A. Table, 3: MC of W+Jets samples Run Channel ? (pb) k-factor 7650 Z(? ee

A. Table, 6: MC of W+cc+Jets samples 4602

B. Table, The number of events (33.7 pb ?1 ) after each selection cut in t ¯ t no full hadronic samples with different top mass in electron channel. The uncertainties shown in the table are statistical in MC. No scale factors have been applied to the number of events

B. Table, The number of events (33.7 pb ?1 ) after each selection cut in t ¯ t no full hadronic samples with different top mass in muon channel. The uncertainties shown in the table are statistical in MC

C. Table, 1: Definition of the ? ? ? bins of the muon for the expression of the trigger SF. The Barrel is divided into 9 regions according to a similar measured SF. Region Trigger SF EC 0

C. Table, Muon trigger scale factors from Z ? µµ data and MC events, using the tag & probe method. The results correspond to data periods E4-I

E. Table, Events are separated by lepton charge for positive and negative as a function of number of jets in electron channel. The uncertainties to the number of events are assumed to be 30%. The results show a charge symmetry in these channels with the assumed uncertainties. e+jets 0 jet 1 jet 2 jets 3 jets ?4 jets t ¯ t no full had

E. Table, Events are separated by lepton charge for positive and negative as a function of number of jets in muon channel. The uncertainties to the number of events are assumed to be 30%. The results show a charge symmetry in these channels with the assumed uncertainties. e+jets 1 jet 2 jets 3 jets ?4 jets data(+)

F. Table, The numbers of events with ?1 tagged are presented as a function of number of jets. The description concerning the channels are common as in Table 5.2. The results shown are in electron channel with statistical uncertainty. µ+jets 1 jet 2 jets 3 jets ?4 jets data(+) 182

F. Table, The numbers of events with ?1 tagged are presented as a function of number of jets. The results shown are in muon channel with statistical uncertainty

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