|
|
(WZ bkg and ZZ bkg) and the rare SM backgrounds. All uncertainties include both the statistical and systematic components. The Gaussian significance of the deviation between the data
|
684 |
|
|
and total background is indicated for signal regions with at least 20 observed events. }
|
685 |
|
|
\begin{tabular}{l|c|c|c|c|c|c}
|
686 |
|
|
|
687 |
|
|
\hline
|
688 |
|
|
\hline
|
689 |
|
|
|
690 |
|
|
\begin{comment}
|
691 |
|
|
Using pfmet out-of-the-box
|
692 |
|
|
Using pT > 40 GeV jets, high MET signal region
|
693 |
|
|
WZ/ZZ selection : (((((((leptype==0 && (ee==1 || isdata==0))||(leptype==1 && (mm==1 || isdata==0)))&&(ngennu>0))&&(csc==0 && hbhe==1 && hcallaser==1 && ecaltp==1 && trkfail==1 && eebadsc==1 && hbhenew==1))&&(dilmass>81 && dilmass<101))&&(lep1.pt()>20.0 && lep2.pt()>10.0))&&(njets40>=2))&&(ht40>=100.0)
|
694 |
|
|
WZ/ZZ weight : weight * 5.1 * vtxweight * trgeff
|
695 |
|
|
Opening ../output/V00-01-04/babylooper_data_ALL_53X_PhotonStitchedTemplate_pfmet_pt40_2012AB_highMet.root
|
696 |
|
|
B-veto? 0
|
697 |
|
|
K 0.13
|
698 |
|
|
ee+mm channels: scale em yield by 0.99
|
699 |
|
|
Yields in 0-60 GeV region
|
700 |
|
|
data : 71590
|
701 |
|
|
gjets : 72503.5
|
702 |
|
|
OF : 717.116
|
703 |
|
|
WZ : 63.8074
|
704 |
|
|
ZZ : 7.50741
|
705 |
|
|
Rare : 8.60544
|
706 |
|
|
Scaling gjets by : 0.976408
|
707 |
|
|
SF events 73711
|
708 |
|
|
OF events 11965
|
709 |
|
|
|
710 |
|
|
ee/#mu#mu events
|
711 |
|
|
\end{comment}
|
712 |
|
|
|
713 |
|
|
|
714 |
|
|
|
715 |
|
|
& \MET\ $>$ 0 GeV & \MET\ $>$ 30 GeV & \MET\ $>$ 60 GeV & \MET\ $>$ 100 GeV & \MET\ $>$ 150 GeV & \MET\ $>$ 300 GeV \\
|
716 |
|
|
\hline
|
717 |
|
|
\zjets\ bkg & 71975 $\pm$ 21593 & 19573 $\pm$ 5873 & 1182 $\pm$ 355 & 70.7 $\pm$ 21.4 & 13.6 $\pm$ 4.2 & 0.4 $\pm$ 0.4 \\
|
718 |
|
|
FS bkg & 1540 $\pm$ 255 & 1293 $\pm$ 214 & 823 $\pm$ 136 & 313 $\pm$ 52 & 68.6 $\pm$ 11.7 & 2.4 $\pm$ 1.1 \\
|
719 |
|
|
WZ bkg & 115.9 $\pm$ 81.2 & 91.8 $\pm$ 64.3 & 52.1 $\pm$ 36.5 & 22.4 $\pm$ 15.7 & 8.9 $\pm$ 6.3 & 0.8 $\pm$ 0.8 \\
|
720 |
|
|
ZZ bkg & 22.6 $\pm$ 11.3 & 20.3 $\pm$ 10.2 & 15.1 $\pm$ 7.6 & 8.8 $\pm$ 4.5 & 4.3 $\pm$ 2.3 & 0.5 $\pm$ 0.5 \\
|
721 |
|
|
rare SM bkg & 20.6 $\pm$ 10.3 & 17.9 $\pm$ 9.0 & 12.0 $\pm$ 6.1 & 6.3 $\pm$ 3.2 & 2.8 $\pm$ 1.5 & 0.3 $\pm$ 0.3 \\
|
722 |
|
|
\hline
|
723 |
|
|
total bkg & 73674 $\pm$ 21595 & 20996 $\pm$ 5877 & 2084 $\pm$ 382 & 421 $\pm$ 59 &{\bf 98.1 $\pm$ 14.2}& 4.5 $\pm$ 1.5 \\
|
724 |
|
|
data & 73711 & 20601 & 2121 & 446 & {\bf 95 } & 4 \\
|
725 |
|
|
significance & 0.0$\sigma$ & -0.1$\sigma$ & 0.1$\sigma$ & 0.4$\sigma$ &{\bf -0.2$\sigma$ } & \\
|
726 |
|
|
|
727 |
|
|
\hline
|
728 |
|
|
\hline
|
729 |
|
|
|
730 |
|
|
\begin{comment}
|
731 |
|
|
Using pfmet out-of-the-box
|
732 |
|
|
Using pT > 40 GeV jets, high MET signal region
|
733 |
|
|
WZ/ZZ selection : (((((((leptype==0 && (ee==1 || isdata==0))||(leptype==1 && (mm==1 || isdata==0)))&&(ngennu>0))&&(csc==0 && hbhe==1 && hcallaser==1 && ecaltp==1 && trkfail==1 && eebadsc==1 && hbhenew==1))&&(dilmass>81 && dilmass<101))&&(lep1.pt()>20.0 && lep2.pt()>10.0))&&(njets40>=2))&&(ht40>=100.0)
|
734 |
|
|
WZ/ZZ weight : weight * 4.1 * vtxweight * trgeff
|
735 |
|
|
Opening ../output/V00-01-04/babylooper_data_ALL_53X_PhotonStitchedTemplate_pfmet_pt40_2012C_highMet.root
|
736 |
|
|
B-veto? 0
|
737 |
|
|
K 0.13
|
738 |
|
|
ee+mm channels: scale em yield by 0.99
|
739 |
|
|
Yields in 0-60 GeV region
|
740 |
|
|
data : 56788
|
741 |
|
|
gjets : 57414.8
|
742 |
|
|
OF : 557.657
|
743 |
|
|
WZ : 51.2961
|
744 |
|
|
ZZ : 6.03537
|
745 |
|
|
Rare : 6.9181
|
746 |
|
|
Scaling gjets by : 0.978251
|
747 |
|
|
SF events 58478
|
748 |
|
|
OF events 9373
|
749 |
|
|
|
750 |
|
|
ee/#mu#mu events
|
751 |
|
|
\end{comment}
|
752 |
|
|
|
753 |
|
|
& \MET\ $>$ 0 GeV & \MET\ $>$ 30 GeV & \MET\ $>$ 60 GeV & \MET\ $>$ 100 GeV & \MET\ $>$ 150 GeV & \MET\ $>$ 300 GeV \\
|
754 |
|
|
\hline
|
755 |
|
|
\zjets\ bkg & 57206 $\pm$ 17163 & 15965 $\pm$ 4790 & 1040 $\pm$ 313 & 68.3 $\pm$ 21.5 & 17.5 $\pm$ 6.0 & 1.4 $\pm$ 0.4 \\
|
756 |
|
|
FS bkg & 1206 $\pm$ 200 & 1015 $\pm$ 168 & 649 $\pm$ 108 & 244 $\pm$ 41 & 48.1 $\pm$ 8.3 & 1.3 $\pm$ 0.6 \\
|
757 |
|
|
WZ bkg & 93.2 $\pm$ 65.3 & 73.8 $\pm$ 51.7 & 41.9 $\pm$ 29.4 & 18.0 $\pm$ 12.7 & 7.1 $\pm$ 5.1 & 0.7 $\pm$ 0.7 \\
|
758 |
|
|
ZZ bkg & 18.2 $\pm$ 9.1 & 16.3 $\pm$ 8.2 & 12.1 $\pm$ 6.1 & 7.1 $\pm$ 3.6 & 3.4 $\pm$ 1.8 & 0.4 $\pm$ 0.4 \\
|
759 |
|
|
rare SM bkg & 16.6 $\pm$ 8.3 & 14.4 $\pm$ 7.2 & 9.7 $\pm$ 4.9 & 5.1 $\pm$ 2.6 & 2.3 $\pm$ 1.2 & 0.3 $\pm$ 0.3 \\
|
760 |
|
|
\hline
|
761 |
|
|
total bkg & 58541 $\pm$ 17164 & 17084 $\pm$ 4793 & 1753 $\pm$ 332 & 343 $\pm$ 48 &{\bf 78.4 $\pm$ 11.7}& 4.0 $\pm$ 1.1 \\
|
762 |
|
|
data & 58478 & 16494 & 1690 & 321 & {\bf 72 } & 1 \\
|
763 |
|
|
significance & -0.0$\sigma$ & -0.1$\sigma$ & -0.2$\sigma$ & -0.4$\sigma$ &{\bf -0.4$\sigma$} & \\
|
764 |
|
|
|
765 |
|
|
\hline
|
766 |
|
|
\hline
|
767 |
|
|
|
768 |
|
|
\end{tabular}
|
769 |
|
|
\end{center}
|
770 |
|
|
\end{table}
|
771 |
|
|
|
772 |
|
|
|
773 |
|
|
\clearpage
|
774 |
|
|
|
775 |
|
|
|
776 |
|
|
|
777 |
|
|
\begin{figure}[!h]
|
778 |
|
|
\begin{center}
|
779 |
|
|
\begin{tabular}{cc}
|
780 |
|
|
\includegraphics[width=0.45\textwidth]{plots/pfmet_pt40_lowMet_all.pdf}
|
781 |
|
|
\includegraphics[width=0.45\textwidth]{plots/pfmet_pt40_highMet_all.pdf}
|
782 |
|
|
%\includegraphics[width=0.48\textwidth]{plots/pfmet_pt40_2012AB_highMet_all_linear.pdf}
|
783 |
|
|
\end{tabular}
|
784 |
|
|
\caption{\footnotesize Results of for the low \MET\ (left) and high \MET\ (right) signal regions for the full 9.2 fb$^{-1}$ sample.
|
785 |
|
|
The observed \MET\ distribution (black points) is compared with the sum of the predicted \MET\
|
786 |
|
|
distributions from \zjets, flavor-symmetric backgrounds, WZ+ZZ backgrounds, and rare SM backgrounds.
|
787 |
|
|
The ratio of observed to predicted yields in each bin is
|
788 |
|
|
indicated. The error bars indicate the statistical uncertainty in the data and the shaded band indicates the total background uncertainty.
|
789 |
|
|
\label{fig:results_fulledge}
|
790 |
|
|
}
|
791 |
|
|
\end{center}
|
792 |
|
|
\end{figure}
|
793 |
|
|
|
794 |
|
|
\begin{table}[htb]
|
795 |
|
|
\begin{center}
|
796 |
|
|
\footnotesize
|
797 |
|
|
\caption{\label{tab:results_edgefull}\footnotesize Results for the low \MET\ signal region (top table) and high \MET\ signal region (bottom table).
|
798 |
|
|
The total background is the sum of the \zjets\ background predicted from
|
799 |
|
|
the \MET\ templates method (\zjets\ bkg), the flavor-symmetric background predicted from e$\mu$ events (FS bkg), the WZ and ZZ backgrounds predicted from MC
|
800 |
|
|
(WZ bkg and ZZ bkg) and the rare SM backgrounds. All uncertainties include both the statistical and systematic components. The Gaussian significance of the deviation between the data
|
801 |
|
|
and total background is indicated for signal regions with at least 20 observed events. }
|
802 |
|
|
\begin{tabular}{l|c|c|c|c|c|c}
|
803 |
|
|
|
804 |
|
|
\hline
|
805 |
|
|
\hline
|
806 |
|
|
|
807 |
|
|
\begin{comment}
|
808 |
|
|
Using pfmet out-of-the-box
|
809 |
|
|
Using pT > 40 GeV jets, low MET signal region
|
810 |
|
|
WZ/ZZ selection : ((((((leptype==0 && (ee==1 || isdata==0))||(leptype==1 && (mm==1 || isdata==0)))&&(ngennu>0))&&(csc==0 && hbhe==1 && hcallaser==1 && ecaltp==1 && trkfail==1 && eebadsc==1 && hbhenew==1))&&(dilmass>81 && dilmass<101))&&(lep1.pt()>20.0 && lep2.pt()>20.0))&&(njets40>=3)
|
811 |
|
|
WZ/ZZ weight : weight * 9.2 * vtxweight * trgeff
|
812 |
|
|
Opening ../output/V00-01-04/babylooper_data_ALL_53X_PhotonStitchedTemplate_pfmet_pt40_lowMet.root
|
813 |
|
|
B-veto? 0
|
814 |
|
|
K 0.14
|
815 |
|
|
ee+mm channels: scale em yield by 0.99
|
816 |
|
|
Yields in 0-60 GeV region
|
817 |
|
|
data : 22782
|
818 |
|
|
gjets : 23298
|
819 |
|
|
OF : 350.242
|
820 |
|
|
WZ : 22.2641
|
821 |
|
|
ZZ : 2.36791
|
822 |
|
|
Rare : 9.60548
|
823 |
|
|
Scaling gjets by : 0.96135
|
824 |
|
|
SF events 23999
|
825 |
|
|
OF events 5826
|
826 |
|
|
|
827 |
|
|
ee/#mu#mu events
|
828 |
|
|
\end{comment}
|
829 |
|
|
& \MET\ $>$ 0 GeV & \MET\ $>$ 30 GeV & \MET\ $>$ 60 GeV & \MET\ $>$ 100 GeV & \MET\ $>$ 200 GeV & \MET\ $>$ 300 GeV \\
|
830 |
|
|
\hline
|
831 |
|
|
\zjets\ bkg & 23072 $\pm$ 6922 & 7566 $\pm$ 2270 & 674 $\pm$ 203 & 47.9 $\pm$ 14.6 & 4.7 $\pm$ 1.6 & 1.1 $\pm$ 0.4 \\
|
832 |
|
|
FS bkg & 807 $\pm$ 126 & 695 $\pm$ 108 & 457 $\pm$ 71 & 184 $\pm$ 29 & 14.1 $\pm$ 3.4 & 1.5 $\pm$ 0.9 \\
|
833 |
|
|
WZ bkg & 43.5 $\pm$ 30.5 & 35.1 $\pm$ 24.6 & 21.3 $\pm$ 14.9 & 10.0 $\pm$ 7.1 & 1.9 $\pm$ 1.7 & 0.4 $\pm$ 0.4 \\
|
834 |
|
|
ZZ bkg & 7.8 $\pm$ 3.9 & 7.0 $\pm$ 3.6 & 5.4 $\pm$ 2.8 & 3.3 $\pm$ 1.8 & 0.9 $\pm$ 0.8 & 0.2 $\pm$ 0.2 \\
|
835 |
|
|
rare SM bkg & 22.0 $\pm$ 11.0 & 19.0 $\pm$ 9.6 & 12.4 $\pm$ 6.3 & 6.3 $\pm$ 3.3 & 1.3 $\pm$ 1.1 & 0.3 $\pm$ 0.3 \\
|
836 |
|
|
\hline
|
837 |
|
|
total bkg & 23952 $\pm$ 6923 & 8323 $\pm$ 2273 & 1170 $\pm$ 216 &{\bf 251 $\pm$ 33} & 22.8 $\pm$ 4.4 & 3.5 $\pm$ 1.1 \\
|
838 |
|
|
data & 23999 & 8134 & 1217 &{\bf 288} & 26 & 4 \\
|
839 |
|
|
significance & 0.0$\sigma$ & -0.1$\sigma$ & 0.2$\sigma$ &{\bf 1.0$\sigma$} & 0.5$\sigma$ & \\
|
840 |
|
|
\hline
|
841 |
|
|
\hline
|
842 |
|
|
|
843 |
|
|
\begin{comment}
|
844 |
|
|
Using pfmet out-of-the-box
|
845 |
|
|
Using pT > 40 GeV jets, high MET signal region
|
846 |
|
|
WZ/ZZ selection : (((((((leptype==0 && (ee==1 || isdata==0))||(leptype==1 && (mm==1 || isdata==0)))&&(ngennu>0))&&(csc==0 && hbhe==1 && hcallaser==1 && ecaltp==1 && trkfail==1 && eebadsc==1 && hbhenew==1))&&(dilmass>81 && dilmass<101))&&(lep1.pt()>20.0 && lep2.pt()>10.0))&&(njets40>=2))&&(ht40>=100.0)
|
847 |
|
|
WZ/ZZ weight : weight * 9.2 * vtxweight * trgeff
|
848 |
|
|
Opening ../output/V00-01-04/babylooper_data_ALL_53X_PhotonStitchedTemplate_pfmet_pt40_highMet.root
|
849 |
|
|
B-veto? 0
|
850 |
|
|
K 0.13
|
851 |
|
|
ee+mm channels: scale em yield by 0.99
|
852 |
|
|
Yields in 0-60 GeV region
|
853 |
|
|
data : 128378
|
854 |
|
|
gjets : 129908
|
855 |
|
|
OF : 1274.77
|
856 |
|
|
WZ : 115.104
|
857 |
|
|
ZZ : 13.5428
|
858 |
|
|
Rare : 15.5235
|
859 |
|
|
Scaling gjets by : 0.977303
|
860 |
|
|
SF events 132189
|
861 |
|
|
OF events 21338
|
862 |
|
|
|
863 |
|
|
ee/#mu#mu events
|
864 |
|
|
\end{comment}
|
865 |
|
|
|
866 |
|
|
& \MET\ $>$ 0 GeV & \MET\ $>$ 30 GeV & \MET\ $>$ 60 GeV & \MET\ $>$ 100 GeV & \MET\ $>$ 150 GeV & \MET\ $>$ 300 GeV \\
|
867 |
|
|
\hline
|
868 |
|
|
\zjets\ bkg &129184 $\pm$ 38756 & 35565 $\pm$ 10670 & 2225 $\pm$ 668 & 140 $\pm$ 43 & 31.6 $\pm$ 10.1 & 1.7 $\pm$ 0.6 \\
|
869 |
|
|
FS bkg & 2746 $\pm$ 454 & 2308 $\pm$ 382 & 1471 $\pm$ 243 & 557 $\pm$ 92 & 117 $\pm$ 20 & 3.7 $\pm$ 1.6 \\
|
870 |
|
|
WZ bkg & 209.2 $\pm$ 146.4 & 165.6 $\pm$ 115.9 & 94.1 $\pm$ 65.9 & 40.5 $\pm$ 28.4 & 16.0 $\pm$ 11.3 & 1.5 $\pm$ 1.5 \\
|
871 |
|
|
ZZ bkg & 40.8 $\pm$ 20.4 & 36.6 $\pm$ 18.4 & 27.2 $\pm$ 13.7 & 16.0 $\pm$ 8.1 & 7.7 $\pm$ 4.1 & 0.9 $\pm$ 0.9 \\
|
872 |
|
|
rare SM bkg & 37.2 $\pm$ 18.7 & 32.2 $\pm$ 16.2 & 21.7 $\pm$ 10.9 & 11.4 $\pm$ 5.8 & 5.1 $\pm$ 2.8 & 0.6 $\pm$ 0.6 \\
|
873 |
|
|
\hline
|
874 |
|
|
total bkg &132217 $\pm$ 38759 & 38108 $\pm$ 10678 & 3839 $\pm$ 714 & 765 $\pm$ 106 &{\bf 177 $\pm$ 25} & 8.4 $\pm$ 2.5 \\
|
875 |
|
|
data & 132189 & 37095 & 3811 & 767 &{\bf 167} & 5 \\
|
876 |
|
|
significance & -0.0$\sigma$ & -0.1$\sigma$ & -0.0$\sigma$ & 0.0$\sigma$ &{\bf -0.4$\sigma$} & \\
|
877 |
|
|
|
878 |
|
|
\hline
|
879 |
|
|
\hline
|
880 |
|
|
|
881 |
|
|
\end{tabular}
|
882 |
|
|
\end{center}
|
883 |
|
|
\end{table}
|
884 |
|
|
|
885 |
|
|
|
886 |
|
|
|
887 |
|
|
|
888 |
|
|
\clearpage
|
889 |
|
|
|
890 |
|
|
|
891 |
|
|
\begin{figure}[t]
|
892 |
|
|
\begin{center}
|
893 |
|
|
\begin{tabular}{cc}
|
894 |
|
|
\includegraphics[width=0.4\textwidth]{plots/Routin_lowmet.pdf} &
|
895 |
|
|
\includegraphics[width=0.4\textwidth]{plots/Routin_highMET.pdf} \\
|
896 |
|
|
\end{tabular}
|
897 |
|
|
\caption{\label{fig:Routin}
|
898 |
|
|
The ratio $R_{low/in}$ of low mass ($15<m_{\ell\ell}<70$ GeV) to on-Z ($81<m_{\ell\ell}<101$ GeV) events, as a function of
|
899 |
|
|
the \MET\ requirement. The left plot corresponds to the low \MET\ signal region (2 \pt\ $>$ 20 GeV leptons with at least 3 jets),
|
900 |
|
|
the right plot corresponds to the high \MET\ signal region (\pt\ $>$ (20,10) GeV leptons with at least 2 jets).
|
901 |
|
|
}
|
902 |
|
|
\end{center}
|
903 |
|
|
\end{figure}
|
904 |
|
|
|
905 |
|
|
Given a prediction for the Z background in the Z mass window, we can extrapolate to estimate the low mass $\gamma^*$/Z contribution.
|
906 |
|
|
We extract the ratio $R_{low/in}$ of low-mass to on-shell Z events from data,
|
907 |
|
|
correcting for the contribution from flavor-symmetric backgrounds, according to:
|
908 |
|
|
|
909 |
|
|
\begin{equation}
|
910 |
|
|
R_{low/in} = (N_{SF}^{low}-N_{OF}^{low})/(N_{SF}^{in}-N_{OF}^{in}).
|
911 |
|
|
\end{equation}
|
912 |
|
|
|
913 |
|
|
Here SF and OF refer to the same-flavor and opposite-flavor data yields in the ``low'' ($15<m_{\ell\ell}<70$ GeV) and ``in''
|
914 |
|
|
($81<m_{\ell\ell}<101$ GeV) dilepton mass regions. To predict the low-mass $\gamma^*$/Z contribution, we scale the total predicted
|
915 |
|
|
Z background by this quantity, which is displayed in Fig.~\ref{fig:Routin}. Here we measure $R_{low/in}$ in several \MET\ regions,
|
916 |
|
|
and assess the uncertainty based on the variation with respect to \MET.
|
917 |
|
|
Based on this plot we choose $R_{low/in}=0.08\pm0.02$ for the low \MET\ signal region and $R_{low/in}=0.13\pm0.03$ for the high \MET\ region.
|
918 |
|
|
|
919 |
|
|
\clearpage
|
920 |
|
|
|
921 |
|
|
We find the following results for the first 5.1 fb$^{-1}$. For the low \MET\ signal region, the total predicted Z background in the Z mass region is $39\pm9.6$
|
922 |
|
|
(sum of the \zjets, WZ+ZZ, and rare SM backgrounds from Table~\ref{tab:results_lowmet}, \MET\ $>$ 100 GeV region),
|
923 |
|
|
resulting in a $\gamma^*$/Z prediction of $3.1\pm1.1$ events.
|
924 |
|
|
For the high \MET\ signal region, the total predicted Z background in the Z mass region is $30\pm8.1$
|
925 |
|
|
(sum of the \zjets, WZ+ZZ, and rare SM backgrounds from Table~\ref{tab:results_highmet}, \MET\ $>$ 150 GeV region),
|
926 |
|
|
resulting in a $\gamma^*$/Z prediction of $3.8\pm1.4$ events.
|
927 |
|
|
Hence we summarize the 5.1 fb$^{-1}$ results as:
|
928 |
|
|
|
929 |
|
|
\begin{itemize}
|
930 |
|
|
\item Low \MET\ signal region
|
931 |
|
|
\begin{itemize}
|
932 |
|
|
\item Total predicted background in Z mass region: $138\pm18$ events
|
933 |
|
|
\item Total observed yield in Z mass region: 175 events ($+1.6\sigma$)
|
934 |
|
|
\item Low-mass $\gamma^*$/Z prediction: $3.1\pm1.1$ events
|
935 |
|
|
\end{itemize}
|
936 |
|
|
\item High \MET\ signal region
|
937 |
|
|
\begin{itemize}
|
938 |
|
|
\item Total predicted background in Z mass region: $98\pm14$ events
|
939 |
|
|
\item Total observed yield in Z mass region: 95 events ($-0.2\sigma$)
|
940 |
|
|
\item Low-mass $\gamma^*$/Z prediction: $3.8\pm1.4$ events
|
941 |
|
|
\end{itemize}
|
942 |
|
|
\end{itemize}
|
943 |
|
|
|
944 |
|
|
We find the following results for the full 9.2 fb$^{-1}$. For the low \MET\ signal region, the total predicted Z background in the Z mass region is $68\pm17$
|
945 |
|
|
(sum of the \zjets, WZ+ZZ, and rare SM backgrounds from Table~\ref{tab:results_edgefull}, \MET\ $>$ 100 GeV region),
|
946 |
|
|
resulting in a $\gamma^*$/Z prediction of $5.4\pm1.9$ events.
|
947 |
|
|
For the high \MET\ signal region, the total predicted Z background in the Z mass region is $60\pm16$
|
948 |
|
|
(sum of the \zjets, WZ+ZZ, and rare SM backgrounds from Table~\ref{tab:results_edgefull}, \MET\ $>$ 150 GeV region),
|
949 |
|
|
resulting in a $\gamma^*$/Z prediction of $7.9\pm2.7$ events.
|
950 |
|
|
Hence we summarize the 9.2 fb$^{-1}$ results as:
|
951 |
|
|
|
952 |
|
|
\begin{itemize}
|
953 |
|
|
\item Low \MET\ signal region
|
954 |
|
|
\begin{itemize}
|
955 |
|
|
\item Total predicted background in Z mass region: $251\pm33$ events
|
956 |
|
|
\item Total observed yield in Z mass region: 288 events ($+1.0\sigma$)
|
957 |
|
|
\item Low-mass $\gamma^*$/Z prediction: $5.4\pm1.9$ events
|
958 |
|
|
\end{itemize}
|
959 |
|
|
\item High \MET\ signal region
|
960 |
|
|
\begin{itemize}
|
961 |
|
|
\item Total predicted background in Z mass region: $177\pm25$ events
|
962 |
|
|
\item Total observed yield in Z mass region: 167 events ($-0.4\sigma$)
|
963 |
|
|
\item Low-mass $\gamma^*$/Z prediction: $7.9\pm2.7$ events
|
964 |
|
|
\end{itemize}
|
965 |
|
|
\end{itemize}
|
966 |
|
|
|
967 |
|
|
\clearpage
|
968 |
|
|
|
969 |
|
|
\subsection{Cross-check with single lepton triggers}
|
970 |
|
|
\label{sec:edge_triggers}
|
971 |
|
|
|
972 |
|
|
The nominal ``edge analysis'' is performed with dilepton triggers. An excess of SF vs. OF events may thus be observed if there
|
973 |
|
|
were some inefficiency for the e$\mu$ triggers used in this analysis. In this section we provide a cross-check of the nominal
|
974 |
|
|
analysis by including events collected with single lepton triggers. The relevant triggers are:
|
975 |
|
|
|
976 |
|
|
\begin{itemize}
|
977 |
|
|
|
978 |
|
|
\item ee channel
|
979 |
|
|
\begin{itemize}
|
980 |
|
|
\item dilepton: {\footnotesize \verb=HLT_Ele17_CaloIdT_CaloIsoVL_TrkIdVL_TrkIsoVL_Ele8_CaloIdT_CaloIsoVL_TrkIdVL_TrkIsoVL=}
|
981 |
|
|
\item single lepton: \verb=HLT_Ele27_WP80=
|
982 |
|
|
\end{itemize}
|
983 |
|
|
|
984 |
|
|
\item $\mu\mu$ channel
|
985 |
|
|
\begin{itemize}
|
986 |
|
|
\item dilepton: \verb=HLT_Mu17_Mu8= OR \verb=HLT_Mu17_TkMu8=
|
987 |
|
|
\item single lepton: \verb=HLT_IsoMu24= OR \verb=HLT_IsoMu24_eta2p1=
|
988 |
|
|
\end{itemize}
|
989 |
|
|
|
990 |
|
|
\item $e\mu$ channel
|
991 |
|
|
\begin{itemize}
|
992 |
|
|
\item dilepton: \verb=HLT_MuX_EleY_CaloIdT_CaloIsoVL_TrkIdVL_TrkIsoVL= (X,Y=17,8 OR 8,17)
|
993 |
|
|
\item single lepton: \verb=HLT_Ele27_WP80= OR \verb=HLT_IsoMu24= OR \verb=HLT_IsoMu24_eta2p1=
|
994 |
|
|
\end{itemize}
|
995 |
|
|
|
996 |
|
|
\end{itemize}
|
997 |
|
|
|
998 |
|
|
|
999 |
|
|
In the nominal analysis based on dilepton triggers only, an ee event is required to satisfy the ee dilepton trigger, a $\mu\mu$ event is required to
|
1000 |
|
|
satisfy one of the two $\mu\mu$ dilepton triggers, and an e$\mu$ event is required to satisfy one of the two e$\mu$ dilepton triggers. Here we compare
|
1001 |
|
|
the results obtained from the nominal dilepton triggers with those obtained by requiring an OR of the dilepton and single lepton triggers. In this cross-check,
|
1002 |
|
|
an ee event is required to satisfy the ee dilepton trigger OR single electron trigger, a $\mu\mu$ event is required to
|
1003 |
|
|
satisfy one of the two $\mu\mu$ dilepton triggers OR one of the two single muon triggers, and an e$\mu$ event is required to satisfy one of the two e$\mu$ dilepton triggers
|
1004 |
benhoob |
1.2 |
OR the single electron trigger OR the single muon trigger. The results are summarized in Table~\ref{tab:triggers}. Including the single lepton triggers increases
|
1005 |
|
|
the yields in the ee, $\mu\mu$ and e$\mu$ final states by (1--7)\%, and does not significantly alter the excess of SF vs. OF data yields.
|
1006 |
benhoob |
1.1 |
|
1007 |
|
|
\begin{table}[htb]
|
1008 |
|
|
\begin{center}
|
1009 |
|
|
\footnotesize
|
1010 |
|
|
\caption{\label{tab:triggers} Summary of results comparing dilepton vs. dilepton OR single lepton triggers, for 5.1 fb$^{-1}$,
|
1011 |
|
|
in the low \MET\ and high \MET\ signal regions (SR). The ratio of the dilepton OR single lepton yield to the dilepton only yield
|
1012 |
|
|
is indicated, along with the excess of SF w.r.t. OF events.}
|
1013 |
|
|
\begin{tabular}{l|c|c|c|c}
|
1014 |
|
|
\hline
|
1015 |
|
|
\hline
|
1016 |
|
|
Region & $N_{\rm{ee}}$ & $N_{\mu\mu}$ & $N_{\rm{e}\mu}$ & $N_{\rm{ee}}+N_{\mu\mu}-N_{\rm{e}\mu}$ \\
|
1017 |
|
|
\hline
|
1018 |
|
|
\hline
|
1019 |
|
|
Low \MET\ SR and $20<m_{\ell\ell}<70$~GeV & & & \\
|
1020 |
|
|
dilepton (nominal) & 106 & 153 & 189 & 70 $\pm$ 21.2 (stat) \\
|
1021 |
|
|
dilepton OR single lepton & 112 & 155 & 199 & 68 $\pm$ 21.6 (stat) \\
|
1022 |
|
|
ratio & 1.06 & 1.01 & 1.05 & \\
|
1023 |
|
|
\hline
|
1024 |
|
|
\hline
|
1025 |
|
|
Low \MET\ SR and $m_{\ell\ell}>20$~GeV & & & \\
|
1026 |
|
|
dilepton (nominal) & 357 & 517 & 693 & 181 $\pm$ 39.6 (stat) \\
|
1027 |
|
|
dilepton OR single lepton & 368 & 534 & 739 & 163 $\pm$ 40.5 (stat) \\
|
1028 |
|
|
ratio & 1.03 & 1.03 & 1.07 & \\
|
1029 |
|
|
\hline
|
1030 |
|
|
\hline
|
1031 |
|
|
High \MET\ SR and $15<m_{\ell\ell}<70$~GeV & & & \\
|
1032 |
|
|
dilepton (nominal) & 89 & 157 & 187 & 59 $\pm$ 20.8 (stat) \\
|
1033 |
|
|
dilepton OR single lepton & 93 & 160 & 197 & 56 $\pm$ 21.2 (stat) \\
|
1034 |
|
|
ratio & 1.04 & 1.02 & 1.05 & \\
|
1035 |
|
|
\hline
|
1036 |
|
|
\hline
|
1037 |
|
|
High \MET\ SR and $m_{\ell\ell}>15$~GeV & & & \\
|
1038 |
|
|
dilepton (nominal) & 258 & 380 & 527 & 111 $\pm$ 34.1 (stat) \\
|
1039 |
|
|
dilepton OR single lepton & 271 & 386 & 553 & 104 $\pm$ 34.8 (stat) \\
|
1040 |
|
|
ratio & 1.05 & 1.02 & 1.05 & \\
|
1041 |
|
|
\hline
|
1042 |
|
|
\hline
|
1043 |
|
|
\end{tabular}
|
1044 |
|
|
\end{center}
|
1045 |
|
|
\end{table}
|
1046 |
|
|
|
1047 |
benhoob |
1.2 |
\clearpage
|
1048 |
benhoob |
1.1 |
|
1049 |
benhoob |
1.2 |
Next, we compare the results obtained with the dilepton triggers to results obtained with single lepton triggers only. Since the single electron (single muon)
|
1050 |
|
|
triggers have \pt\ thresholds of 27 (24) GeV, we use a dilepton \pt\ $>$ (30,20) selection. The results are summarized in Table~\ref{tab:trigger2}.
|
1051 |
|
|
Switching from dilepton to single lepton triggers alters the yields by (-2--5)\%, and does not significantly alter the excess of SF vs. OF data yields.
|
1052 |
benhoob |
1.1 |
|
1053 |
|
|
\begin{table}[htb]
|
1054 |
|
|
\begin{center}
|
1055 |
|
|
\footnotesize
|
1056 |
|
|
\caption{\label{tab:trigger2} Summary of results comparing dilepton vs. single lepton triggers (with a dilepton \pt\ $>$ (30,20) GeV selection,
|
1057 |
|
|
for 5.1 fb$^{-1}$, in the low \MET\ and high \MET\ signal regions (SR). The ratio of the single lepton trigger yield to the dilepton trigger yield
|
1058 |
|
|
is indicated, along with the excess of SF w.r.t. OF events.}
|
1059 |
|
|
\begin{tabular}{l|c|c|c|c}
|
1060 |
|
|
\hline
|
1061 |
|
|
\hline
|
1062 |
|
|
Region & $N_{\rm{ee}}$ & $N_{\mu\mu}$ & $N_{\rm{e}\mu}$ & $N_{\rm{ee}}+N_{\mu\mu}-N_{\rm{e}\mu}$ \\
|
1063 |
|
|
\hline
|
1064 |
|
|
\hline
|
1065 |
|
|
Low \MET\ SR and $20<m_{\ell\ell}<70$~GeV & & & \\
|
1066 |
|
|
dilepton & 95 & 135 & 169 & 61 $\pm$ 20.0 (stat) \\
|
1067 |
|
|
single lepton & 93 & 134 & 172 & 55 $\pm$ 20.0 (stat) \\
|
1068 |
|
|
ratio & 0.98 & 0.99 & 1.02 & \\
|
1069 |
|
|
\hline
|
1070 |
|
|
\hline
|
1071 |
|
|
Low \MET\ SR and $m_{\ell\ell}>20$~GeV & & & \\
|
1072 |
|
|
dilepton & 345 & 497 & 669 & 173 $\pm$ 38.9 (stat) \\
|
1073 |
|
|
single lepton & 346 & 499 & 700 & 145 $\pm$ 39.3 (stat) \\
|
1074 |
|
|
ratio & 1.00 & 1.00 & 1.05 & \\
|
1075 |
|
|
\hline
|
1076 |
|
|
\hline
|
1077 |
|
|
High \MET\ SR and $15<m_{\ell\ell}<70$~GeV & & & \\
|
1078 |
|
|
dilepton & 48 & 72 & 79 & 41 $\pm$ 14.1 (stat) \\
|
1079 |
|
|
single lepton & 47 & 72 & 81 & 38 $\pm$ 14.1 (stat) \\
|
1080 |
|
|
ratio & 0.98 & 1.00 & 1.03 & \\
|
1081 |
|
|
\hline
|
1082 |
|
|
\hline
|
1083 |
|
|
High \MET\ SR and $m_{\ell\ell}>15$~GeV & & & \\
|
1084 |
|
|
dilepton & 197 & 270 & 367 & 100 $\pm$ 28.9 (stat) \\
|
1085 |
|
|
single lepton & 200 & 269 & 377 & 92 $\pm$ 29.1 (stat) \\
|
1086 |
|
|
ratio & 1.02 & 1.00 & 1.03 & \\
|
1087 |
|
|
\hline
|
1088 |
|
|
\hline
|
1089 |
|
|
\end{tabular}
|
1090 |
|
|
\end{center}
|
1091 |
|
|
\end{table}
|
1092 |
|
|
|
1093 |
benhoob |
1.2 |
|