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In 30 pb$^{-1}$ we expect $\approx$ 1 SM event in |
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the signal region. The expectations from the LMO |
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and LM1 SUSY benchmark points are 5.6 and |
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2.2 events respectively. {\color{red} I took these |
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numbers from the twiki, rescaling from 11.06 to 30/pb. |
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They seem too large...are they really right?} |
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2.2 events respectively. |
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%{\color{red} I took these |
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%numbers from the twiki, rescaling from 11.06 to 30/pb. |
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%They seem too large...are they really right?} |
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|
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|
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\subsection{ABCD method} |
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\begin{center} |
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\caption{\label{tab:victorybad} Test of the data driven method in Monte Carlo |
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under different assumptions. See text for details.} |
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< |
\begin{tabular}{|l|c|c|c|c|c|c|c|} |
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\begin{tabular}{|l|c|c|c|c|c|c|c|c|} |
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\hline |
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& True $t\bar{t}$ dilepton & $t\to W\to\tau$& other SM & GEN or & Z Veto, Lepton $P_T$ & \met $>$ 50& obs/pred \\ |
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& included & included & included & RECOSIM & and $\eta$ cuts & & \\ \hline |
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1&Y & N & N & GEN & N & N & 2.16 \\ |
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2&Y & N & N & GEN & Y & N & 1.48 \\ |
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3&Y & N & N & GEN & Y & Y & 1.52 \\ |
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4&Y & N & N & RECOSIM & Y & Y & 1.51 \\ |
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5&Y & Y & N & RECOSIM & Y & Y & 1.58 \\ |
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6&Y & Y & Y & RECOSIM & Y & Y & 1.18 \\ |
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& True $t\bar{t}$ dilepton & $t\to W\to\tau$& other SM & GEN or & Lepton $P_T$ & Z veto & \met $>$ 50& obs/pred \\ |
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& included & included & included & RECOSIM & and $\eta$ cuts & & & \\ \hline |
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1&Y & N & N & GEN & N & N & N & 1.90 \\ |
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2&Y & N & N & GEN & Y & N & N & 1.64 \\ |
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> |
3&Y & N & N & GEN & Y & Y & N & 1.59 \\ |
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> |
4&Y & N & N & GEN & Y & Y & Y & 1.55 \\ |
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5&Y & N & N & RECOSIM & Y & Y & Y & 1.51 \\ |
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6&Y & Y & N & RECOSIM & Y & Y & Y & 1.58 \\ |
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7&Y & Y & Y & RECOSIM & Y & Y & Y & 1.18 \\ |
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\hline |
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\end{tabular} |
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\end{center} |
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cuts. We have verified that this effect is due to the polarization of |
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the $W$ (we remove the polarization by reweighting the events and we get |
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good agreement between prediction and observation). The kinematical |
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requirements (lines 2 and 3) do not have a significant additional effect. |
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Going from GEN to RECOSIM there is a significant change in observed/predicted. |
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We have tracked this down to the fact that tcMET underestimates the true \met |
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by $\approx 4\%$\footnote{We find that observed/predicted changes by roughly 0.1 |
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for each 1.5\% change in \met response.}. Finally, contamination from non $t\bar{t}$ |
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requirements (lines 2,3,4) compensate somewhat for the effect of W polarization. |
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Going from GEN to RECOSIM, the change in observed/predicted is small. |
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% We have tracked this down to the fact that tcMET underestimates the true \met |
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> |
% by $\approx 4\%$\footnote{We find that observed/predicted changes by roughly 0.1 |
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%for each 1.5\% change in \met response.}. |
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Finally, contamination from non $t\bar{t}$ |
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events can have a significant impact on the BG prediction. The changes between |
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lines 5 and 6 of Table~\ref{tab:victorybad} is driven by only {\color{red} 3} |
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Drell Yan events that pass the \met selection. |
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lines 6 and 7 of Table~\ref{tab:victorybad} is driven by 3 |
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Drell Yan events that pass the \met selection in Monte Carlo (thus the effect |
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> |
is statistically not well quantified). |
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|
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An additional source of concern is that the CMS Madgraph $t\bar{t}$ MC does |
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not include effects of spin correlations between the two top quarks. |
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that the bias is a the few percent level. |
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|
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Based on the results of Table~\ref{tab:victorybad}, we conclude that the |
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naive data driven background estimate based on $P_T{\ell\ell)}$ needs to |
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be corrected by a factor of {\color{red} $1.4 \pm 0.3$ (We need to |
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decide what this number should be)}. The quoted |
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> |
naive data driven background estimate based on $P_T{(\ell\ell)}$ needs to |
177 |
> |
be corrected by a factor of {\color{red} $1.2 \pm 0.3$ (We need to talk |
178 |
> |
about this)} . The quoted |
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uncertainty is based on the stability of the Monte Carlo tests under |
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variations of event selections, choices of \met algorithm, etc. |
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|
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|
|
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+ |
|
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\subsection{Signal Contamination} |
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\label{sec:sigcont} |
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|
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All data-driven methods are principle subject to signal contaminations |
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All data-driven methods are in principle subject to signal contaminations |
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in the control regions, and the methods described in |
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Sections~\ref{sec:abcd} and~\ref{sec:victory} are not exceptions. |
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Signal contamination tends to dilute the significance of a signal |
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|
in the different control regions for the two methods. |
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For example, in the extreme case of a |
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new physics signal |
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with $P_T(\ell \ell) = \met$, an excess of ev ents would be seen |
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> |
with $P_T(\ell \ell) = \met$, an excess of events would be seen |
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|
in the ABCD method but not in the $P_T(\ell \ell)$ method. |
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|
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|
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\hline |
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|
SM & LM0 & BG Prediction & LM1 & BG Prediction \\ |
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Background & Contribution& Including LM0 & Contribution & Including LM1 \\ \hline |
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x & x & x & x & x \\ |
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1.2 & 5.6 & 3.7 & 2.2 & 1.3 \\ |
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|
\hline |
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|
\end{tabular} |
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\end{center} |
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\caption{\label{tab:sigcontPT} Effects of signal contamination |
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for the background predictions of the $P_T(\ell\ell)$ method including LM0 or |
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LM1. Results |
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are normalized to 30 pb$^{-1}$.} |
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> |
are normalized to 30 pb$^{-1}$. {\color{red} Does this BG prediction include |
234 |
> |
the fudge factor of 1.4 or watever because the method is not perfect.}} |
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\begin{tabular}{|c||c|c||c|c|} |
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\hline |
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|
SM & LM0 & BG Prediction & LM1 & BG Prediction \\ |
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|
Background & Contribution& Including LM0 & Contribution & Including LM1 \\ \hline |
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< |
x & x & x & x & x \\ |
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> |
1.2 & 5.6 & 2.2 & 2.2 & 1.5 \\ |
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|
\hline |
241 |
|
\end{tabular} |
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\end{center} |