***************************************** * Minutes of the meeting held on nov.5 * ***************************************** 1. Marie Noelle reports that she is trying to extract the number of hadrons per bunch for the 95 data. This has been requested by Brigitte in order to cross-check the luminosity per bunch. Working with MINIs Marie Noelle gets incoherent results depending on whether she relies on the bunch train number or on the t0 from the Ecal wires. To clarify this, she is now starting the selection from DSTs. 2. Arnaud reports that he is advancing with the note and that he has generated 7 million qqbar at Kingal level to finalise the numbers for efficiency and gg background for the data from 90 and 91. 3. We went back to the old discussion on what is the minimum invariant mass square used in the analyses. This bound is set in the Monte Carlo event generation when evaluating detector acceptances, and the same value should appear in the fitting functions. In the latest Koralz version this bound is hard wired to 4*(m_tau)**2 . So this is the s' min to be set in MIZA for taus and muons (andrea's analysis). (What about Imma's analysis???) For the Bhabhas the situation is more complicated. There are 3 steps involved: 1.efficiency correction using UNIBAB 2.t-channel subtraction with ALIBABA 3.Acceptance correction to evaluate impact of cuts on costheta* and acollinearity with KORALZ. Step 3 clarly uses the same s'_min of 4*m_tau**2, so it is coherent with the other leptons. It was not clear at the meeting whether we should also worry about steps 1 and 2. 4. The discussion went on on how to deal with events with fermion pair production (llv). - Pair production from the initial legs. This situation is treated in the fitting program together with the beam spread corrections, since it is equivalent to a smearing of the beam energy. But the Monte Carlo does not contain a correction for these pairs, therefore the acceptance is not exact. - Pair production from final legs. These type of events should be kept since they contribute to the physical width, but again KORALZ doesnt have this type of evts and therefore a 4-fermion generator should be used. Clearly it should be kept in mind that pair production is suppressed by a term proportional to (alpha/pi)**2), so that we are talking of small effects. Andrea is trying to clarify these points with the help of Manel. Next meetings. ------------- We will meet again next tuesday 12 nov. at 14:30 in room 13-3-005 to review what will be discussed at the EW meeting of friday 15.