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- Timestamp:
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Apr 12, 2010, 11:09:30 AM (15 years ago)
- Author:
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ohl
- Comment:
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--
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| 1 | We're in the standard model |
1 | 2 | {{{ |
2 | 3 | model = SM |
3 | 4 | }}} |
4 | | Set up the process |
| 5 | Set up the process, restricting ourselves to up- and downquarks in the proton, together with gluons |
5 | 6 | {{{ |
6 | 7 | alias parton = u:U:d:D:g |
7 | 8 | alias jet = parton |
8 | 9 | }}} |
9 | | We could have added strange and charm jets: |
| 10 | We could have added strange and charm jets (but we chose not to) |
10 | 11 | {{{ |
11 | 12 | # alias jet = parton:s:S:c:C |
12 | 13 | }}} |
| 14 | Allow muons as well as electrons, but assume that we can identify charges and ignore antimuons and positrons |
13 | 15 | {{{ |
14 | 16 | alias lepton = e1:e2 |
15 | 17 | alias neutrino = n1:N1:n2:N2 |
16 | 18 | }}} |
| 19 | Define the process, call O'Mega and compile the matrix element |
17 | 20 | {{{ |
18 | 21 | process enj = parton, parton => lepton, neutrino, jet |
… |
… |
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63 | 66 | and record e_jet (eval E [extract index 1 [sort by Pt [jet]]]) |
64 | 67 | }}} |
| 68 | Generate 1000 events |
65 | 69 | {{{ |
66 | 70 | simulate (enj) { n_events = 1000 } |
67 | 71 | }}} |
| 72 | and write the events to file |
68 | 73 | {{{ |
69 | 74 | $analysis_filename = "W-endpoint" |