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| 3 | <title>Electroweak Processes</title> |
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| 28 | <form method='post' action='ElectroweakProcesses.php'> |
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| 29 | |
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| 30 | <h2>Electroweak Processes</h2> |
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| 31 | |
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| 32 | This page contains processes involving Prompt-photon, <i>gamma^*/Z^0</i> |
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| 33 | and <i>W^+-</i> production, plus a few with <i>t</i>-channel boson |
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| 34 | exchange. |
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| 35 | |
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| 36 | <h3>Prompt photon processes</h3> |
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| 37 | |
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| 38 | This group collects the processes where one or two photons are |
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| 39 | produced by the hard process. Additional sources of photons |
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| 40 | include parton showers and hadron decays. A <i>pT</i> cut |
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| 41 | is required to stay away from the unphysical low-<i>pT</i> region. |
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| 42 | An eikonalized description, intended to be valid at all <i>pT</i>, |
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| 43 | is included as part of the multiparton-interactions framework. |
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| 44 | |
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| 45 | <br/><br/><strong>PromptPhoton:all</strong> <input type="radio" name="1" value="on"><strong>On</strong> |
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| 46 | <input type="radio" name="1" value="off" checked="checked"><strong>Off</strong> |
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| 47 | (<code>default = <strong>off</strong></code>)<br/> |
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| 48 | Common switch for the group of all prompt photon processes, |
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| 49 | as listed separately in the following. |
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| 50 | |
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| 51 | |
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| 52 | <br/><br/><strong>PromptPhoton:qg2qgamma</strong> <input type="radio" name="2" value="on"><strong>On</strong> |
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| 53 | <input type="radio" name="2" value="off" checked="checked"><strong>Off</strong> |
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| 54 | (<code>default = <strong>off</strong></code>)<br/> |
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| 55 | Scattering <i>q g -> q gamma</i>. |
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| 56 | Code 201. |
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| 57 | |
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| 58 | |
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| 59 | <br/><br/><strong>PromptPhoton:qqbar2ggamma</strong> <input type="radio" name="3" value="on"><strong>On</strong> |
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| 60 | <input type="radio" name="3" value="off" checked="checked"><strong>Off</strong> |
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| 61 | (<code>default = <strong>off</strong></code>)<br/> |
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| 62 | Scattering <i>q qbar -> g gamma</i>. |
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| 63 | Code 202. |
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| 64 | |
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| 65 | |
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| 66 | <br/><br/><strong>PromptPhoton:gg2ggamma</strong> <input type="radio" name="4" value="on"><strong>On</strong> |
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| 67 | <input type="radio" name="4" value="off" checked="checked"><strong>Off</strong> |
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| 68 | (<code>default = <strong>off</strong></code>)<br/> |
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| 69 | Scattering <i>g g -> g gamma</i>. |
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| 70 | <br/><b>Note:</b> This is a box graph. The full quark-mass dependence |
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| 71 | in the loop leads to very complicated expressions. The current |
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| 72 | implementation is based on assuming five massless quarks (see below), |
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| 73 | and thus is questionable at small (<i>pT < m_b</i>) or large |
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| 74 | (<i>pT > m_t</i>) transverse momenta. |
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| 75 | Code 203. |
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| 76 | |
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| 77 | |
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| 78 | <br/><br/><strong>PromptPhoton:ffbar2gammagamma</strong> <input type="radio" name="5" value="on"><strong>On</strong> |
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| 79 | <input type="radio" name="5" value="off" checked="checked"><strong>Off</strong> |
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| 80 | (<code>default = <strong>off</strong></code>)<br/> |
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| 81 | Scattering <i>q qbar -> gamma gamma</i>. |
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| 82 | Code 204. |
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| 83 | |
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| 84 | |
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| 85 | <br/><br/><strong>PromptPhoton:gg2gammagamma</strong> <input type="radio" name="6" value="on"><strong>On</strong> |
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| 86 | <input type="radio" name="6" value="off" checked="checked"><strong>Off</strong> |
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| 87 | (<code>default = <strong>off</strong></code>)<br/> |
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| 88 | Scattering <i>g g -> gamma gamma</i>. |
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| 89 | <br/><b>Note:</b> This is a box graph. The full quark-mass dependence |
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| 90 | in the loop leads to very complicated expressions. The current |
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| 91 | implementation is based on assuming five massless quarks (see below), |
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| 92 | and thus is questionable at small (<i>pT < m_b</i>) or large |
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| 93 | (<i>pT > m_t</i>) transverse momenta. |
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| 94 | Code 205. |
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| 95 | |
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| 96 | |
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| 97 | <br/><br/><table><tr><td><strong>PromptPhoton:nQuarkLoop </td><td></td><td> <input type="text" name="7" value="5" size="20"/> (<code>default = <strong>5</strong></code>; <code>minimum = 3</code>; <code>maximum = 6</code>)</td></tr></table> |
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| 98 | Number of quark flavours included in the box graphs resposible for |
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| 99 | <i>g g -> g gamma</i> and <i>g g-> gamma gamma</i> processes. |
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| 100 | Owing to the complexity if the massive expressions, quarks are treated |
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| 101 | as massless. The default value should be applicable in the range of |
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| 102 | transverse momenta above the <i>b</i> mass but below the <i>t</i> one. |
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| 103 | |
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| 104 | |
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| 105 | <h3>Weak boson processes</h3> |
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| 106 | |
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| 107 | Under this heading we group processes involving the production |
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| 108 | of a single electroweak gauge boson, i.e. a <i>gamma^*/Z^0</i> |
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| 109 | or a <i>W^+-</i>, or a pair of them, or one of them in |
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| 110 | combination with a parton. Since the three sets are partly |
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| 111 | conflicting, each is associated with its own group flag. |
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| 112 | In addition, <i>t</i>-channel exchange of such a boson |
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| 113 | between two fermions form a separate group. |
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| 114 | |
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| 115 | <p/> |
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| 116 | There is one flag that can be used to influence the <i>gamma^*/Z^0</i> |
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| 117 | structure in all the processes below where it is produced, unless |
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| 118 | otherwise stated. |
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| 119 | <br/><br/><table><tr><td><strong>WeakZ0:gmZmode </td><td> (<code>default = <strong>0</strong></code>; <code>minimum = 0</code>; <code>maximum = 2</code>)</td></tr></table> |
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| 120 | Choice of full <ei>gamma^*/Z^0</ei> structure or not in relevant |
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| 121 | processes. |
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| 122 | <br/> |
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| 123 | <input type="radio" name="8" value="0" checked="checked"><strong>0 </strong>: full <ei>gamma^*/Z^0</ei> structure, with interference included.<br/> |
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| 124 | <input type="radio" name="8" value="1"><strong>1 </strong>: only pure <ei>gamma^*</ei> contribution.<br/> |
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| 125 | <input type="radio" name="8" value="2"><strong>2 </strong>: only pure <ei>Z^0</ei> contribution.<br/> |
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| 126 | <br/><b>Note</b>: irrespective of the option used, the particle produced |
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| 127 | will always be assigned code 23 for <ei>Z^0</ei>, and open decay channels |
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| 128 | is purely dictated by what is set for the <ei>Z^0</ei>. |
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| 129 | |
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| 130 | <h4>Boson exchange</h4> |
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| 131 | |
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| 132 | The two processes in this subgroup is included as part of the |
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| 133 | multiparton-interactions framework. |
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| 134 | |
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| 135 | <br/><br/><strong>WeakBosonExchange:all</strong> <input type="radio" name="9" value="on"><strong>On</strong> |
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| 136 | <input type="radio" name="9" value="off" checked="checked"><strong>Off</strong> |
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| 137 | (<code>default = <strong>off</strong></code>)<br/> |
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| 138 | Common switch for the group of <i>gamma^*/Z^0</i> |
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| 139 | or <i>W^+-</i> exchange between two fermions. |
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| 140 | |
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| 141 | |
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| 142 | <br/><br/><strong>WeakBosonExchange:ff2ff(t:gmZ)</strong> <input type="radio" name="10" value="on"><strong>On</strong> |
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| 143 | <input type="radio" name="10" value="off" checked="checked"><strong>Off</strong> |
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| 144 | (<code>default = <strong>off</strong></code>)<br/> |
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| 145 | Scattering <i>f f' -> f f'</i> via </i>gamma^*/Z^0</i> |
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| 146 | <i>t</i>-channel exchange, with full interference |
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| 147 | between the <i>gamma^*</i> and <i>Z^0</i>. |
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| 148 | Code 211. |
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| 149 | |
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| 150 | |
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| 151 | <br/><br/><strong>WeakBosonExchange:ff2ff(t:W)</strong> <input type="radio" name="11" value="on"><strong>On</strong> |
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| 152 | <input type="radio" name="11" value="off" checked="checked"><strong>Off</strong> |
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| 153 | (<code>default = <strong>off</strong></code>)<br/> |
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| 154 | Scattering <i>f_1 f_2 -> f_3 f_4</i> via </i>W^+-</i> |
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| 155 | <i>t</i>-channel exchange. |
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| 156 | Code 212. |
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| 157 | |
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| 158 | |
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| 159 | <h4>Single boson</h4> |
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| 160 | |
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| 161 | <br/><br/><strong>WeakSingleBoson:all</strong> <input type="radio" name="12" value="on"><strong>On</strong> |
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| 162 | <input type="radio" name="12" value="off" checked="checked"><strong>Off</strong> |
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| 163 | (<code>default = <strong>off</strong></code>)<br/> |
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| 164 | Common switch for the group of a single <i>gamma^*/Z^0</i> |
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| 165 | or <i>W^+-</i> production. |
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| 166 | |
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| 167 | |
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| 168 | <br/><br/><strong>WeakSingleBoson:ffbar2gmZ</strong> <input type="radio" name="13" value="on"><strong>On</strong> |
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| 169 | <input type="radio" name="13" value="off" checked="checked"><strong>Off</strong> |
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| 170 | (<code>default = <strong>off</strong></code>)<br/> |
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| 171 | Scattering <i>f fbar -> gamma^*/Z^0</i>, with full interference |
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| 172 | between the <i>gamma^*</i> and <i>Z^0</i>. |
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| 173 | Code 221. |
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| 174 | |
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| 175 | |
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| 176 | <br/><br/><strong>WeakSingleBoson:ffbar2W</strong> <input type="radio" name="14" value="on"><strong>On</strong> |
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| 177 | <input type="radio" name="14" value="off" checked="checked"><strong>Off</strong> |
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| 178 | (<code>default = <strong>off</strong></code>)<br/> |
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| 179 | Scattering <i>f fbar' -> W^+-</i>. |
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| 180 | Code 222. |
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| 181 | |
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| 182 | |
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| 183 | <br/><br/><strong>WeakSingleBoson:ffbar2ffbar(s:gm)</strong> <input type="radio" name="15" value="on"><strong>On</strong> |
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| 184 | <input type="radio" name="15" value="off" checked="checked"><strong>Off</strong> |
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| 185 | (<code>default = <strong>off</strong></code>)<br/> |
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| 186 | Scattering <i>f fbar -> gamma^* -> f' fbar'</i>. Subset of |
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| 187 | process 221, but written as a <i>2 -> 2</i> process, so that |
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| 188 | <i>pT</i> can be used as ordering variable, e.g. in multiparton |
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| 189 | interactions. Hardcoded for the final state being either of the |
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| 190 | five quark flavours or three lepton ones. Not included in the |
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| 191 | <code>WeakSingleBoson:all</code> set, but included in the |
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| 192 | multiparton-interactions framework. |
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| 193 | Code 223. |
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| 194 | |
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| 195 | |
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| 196 | <h4>Boson pair</h4> |
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| 197 | |
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| 198 | Note that, in the decay of the two vector bosons produced by an |
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| 199 | <i>f fbar -> V V</i> process, the full four-fermion correlations |
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| 200 | from the leading-order <i>f fbar -> V V -> 4f</i> matrix elements |
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| 201 | are included [<a href="Bibliography.php" target="page">Gun86</a>] (with some extensions by the authors). |
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| 202 | The matrix elements are provided in the double-resonant approach, i.e. |
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| 203 | excludes graph like <i>f fbar -> V -> f fbar -> f fbar V -> 4f</i>. |
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| 204 | |
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| 205 | <br/><br/><strong>WeakDoubleBoson:all</strong> <input type="radio" name="16" value="on"><strong>On</strong> |
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| 206 | <input type="radio" name="16" value="off" checked="checked"><strong>Off</strong> |
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| 207 | (<code>default = <strong>off</strong></code>)<br/> |
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| 208 | Common switch for the group of pair production of <i>gamma^*/Z^0</i> |
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| 209 | and <i>W^+-</i>. |
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| 210 | |
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| 211 | |
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| 212 | <br/><br/><strong>WeakDoubleBoson:ffbar2gmZgmZ</strong> <input type="radio" name="17" value="on"><strong>On</strong> |
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| 213 | <input type="radio" name="17" value="off" checked="checked"><strong>Off</strong> |
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| 214 | (<code>default = <strong>off</strong></code>)<br/> |
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| 215 | Scattering <i>f fbar' -> gamma^*/Z^0 gamma^*/Z^0</i>. |
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| 216 | Code 231. |
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| 217 | |
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| 218 | |
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| 219 | <br/><br/><strong>WeakDoubleBoson:ffbar2ZW</strong> <input type="radio" name="18" value="on"><strong>On</strong> |
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| 220 | <input type="radio" name="18" value="off" checked="checked"><strong>Off</strong> |
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| 221 | (<code>default = <strong>off</strong></code>)<br/> |
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| 222 | Scattering <i>f fbar' -> Z^0 W^+-</i>. Note that here the |
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| 223 | <i>gamma^*</i> contribution is not (currently) included. |
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| 224 | Code 232. |
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| 225 | |
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| 226 | |
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| 227 | <br/><br/><strong>WeakDoubleBoson:ffbar2WW</strong> <input type="radio" name="19" value="on"><strong>On</strong> |
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| 228 | <input type="radio" name="19" value="off" checked="checked"><strong>Off</strong> |
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| 229 | (<code>default = <strong>off</strong></code>)<br/> |
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| 230 | Scattering <i>f fbar -> W^+ W^-</i>. |
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| 231 | Code 233. |
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| 232 | |
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| 233 | |
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| 234 | <h4>Boson and parton</h4> |
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| 235 | |
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| 236 | <br/><br/><strong>WeakBosonAndParton:all</strong> <input type="radio" name="20" value="on"><strong>On</strong> |
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| 237 | <input type="radio" name="20" value="off" checked="checked"><strong>Off</strong> |
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| 238 | (<code>default = <strong>off</strong></code>)<br/> |
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| 239 | Common switch for the group of production of a single electroweak |
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| 240 | gauge boson, i.e. a <i>gamma^*/Z^0</i> or a <i>W^+-</i>, in |
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| 241 | association with a parton, i.e. a quark, gluon, photon or lepton. |
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| 242 | These processes give first-order corrections to the ones in the |
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| 243 | <code>WeakSingleBoson</code> class, and both sets cannot be used |
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| 244 | simultaneously without unphysical doublecounting. The current class |
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| 245 | should only be used to study the high-<i>pT</i> tail of the |
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| 246 | gauge-boson production processes (for LHC applications at least |
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| 247 | <i>pT</i> > 20 GeV), while the ones in <code>WeakSingleBoson</code> |
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| 248 | should be used for inclusive production. |
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| 249 | |
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| 250 | |
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| 251 | <br/><br/><strong>WeakBosonAndParton:qqbar2gmZg</strong> <input type="radio" name="21" value="on"><strong>On</strong> |
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| 252 | <input type="radio" name="21" value="off" checked="checked"><strong>Off</strong> |
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| 253 | (<code>default = <strong>off</strong></code>)<br/> |
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| 254 | Scattering <i>q qbar -> gamma^*/Z^0 g</i>. |
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| 255 | Code 241. |
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| 256 | |
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| 257 | |
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| 258 | <br/><br/><strong>WeakBosonAndParton:qg2gmZq</strong> <input type="radio" name="22" value="on"><strong>On</strong> |
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| 259 | <input type="radio" name="22" value="off" checked="checked"><strong>Off</strong> |
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| 260 | (<code>default = <strong>off</strong></code>)<br/> |
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| 261 | Scattering <i>q g -> gamma^*/Z^0 q </i>. |
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| 262 | Code 242. |
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| 263 | |
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| 264 | |
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| 265 | <br/><br/><strong>WeakBosonAndParton:ffbar2gmZgm</strong> <input type="radio" name="23" value="on"><strong>On</strong> |
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| 266 | <input type="radio" name="23" value="off" checked="checked"><strong>Off</strong> |
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| 267 | (<code>default = <strong>off</strong></code>)<br/> |
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| 268 | Scattering <i>f fbar -> gamma^*/Z^0 gamma</i>. |
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| 269 | Code 243. |
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| 270 | |
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| 271 | |
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| 272 | <br/><br/><strong>WeakBosonAndParton:fgm2gmZf</strong> <input type="radio" name="24" value="on"><strong>On</strong> |
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| 273 | <input type="radio" name="24" value="off" checked="checked"><strong>Off</strong> |
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| 274 | (<code>default = <strong>off</strong></code>)<br/> |
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| 275 | Scattering <i>f gamma -> gamma^*/Z^0 f</i>. |
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| 276 | Code 244. |
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| 277 | |
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| 278 | |
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| 279 | <br/><br/><strong>WeakBosonAndParton:qqbar2Wg</strong> <input type="radio" name="25" value="on"><strong>On</strong> |
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| 280 | <input type="radio" name="25" value="off" checked="checked"><strong>Off</strong> |
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| 281 | (<code>default = <strong>off</strong></code>)<br/> |
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| 282 | Scattering <i>q qbar -> W^+- g</i>. |
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| 283 | Code 251. |
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| 284 | |
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| 285 | |
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| 286 | <br/><br/><strong>WeakBosonAndParton:qg2Wq</strong> <input type="radio" name="26" value="on"><strong>On</strong> |
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| 287 | <input type="radio" name="26" value="off" checked="checked"><strong>Off</strong> |
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| 288 | (<code>default = <strong>off</strong></code>)<br/> |
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| 289 | Scattering <i>q g -> W^+- q</i>. |
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| 290 | Code 252. |
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| 291 | |
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| 292 | |
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| 293 | <br/><br/><strong>WeakBosonAndParton:ffbar2Wgm</strong> <input type="radio" name="27" value="on"><strong>On</strong> |
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| 294 | <input type="radio" name="27" value="off" checked="checked"><strong>Off</strong> |
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| 295 | (<code>default = <strong>off</strong></code>)<br/> |
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| 296 | Scattering <i>f fbar -> W^+- gamma</i>. |
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| 297 | Code 253. |
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| 298 | |
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| 299 | |
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| 300 | <br/><br/><strong>WeakBosonAndParton:fgm2Wf</strong> <input type="radio" name="28" value="on"><strong>On</strong> |
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| 301 | <input type="radio" name="28" value="off" checked="checked"><strong>Off</strong> |
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| 302 | (<code>default = <strong>off</strong></code>)<br/> |
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| 303 | Scattering <i>f gamma -> W^+- f</i>. |
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| 304 | Code 254. |
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| 305 | |
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| 306 | |
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| 307 | <h3> Photon Collision Processes</h3> |
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| 308 | |
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| 309 | A few electroweak two-photon production processes are available. |
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| 310 | To use them, photon PDFs have to be defined for the incoming |
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| 311 | beam particles. For proton beams an appropriate set would be |
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| 312 | MRST QED 2004 [<a href="Bibliography.php" target="page">Mar05</a>], available in the LHAPDF library. |
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| 313 | |
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| 314 | <br/><br/><strong>PhotonCollision:all</strong> <input type="radio" name="29" value="on"><strong>On</strong> |
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| 315 | <input type="radio" name="29" value="off" checked="checked"><strong>Off</strong> |
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| 316 | (<code>default = <strong>off</strong></code>)<br/> |
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| 317 | Common switch for the group of six processes presented below. |
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| 318 | |
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| 319 | |
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| 320 | <br/><br/><strong>PhotonCollision:gmgm2qqbar</strong> <input type="radio" name="30" value="on"><strong>On</strong> |
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| 321 | <input type="radio" name="30" value="off" checked="checked"><strong>Off</strong> |
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| 322 | (<code>default = <strong>off</strong></code>)<br/> |
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| 323 | Scatterings <i>gamma gamma -> q qbar</i>, where <i>q</i> |
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| 324 | is a light quark (<i>u, d, s</i>) . |
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| 325 | Code 261. |
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| 326 | |
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| 327 | |
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| 328 | <br/><br/><strong>PhotonCollision:gmgm2ccbar</strong> <input type="radio" name="31" value="on"><strong>On</strong> |
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| 329 | <input type="radio" name="31" value="off" checked="checked"><strong>Off</strong> |
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| 330 | (<code>default = <strong>off</strong></code>)<br/> |
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| 331 | Scattering <i>gamma gamma -> c cbar</i>. |
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| 332 | Code 262. |
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| 333 | |
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| 334 | |
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| 335 | <br/><br/><strong>PhotonCollision:gmgm2bbbar</strong> <input type="radio" name="32" value="on"><strong>On</strong> |
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| 336 | <input type="radio" name="32" value="off" checked="checked"><strong>Off</strong> |
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| 337 | (<code>default = <strong>off</strong></code>)<br/> |
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| 338 | Scattering <i>gamma gamma -> b bbar</i>. |
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| 339 | Code 263. |
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| 340 | |
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| 341 | |
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| 342 | <br/><br/><strong>PhotonCollision:gmgm2ee</strong> <input type="radio" name="33" value="on"><strong>On</strong> |
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| 343 | <input type="radio" name="33" value="off" checked="checked"><strong>Off</strong> |
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| 344 | (<code>default = <strong>off</strong></code>)<br/> |
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| 345 | Scattering <i>gamma gamma -> e+ e-</i>. |
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| 346 | Code 264. |
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| 347 | |
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| 348 | |
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| 349 | <br/><br/><strong>PhotonCollision:gmgm2mumu</strong> <input type="radio" name="34" value="on"><strong>On</strong> |
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| 350 | <input type="radio" name="34" value="off" checked="checked"><strong>Off</strong> |
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| 351 | (<code>default = <strong>off</strong></code>)<br/> |
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| 352 | Scattering <i>gamma gamma -> mu+ mu-</i>. |
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| 353 | Code 265. |
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| 354 | |
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| 355 | |
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| 356 | <br/><br/><strong>PhotonCollision:gmgm2tautau</strong> <input type="radio" name="35" value="on"><strong>On</strong> |
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| 357 | <input type="radio" name="35" value="off" checked="checked"><strong>Off</strong> |
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| 358 | (<code>default = <strong>off</strong></code>)<br/> |
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| 359 | Scattering <i>gamma gamma -> tau+ tau-</i>. |
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| 360 | Code 266. |
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| 361 | |
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| 362 | |
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| 363 | <input type="hidden" name="saved" value="1"/> |
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| 364 | |
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| 365 | <?php |
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| 366 | echo "<input type='hidden' name='filepath' value='".$_GET["filepath"]."'/>"?> |
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| 367 | |
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| 368 | <table width="100%"><tr><td align="right"><input type="submit" value="Save Settings" /></td></tr></table> |
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| 369 | </form> |
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| 370 | |
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| 371 | <?php |
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| 372 | |
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| 373 | if($_POST["saved"] == 1) |
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| 374 | { |
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| 375 | $filepath = $_POST["filepath"]; |
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| 376 | $handle = fopen($filepath, 'a'); |
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| 377 | |
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| 378 | if($_POST["1"] != "off") |
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| 379 | { |
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| 380 | $data = "PromptPhoton:all = ".$_POST["1"]."\n"; |
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| 381 | fwrite($handle,$data); |
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| 382 | } |
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| 383 | if($_POST["2"] != "off") |
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| 384 | { |
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| 385 | $data = "PromptPhoton:qg2qgamma = ".$_POST["2"]."\n"; |
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| 386 | fwrite($handle,$data); |
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| 387 | } |
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| 388 | if($_POST["3"] != "off") |
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| 389 | { |
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| 390 | $data = "PromptPhoton:qqbar2ggamma = ".$_POST["3"]."\n"; |
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| 391 | fwrite($handle,$data); |
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| 392 | } |
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| 393 | if($_POST["4"] != "off") |
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| 394 | { |
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| 395 | $data = "PromptPhoton:gg2ggamma = ".$_POST["4"]."\n"; |
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| 396 | fwrite($handle,$data); |
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| 397 | } |
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| 398 | if($_POST["5"] != "off") |
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| 399 | { |
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| 400 | $data = "PromptPhoton:ffbar2gammagamma = ".$_POST["5"]."\n"; |
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| 401 | fwrite($handle,$data); |
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| 402 | } |
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| 403 | if($_POST["6"] != "off") |
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| 404 | { |
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| 405 | $data = "PromptPhoton:gg2gammagamma = ".$_POST["6"]."\n"; |
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| 406 | fwrite($handle,$data); |
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| 407 | } |
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| 408 | if($_POST["7"] != "5") |
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| 409 | { |
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| 410 | $data = "PromptPhoton:nQuarkLoop = ".$_POST["7"]."\n"; |
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| 411 | fwrite($handle,$data); |
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| 412 | } |
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| 413 | if($_POST["8"] != "0") |
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| 414 | { |
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| 415 | $data = "WeakZ0:gmZmode = ".$_POST["8"]."\n"; |
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| 416 | fwrite($handle,$data); |
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| 417 | } |
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| 418 | if($_POST["9"] != "off") |
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| 419 | { |
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| 420 | $data = "WeakBosonExchange:all = ".$_POST["9"]."\n"; |
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| 421 | fwrite($handle,$data); |
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| 422 | } |
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| 423 | if($_POST["10"] != "off") |
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| 424 | { |
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| 425 | $data = "WeakBosonExchange:ff2ff(t:gmZ) = ".$_POST["10"]."\n"; |
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| 426 | fwrite($handle,$data); |
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| 427 | } |
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| 428 | if($_POST["11"] != "off") |
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| 429 | { |
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| 430 | $data = "WeakBosonExchange:ff2ff(t:W) = ".$_POST["11"]."\n"; |
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| 431 | fwrite($handle,$data); |
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| 432 | } |
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| 433 | if($_POST["12"] != "off") |
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| 434 | { |
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| 435 | $data = "WeakSingleBoson:all = ".$_POST["12"]."\n"; |
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| 436 | fwrite($handle,$data); |
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| 437 | } |
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| 438 | if($_POST["13"] != "off") |
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| 439 | { |
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| 440 | $data = "WeakSingleBoson:ffbar2gmZ = ".$_POST["13"]."\n"; |
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| 441 | fwrite($handle,$data); |
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| 442 | } |
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| 443 | if($_POST["14"] != "off") |
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| 444 | { |
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| 445 | $data = "WeakSingleBoson:ffbar2W = ".$_POST["14"]."\n"; |
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| 446 | fwrite($handle,$data); |
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| 447 | } |
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| 448 | if($_POST["15"] != "off") |
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| 449 | { |
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| 450 | $data = "WeakSingleBoson:ffbar2ffbar(s:gm) = ".$_POST["15"]."\n"; |
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| 451 | fwrite($handle,$data); |
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| 452 | } |
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| 453 | if($_POST["16"] != "off") |
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| 454 | { |
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| 455 | $data = "WeakDoubleBoson:all = ".$_POST["16"]."\n"; |
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| 456 | fwrite($handle,$data); |
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| 457 | } |
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| 458 | if($_POST["17"] != "off") |
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| 459 | { |
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| 460 | $data = "WeakDoubleBoson:ffbar2gmZgmZ = ".$_POST["17"]."\n"; |
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| 461 | fwrite($handle,$data); |
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| 462 | } |
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| 463 | if($_POST["18"] != "off") |
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| 464 | { |
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| 465 | $data = "WeakDoubleBoson:ffbar2ZW = ".$_POST["18"]."\n"; |
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| 466 | fwrite($handle,$data); |
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| 467 | } |
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| 468 | if($_POST["19"] != "off") |
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| 469 | { |
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| 470 | $data = "WeakDoubleBoson:ffbar2WW = ".$_POST["19"]."\n"; |
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| 471 | fwrite($handle,$data); |
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| 472 | } |
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| 473 | if($_POST["20"] != "off") |
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| 474 | { |
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| 475 | $data = "WeakBosonAndParton:all = ".$_POST["20"]."\n"; |
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| 476 | fwrite($handle,$data); |
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| 477 | } |
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| 478 | if($_POST["21"] != "off") |
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| 479 | { |
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| 480 | $data = "WeakBosonAndParton:qqbar2gmZg = ".$_POST["21"]."\n"; |
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| 481 | fwrite($handle,$data); |
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| 482 | } |
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| 483 | if($_POST["22"] != "off") |
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| 484 | { |
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| 485 | $data = "WeakBosonAndParton:qg2gmZq = ".$_POST["22"]."\n"; |
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| 486 | fwrite($handle,$data); |
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| 487 | } |
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| 488 | if($_POST["23"] != "off") |
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| 489 | { |
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| 490 | $data = "WeakBosonAndParton:ffbar2gmZgm = ".$_POST["23"]."\n"; |
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| 491 | fwrite($handle,$data); |
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| 492 | } |
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| 493 | if($_POST["24"] != "off") |
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| 494 | { |
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| 495 | $data = "WeakBosonAndParton:fgm2gmZf = ".$_POST["24"]."\n"; |
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| 496 | fwrite($handle,$data); |
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| 497 | } |
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| 498 | if($_POST["25"] != "off") |
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| 499 | { |
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| 500 | $data = "WeakBosonAndParton:qqbar2Wg = ".$_POST["25"]."\n"; |
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| 501 | fwrite($handle,$data); |
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| 502 | } |
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| 503 | if($_POST["26"] != "off") |
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| 504 | { |
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| 505 | $data = "WeakBosonAndParton:qg2Wq = ".$_POST["26"]."\n"; |
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| 506 | fwrite($handle,$data); |
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| 507 | } |
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| 508 | if($_POST["27"] != "off") |
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| 509 | { |
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| 510 | $data = "WeakBosonAndParton:ffbar2Wgm = ".$_POST["27"]."\n"; |
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| 511 | fwrite($handle,$data); |
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| 512 | } |
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| 513 | if($_POST["28"] != "off") |
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| 514 | { |
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| 515 | $data = "WeakBosonAndParton:fgm2Wf = ".$_POST["28"]."\n"; |
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| 516 | fwrite($handle,$data); |
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| 517 | } |
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| 518 | if($_POST["29"] != "off") |
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| 519 | { |
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| 520 | $data = "PhotonCollision:all = ".$_POST["29"]."\n"; |
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| 521 | fwrite($handle,$data); |
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| 522 | } |
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| 523 | if($_POST["30"] != "off") |
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| 524 | { |
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| 525 | $data = "PhotonCollision:gmgm2qqbar = ".$_POST["30"]."\n"; |
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| 526 | fwrite($handle,$data); |
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| 527 | } |
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| 528 | if($_POST["31"] != "off") |
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| 529 | { |
---|
| 530 | $data = "PhotonCollision:gmgm2ccbar = ".$_POST["31"]."\n"; |
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| 531 | fwrite($handle,$data); |
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| 532 | } |
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| 533 | if($_POST["32"] != "off") |
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| 534 | { |
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| 535 | $data = "PhotonCollision:gmgm2bbbar = ".$_POST["32"]."\n"; |
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| 536 | fwrite($handle,$data); |
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| 537 | } |
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| 538 | if($_POST["33"] != "off") |
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| 539 | { |
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| 540 | $data = "PhotonCollision:gmgm2ee = ".$_POST["33"]."\n"; |
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| 541 | fwrite($handle,$data); |
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| 542 | } |
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| 543 | if($_POST["34"] != "off") |
---|
| 544 | { |
---|
| 545 | $data = "PhotonCollision:gmgm2mumu = ".$_POST["34"]."\n"; |
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| 546 | fwrite($handle,$data); |
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| 547 | } |
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| 548 | if($_POST["35"] != "off") |
---|
| 549 | { |
---|
| 550 | $data = "PhotonCollision:gmgm2tautau = ".$_POST["35"]."\n"; |
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| 551 | fwrite($handle,$data); |
---|
| 552 | } |
---|
| 553 | fclose($handle); |
---|
| 554 | } |
---|
| 555 | |
---|
| 556 | ?> |
---|
| 557 | </body> |
---|
| 558 | </html> |
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| 559 | |
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| 560 | <!-- Copyright (C) 2012 Torbjorn Sjostrand --> |
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| 561 | |
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