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%\section{Systematics Uncertainties on the Background Prediction} |
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%\label{sec:systematics} |
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|
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[ADD INTRODUCTORY BLURB ON UNCERTAINTIES \\ |
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ADD COMPARISONS OF ALL THE ALTERNATIVE SAMPLES FOR ALL THE SIGNAL |
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REGIONS \\ |
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LIST ALL THE UNCERTAINTIES INCLUDED AND THEIR VALUES] |
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[DESCRIBE HERE ONE BY ONE THE UNCERTAINTIES THAT ARE PRESENT IN THE SPREADSHHET |
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FROM WHICH WE CALCULATE THE TOTAL UNCERTAINTY. WE KNOW HOW TO DO THIS |
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AND |
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WE HAVE THE TECHNOLOGY FROM THE 7 TEV ANALYSIS TO PROPAGATE ALL |
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UNCERTAINTIES |
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CORRECTLY THROUGH. WE WILL DO IT ONCE WE HAVE SETTLED ON THE |
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INDIVIDUAL PIECES WHICH ARE STILL IN FLUX] |
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|
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In this Section we discuss the systematic uncertainty on the BG |
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prediction. This prediction is assembled from the event |
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counts in the peak region of the transverse mass distribution as |
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well as Monte Carlo |
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with a number of correction factors, as described previously. |
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The |
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final uncertainty on the prediction is built up from the uncertainties in these |
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individual |
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components. |
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The calculation is done for each signal |
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region, |
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for electrons and muons separately. |
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|
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The choice to normalizing to the peak region of $M_T$ has the |
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advantage that some uncertainties, e.g., luminosity, cancel. |
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It does however introduce complications because it couples |
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some of the uncertainties in non-trivial ways. For example, |
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the primary effect of an uncertainty on the rare MC cross-section |
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is to introduce an uncertainty in the rare MC background estimate |
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which comes entirely from MC. But this uncertainty also affects, |
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for example, |
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the $t\bar{t} \to$ dilepton BG estimate because it changes the |
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$t\bar{t}$ normalization to the peak region (because some of the |
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events in the peak region are from rare processes). These effects |
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are carefully accounted for. The contribution to the overall |
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uncertainty from each BG source is tabulated in |
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Section~\ref{sec:bgunc-bottomline}. |
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First, however, we discuss the uncertainties one-by-one and we comment |
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on their impact on the overall result, at least to first order. |
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Second order effects, such as the one described, are also included. |
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|
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\subsection{Statistical uncertainties on the event counts in the $M_T$ |
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peak regions} |
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These vary between XX and XX \%, depending on the signal region |
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(different |
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signal regions have different \met\ requirements, thus they also have |
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different $M_T$ regions used as control. |
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Since |
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the major BG, eg, $t\bar{t}$ are normalized to the peak regions, this |
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fractional uncertainty is pretty much carried through all the way to |
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the end. There is also an uncertainty from the finite MC event counts |
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in the $M_T$ peak regions. This is also included, but it is smaller. |
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|
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\subsection{Uncertainty from the choice of $M_T$ peak region} |
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IN 7 TEV DATA WE HAD SOME SHAPE DIFFERENCES IN THE MTRANS REGION THAT |
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LED US TO CONSERVATIVELY INCLUDE THIS UNCERTAINTY. WE NEED TO LOOK |
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INTO THIS AGAIN |
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|
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\subsection{Uncertainty on the Wjets cross-section and the rare MC cross-sections} |
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These are taken as 50\%, uncorrelated. |
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The primary effect is to introduce a 50\% |
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uncertainty |
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on the $W +$ jets and rare BG |
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background predictions, respectively. However they also |
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have an effect on the other BGs via the $M_T$ peak normalization |
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in a way that tends to reduce the uncertainty. This is easy |
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to understand: if the $W$ cross-section is increased by 50\%, then |
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the $W$ background goes up. But the number of $M_T$ peak events |
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attributed to $t\bar{t}$ goes down, and since the $t\bar{t}$ BG is |
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scaled to the number of $t\bar{t}$ events in the peak, the $t\bar{t}$ |
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BG goes down. |
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|
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\subsection{Scale factors for the tail-to-peak ratios for lepton + |
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jets top and W events} |
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These tail-to-peak ratios are described in Section~\ref{sec:ttp}. |
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They are studied in CR1 and CR2. The studies are described |
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in Sections~\ref{sec:cr1} and~\ref{sec:cr2}), respectively, where |
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we also give the uncertainty on the scale factors. |
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|
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\subsection{Uncertainty on extra jet radiation for dilepton |
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background} |
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As discussed in Section~\ref{sec:jetmultiplicity}, the |
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jet distribution in |
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$t\bar{t} \to$ |
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dilepton MC is rescaled by the factors $K_3$ and $K_4$ to make |
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it agree with the data. The XX\% uncertainties on $K_3$ and $K_4$ |
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comes from data/MC statistics. This |
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result directly in a XX\% uncertainty on the dilepton BG, which is by far |
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the most important one. |
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|
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|
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\subsection{Uncertainty on the \ttll\ Acceptance} |
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alternative sample predictions are indicated by the |
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datapoints. The uncertainties on the alternative predictions |
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correspond to the uncorrelated statistical uncertainty from |
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the size of the alternative sample only.} |
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the size of the alternative sample only. |
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[TO BE UPDATED WITH THE LATEST SELECTION AND SFS]} |
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\end{center} |
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\end{figure} |
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|
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\clearpage |
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|
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% |
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% |
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%\end{center} |
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%\end{table} |
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\subsection{Uncertainty from the isolated track veto} |
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This is the uncertainty associated with how well the isolated track |
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veto performance is modeled by the Monte Carlo. This uncertainty |
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only applies to the fraction of dilepton BG events that have |
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a second e/$\mu$ or a one prong $\tau \to h$, with |
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$P_T > 10$ GeV in $|\eta| < 2.4$. This fraction is 1/3 (THIS WAS THE |
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7 TEV NUMBER, CHECK). The uncertainty for these events |
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is XX\% and is obtained from Tag and Probe studies of Section~\ref{sec:trkveto} |
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|
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\subsection{Isolated Track Veto: Tag and Probe Studies} |
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\subsubsection{Isolated Track Veto: Tag and Probe Studies} |
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\label{sec:trkveto} |
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[EVERYTHING IS 7TEV HERE, UPDATE WITH NEW RESULTS \\ |
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ADD TABLE WITH FRACTION OF EVENTS THAT HAVE A TRUE ISOLATED TRACK] |
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\caption{\label{tab:isotrk} Comparison of the data vs. MC efficiencies to satisfy the indicated requirements |
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on the absolute track isolation, and the ratio of these two efficiencies. Results are indicated separately for electrons and muons and for various |
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jet multiplicity requirements.} |
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\begin{tabular}{l|l|c|c|c|c|c} |
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\begin{tabular}{l|c|c|c|c|c} |
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|
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%Electrons: |
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%Total MC yields : 323790 |
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%Total DATA yields : 2772586 |
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%Muons: |
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%Total MC yields : 456138 |
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%Total DATA yields : 4210022 |
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|
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\hline |
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\hline |
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e + $\geq$0 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
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|
\hline |
| 434 |
< |
e + $\geq$0 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 434 |
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data & 0.097 $\pm$ 0.0002 & 0.035 $\pm$ 0.0001 & 0.016 $\pm$ 0.0001 & 0.009 $\pm$ 0.0001 & 0.005 $\pm$ 0.0000 \\ |
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mc & 0.096 $\pm$ 0.0005 & 0.034 $\pm$ 0.0003 & 0.015 $\pm$ 0.0002 & 0.008 $\pm$ 0.0002 & 0.005 $\pm$ 0.0001 \\ |
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data/mc & 1.01 $\pm$ 0.01 & 1.04 $\pm$ 0.01 & 1.06 $\pm$ 0.02 & 1.04 $\pm$ 0.02 & 1.01 $\pm$ 0.02 \\ |
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|
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\hline |
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data & 0.088 $\pm$ 0.0003 & 0.030 $\pm$ 0.0002 & 0.013 $\pm$ 0.0001 & 0.007 $\pm$ 0.0001 & 0.005 $\pm$ 0.0001 \\ |
| 333 |
– |
mc & 0.087 $\pm$ 0.0001 & 0.030 $\pm$ 0.0001 & 0.014 $\pm$ 0.0001 & 0.008 $\pm$ 0.0000 & 0.005 $\pm$ 0.0000 \\ |
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data/mc & 1.01 $\pm$ 0.00 & 0.99 $\pm$ 0.01 & 0.97 $\pm$ 0.01 & 0.95 $\pm$ 0.01 & 0.93 $\pm$ 0.01 \\ |
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\hline |
| 440 |
+ |
$\mu$ + $\geq$0 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
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\hline |
| 442 |
< |
$\mu$ + $\geq$0 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 442 |
> |
data & 0.094 $\pm$ 0.0001 & 0.034 $\pm$ 0.0001 & 0.016 $\pm$ 0.0001 & 0.009 $\pm$ 0.0000 & 0.006 $\pm$ 0.0000 \\ |
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mc & 0.093 $\pm$ 0.0004 & 0.033 $\pm$ 0.0003 & 0.015 $\pm$ 0.0002 & 0.008 $\pm$ 0.0001 & 0.005 $\pm$ 0.0001 \\ |
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data/mc & 1.01 $\pm$ 0.00 & 1.04 $\pm$ 0.01 & 1.05 $\pm$ 0.01 & 1.06 $\pm$ 0.02 & 1.07 $\pm$ 0.02 \\ |
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> |
|
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\hline |
| 339 |
– |
data & 0.087 $\pm$ 0.0002 & 0.031 $\pm$ 0.0001 & 0.015 $\pm$ 0.0001 & 0.008 $\pm$ 0.0001 & 0.005 $\pm$ 0.0001 \\ |
| 340 |
– |
mc & 0.085 $\pm$ 0.0001 & 0.030 $\pm$ 0.0001 & 0.014 $\pm$ 0.0000 & 0.008 $\pm$ 0.0000 & 0.005 $\pm$ 0.0000 \\ |
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data/mc & 1.02 $\pm$ 0.00 & 1.06 $\pm$ 0.00 & 1.06 $\pm$ 0.01 & 1.03 $\pm$ 0.01 & 1.02 $\pm$ 0.01 \\ |
| 447 |
|
\hline |
| 448 |
< |
\hline |
| 344 |
< |
e + $\geq$1 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 448 |
> |
e + $\geq$1 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 449 |
|
\hline |
| 450 |
< |
data & 0.099 $\pm$ 0.0008 & 0.038 $\pm$ 0.0005 & 0.019 $\pm$ 0.0004 & 0.011 $\pm$ 0.0003 & 0.008 $\pm$ 0.0002 \\ |
| 451 |
< |
mc & 0.100 $\pm$ 0.0004 & 0.038 $\pm$ 0.0003 & 0.019 $\pm$ 0.0002 & 0.012 $\pm$ 0.0002 & 0.008 $\pm$ 0.0001 \\ |
| 452 |
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data/mc & 0.99 $\pm$ 0.01 & 1.00 $\pm$ 0.02 & 0.99 $\pm$ 0.02 & 0.98 $\pm$ 0.03 & 0.97 $\pm$ 0.03 \\ |
| 450 |
> |
data & 0.109 $\pm$ 0.0005 & 0.043 $\pm$ 0.0003 & 0.022 $\pm$ 0.0002 & 0.013 $\pm$ 0.0002 & 0.009 $\pm$ 0.0002 \\ |
| 451 |
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mc & 0.109 $\pm$ 0.0014 & 0.042 $\pm$ 0.0009 & 0.020 $\pm$ 0.0006 & 0.012 $\pm$ 0.0005 & 0.008 $\pm$ 0.0004 \\ |
| 452 |
> |
data/mc & 1.00 $\pm$ 0.01 & 1.04 $\pm$ 0.02 & 1.08 $\pm$ 0.04 & 1.13 $\pm$ 0.05 & 1.13 $\pm$ 0.06 \\ |
| 453 |
> |
|
| 454 |
|
\hline |
| 455 |
|
\hline |
| 456 |
< |
$\mu$ + $\geq$1 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 456 |
> |
$\mu$ + $\geq$1 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 457 |
|
\hline |
| 458 |
< |
data & 0.100 $\pm$ 0.0006 & 0.041 $\pm$ 0.0004 & 0.022 $\pm$ 0.0003 & 0.014 $\pm$ 0.0002 & 0.010 $\pm$ 0.0002 \\ |
| 459 |
< |
mc & 0.099 $\pm$ 0.0004 & 0.039 $\pm$ 0.0002 & 0.020 $\pm$ 0.0002 & 0.013 $\pm$ 0.0001 & 0.009 $\pm$ 0.0001 \\ |
| 460 |
< |
data/mc & 1.01 $\pm$ 0.01 & 1.05 $\pm$ 0.01 & 1.05 $\pm$ 0.02 & 1.06 $\pm$ 0.02 & 1.06 $\pm$ 0.03 \\ |
| 458 |
> |
data & 0.106 $\pm$ 0.0004 & 0.043 $\pm$ 0.0003 & 0.023 $\pm$ 0.0002 & 0.014 $\pm$ 0.0002 & 0.010 $\pm$ 0.0001 \\ |
| 459 |
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mc & 0.107 $\pm$ 0.0012 & 0.042 $\pm$ 0.0008 & 0.021 $\pm$ 0.0005 & 0.013 $\pm$ 0.0004 & 0.009 $\pm$ 0.0004 \\ |
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data/mc & 1.00 $\pm$ 0.01 & 1.03 $\pm$ 0.02 & 1.07 $\pm$ 0.03 & 1.12 $\pm$ 0.04 & 1.17 $\pm$ 0.05 \\ |
| 461 |
> |
|
| 462 |
|
\hline |
| 463 |
|
\hline |
| 464 |
< |
e + $\geq$2 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 464 |
> |
e + $\geq$2 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 465 |
|
\hline |
| 466 |
< |
data & 0.105 $\pm$ 0.0020 & 0.042 $\pm$ 0.0013 & 0.021 $\pm$ 0.0009 & 0.013 $\pm$ 0.0007 & 0.009 $\pm$ 0.0006 \\ |
| 467 |
< |
mc & 0.109 $\pm$ 0.0011 & 0.043 $\pm$ 0.0007 & 0.021 $\pm$ 0.0005 & 0.013 $\pm$ 0.0004 & 0.009 $\pm$ 0.0003 \\ |
| 468 |
< |
data/mc & 0.96 $\pm$ 0.02 & 0.97 $\pm$ 0.03 & 1.00 $\pm$ 0.05 & 1.01 $\pm$ 0.06 & 0.97 $\pm$ 0.08 \\ |
| 466 |
> |
data & 0.115 $\pm$ 0.0012 & 0.049 $\pm$ 0.0008 & 0.026 $\pm$ 0.0006 & 0.017 $\pm$ 0.0005 & 0.012 $\pm$ 0.0004 \\ |
| 467 |
> |
mc & 0.114 $\pm$ 0.0032 & 0.046 $\pm$ 0.0021 & 0.023 $\pm$ 0.0015 & 0.015 $\pm$ 0.0012 & 0.010 $\pm$ 0.0010 \\ |
| 468 |
> |
data/mc & 1.01 $\pm$ 0.03 & 1.09 $\pm$ 0.05 & 1.13 $\pm$ 0.08 & 1.09 $\pm$ 0.09 & 1.14 $\pm$ 0.12 \\ |
| 469 |
> |
|
| 470 |
|
\hline |
| 471 |
|
\hline |
| 472 |
< |
$\mu$ + $\geq$2 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 472 |
> |
$\mu$ + $\geq$2 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 473 |
|
\hline |
| 474 |
< |
data & 0.106 $\pm$ 0.0016 & 0.045 $\pm$ 0.0011 & 0.025 $\pm$ 0.0008 & 0.016 $\pm$ 0.0007 & 0.012 $\pm$ 0.0006 \\ |
| 475 |
< |
mc & 0.108 $\pm$ 0.0009 & 0.044 $\pm$ 0.0006 & 0.024 $\pm$ 0.0004 & 0.016 $\pm$ 0.0004 & 0.011 $\pm$ 0.0003 \\ |
| 476 |
< |
data/mc & 0.98 $\pm$ 0.02 & 1.04 $\pm$ 0.03 & 1.04 $\pm$ 0.04 & 1.04 $\pm$ 0.05 & 1.06 $\pm$ 0.06 \\ |
| 474 |
> |
data & 0.111 $\pm$ 0.0010 & 0.048 $\pm$ 0.0007 & 0.026 $\pm$ 0.0005 & 0.018 $\pm$ 0.0004 & 0.013 $\pm$ 0.0004 \\ |
| 475 |
> |
mc & 0.114 $\pm$ 0.0027 & 0.046 $\pm$ 0.0018 & 0.024 $\pm$ 0.0013 & 0.014 $\pm$ 0.0010 & 0.010 $\pm$ 0.0009 \\ |
| 476 |
> |
data/mc & 0.98 $\pm$ 0.03 & 1.04 $\pm$ 0.04 & 1.12 $\pm$ 0.07 & 1.26 $\pm$ 0.10 & 1.30 $\pm$ 0.12 \\ |
| 477 |
> |
|
| 478 |
|
\hline |
| 479 |
|
\hline |
| 480 |
< |
e + $\geq$3 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 480 |
> |
e + $\geq$3 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 481 |
|
\hline |
| 482 |
< |
data & 0.117 $\pm$ 0.0055 & 0.051 $\pm$ 0.0038 & 0.029 $\pm$ 0.0029 & 0.018 $\pm$ 0.0023 & 0.012 $\pm$ 0.0019 \\ |
| 483 |
< |
mc & 0.120 $\pm$ 0.0031 & 0.052 $\pm$ 0.0021 & 0.027 $\pm$ 0.0015 & 0.018 $\pm$ 0.0012 & 0.013 $\pm$ 0.0011 \\ |
| 484 |
< |
data/mc & 0.97 $\pm$ 0.05 & 0.99 $\pm$ 0.08 & 1.10 $\pm$ 0.13 & 1.03 $\pm$ 0.15 & 0.91 $\pm$ 0.16 \\ |
| 482 |
> |
data & 0.122 $\pm$ 0.0030 & 0.058 $\pm$ 0.0022 & 0.034 $\pm$ 0.0017 & 0.023 $\pm$ 0.0014 & 0.017 $\pm$ 0.0012 \\ |
| 483 |
> |
mc & 0.125 $\pm$ 0.0080 & 0.060 $\pm$ 0.0057 & 0.032 $\pm$ 0.0043 & 0.023 $\pm$ 0.0036 & 0.017 $\pm$ 0.0031 \\ |
| 484 |
> |
data/mc & 0.98 $\pm$ 0.07 & 0.97 $\pm$ 0.10 & 1.06 $\pm$ 0.15 & 1.01 $\pm$ 0.17 & 1.01 $\pm$ 0.20 \\ |
| 485 |
> |
|
| 486 |
|
\hline |
| 487 |
|
\hline |
| 488 |
< |
$\mu$ + $\geq$3 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 488 |
> |
$\mu$ + $\geq$3 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 489 |
|
\hline |
| 490 |
< |
data & 0.111 $\pm$ 0.0044 & 0.050 $\pm$ 0.0030 & 0.029 $\pm$ 0.0024 & 0.019 $\pm$ 0.0019 & 0.014 $\pm$ 0.0017 \\ |
| 491 |
< |
mc & 0.115 $\pm$ 0.0025 & 0.051 $\pm$ 0.0017 & 0.030 $\pm$ 0.0013 & 0.020 $\pm$ 0.0011 & 0.015 $\pm$ 0.0009 \\ |
| 492 |
< |
data/mc & 0.97 $\pm$ 0.04 & 0.97 $\pm$ 0.07 & 0.95 $\pm$ 0.09 & 0.97 $\pm$ 0.11 & 0.99 $\pm$ 0.13 \\ |
| 490 |
> |
data & 0.121 $\pm$ 0.0025 & 0.055 $\pm$ 0.0018 & 0.033 $\pm$ 0.0014 & 0.022 $\pm$ 0.0011 & 0.017 $\pm$ 0.0010 \\ |
| 491 |
> |
mc & 0.125 $\pm$ 0.0070 & 0.053 $\pm$ 0.0047 & 0.027 $\pm$ 0.0035 & 0.018 $\pm$ 0.0028 & 0.013 $\pm$ 0.0024 \\ |
| 492 |
> |
data/mc & 0.97 $\pm$ 0.06 & 1.05 $\pm$ 0.10 & 1.20 $\pm$ 0.16 & 1.19 $\pm$ 0.20 & 1.28 $\pm$ 0.25 \\ |
| 493 |
> |
|
| 494 |
|
\hline |
| 495 |
|
\hline |
| 496 |
< |
e + $\geq$4 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 496 |
> |
e + $\geq$4 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 497 |
|
\hline |
| 498 |
< |
data & 0.113 $\pm$ 0.0148 & 0.048 $\pm$ 0.0100 & 0.033 $\pm$ 0.0083 & 0.020 $\pm$ 0.0065 & 0.017 $\pm$ 0.0062 \\ |
| 499 |
< |
mc & 0.146 $\pm$ 0.0092 & 0.064 $\pm$ 0.0064 & 0.034 $\pm$ 0.0048 & 0.024 $\pm$ 0.0040 & 0.021 $\pm$ 0.0037 \\ |
| 500 |
< |
data/mc & 0.78 $\pm$ 0.11 & 0.74 $\pm$ 0.17 & 0.96 $\pm$ 0.28 & 0.82 $\pm$ 0.30 & 0.85 $\pm$ 0.34 \\ |
| 498 |
> |
data & 0.130 $\pm$ 0.0079 & 0.069 $\pm$ 0.0060 & 0.044 $\pm$ 0.0048 & 0.031 $\pm$ 0.0041 & 0.021 $\pm$ 0.0034 \\ |
| 499 |
> |
mc & 0.136 $\pm$ 0.0219 & 0.045 $\pm$ 0.0134 & 0.027 $\pm$ 0.0108 & 0.022 $\pm$ 0.0093 & 0.016 $\pm$ 0.0084 \\ |
| 500 |
> |
data/mc & 0.96 $\pm$ 0.17 & 1.55 $\pm$ 0.48 & 1.62 $\pm$ 0.67 & 1.41 $\pm$ 0.63 & 1.28 $\pm$ 0.68 \\ |
| 501 |
> |
|
| 502 |
|
\hline |
| 503 |
|
\hline |
| 504 |
< |
$\mu$ + $\geq$4 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 504 |
> |
$\mu$ + $\geq$4 jets & $>$ 1 GeV & $>$ 2 GeV & $>$ 3 GeV & $>$ 4 GeV & $>$ 5 GeV \\ |
| 505 |
|
\hline |
| 506 |
< |
data & 0.130 $\pm$ 0.0128 & 0.052 $\pm$ 0.0085 & 0.028 $\pm$ 0.0063 & 0.019 $\pm$ 0.0052 & 0.019 $\pm$ 0.0052 \\ |
| 507 |
< |
mc & 0.105 $\pm$ 0.0064 & 0.045 $\pm$ 0.0043 & 0.027 $\pm$ 0.0034 & 0.019 $\pm$ 0.0028 & 0.014 $\pm$ 0.0024 \\ |
| 508 |
< |
data/mc & 1.23 $\pm$ 0.14 & 1.18 $\pm$ 0.22 & 1.03 $\pm$ 0.27 & 1.01 $\pm$ 0.32 & 1.37 $\pm$ 0.45 \\ |
| 506 |
> |
data & 0.136 $\pm$ 0.0067 & 0.064 $\pm$ 0.0048 & 0.041 $\pm$ 0.0039 & 0.029 $\pm$ 0.0033 & 0.024 $\pm$ 0.0030 \\ |
| 507 |
> |
mc & 0.127 $\pm$ 0.0187 & 0.062 $\pm$ 0.0134 & 0.042 $\pm$ 0.0113 & 0.034 $\pm$ 0.0104 & 0.028 $\pm$ 0.0095 \\ |
| 508 |
> |
data/mc & 1.07 $\pm$ 0.17 & 1.04 $\pm$ 0.24 & 0.98 $\pm$ 0.28 & 0.85 $\pm$ 0.28 & 0.87 $\pm$ 0.32 \\ |
| 509 |
|
\hline |
| 510 |
|
\hline |
| 511 |
|
|
| 594 |
|
% \end{center} |
| 595 |
|
%\end{figure} |
| 596 |
|
|
| 597 |
+ |
\subsection{Summary of uncertainties} |
| 598 |
+ |
\label{sec:bgunc-bottomline}. |
| 599 |
+ |
|
| 600 |
+ |
THIS NEEDS TO BE WRITTEN |
