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\appendix |
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\section{Comparison of data and MC distributions} |
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\label{sec:appendix} |
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Here we compare data and MC distributions for data passing the |
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\begin{itemize} |
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\item $MT2$ in Figure A29 is a kinematical quantity |
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\item $MT2$ in Figure B29 is a kinematical quantity |
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built from the two leptons and the \met. For events with |
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two $W \to \ell$ decays it should have a sharp kinematical cutoff |
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at $W$ mass. For more details, see Reference~\cite{ref:MT2}. |
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\item $MT2J$ in Figure A30 is very muck like $MT2$ but it is built |
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\item $MT2J$ in Figure B30 is very muck like $MT2$ but it is built |
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out of the leptons the \met and the two jets. For $t\bar{t}$ |
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events it has a kinematical cutoff at $M_{\rm top}$, with tails |
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due to the fact that occasionally one of the $b$-jets is not |
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found and is replaced by a gluon jet from ISR or FSR. |
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For more details, see Reference~\cite{ref:MT2J}. |
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\item The reconstructed top mass in Figure A6 is from the |
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\item The reconstructed top mass in Figure B6 is from the |
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kinematical mass reconstruction of the top dilepton group. |
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In this case we are using the $D0$ matrix-element technique. |
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See Reference~\cite{ref:brown} for more details. |
