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# Content
1 \section{Non $t\bar{t}$ Backgrounds}
2 \label{sec:othBG}
3
4 Backgrounds from divector bosons and single top
5 can be reliably estimated from Monte Carlo.
6 They are negligible compared to $t\bar{t}$.
7
8 Backgrounds from Drell Yan are also expected
9 to be negligible from MC. However one always
10 worries about the modeling of tails of the \met.
11 In the context of other dilepton analyses we
12 have developed a data driven method to estimate
13 the number of Drell Yan events\cite{ref:dy}.
14 The method is based on counting the number of
15 $Z$ candidates passing the full selection, and
16 then scaling by the expected ratio of Drell Yan
17 events outside vs. inside the $Z$ mass
18 window.\footnote{A correction based on $e\mu$ events
19 is also applied.} This ratio is typically 0.1.
20
21 When find no dilepton events with invariant mass
22 consistent with the $Z$ in the signal region.
23 Using the value of 0.1 for the ratio described above, this
24 means that the Drell Yan background in our signal
25 region is $< 0.23\%$ events at the 90\% confidence level.
26 {\color{red} (If we find 1 event this will need to be adjusted)}.
27
28 Finally, we can use the ``Fake Rate'' method\cite{ref:FR}
29 to predict
30 the number of events with one fake lepton. We select
31 events where one of the leptons passes the full selection and
32 the other one fails the full selection but passes the
33 ``Fakeable Object'' selection of
34 Reference~\cite{ref:FR}.\footnote{For electrons we use
35 the V3 fakeable object definition to avoid complications
36 associated with electron ID cuts applied in the trigger.}
37 We then weight each event passing the full selection
38 by FR/(1-FR) where FR is the ``fake rate'' for the
39 fakeable object. {\color{red} The results are...}