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W Pair Production

At LEP2, the three basic W-pair production diagrams contain Z $ \rightarrow$ WW, $ \gamma$ $ \rightarrow$ WW and t-channel neutrino exchange (which dominates near the W-pair threshold). The issue of directly reconstructing the mass of a heavy boson naturally focusses on these events, since W-pairs have already been produced in their thousands in each of the four LEP detectors. Typical statistics of W pair events are shown in Table 1.


Table 1: Year, e+e- centre-of-mass energy, integrated luminosity per LEP experiment and approximate number of W-pair events per LEP experiment.
Year $ \sqrt{s}$ (GeV) $ \mathcal {L}$(pb-1)/expt NWW/expt
1996 161 $ \sim$ 10 $ \sim$ 35
172 $ \sim$ 10 $ \sim$ 120
1997 183 $ \sim$ 57 $ \sim$ 850
1998 189 $ \sim$ 175 $ \sim$ 2700

Given that BR(W $ \rightarrow$ q$ \overline{q}$) $ \simeq$ 68% and that the remaining decays are leptonic, one sees that the W pair sample subdivides as follows: hadronic channel (WW $ \rightarrow$ q$ \overline{q}$q$ \overline{q}$) $ \simeq$ 46%, semileptonic channels (WW $ \rightarrow$ l$ \nu$q$ \overline{q}$) $ \simeq$ 44% and the fully leptonic channels (WW $ \rightarrow$ l$ \nu$l$ \nu$) are $ \simeq$ 10%, where l denotes e,$ \mu$ or $ \tau$.


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Next: Selecting WW Events Up: W Mass by Direct Previous: W Mass by Direct
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