Changeset 341 in svn
- Timestamp:
- Mar 18, 2009, 9:46:22 PM (16 years ago)
- Location:
- trunk/paper
- Files:
-
- 2 edited
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trunk/paper/notes.tex
r338 r341 490 490 491 491 \subsubsection*{Purity} 492 Once both electromagnetic collimation and tracking isolation are applied, a threshold on the $p_T$ of the $\tau$-jet candidate is requested to purify the collection. This procedure selects $\tau$ leptons decaying hadronically with a typical efficiency of $6 0\%$.492 Once both electromagnetic collimation and tracking isolation are applied, a threshold on the $p_T$ of the $\tau$-jet candidate is requested to purify the collection. This procedure selects $\tau$ leptons decaying hadronically with a typical efficiency of $66\%$. 493 493 494 494 \subsection{Missing transverse energy} … … 540 540 541 541 \textsc{Delphes} performs a fast simulation of a collider experiment. 542 Its quality and validity are assessed by comparing to resolution of the reconstructed data to the \textsc{cms} detector expectations. 542 Its performances in terms of computing time and data size are directly proportional to the number of simulated events and on the considered physics process. As an example, $10,000$ $pp \rightarrow t \bar t X$ events are processed in $110~\textrm{s}$ on a regular laptop and use less than $250~\textrm{MB}$ of disk space. 543 The quality and validity of the output are assessed by comparing to resolution of the reconstructed data to the \textsc{cms} detector expectations. 543 544 544 545 Electrons and muons are by construction equal to the experiment designs, as the Gaussian smearing of their kinematics properties is defined according to their resolutions.
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