| 1 | (* Content-type: application/mathematica *)
|
|---|
| 2 |
|
|---|
| 3 | (*** Wolfram Notebook File ***)
|
|---|
| 4 | (* http://www.wolfram.com/nb *)
|
|---|
| 5 |
|
|---|
| 6 | (* CreatedBy='Mathematica 6.0' *)
|
|---|
| 7 |
|
|---|
| 8 | (*CacheID: 234*)
|
|---|
| 9 | (* Internal cache information:
|
|---|
| 10 | NotebookFileLineBreakTest
|
|---|
| 11 | NotebookFileLineBreakTest
|
|---|
| 12 | NotebookDataPosition[ 145, 7]
|
|---|
| 13 | NotebookDataLength[ 29348, 888]
|
|---|
| 14 | NotebookOptionsPosition[ 23926, 711]
|
|---|
| 15 | NotebookOutlinePosition[ 24399, 730]
|
|---|
| 16 | CellTagsIndexPosition[ 24356, 727]
|
|---|
| 17 | WindowFrame->Normal*)
|
|---|
| 18 |
|
|---|
| 19 | (* Beginning of Notebook Content *)
|
|---|
| 20 | Notebook[{
|
|---|
| 21 | Cell[BoxData[
|
|---|
| 22 | RowBox[{"Quit", "[", "]"}]], "Input",
|
|---|
| 23 | CellChangeTimes->{{3.4921467751527157`*^9, 3.492146776183146*^9}}],
|
|---|
| 24 |
|
|---|
| 25 | Cell[BoxData[
|
|---|
| 26 | RowBox[{"$FeynRulesPath", "=",
|
|---|
| 27 | RowBox[{
|
|---|
| 28 | "SetDirectory", "[", "\"\<< address of the package >\>\"", "]"}]}]], "Input",\
|
|---|
| 29 |
|
|---|
| 30 | CellChangeTimes->{{3.41265862251538*^9, 3.412658649947229*^9}, {
|
|---|
| 31 | 3.423415585782702*^9, 3.423415597189939*^9}, {3.4234163173467493`*^9,
|
|---|
| 32 | 3.4234163227881193`*^9}}],
|
|---|
| 33 |
|
|---|
| 34 | Cell[BoxData[
|
|---|
| 35 | RowBox[{"<<", "FeynRules`"}]], "Input",
|
|---|
| 36 | CellChangeTimes->{{3.547535564344927*^9, 3.547535564971527*^9}}],
|
|---|
| 37 |
|
|---|
| 38 | Cell[BoxData[
|
|---|
| 39 | RowBox[{
|
|---|
| 40 | RowBox[{"SetDirectory", "[",
|
|---|
| 41 | RowBox[{"$FeynRulesPath", "<>", "\"\</Models/SM\>\""}], "]"}],
|
|---|
| 42 | ";"}]], "Input",
|
|---|
| 43 | CellChangeTimes->{{3.419073170860696*^9, 3.419073182827229*^9}}],
|
|---|
| 44 |
|
|---|
| 45 | Cell[CellGroupData[{
|
|---|
| 46 |
|
|---|
| 47 | Cell["The Standard Model", "Title"],
|
|---|
| 48 |
|
|---|
| 49 | Cell["We first load in the Standard Model model-file", "Text"],
|
|---|
| 50 |
|
|---|
| 51 | Cell[BoxData[
|
|---|
| 52 | RowBox[{"LoadModel", "[", "\"\<SM.fr\>\"", "]"}]], "Input",
|
|---|
| 53 | CellChangeTimes->{{3.4022069973481913`*^9, 3.402207011768662*^9},
|
|---|
| 54 | 3.4022081212072697`*^9, {3.402208250379383*^9, 3.402208254043104*^9},
|
|---|
| 55 | 3.4027466057480917`*^9, {3.403240270135737*^9, 3.403240277228945*^9},
|
|---|
| 56 | 3.403266503388291*^9, {3.403267649630335*^9, 3.40326765417397*^9}, {
|
|---|
| 57 | 3.403269919787421*^9, 3.403269921965273*^9}, {3.403347551273425*^9,
|
|---|
| 58 | 3.403347555049163*^9}, 3.4044490490588417`*^9, {3.411744339876704*^9,
|
|---|
| 59 | 3.411744340012457*^9}, {3.4121886924550533`*^9, 3.412188699157571*^9},
|
|---|
| 60 | 3.412188808811866*^9, 3.4121888580521603`*^9, {3.412450464077868*^9,
|
|---|
| 61 | 3.412450464378695*^9}, {3.413715097460478*^9, 3.41371509757642*^9}, {
|
|---|
| 62 | 3.41440825334604*^9, 3.414408254159686*^9}, {3.41862573831756*^9,
|
|---|
| 63 | 3.4186257392223186`*^9}, {3.4190731862389174`*^9, 3.419073187003003*^9}, {
|
|---|
| 64 | 3.419073336802393*^9, 3.4190733374513063`*^9}, {3.4190828041801767`*^9,
|
|---|
| 65 | 3.4190828048079023`*^9}, 3.542453089813714*^9, 3.547534567644828*^9}],
|
|---|
| 66 |
|
|---|
| 67 | Cell[BoxData[
|
|---|
| 68 | RowBox[{"LoadRestriction", "[",
|
|---|
| 69 | RowBox[{"\"\<Massless.rst\>\"", ",", "\"\<DiagonalCKM.rst\>\""}],
|
|---|
| 70 | "]"}]], "Input",
|
|---|
| 71 | CellChangeTimes->{{3.547535575308606*^9, 3.547535589236651*^9}}],
|
|---|
| 72 |
|
|---|
| 73 | Cell[CellGroupData[{
|
|---|
| 74 |
|
|---|
| 75 | Cell["The SM lagrangian", "Section",
|
|---|
| 76 | CellChangeTimes->{{3.411910065227421*^9, 3.411910071535137*^9}}],
|
|---|
| 77 |
|
|---|
| 78 | Cell[CellGroupData[{
|
|---|
| 79 |
|
|---|
| 80 | Cell["Unitary Gauge", "Subsection",
|
|---|
| 81 | CellChangeTimes->{{3.411910080775518*^9, 3.41191008414785*^9}}],
|
|---|
| 82 |
|
|---|
| 83 | Cell["\<\
|
|---|
| 84 | The full lagrangian in unitary gauge can be accessed immediatly via\
|
|---|
| 85 | \>", "Text",
|
|---|
| 86 | CellChangeTimes->{{3.411910016771447*^9, 3.411910062087528*^9}, {
|
|---|
| 87 | 3.411910094087652*^9, 3.411910096590087*^9}, {3.411910215381351*^9,
|
|---|
| 88 | 3.4119102162371798`*^9}}],
|
|---|
| 89 |
|
|---|
| 90 | Cell[BoxData["LSM"], "Input",
|
|---|
| 91 | CellChangeTimes->{{3.411910106011015*^9, 3.411910106351081*^9}}],
|
|---|
| 92 |
|
|---|
| 93 | Cell[CellGroupData[{
|
|---|
| 94 |
|
|---|
| 95 | Cell["Gauge sector", "Subsubsection",
|
|---|
| 96 | CellChangeTimes->{{3.4119102216473637`*^9, 3.411910224608881*^9}}],
|
|---|
| 97 |
|
|---|
| 98 | Cell["\<\
|
|---|
| 99 | The part of the lagrangian representing the gauge sector can be accessed via\
|
|---|
| 100 | \>", "Text",
|
|---|
| 101 | CellChangeTimes->{{3.4119101255458603`*^9, 3.411910192225008*^9}, {
|
|---|
| 102 | 3.411910235813308*^9, 3.4119102509651337`*^9}}],
|
|---|
| 103 |
|
|---|
| 104 | Cell[BoxData["LGauge"], "Input",
|
|---|
| 105 | CellChangeTimes->{{3.411910181169772*^9, 3.411910184667088*^9}}]
|
|---|
| 106 | }, Open ]],
|
|---|
| 107 |
|
|---|
| 108 | Cell[CellGroupData[{
|
|---|
| 109 |
|
|---|
| 110 | Cell["Scalar sector", "Subsubsection",
|
|---|
| 111 | CellChangeTimes->{{3.4119102216473637`*^9, 3.411910224608881*^9}, {
|
|---|
| 112 | 3.411910274288354*^9, 3.41191027703699*^9}}],
|
|---|
| 113 |
|
|---|
| 114 | Cell["\<\
|
|---|
| 115 | The part of the lagrangian representing the scalar sector can be accessed via\
|
|---|
| 116 | \
|
|---|
| 117 | \>", "Text",
|
|---|
| 118 | CellChangeTimes->{{3.4119101255458603`*^9, 3.411910192225008*^9}, {
|
|---|
| 119 | 3.411910235813308*^9, 3.4119102509651337`*^9}, {3.41191028690167*^9,
|
|---|
| 120 | 3.411910287709094*^9}}],
|
|---|
| 121 |
|
|---|
| 122 | Cell[BoxData["LHiggs"], "Input",
|
|---|
| 123 | CellChangeTimes->{{3.411910181169772*^9, 3.411910184667088*^9}, {
|
|---|
| 124 | 3.411910290186841*^9, 3.411910292005392*^9}}]
|
|---|
| 125 | }, Open ]],
|
|---|
| 126 |
|
|---|
| 127 | Cell[CellGroupData[{
|
|---|
| 128 |
|
|---|
| 129 | Cell["Fermion sector", "Subsubsection",
|
|---|
| 130 | CellChangeTimes->{{3.4119102216473637`*^9, 3.411910224608881*^9}, {
|
|---|
| 131 | 3.4119103528868923`*^9, 3.411910357404933*^9}}],
|
|---|
| 132 |
|
|---|
| 133 | Cell["\<\
|
|---|
| 134 | The part of the lagrangian representing the fermion sector can be accessed via\
|
|---|
| 135 | \>", "Text",
|
|---|
| 136 | CellChangeTimes->{{3.4119101255458603`*^9, 3.411910192225008*^9}, {
|
|---|
| 137 | 3.411910235813308*^9, 3.4119102509651337`*^9}, {3.4119103873434134`*^9,
|
|---|
| 138 | 3.411910388077118*^9}}],
|
|---|
| 139 |
|
|---|
| 140 | Cell[BoxData["LFermions"], "Input",
|
|---|
| 141 | CellChangeTimes->{{3.411910181169772*^9, 3.411910184667088*^9}, {
|
|---|
| 142 | 3.411910379677638*^9, 3.4119103807255*^9}}]
|
|---|
| 143 | }, Open ]],
|
|---|
| 144 |
|
|---|
| 145 | Cell[CellGroupData[{
|
|---|
| 146 |
|
|---|
| 147 | Cell["Yukawa sector", "Subsubsection",
|
|---|
| 148 | CellChangeTimes->{{3.4119102216473637`*^9, 3.411910224608881*^9}, {
|
|---|
| 149 | 3.411910393742139*^9, 3.411910394852953*^9}}],
|
|---|
| 150 |
|
|---|
| 151 | Cell["\<\
|
|---|
| 152 | The part of the lagrangian representing the Yukawa sector can be accessed via\
|
|---|
| 153 | \
|
|---|
| 154 | \>", "Text",
|
|---|
| 155 | CellChangeTimes->{{3.4119101255458603`*^9, 3.411910192225008*^9}, {
|
|---|
| 156 | 3.411910235813308*^9, 3.4119102509651337`*^9}, {3.411910399061659*^9,
|
|---|
| 157 | 3.411910400421185*^9}}],
|
|---|
| 158 |
|
|---|
| 159 | Cell[BoxData["LYukawa"], "Input",
|
|---|
| 160 | CellChangeTimes->{{3.411910181169772*^9, 3.411910184667088*^9}, {
|
|---|
| 161 | 3.4119104032372026`*^9, 3.411910404165523*^9}}]
|
|---|
| 162 | }, Open ]]
|
|---|
| 163 | }, Open ]],
|
|---|
| 164 |
|
|---|
| 165 | Cell[CellGroupData[{
|
|---|
| 166 |
|
|---|
| 167 | Cell["Feynman Gauge", "Subsection",
|
|---|
| 168 | CellChangeTimes->{{3.411910080775518*^9, 3.41191008414785*^9}, {
|
|---|
| 169 | 3.411910431304595*^9, 3.41191043361451*^9}}],
|
|---|
| 170 |
|
|---|
| 171 | Cell["\<\
|
|---|
| 172 | By default, SM lagrangian is loaded in unitary gauge. However, Feynman gauge \
|
|---|
| 173 | can be obtained by putting\
|
|---|
| 174 | \>", "Text",
|
|---|
| 175 | CellChangeTimes->{{3.411910440565042*^9, 3.411910480762147*^9}}],
|
|---|
| 176 |
|
|---|
| 177 | Cell[BoxData[
|
|---|
| 178 | RowBox[{
|
|---|
| 179 | RowBox[{"FeynmanGauge", "=", "True"}], ";"}]], "Input",
|
|---|
| 180 | CellChangeTimes->{{3.411910487433539*^9, 3.4119104927114267`*^9}}],
|
|---|
| 181 |
|
|---|
| 182 | Cell["\<\
|
|---|
| 183 | The full lagrangian in Feynman gauge can be accessed immediatly via\
|
|---|
| 184 | \>", "Text",
|
|---|
| 185 | CellChangeTimes->{{3.411910016771447*^9, 3.411910062087528*^9}, {
|
|---|
| 186 | 3.411910094087652*^9, 3.411910096590087*^9}, {3.411910215381351*^9,
|
|---|
| 187 | 3.4119102162371798`*^9}, {3.411910436148773*^9, 3.411910437013105*^9}}],
|
|---|
| 188 |
|
|---|
| 189 | Cell[BoxData["LSM"], "Input",
|
|---|
| 190 | CellChangeTimes->{{3.411910106011015*^9, 3.411910106351081*^9}}],
|
|---|
| 191 |
|
|---|
| 192 | Cell[CellGroupData[{
|
|---|
| 193 |
|
|---|
| 194 | Cell["Gauge sector", "Subsubsection",
|
|---|
| 195 | CellChangeTimes->{{3.4119102216473637`*^9, 3.411910224608881*^9}}],
|
|---|
| 196 |
|
|---|
| 197 | Cell["\<\
|
|---|
| 198 | The part of the lagrangian representing the gauge sector can be accessed via\
|
|---|
| 199 | \>", "Text",
|
|---|
| 200 | CellChangeTimes->{{3.4119101255458603`*^9, 3.411910192225008*^9}, {
|
|---|
| 201 | 3.411910235813308*^9, 3.4119102509651337`*^9}}],
|
|---|
| 202 |
|
|---|
| 203 | Cell[BoxData["LGauge"], "Input",
|
|---|
| 204 | CellChangeTimes->{{3.411910181169772*^9, 3.411910184667088*^9}}]
|
|---|
| 205 | }, Open ]],
|
|---|
| 206 |
|
|---|
| 207 | Cell[CellGroupData[{
|
|---|
| 208 |
|
|---|
| 209 | Cell["Scalar sector", "Subsubsection",
|
|---|
| 210 | CellChangeTimes->{{3.4119102216473637`*^9, 3.411910224608881*^9}, {
|
|---|
| 211 | 3.411910274288354*^9, 3.41191027703699*^9}}],
|
|---|
| 212 |
|
|---|
| 213 | Cell["\<\
|
|---|
| 214 | The part of the lagrangian representing the scalar sector can be accessed via\
|
|---|
| 215 | \
|
|---|
| 216 | \>", "Text",
|
|---|
| 217 | CellChangeTimes->{{3.4119101255458603`*^9, 3.411910192225008*^9}, {
|
|---|
| 218 | 3.411910235813308*^9, 3.4119102509651337`*^9}, {3.41191028690167*^9,
|
|---|
| 219 | 3.411910287709094*^9}}],
|
|---|
| 220 |
|
|---|
| 221 | Cell[BoxData["LHiggs"], "Input",
|
|---|
| 222 | CellChangeTimes->{{3.411910181169772*^9, 3.411910184667088*^9}, {
|
|---|
| 223 | 3.411910290186841*^9, 3.411910292005392*^9}}]
|
|---|
| 224 | }, Open ]],
|
|---|
| 225 |
|
|---|
| 226 | Cell[CellGroupData[{
|
|---|
| 227 |
|
|---|
| 228 | Cell["Fermion sector", "Subsubsection",
|
|---|
| 229 | CellChangeTimes->{{3.4119102216473637`*^9, 3.411910224608881*^9}, {
|
|---|
| 230 | 3.4119103528868923`*^9, 3.411910357404933*^9}}],
|
|---|
| 231 |
|
|---|
| 232 | Cell["\<\
|
|---|
| 233 | The part of the lagrangian representing the fermion sector can be accessed via\
|
|---|
| 234 | \>", "Text",
|
|---|
| 235 | CellChangeTimes->{{3.4119101255458603`*^9, 3.411910192225008*^9}, {
|
|---|
| 236 | 3.411910235813308*^9, 3.4119102509651337`*^9}, {3.4119103873434134`*^9,
|
|---|
| 237 | 3.411910388077118*^9}}],
|
|---|
| 238 |
|
|---|
| 239 | Cell[BoxData["LFermions"], "Input",
|
|---|
| 240 | CellChangeTimes->{{3.411910181169772*^9, 3.411910184667088*^9}, {
|
|---|
| 241 | 3.411910379677638*^9, 3.4119103807255*^9}}]
|
|---|
| 242 | }, Open ]],
|
|---|
| 243 |
|
|---|
| 244 | Cell[CellGroupData[{
|
|---|
| 245 |
|
|---|
| 246 | Cell["Yukawa sector", "Subsubsection",
|
|---|
| 247 | CellChangeTimes->{{3.4119102216473637`*^9, 3.411910224608881*^9}, {
|
|---|
| 248 | 3.411910393742139*^9, 3.411910394852953*^9}}],
|
|---|
| 249 |
|
|---|
| 250 | Cell["\<\
|
|---|
| 251 | The part of the lagrangian representing the Yukawa sector can be accessed via\
|
|---|
| 252 | \
|
|---|
| 253 | \>", "Text",
|
|---|
| 254 | CellChangeTimes->{{3.4119101255458603`*^9, 3.411910192225008*^9}, {
|
|---|
| 255 | 3.411910235813308*^9, 3.4119102509651337`*^9}, {3.411910399061659*^9,
|
|---|
| 256 | 3.411910400421185*^9}}],
|
|---|
| 257 |
|
|---|
| 258 | Cell[BoxData["LYukawa"], "Input",
|
|---|
| 259 | CellChangeTimes->{{3.411910181169772*^9, 3.411910184667088*^9}, {
|
|---|
| 260 | 3.4119104032372026`*^9, 3.411910404165523*^9}}]
|
|---|
| 261 | }, Open ]],
|
|---|
| 262 |
|
|---|
| 263 | Cell[CellGroupData[{
|
|---|
| 264 |
|
|---|
| 265 | Cell["Ghost sector", "Subsubsection",
|
|---|
| 266 | CellChangeTimes->{{3.4119102216473637`*^9, 3.411910224608881*^9}, {
|
|---|
| 267 | 3.411910393742139*^9, 3.411910394852953*^9}, {3.4119106057673063`*^9,
|
|---|
| 268 | 3.411910606397141*^9}}],
|
|---|
| 269 |
|
|---|
| 270 | Cell["\<\
|
|---|
| 271 | The part of the lagrangian representing the ghost sector can be accessed via\
|
|---|
| 272 | \>", "Text",
|
|---|
| 273 | CellChangeTimes->{{3.4119101255458603`*^9, 3.411910192225008*^9}, {
|
|---|
| 274 | 3.411910235813308*^9, 3.4119102509651337`*^9}, {3.411910399061659*^9,
|
|---|
| 275 | 3.411910400421185*^9}, {3.4119106110136833`*^9, 3.411910611661195*^9}}],
|
|---|
| 276 |
|
|---|
| 277 | Cell[BoxData["LGhost"], "Input",
|
|---|
| 278 | CellChangeTimes->{{3.411910181169772*^9, 3.411910184667088*^9}, {
|
|---|
| 279 | 3.4119104032372026`*^9, 3.411910404165523*^9}, {3.411910615100849*^9,
|
|---|
| 280 | 3.411910615781582*^9}}]
|
|---|
| 281 | }, Open ]]
|
|---|
| 282 | }, Open ]]
|
|---|
| 283 | }, Closed]],
|
|---|
| 284 |
|
|---|
| 285 | Cell[CellGroupData[{
|
|---|
| 286 |
|
|---|
| 287 | Cell["Checking the Lagrangian", "Section",
|
|---|
| 288 | CellChangeTimes->{{3.4234156496121893`*^9, 3.423415657027569*^9}}],
|
|---|
| 289 |
|
|---|
| 290 | Cell[BoxData[
|
|---|
| 291 | RowBox[{
|
|---|
| 292 | RowBox[{"FeynmanGauge", "=", "False"}], ";"}]], "Input",
|
|---|
| 293 | CellChangeTimes->{{3.4234159280429783`*^9, 3.423415934798614*^9}, {
|
|---|
| 294 | 3.588417616520516*^9, 3.588417617062751*^9}}],
|
|---|
| 295 |
|
|---|
| 296 | Cell[CellGroupData[{
|
|---|
| 297 |
|
|---|
| 298 | Cell["Checking hermiticity", "Subsection",
|
|---|
| 299 | CellChangeTimes->{{3.4234156831783743`*^9, 3.423415689540821*^9}}],
|
|---|
| 300 |
|
|---|
| 301 | Cell["The hermiticity of the Lagrangian can be checked via", "Text",
|
|---|
| 302 | CellChangeTimes->{{3.423415694323595*^9, 3.423415707867804*^9}}],
|
|---|
| 303 |
|
|---|
| 304 | Cell[BoxData[
|
|---|
| 305 | RowBox[{"CheckHermiticity", "[", "LSM", "]"}]], "Input",
|
|---|
| 306 | CellChangeTimes->{{3.414763473002973*^9, 3.4147634845507174`*^9}, {
|
|---|
| 307 | 3.5884182415538187`*^9, 3.5884182416874647`*^9}}],
|
|---|
| 308 |
|
|---|
| 309 | Cell["\<\
|
|---|
| 310 | The same command can be applied to the flavor - expanded Lagrangian\
|
|---|
| 311 | \>", "Text",
|
|---|
| 312 | CellChangeTimes->{{3.423415721582508*^9, 3.423415739787958*^9}}],
|
|---|
| 313 |
|
|---|
| 314 | Cell[BoxData[
|
|---|
| 315 | RowBox[{"CheckHermiticity", "[",
|
|---|
| 316 | RowBox[{"LSM", ",",
|
|---|
| 317 | RowBox[{"FlavorExpand", "\[Rule]", "True"}]}], "]"}]], "Input",
|
|---|
| 318 | CellChangeTimes->{{3.414763604111637*^9, 3.4147636044973803`*^9}}]
|
|---|
| 319 | }, Open ]],
|
|---|
| 320 |
|
|---|
| 321 | Cell[CellGroupData[{
|
|---|
| 322 |
|
|---|
| 323 | Cell["Checking the mass spectrum", "Subsection",
|
|---|
| 324 | CellChangeTimes->{{3.423415831209465*^9, 3.423415835278742*^9}}],
|
|---|
| 325 |
|
|---|
| 326 | Cell["\<\
|
|---|
| 327 | FeynRules can check whether all the values of the masses given in the model \
|
|---|
| 328 | file ar ein agreement with the masses given in the Lagrangian:\
|
|---|
| 329 | \>", "Text",
|
|---|
| 330 | CellChangeTimes->{{3.423415751305388*^9, 3.423415792594919*^9}}],
|
|---|
| 331 |
|
|---|
| 332 | Cell[BoxData[
|
|---|
| 333 | RowBox[{"CheckMassSpectrum", "[", "LSM", "]"}]], "Input",
|
|---|
| 334 | CellChangeTimes->{{3.414736325829801*^9, 3.414736326065997*^9},
|
|---|
| 335 | 3.4147528281460342`*^9}]
|
|---|
| 336 | }, Open ]],
|
|---|
| 337 |
|
|---|
| 338 | Cell[CellGroupData[{
|
|---|
| 339 |
|
|---|
| 340 | Cell["Checking the kinetic terms", "Subsection",
|
|---|
| 341 | CellChangeTimes->{{3.423415843532096*^9, 3.42341584850035*^9}}],
|
|---|
| 342 |
|
|---|
| 343 | Cell["\<\
|
|---|
| 344 | In the same way, FeynRules can check whether all kinetic terms are correctly \
|
|---|
| 345 | normalized :\
|
|---|
| 346 | \>", "Text",
|
|---|
| 347 | CellChangeTimes->{{3.423415798800013*^9, 3.423415817964087*^9}}],
|
|---|
| 348 |
|
|---|
| 349 | Cell[BoxData[
|
|---|
| 350 | RowBox[{"CheckKineticTermNormalisation", "[",
|
|---|
| 351 | RowBox[{"LSM", ",",
|
|---|
| 352 | RowBox[{"FlavorExpand", "\[Rule]", "SU2W"}]}], "]"}]], "Input",
|
|---|
| 353 | CellChangeTimes->{{3.4147636651636972`*^9, 3.414763667250185*^9}}],
|
|---|
| 354 |
|
|---|
| 355 | Cell["\<\
|
|---|
| 356 | The same command cen be used at the level of the flavor - expanded Lagrangian \
|
|---|
| 357 | :\
|
|---|
| 358 | \>", "Text",
|
|---|
| 359 | CellChangeTimes->{{3.423415868906054*^9, 3.4234158864202538`*^9}}],
|
|---|
| 360 |
|
|---|
| 361 | Cell[BoxData[
|
|---|
| 362 | RowBox[{"CheckKineticTermNormalisation", "[",
|
|---|
| 363 | RowBox[{"LSM", ",",
|
|---|
| 364 | RowBox[{"FlavorExpand", "\[Rule]", "True"}]}], "]"}]], "Input"]
|
|---|
| 365 | }, Open ]]
|
|---|
| 366 | }, Closed]],
|
|---|
| 367 |
|
|---|
| 368 | Cell[CellGroupData[{
|
|---|
| 369 |
|
|---|
| 370 | Cell["Calculation of the Feynman rules", "Section",
|
|---|
| 371 | CellChangeTimes->{{3.411910637332127*^9, 3.41191064360071*^9}}],
|
|---|
| 372 |
|
|---|
| 373 | Cell["\<\
|
|---|
| 374 | We will calculate now explicitly the Feynman rules for the SM in Feynman \
|
|---|
| 375 | gauge.\
|
|---|
| 376 | \>", "Text",
|
|---|
| 377 | CellChangeTimes->{{3.41191064804084*^9, 3.411910672936666*^9}}],
|
|---|
| 378 |
|
|---|
| 379 | Cell[BoxData[
|
|---|
| 380 | RowBox[{
|
|---|
| 381 | RowBox[{"FeynmanGauge", "=", "True"}], ";"}]], "Input",
|
|---|
| 382 | CellChangeTimes->{{3.411910674121689*^9, 3.4119106799564953`*^9}}],
|
|---|
| 383 |
|
|---|
| 384 | Cell[CellGroupData[{
|
|---|
| 385 |
|
|---|
| 386 | Cell["Gauge sector", "Subsection",
|
|---|
| 387 | CellChangeTimes->{{3.411910690443768*^9, 3.411910692233274*^9}}],
|
|---|
| 388 |
|
|---|
| 389 | Cell[BoxData[
|
|---|
| 390 | RowBox[{
|
|---|
| 391 | RowBox[{"vertsGauge", "=",
|
|---|
| 392 | RowBox[{"FeynmanRules", "[",
|
|---|
| 393 | RowBox[{"LGauge", ",",
|
|---|
| 394 | RowBox[{"FlavorExpand", "\[Rule]", "SU2W"}]}], "]"}]}], ";"}]], "Input",
|
|---|
| 395 | CellChangeTimes->{
|
|---|
| 396 | 3.40274690437012*^9, {3.402746954727231*^9, 3.4027469691642714`*^9}, {
|
|---|
| 397 | 3.4032592998045692`*^9, 3.403259304564069*^9}, 3.403267976055098*^9, {
|
|---|
| 398 | 3.411910705212987*^9, 3.411910705553741*^9}, {3.423415993272615*^9,
|
|---|
| 399 | 3.42341600147605*^9}}]
|
|---|
| 400 | }, Open ]],
|
|---|
| 401 |
|
|---|
| 402 | Cell[CellGroupData[{
|
|---|
| 403 |
|
|---|
| 404 | Cell["Higgs Sector", "Subsection",
|
|---|
| 405 | CellChangeTimes->{3.404470070069872*^9}],
|
|---|
| 406 |
|
|---|
| 407 | Cell[BoxData[
|
|---|
| 408 | RowBox[{
|
|---|
| 409 | RowBox[{"vertsHiggs", "=",
|
|---|
| 410 | RowBox[{"FeynmanRules", "[", "LHiggs", "]"}]}], ";"}]], "Input",
|
|---|
| 411 | CellChangeTimes->{{3.411910728609757*^9, 3.41191072908109*^9}, {
|
|---|
| 412 | 3.423416009086747*^9, 3.423416012982971*^9}, 3.423416065626593*^9}]
|
|---|
| 413 | }, Open ]],
|
|---|
| 414 |
|
|---|
| 415 | Cell[CellGroupData[{
|
|---|
| 416 |
|
|---|
| 417 | Cell["Matter sector", "Subsection"],
|
|---|
| 418 |
|
|---|
| 419 | Cell[BoxData[
|
|---|
| 420 | RowBox[{
|
|---|
| 421 | RowBox[{"vertsFermions", "=",
|
|---|
| 422 | RowBox[{"FeynmanRules", "[", "LFermions", "]"}]}], ";"}]], "Input",
|
|---|
| 423 | CellChangeTimes->{{3.402205118991502*^9, 3.4022051228508387`*^9},
|
|---|
| 424 | 3.402747846432675*^9, {3.4032613449872217`*^9, 3.403261349245253*^9}, {
|
|---|
| 425 | 3.403266977133403*^9, 3.4032669793125563`*^9}, {3.411910788644576*^9,
|
|---|
| 426 | 3.411910789233307*^9}, {3.423416034294303*^9, 3.423416042739814*^9}}]
|
|---|
| 427 | }, Open ]],
|
|---|
| 428 |
|
|---|
| 429 | Cell[CellGroupData[{
|
|---|
| 430 |
|
|---|
| 431 | Cell["Yukawa sector", "Subsection"],
|
|---|
| 432 |
|
|---|
| 433 | Cell[BoxData[
|
|---|
| 434 | RowBox[{
|
|---|
| 435 | RowBox[{"vertsYukawa", "=",
|
|---|
| 436 | RowBox[{"FeynmanRules", "[",
|
|---|
| 437 | RowBox[{"LYukawa", ",",
|
|---|
| 438 | RowBox[{"FlavorExpand", "\[Rule]", "True"}]}], "]"}]}], ";"}]], "Input",
|
|---|
| 439 | CellChangeTimes->{{3.403266987858165*^9, 3.4032670026080303`*^9}, {
|
|---|
| 440 | 3.411910826105542*^9, 3.411910826777452*^9}, {3.423416089772278*^9,
|
|---|
| 441 | 3.423416095643961*^9}}]
|
|---|
| 442 | }, Open ]],
|
|---|
| 443 |
|
|---|
| 444 | Cell[CellGroupData[{
|
|---|
| 445 |
|
|---|
| 446 | Cell["LGhost sector", "Subsection",
|
|---|
| 447 | CellChangeTimes->{{3.411910849714159*^9, 3.411910851088325*^9}}],
|
|---|
| 448 |
|
|---|
| 449 | Cell[BoxData[
|
|---|
| 450 | RowBox[{
|
|---|
| 451 | RowBox[{"vertsGhosts", "=",
|
|---|
| 452 | RowBox[{"FeynmanRules", "[",
|
|---|
| 453 | RowBox[{"LGhost", ",",
|
|---|
| 454 | RowBox[{"FlavorExpand", "\[Rule]", "SU2W"}]}], "]"}]}], ";"}]], "Input",
|
|---|
| 455 | CellChangeTimes->{{3.403266987858165*^9, 3.4032670026080303`*^9}, {
|
|---|
| 456 | 3.411910826105542*^9, 3.411910826777452*^9}, {3.411910857580064*^9,
|
|---|
| 457 | 3.411910870001601*^9}, 3.415256462464088*^9, {3.423416107236608*^9,
|
|---|
| 458 | 3.423416112835993*^9}}]
|
|---|
| 459 | }, Open ]]
|
|---|
| 460 | }, Closed]],
|
|---|
| 461 |
|
|---|
| 462 | Cell[CellGroupData[{
|
|---|
| 463 |
|
|---|
| 464 | Cell["Outputs and interfaces", "Section",
|
|---|
| 465 | CellChangeTimes->{
|
|---|
| 466 | 3.411910944409371*^9, {3.412185514054689*^9, 3.412185517014236*^9}}],
|
|---|
| 467 |
|
|---|
| 468 | Cell[CellGroupData[{
|
|---|
| 469 |
|
|---|
| 470 | Cell["FeynArts output", "Subsection",
|
|---|
| 471 | CellChangeTimes->{{3.411911000132907*^9, 3.411911005135379*^9}}],
|
|---|
| 472 |
|
|---|
| 473 | Cell["The FeynArts output for the SM can be obtained via", "Text",
|
|---|
| 474 | CellChangeTimes->{{3.411910955110715*^9, 3.4119109690877657`*^9}, {
|
|---|
| 475 | 3.411911062212926*^9, 3.4119110634765463`*^9}}],
|
|---|
| 476 |
|
|---|
| 477 | Cell[BoxData[{
|
|---|
| 478 | RowBox[{
|
|---|
| 479 | RowBox[{
|
|---|
| 480 | RowBox[{"FeynmanGauge", " ", "=", " ", "False"}], ";"}],
|
|---|
| 481 | "\[IndentingNewLine]"}], "\[IndentingNewLine]",
|
|---|
| 482 | RowBox[{"WriteFeynArtsOutput", "[",
|
|---|
| 483 | RowBox[{"LGauge", ",", "LHiggs", ",", "LFermions", ",", "LYukawa", ",",
|
|---|
| 484 | RowBox[{"FlavorExpand", "\[Rule]", "SU2W"}]}], "]"}]}], "Input",
|
|---|
| 485 | CellChangeTimes->{{3.411911018354619*^9, 3.4119110196967573`*^9}, {
|
|---|
| 486 | 3.412185470680571*^9, 3.412185480912915*^9}, {3.41245048911446*^9,
|
|---|
| 487 | 3.4124504892674522`*^9}, 3.414315634453483*^9, {3.423416180751266*^9,
|
|---|
| 488 | 3.423416182892613*^9}}],
|
|---|
| 489 |
|
|---|
| 490 | Cell["FeynArts also supports the Feynman gauge", "Text",
|
|---|
| 491 | CellChangeTimes->{{3.4121854851672792`*^9, 3.412185494183435*^9}}],
|
|---|
| 492 |
|
|---|
| 493 | Cell[BoxData[{
|
|---|
| 494 | RowBox[{
|
|---|
| 495 | RowBox[{
|
|---|
| 496 | RowBox[{"FeynmanGauge", " ", "=", " ", "True"}], ";"}],
|
|---|
| 497 | "\[IndentingNewLine]"}], "\[IndentingNewLine]",
|
|---|
| 498 | RowBox[{"WriteFeynArtsOutput", "[",
|
|---|
| 499 | RowBox[{
|
|---|
| 500 | "LGauge", ",", "LHiggs", ",", "LFermions", ",", "LYukawa", ",", "LGhost",
|
|---|
| 501 | ",",
|
|---|
| 502 | RowBox[{"FlavorExpand", "\[Rule]", "SU2W"}], ",",
|
|---|
| 503 | RowBox[{"Output", "\[Rule]", "\"\<SM.mod\>\""}]}], "]"}]}], "Input",
|
|---|
| 504 | CellChangeTimes->{{3.411911018354619*^9, 3.4119110196967573`*^9}, {
|
|---|
| 505 | 3.412185470680571*^9, 3.412185506240796*^9}, {3.4234161971513453`*^9,
|
|---|
| 506 | 3.423416209716672*^9}}]
|
|---|
| 507 | }, Open ]],
|
|---|
| 508 |
|
|---|
| 509 | Cell[CellGroupData[{
|
|---|
| 510 |
|
|---|
| 511 | Cell["Sherpa output", "Subsection",
|
|---|
| 512 | CellChangeTimes->{{3.4119110460271273`*^9, 3.411911049405038*^9}}],
|
|---|
| 513 |
|
|---|
| 514 | Cell["The Sherpa output for the SM can be obtained via", "Text",
|
|---|
| 515 | CellChangeTimes->{{3.411910955110715*^9, 3.4119109690877657`*^9}, {
|
|---|
| 516 | 3.411911059590749*^9, 3.4119110601885567`*^9}}],
|
|---|
| 517 |
|
|---|
| 518 | Cell[BoxData[{
|
|---|
| 519 | RowBox[{
|
|---|
| 520 | RowBox[{
|
|---|
| 521 | RowBox[{"FeynmanGauge", "=", "False"}], ";"}],
|
|---|
| 522 | "\[IndentingNewLine]"}], "\[IndentingNewLine]",
|
|---|
| 523 | RowBox[{"WriteSHOutput", "[",
|
|---|
| 524 | RowBox[{"LGauge", ",", "LHiggs", ",", "LFermions", ",", "LYukawa"}],
|
|---|
| 525 | "]"}]}], "Input",
|
|---|
| 526 | CellChangeTimes->{{3.4119110943383636`*^9, 3.41191110054212*^9}, {
|
|---|
| 527 | 3.412185455856553*^9, 3.412185456628922*^9}, {3.4143156544792233`*^9,
|
|---|
| 528 | 3.414315668290971*^9}, {3.423416222700699*^9, 3.423416235756197*^9}}]
|
|---|
| 529 | }, Open ]],
|
|---|
| 530 |
|
|---|
| 531 | Cell[CellGroupData[{
|
|---|
| 532 |
|
|---|
| 533 | Cell["CalcHep output", "Subsection",
|
|---|
| 534 | CellChangeTimes->{{3.4119110460271273`*^9, 3.411911049405038*^9}, {
|
|---|
| 535 | 3.411911150323291*^9, 3.4119111515122623`*^9}}],
|
|---|
| 536 |
|
|---|
| 537 | Cell["CalcHep also supports the Feynman gauge", "Text",
|
|---|
| 538 | CellChangeTimes->{{3.4121853722243843`*^9, 3.412185380407339*^9}}],
|
|---|
| 539 |
|
|---|
| 540 | Cell[BoxData[{
|
|---|
| 541 | RowBox[{
|
|---|
| 542 | RowBox[{
|
|---|
| 543 | RowBox[{"FeynmanGauge", "=", "True"}], ";"}],
|
|---|
| 544 | "\[IndentingNewLine]"}], "\[IndentingNewLine]",
|
|---|
| 545 | RowBox[{
|
|---|
| 546 | RowBox[{"WriteCHOutput", "[",
|
|---|
| 547 | RowBox[{
|
|---|
| 548 | "LGauge", ",", "LHiggs", ",", "LFermions", ",", "LYukawa", ",", "LGhost"}],
|
|---|
| 549 | "]"}], ";"}]}], "Input",
|
|---|
| 550 | CellChangeTimes->{{3.4119110943383636`*^9, 3.41191110054212*^9}, {
|
|---|
| 551 | 3.412185409690489*^9, 3.4121854275198507`*^9}, {3.412450479942018*^9,
|
|---|
| 552 | 3.4124504817138367`*^9}}],
|
|---|
| 553 |
|
|---|
| 554 | Cell[BoxData[""], "Input",
|
|---|
| 555 | CellChangeTimes->{3.412185367693318*^9, 3.412185407947097*^9}]
|
|---|
| 556 | }, Open ]],
|
|---|
| 557 |
|
|---|
| 558 | Cell[CellGroupData[{
|
|---|
| 559 |
|
|---|
| 560 | Cell["Whizard output", "Subsection",
|
|---|
| 561 | CellChangeTimes->{{3.4119110460271273`*^9, 3.411911049405038*^9}, {
|
|---|
| 562 | 3.411911150323291*^9, 3.4119111515122623`*^9}, {3.5074389822322817`*^9,
|
|---|
| 563 | 3.507438983565652*^9}}],
|
|---|
| 564 |
|
|---|
| 565 | Cell["Whizard also supports the Feynman gauge", "Text",
|
|---|
| 566 | CellChangeTimes->{{3.4121853722243843`*^9, 3.412185380407339*^9}, {
|
|---|
| 567 | 3.507438990997637*^9, 3.507438992828805*^9}}],
|
|---|
| 568 |
|
|---|
| 569 | Cell[BoxData[{
|
|---|
| 570 | RowBox[{
|
|---|
| 571 | RowBox[{
|
|---|
| 572 | RowBox[{"FeynmanGauge", "=", "True"}], ";"}],
|
|---|
| 573 | "\[IndentingNewLine]"}], "\[IndentingNewLine]",
|
|---|
| 574 | RowBox[{
|
|---|
| 575 | RowBox[{"WriteWOOutput", "[",
|
|---|
| 576 | RowBox[{
|
|---|
| 577 | "LGauge", ",", "LHiggs", ",", "LFermions", ",", "LYukawa", ",", "LGhost"}],
|
|---|
| 578 | "]"}], ";"}]}], "Input",
|
|---|
| 579 | CellChangeTimes->{{3.4119110943383636`*^9, 3.41191110054212*^9}, {
|
|---|
| 580 | 3.412185409690489*^9, 3.4121854275198507`*^9}, {3.412450479942018*^9,
|
|---|
| 581 | 3.4124504817138367`*^9}, {3.507438986168689*^9, 3.507438987383316*^9}}],
|
|---|
| 582 |
|
|---|
| 583 | Cell[BoxData[""], "Input",
|
|---|
| 584 | CellChangeTimes->{3.412185367693318*^9, 3.412185407947097*^9}]
|
|---|
| 585 | }, Open ]],
|
|---|
| 586 |
|
|---|
| 587 | Cell[CellGroupData[{
|
|---|
| 588 |
|
|---|
| 589 | Cell["UFO output", "Subsection",
|
|---|
| 590 | CellChangeTimes->{{3.4119110460271273`*^9, 3.411911049405038*^9}, {
|
|---|
| 591 | 3.411911150323291*^9, 3.4119111515122623`*^9}, {3.5074389822322817`*^9,
|
|---|
| 592 | 3.507438983565652*^9}, {3.507439158477231*^9, 3.507439159035309*^9}}],
|
|---|
| 593 |
|
|---|
| 594 | Cell[BoxData[
|
|---|
| 595 | RowBox[{
|
|---|
| 596 | RowBox[{"WriteUFO", "[",
|
|---|
| 597 | RowBox[{
|
|---|
| 598 | "LGauge", ",", "LHiggs", ",", "LFermions", ",", "LYukawa", ",", "LGhost"}],
|
|---|
| 599 | "]"}], ";"}]], "Input",
|
|---|
| 600 | CellChangeTimes->{
|
|---|
| 601 | 3.412185367693318*^9, 3.412185407947097*^9, {3.5074391727475023`*^9,
|
|---|
| 602 | 3.5074391804929533`*^9}}]
|
|---|
| 603 | }, Open ]]
|
|---|
| 604 | }, Closed]],
|
|---|
| 605 |
|
|---|
| 606 | Cell[CellGroupData[{
|
|---|
| 607 |
|
|---|
| 608 | Cell["NLO (QCD)", "Subsubtitle",
|
|---|
| 609 | CellChangeTimes->{{3.606568224887179*^9, 3.606568225228436*^9}, {
|
|---|
| 610 | 3.606568338418679*^9, 3.606568340840477*^9}}],
|
|---|
| 611 |
|
|---|
| 612 | Cell[BoxData[
|
|---|
| 613 | RowBox[{"(*",
|
|---|
| 614 | RowBox[{
|
|---|
| 615 | "Renormalization", " ", "and", " ", "output", " ", "to", " ", "FA"}],
|
|---|
| 616 | "*)"}]], "Input",
|
|---|
| 617 | CellChangeTimes->{{3.606568280586434*^9, 3.606568289181669*^9}, {
|
|---|
| 618 | 3.606568347601158*^9, 3.606568356208818*^9}}],
|
|---|
| 619 |
|
|---|
| 620 | Cell[BoxData[{
|
|---|
| 621 | RowBox[{
|
|---|
| 622 | RowBox[{"Lren", "=",
|
|---|
| 623 | RowBox[{"OnShellRenormalization", "[",
|
|---|
| 624 | RowBox[{"LSM", ",",
|
|---|
| 625 | RowBox[{"QCDOnly", "\[Rule]", "True"}], ",",
|
|---|
| 626 | RowBox[{"FlavorMixing", "\[Rule]", "False"}]}], "]"}]}],
|
|---|
| 627 | ";"}], "\[IndentingNewLine]",
|
|---|
| 628 | RowBox[{
|
|---|
| 629 | RowBox[{"SetDirectory", "[", "\"\<~/celine/FeynArts-3.7/Models\>\"", "]"}],
|
|---|
| 630 | ";"}], "\[IndentingNewLine]",
|
|---|
| 631 | RowBox[{"WriteFeynArtsOutput", "[",
|
|---|
| 632 | RowBox[{"Lren", ",",
|
|---|
| 633 | RowBox[{"Output", "\[Rule]", "\"\<SMQCDrenoL\>\""}], ",",
|
|---|
| 634 | RowBox[{"GenericFile", "\[Rule]", "False"}]}], "]"}]}], "Input",
|
|---|
| 635 | CellChangeTimes->{{3.606568250159355*^9, 3.6065682552288523`*^9}, {
|
|---|
| 636 | 3.6065683087252502`*^9, 3.6065683093453608`*^9}, {3.6065684035728207`*^9,
|
|---|
| 637 | 3.606568404147846*^9}}],
|
|---|
| 638 |
|
|---|
| 639 | Cell[BoxData[
|
|---|
| 640 | RowBox[{"(*",
|
|---|
| 641 | RowBox[{"Computation", " ", "of", " ", "the", " ", "Counterterms"}],
|
|---|
| 642 | "*)"}]], "Input",
|
|---|
| 643 | CellChangeTimes->{{3.606568413917823*^9, 3.6065684261433983`*^9}}],
|
|---|
| 644 |
|
|---|
| 645 | Cell[BoxData[
|
|---|
| 646 | RowBox[{"Quit", "[", "]"}]], "Input",
|
|---|
| 647 | CellChangeTimes->{{3.606568433162343*^9, 3.606568438694559*^9}}],
|
|---|
| 648 |
|
|---|
| 649 | Cell[BoxData[{
|
|---|
| 650 | RowBox[{
|
|---|
| 651 | RowBox[{"SetDirectory", "[", "\"\<< FeynArts directory >\>\"", "]"}],
|
|---|
| 652 | ";"}], "\[IndentingNewLine]",
|
|---|
| 653 | RowBox[{"<<", " ", "FeynArts`"}], "\[IndentingNewLine]",
|
|---|
| 654 | RowBox[{
|
|---|
| 655 | RowBox[{"SetDirectory", "[", "\"\<< NLOCT directory >\>\"", "]"}],
|
|---|
| 656 | ";"}], "\[IndentingNewLine]",
|
|---|
| 657 | RowBox[{"<<", " ", "NLOCT`"}]}], "Input",
|
|---|
| 658 | CellChangeTimes->{{3.6065684720815067`*^9, 3.6065685038224916`*^9}}],
|
|---|
| 659 |
|
|---|
| 660 | Cell[BoxData[
|
|---|
| 661 | RowBox[{
|
|---|
| 662 | RowBox[{"WriteCT", "[",
|
|---|
| 663 | RowBox[{
|
|---|
| 664 | "\"\<SMQCDrenoL/SMQCDrenoL\>\"", ",", "\"\<Lorentz\>\"", ",",
|
|---|
| 665 | "\"\<SMQCDreno\>\"", ",",
|
|---|
| 666 | RowBox[{"LabelInternal", "\[Rule]", "True"}], ",",
|
|---|
| 667 | RowBox[{"QCDOnly", "\[Rule]", "True"}], ",",
|
|---|
| 668 | RowBox[{"KeptIndices", "\[Rule]",
|
|---|
| 669 | RowBox[{"{", "}"}]}], ",",
|
|---|
| 670 | RowBox[{"ZeroMom", "\[Rule]",
|
|---|
| 671 | RowBox[{"{",
|
|---|
| 672 | RowBox[{"{",
|
|---|
| 673 | RowBox[{"aS", ",",
|
|---|
| 674 | RowBox[{"{",
|
|---|
| 675 | RowBox[{
|
|---|
| 676 | RowBox[{"F", "[", "7", "]"}], ",",
|
|---|
| 677 | RowBox[{"V", "[", "4", "]"}], ",",
|
|---|
| 678 | RowBox[{"-",
|
|---|
| 679 | RowBox[{"F", "[", "7", "]"}]}]}], "}"}], ",", "0"}], "}"}],
|
|---|
| 680 | "}"}]}], ",",
|
|---|
| 681 | RowBox[{"ComplexMass", "\[Rule]", "False"}]}], "]"}], "//", "Timing",
|
|---|
| 682 | " "}]], "Input",
|
|---|
| 683 | CellChangeTimes->{{3.606569782037321*^9, 3.606569798425932*^9}}],
|
|---|
| 684 |
|
|---|
| 685 | Cell[BoxData[
|
|---|
| 686 | RowBox[{"(*",
|
|---|
| 687 | RowBox[{
|
|---|
| 688 | "Quit", " ", "and", " ", "reload", " ", "FeynRules", " ", "and", " ", "the",
|
|---|
| 689 | " ", "model", " ", "with", " ", "the", " ", "restrictions"}],
|
|---|
| 690 | "*)"}]], "Input",
|
|---|
| 691 | CellChangeTimes->{{3.6065685476941853`*^9, 3.6065685843784647`*^9}}],
|
|---|
| 692 |
|
|---|
| 693 | Cell[BoxData[{
|
|---|
| 694 | RowBox[{
|
|---|
| 695 | RowBox[{
|
|---|
| 696 | "SetDirectory", "[",
|
|---|
| 697 | "\"\<~/celine/feynrules/trunk/feynrules-development/R2\>\"", "]"}],
|
|---|
| 698 | ";"}], "\[IndentingNewLine]",
|
|---|
| 699 | RowBox[{
|
|---|
| 700 | RowBox[{"Get", "[", "\"\<SMQCDreno.nlo\>\"", "]"}], ";"}]}], "Input"],
|
|---|
| 701 |
|
|---|
| 702 | Cell[BoxData[
|
|---|
| 703 | RowBox[{"WriteUFO", "[",
|
|---|
| 704 | RowBox[{"LSM", ",",
|
|---|
| 705 | RowBox[{"UVCounterterms", "\[Rule]", "UV$vertlist"}], ",",
|
|---|
| 706 | RowBox[{"R2Vertices", "\[Rule]", "R2$vertlist"}], ",",
|
|---|
| 707 | RowBox[{"Output", "\[Rule]", "\"\<SM_NLO\>\""}]}], "]"}]], "Input",
|
|---|
| 708 | CellChangeTimes->{{3.60656864069383*^9, 3.606568704839243*^9}}]
|
|---|
| 709 | }, Open ]]
|
|---|
| 710 | }, Open ]]
|
|---|
| 711 | },
|
|---|
| 712 | WindowSize->{1276, 756},
|
|---|
| 713 | WindowMargins->{{0, Automatic}, {Automatic, 0}},
|
|---|
| 714 | ShowSelection->True,
|
|---|
| 715 | Magnification:>FEPrivate`If[
|
|---|
| 716 | FEPrivate`Equal[FEPrivate`$VersionNumber, 6.], 2., 2. Inherited],
|
|---|
| 717 | FrontEndVersion->"8.0 for Mac OS X x86 (32-bit, 64-bit Kernel) (November 6, \
|
|---|
| 718 | 2010)",
|
|---|
| 719 | StyleDefinitions->"Default.nb"
|
|---|
| 720 | ]
|
|---|
| 721 | (* End of Notebook Content *)
|
|---|
| 722 |
|
|---|
| 723 | (* Internal cache information *)
|
|---|
| 724 | (*CellTagsOutline
|
|---|
| 725 | CellTagsIndex->{}
|
|---|
| 726 | *)
|
|---|
| 727 | (*CellTagsIndex
|
|---|
| 728 | CellTagsIndex->{}
|
|---|
| 729 | *)
|
|---|
| 730 | (*NotebookFileOutline
|
|---|
| 731 | Notebook[{
|
|---|
| 732 | Cell[545, 20, 120, 2, 54, "Input"],
|
|---|
| 733 | Cell[668, 24, 306, 7, 54, "Input"],
|
|---|
| 734 | Cell[977, 33, 120, 2, 54, "Input"],
|
|---|
| 735 | Cell[1100, 37, 207, 5, 54, "Input"],
|
|---|
| 736 | Cell[CellGroupData[{
|
|---|
| 737 | Cell[1332, 46, 35, 0, 152, "Title"],
|
|---|
| 738 | Cell[1370, 48, 62, 0, 52, "Text"],
|
|---|
| 739 | Cell[1435, 50, 1026, 14, 54, "Input"],
|
|---|
| 740 | Cell[2464, 66, 201, 4, 54, "Input"],
|
|---|
| 741 | Cell[CellGroupData[{
|
|---|
| 742 | Cell[2690, 74, 102, 1, 134, "Section"],
|
|---|
| 743 | Cell[CellGroupData[{
|
|---|
| 744 | Cell[2817, 79, 100, 1, 136, "Subsection"],
|
|---|
| 745 | Cell[2920, 82, 257, 5, 104, "Text"],
|
|---|
| 746 | Cell[3180, 89, 95, 1, 108, "Input"],
|
|---|
| 747 | Cell[CellGroupData[{
|
|---|
| 748 | Cell[3300, 94, 105, 1, 96, "Subsubsection"],
|
|---|
| 749 | Cell[3408, 97, 219, 4, 104, "Text"],
|
|---|
| 750 | Cell[3630, 103, 98, 1, 108, "Input"]
|
|---|
| 751 | }, Open ]],
|
|---|
| 752 | Cell[CellGroupData[{
|
|---|
| 753 | Cell[3765, 109, 154, 2, 96, "Subsubsection"],
|
|---|
| 754 | Cell[3922, 113, 270, 6, 104, "Text"],
|
|---|
| 755 | Cell[4195, 121, 147, 2, 108, "Input"]
|
|---|
| 756 | }, Open ]],
|
|---|
| 757 | Cell[CellGroupData[{
|
|---|
| 758 | Cell[4379, 128, 158, 2, 96, "Subsubsection"],
|
|---|
| 759 | Cell[4540, 132, 272, 5, 104, "Text"],
|
|---|
| 760 | Cell[4815, 139, 148, 2, 108, "Input"]
|
|---|
| 761 | }, Open ]],
|
|---|
| 762 | Cell[CellGroupData[{
|
|---|
| 763 | Cell[5000, 146, 155, 2, 96, "Subsubsection"],
|
|---|
| 764 | Cell[5158, 150, 271, 6, 104, "Text"],
|
|---|
| 765 | Cell[5432, 158, 150, 2, 108, "Input"]
|
|---|
| 766 | }, Open ]]
|
|---|
| 767 | }, Open ]],
|
|---|
| 768 | Cell[CellGroupData[{
|
|---|
| 769 | Cell[5631, 166, 148, 2, 136, "Subsection"],
|
|---|
| 770 | Cell[5782, 170, 195, 4, 104, "Text"],
|
|---|
| 771 | Cell[5980, 176, 149, 3, 108, "Input"],
|
|---|
| 772 | Cell[6132, 181, 303, 5, 104, "Text"],
|
|---|
| 773 | Cell[6438, 188, 95, 1, 108, "Input"],
|
|---|
| 774 | Cell[CellGroupData[{
|
|---|
| 775 | Cell[6558, 193, 105, 1, 96, "Subsubsection"],
|
|---|
| 776 | Cell[6666, 196, 219, 4, 104, "Text"],
|
|---|
| 777 | Cell[6888, 202, 98, 1, 108, "Input"]
|
|---|
| 778 | }, Open ]],
|
|---|
| 779 | Cell[CellGroupData[{
|
|---|
| 780 | Cell[7023, 208, 154, 2, 96, "Subsubsection"],
|
|---|
| 781 | Cell[7180, 212, 270, 6, 104, "Text"],
|
|---|
| 782 | Cell[7453, 220, 147, 2, 108, "Input"]
|
|---|
| 783 | }, Open ]],
|
|---|
| 784 | Cell[CellGroupData[{
|
|---|
| 785 | Cell[7637, 227, 158, 2, 96, "Subsubsection"],
|
|---|
| 786 | Cell[7798, 231, 272, 5, 104, "Text"],
|
|---|
| 787 | Cell[8073, 238, 148, 2, 108, "Input"]
|
|---|
| 788 | }, Open ]],
|
|---|
| 789 | Cell[CellGroupData[{
|
|---|
| 790 | Cell[8258, 245, 155, 2, 96, "Subsubsection"],
|
|---|
| 791 | Cell[8416, 249, 271, 6, 104, "Text"],
|
|---|
| 792 | Cell[8690, 257, 150, 2, 108, "Input"]
|
|---|
| 793 | }, Open ]],
|
|---|
| 794 | Cell[CellGroupData[{
|
|---|
| 795 | Cell[8877, 264, 205, 3, 96, "Subsubsection"],
|
|---|
| 796 | Cell[9085, 269, 316, 5, 104, "Text"],
|
|---|
| 797 | Cell[9404, 276, 198, 3, 108, "Input"]
|
|---|
| 798 | }, Open ]]
|
|---|
| 799 | }, Open ]]
|
|---|
| 800 | }, Closed]],
|
|---|
| 801 | Cell[CellGroupData[{
|
|---|
| 802 | Cell[9663, 286, 110, 1, 70, "Section"],
|
|---|
| 803 | Cell[9776, 289, 199, 4, 108, "Input"],
|
|---|
| 804 | Cell[CellGroupData[{
|
|---|
| 805 | Cell[10000, 297, 110, 1, 136, "Subsection"],
|
|---|
| 806 | Cell[10113, 300, 134, 1, 104, "Text"],
|
|---|
| 807 | Cell[10250, 303, 192, 3, 108, "Input"],
|
|---|
| 808 | Cell[10445, 308, 157, 3, 104, "Text"],
|
|---|
| 809 | Cell[10605, 313, 206, 4, 108, "Input"]
|
|---|
| 810 | }, Open ]],
|
|---|
| 811 | Cell[CellGroupData[{
|
|---|
| 812 | Cell[10848, 322, 114, 1, 136, "Subsection"],
|
|---|
| 813 | Cell[10965, 325, 230, 4, 164, "Text"],
|
|---|
| 814 | Cell[11198, 331, 166, 3, 108, "Input"]
|
|---|
| 815 | }, Open ]],
|
|---|
| 816 | Cell[CellGroupData[{
|
|---|
| 817 | Cell[11401, 339, 113, 1, 136, "Subsection"],
|
|---|
| 818 | Cell[11517, 342, 181, 4, 104, "Text"],
|
|---|
| 819 | Cell[11701, 348, 219, 4, 108, "Input"],
|
|---|
| 820 | Cell[11923, 354, 173, 4, 104, "Text"],
|
|---|
| 821 | Cell[12099, 360, 151, 3, 108, "Input"]
|
|---|
| 822 | }, Open ]]
|
|---|
| 823 | }, Closed]],
|
|---|
| 824 | Cell[CellGroupData[{
|
|---|
| 825 | Cell[12299, 369, 116, 1, 70, "Section"],
|
|---|
| 826 | Cell[12418, 372, 170, 4, 104, "Text"],
|
|---|
| 827 | Cell[12591, 378, 149, 3, 108, "Input"],
|
|---|
| 828 | Cell[CellGroupData[{
|
|---|
| 829 | Cell[12765, 385, 100, 1, 136, "Subsection"],
|
|---|
| 830 | Cell[12868, 388, 457, 10, 108, "Input"]
|
|---|
| 831 | }, Open ]],
|
|---|
| 832 | Cell[CellGroupData[{
|
|---|
| 833 | Cell[13362, 403, 76, 1, 136, "Subsection"],
|
|---|
| 834 | Cell[13441, 406, 258, 5, 108, "Input"]
|
|---|
| 835 | }, Open ]],
|
|---|
| 836 | Cell[CellGroupData[{
|
|---|
| 837 | Cell[13736, 416, 35, 0, 136, "Subsection"],
|
|---|
| 838 | Cell[13774, 418, 417, 7, 108, "Input"]
|
|---|
| 839 | }, Open ]],
|
|---|
| 840 | Cell[CellGroupData[{
|
|---|
| 841 | Cell[14228, 430, 35, 0, 136, "Subsection"],
|
|---|
| 842 | Cell[14266, 432, 360, 8, 108, "Input"]
|
|---|
| 843 | }, Open ]],
|
|---|
| 844 | Cell[CellGroupData[{
|
|---|
| 845 | Cell[14663, 445, 101, 1, 136, "Subsection"],
|
|---|
| 846 | Cell[14767, 448, 433, 9, 108, "Input"]
|
|---|
| 847 | }, Open ]]
|
|---|
| 848 | }, Closed]],
|
|---|
| 849 | Cell[CellGroupData[{
|
|---|
| 850 | Cell[15249, 463, 132, 2, 70, "Section"],
|
|---|
| 851 | Cell[CellGroupData[{
|
|---|
| 852 | Cell[15406, 469, 103, 1, 136, "Subsection"],
|
|---|
| 853 | Cell[15512, 472, 185, 2, 104, "Text"],
|
|---|
| 854 | Cell[15700, 476, 569, 11, 290, "Input"],
|
|---|
| 855 | Cell[16272, 489, 124, 1, 104, "Text"],
|
|---|
| 856 | Cell[16399, 492, 575, 13, 290, "Input"]
|
|---|
| 857 | }, Open ]],
|
|---|
| 858 | Cell[CellGroupData[{
|
|---|
| 859 | Cell[17011, 510, 103, 1, 136, "Subsection"],
|
|---|
| 860 | Cell[17117, 513, 183, 2, 104, "Text"],
|
|---|
| 861 | Cell[17303, 517, 474, 10, 230, "Input"]
|
|---|
| 862 | }, Open ]],
|
|---|
| 863 | Cell[CellGroupData[{
|
|---|
| 864 | Cell[17814, 532, 155, 2, 272, "Subsection"],
|
|---|
| 865 | Cell[17972, 536, 123, 1, 208, "Text"],
|
|---|
| 866 | Cell[18098, 539, 468, 12, 460, "Input"],
|
|---|
| 867 | Cell[18569, 553, 90, 1, 216, "Input"]
|
|---|
| 868 | }, Open ]],
|
|---|
| 869 | Cell[CellGroupData[{
|
|---|
| 870 | Cell[18696, 559, 206, 3, 272, "Subsection"],
|
|---|
| 871 | Cell[18905, 564, 172, 2, 208, "Text"],
|
|---|
| 872 | Cell[19080, 568, 514, 12, 460, "Input"],
|
|---|
| 873 | Cell[19597, 582, 90, 1, 216, "Input"]
|
|---|
| 874 | }, Open ]],
|
|---|
| 875 | Cell[CellGroupData[{
|
|---|
| 876 | Cell[19724, 588, 248, 3, 272, "Subsection"],
|
|---|
| 877 | Cell[19975, 593, 291, 8, 216, "Input"]
|
|---|
| 878 | }, Open ]]
|
|---|
| 879 | }, Closed]],
|
|---|
| 880 | Cell[CellGroupData[{
|
|---|
| 881 | Cell[20315, 607, 147, 2, 52, "Subsubtitle"],
|
|---|
| 882 | Cell[20465, 611, 248, 6, 54, "Input"],
|
|---|
| 883 | Cell[20716, 619, 749, 17, 115, "Input"],
|
|---|
| 884 | Cell[21468, 638, 189, 4, 54, "Input"],
|
|---|
| 885 | Cell[21660, 644, 118, 2, 54, "Input"],
|
|---|
| 886 | Cell[21781, 648, 415, 9, 145, "Input"],
|
|---|
| 887 | Cell[22199, 659, 847, 23, 145, "Input"],
|
|---|
| 888 | Cell[23049, 684, 276, 6, 54, "Input"],
|
|---|
| 889 | Cell[23328, 692, 246, 7, 85, "Input"],
|
|---|
| 890 | Cell[23577, 701, 321, 6, 85, "Input"]
|
|---|
| 891 | }, Open ]]
|
|---|
| 892 | }, Open ]]
|
|---|
| 893 | }
|
|---|
| 894 | ]
|
|---|
| 895 | *)
|
|---|
| 896 |
|
|---|
| 897 | (* End of internal cache information *)
|
|---|