VBFNLO - A parton level Monte Carlo for processes with electroweak bosons
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documentation:proclist [2012/07/23 10:24]
sophy 		documentation:proclist [2012/07/23 10:29]
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 +======= Process List =======
  
 +The complete list of implemented production processes and decay modes in VBFNLO is summarized in the following.
 +Except for gluon fusion, all processes are implemented in NLO QCD. For Higgs boson production plus two jets
 +the NLO electroweak corrections are also implemented.
 +All processes can be run in the Standard Model. Several processes also allow for Beyond the Standard Model Physics effects. These options are shown in the third column.
 +
 +Jump to:\\
 +[[documentation:proclist#Higgs boson production plus two jets via Vector Boson Fusion|Higgs boson production plus two jets via Vector Boson Fusion]] \\
 +[[documentation:proclist#Higgs boson production plus three jets via Vector Boson Fusion|Higgs boson production plus three jets via Vector Boson Fusion]] \\
 +[[documentation:proclist#Higgs boson production with a photon and two jets via Vector Boson Fusion|Higgs boson production with a photon and two jets via Vector Boson Fusion]]\\
 +[[documentation:proclist#Single vector boson production plus two jets via Vector Boson Fusion|Single vector boson production plus two jets via Vector Boson Fusion]]\\
 +[[documentation:proclist#VBF production of a spin-2 particle|VBF production of a spin-2 particle]]\\
 +[[documentation:proclist#Vector boson pair production plus two jets via Vector Boson Fusion|Vector boson pair production plus two jets via Vector Boson Fusion]]\\
 +[[documentation:proclist#Diboson production|Diboson production]]\\
 +[[documentation:proclist#Triple vector boson production|Triple vector boson production]]\\
 +[[documentation:proclist#Double vector boson production in association with a hadronic jet|Double vector boson production in association with a hadronic jet]]\\
 +[[documentation:proclist#Triple vector boson production in association with a hadronic jet|Triple vector boson production in association with a hadronic jet]]\\
 +[[documentation:proclist#Higgs boson production plus two jets via Gluon Fusion|Higgs boson production plus two jets via Gluon Fusion]]\\
 +[[documentation:proclist#Gluon-induced diboson production|Gluon-induced diboson production]]
 +
 +\\
 +
 +== Higgs boson production plus two jets via Vector Boson Fusion ==
 +
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 100    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj$     | anomalous HVV couplings, MSSM        |
 +| 101    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to \gamma\gamma \, jj$     | :::        |
 +| 102    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to \mu^+\mu^- \, jj$     | :::        |
 +| 103    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to \tau^+\tau^- \, jj$     | :::        |
 +| 104    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to b\bar{b} \, jj$     | :::        |
 +| 105    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to W^{+}W^{-} \, jj\to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^- 
 +\bar{\nu}_{\ell_{2}} \, jj$     | :::        |
 +| 106    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \ell_{2}^+ 
 +\ell_{2}^- \, jj$     | :::        |
 +| 107    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}}  
 +\bar{\nu}_{\ell_{2}} \, jj$     | :::        |
 +
 +\\
 +
 +== Higgs boson production plus three jets via Vector Boson Fusion ==
 +
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 110    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jjj$     | ---        |
 +| 111    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jjj\to \gamma\gamma \, jjj$     | :::        |
 +| 112    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jjj\to \mu^+\mu^- \, jjj$     | :::        |
 +| 113    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jjj\to \tau^+\tau^- \, jjj$     | :::        |
 +| 114    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jjj\to b\bar{b} \, jjj$     | :::        |
 +| 115    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jjj\to W^{+}W^{-} \, jj\to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^- 
 +\bar{\nu}_{\ell_{2}} \, jjj$     | :::        |
 +| 116    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jjj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \ell_{2}^+ 
 +\ell_{2}^- \, jjj$     | :::        |
 +| 117    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jjj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}}  
 +\bar{\nu}_{\ell_{2}} \, jjj$     | :::        |
 +
 +\\
 +
 +== Higgs boson production with a photon and two jets via Vector Boson Fusion ==
 +
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 2100    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \gamma \, jj$     | ---        |
 +| 2101    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \gamma \, jj\to \gamma\gamma \gamma \, jj$     | :::        |
 +| 2102    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \gamma \, jj\to \mu^+\mu^- \gamma \, jj$     | :::        |
 +| 2103    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \gamma \, jj\to \tau^+\tau^- \gamma \, jj$     | :::        |
 +| 2104    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \gamma \, jj\to b\bar{b} \gamma \, jj$     | :::        |
 +| 2105    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \gamma \, jj\to W^{+}W^{-} \gamma \, jj\to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^- \bar{\nu}_{\ell_{2}} \gamma \, jj$     | :::        |
 +| 2106    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \gamma \, jj\to ZZ \gamma \, jj\to \ell_{1}^+ \ell_{1}^- \ell_{2}^+ 
 +\ell_{2}^- \gamma \, jj$     | :::        |
 +| 2107    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \gamma \, jj\to ZZ \gamma \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}}  
 +\bar{\nu}_{\ell_{2}} \gamma \, jj$     | :::        |
 +
 +\\
 +
 +== Single vector boson production plus two jets via Vector Boson Fusion ==
 +
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 120    | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z \, jj \to \ell^{+} \ell^{-} \, jj$     | Anomalous VVV couplings        |
 +| 121    | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z  \, jj\to \nu_\ell \bar{\nu}_\ell \, jj$     | :::        |
 +| 130    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+} \,  jj\to \ell^{+} \nu_\ell \, jj$     | :::        |
 +| 140    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-} \, jj\to \ell^{-} \bar{\nu}_\ell  \, jj$     | :::        |
 +| 150    | $p \overset{\mbox{\tiny{(--)}}}{p} \to \gamma \, jj$     | :::        |
 +
 +\\
 +
 +== VBF production of a spin-2 particle ==
 +
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 191    | $p \overset{\mbox{\tiny{(--)}}}{p} \to S_{2} \, jj\to \gamma\gamma \, jj$     | only spin-2 resonant production        |
 +
 +
 +\\
 +
 +== Vector boson pair production plus two jets via Vector Boson Fusion ==
 +
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 200    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-} \, jj \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} \, jj$     | anomalous couplings, Kaluza-Klein models, spin-2 models        |
 +| 210    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZ  \, jj\to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \ell_{2}^{-} \, jj$ |Kaluza-Klein models, spin-2 models        |
 +| 211    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZ  \, jj\to \ell_{1}^{+} \ell_{1}^{-} \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \, jj$     | :::        |
 +| 220    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}Z \,  jj\to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{+} \ell_{2}^{-} \, jj$     | :::        |
 +| 230    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}Z \, jj\to \ell_{1}^{-} \bar{\nu}_{\ell _{1}} \ell_{2}^{+} \ell_{2}^{-} \, jj$     | :::        |
 +| 250    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{+} \, jj\to \ell_{1}^{+} \nu_{\ell _{1}} \ell_{2}^{+} \nu_{\ell_{2}} \, jj$     | ---        |
 +| 260    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}W^{-} \, jj\to \ell_{1}^{-} \bar{\nu}_{\ell _{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} \, jj$     | :::        |
 +
 +
 +\\
 +
 +== Diboson production ==
 +
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 300    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-} \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{-}\bar{\nu}_{\ell_{2}}$     | Anomalous HVV and VVV couplings        |
 +| 310    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}Z \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{+}\ell_{2}^{-}$     | Anomalous VVV couplings        |
 +| 320    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}Z \to \ell_{1}^{-} \bar{\nu}_{\ell_{1}} \ell_{2}^{+}\ell_{2}^{-}$     | :::       |
 +| 330    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZ \to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+}\ell_{2}^{-}$     | Anomalous HVV couplings        |
 +| 340    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}\gamma \to \ell_{1}^{+} \nu_{\ell_{1}} \gamma$     | Anomalous VVV couplings        |
 +| 350    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}\gamma \to \ell_{1}^{-} \bar{\nu}_{\ell_{1}} \gamma$     | :::       |
 +| 360    | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z\gamma \to \ell_{1}^{+} \ell_{1}^{-} \gamma$     | Anomalous HVV couplings        |
 +| 370    | $p \overset{\mbox{\tiny{(--)}}}{p} \to \gamma\gamma $     | :::        |
 +
 +\\
 +
 +== Triple vector boson production ==
 +
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 400    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-}Z \to \ell_{1}^{+}\nu_{\ell_{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} {\ell_3}^{+} {\ell_3}^{-}$     | anomalous couplings, Kaluza-Klein models        |
 +| 410    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZW^{+} \to  \ell_{1}^{+} \ell_{1}^{-}  \ell_{2}^{+} \ell_{2}^{-} 
 + {\ell_3}^{+} \nu_{\ell_3}$     | :::        |
 +| 420    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZW^{-} \to \ell_{1}^{+} \ell_{1}^{-}  \ell_{2}^{+} \ell_{2}^{-} 
 + {\ell_3}^{-}  \bar{\nu}_{\ell_3}$     | :::        |
 +| 430    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-}W^{+} \to \ell_{1}^{+}\nu_{\ell_1} \ell_{2}^{-}
 +\bar{\nu}_{\ell_2} {\ell_3}^{+}\nu_{\ell_3}$     | :::        |
 +| 440    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}W^{+}W^{-} \to \ell_{1}^{-} \bar{\nu}_{\ell_1}\ell_{2}^{+}\nu_{\ell_2}
 +{\ell_3}^{-} \bar{\nu}_{\ell_3}$     | :::        |
 +| 450    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZZ \to \ell_{1}^{-} \ell_{1}^{+} \ell_{2}^{-}
 +\ell_{2}^{+} {\ell_3}^{-} {\ell_3}^{+}$     | ---        |
 +| 460    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}W^{+} \gamma \to \ell_{1}^{-} \bar{\nu}_{\ell_1}
 +\ell_{2}^{+}\nu_{\ell_2} \gamma$     | :::        |
 +| 470    | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z Z \gamma \to \ell_{1}^{-} \ell_{1}^{+} \ell_{2}^{-}
 +\ell_{2}^{+} \gamma$     | :::        |
 +| 480    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+} Z \gamma \to \ell_{1}^{+}\nu_{\ell_1} \ell_{2}^{-}
 +\ell_{2}^{+} \gamma$     | :::        |
 +| 490    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-} Z \gamma \to \ell_{1}^{-} \bar{\nu}_{\ell_1} \ell_{2}^{-}
 +\ell_{2}^{+} \gamma$     | :::        |
 +| 500    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+} \gamma \gamma \to {\ell}^{+}\nu_{\ell} 
 +\gamma \gamma$     | :::        |
 +| 510    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-} \gamma \gamma \to {\ell}^{-} \bar{\nu}_{\ell} 
 +\gamma \gamma$     | :::        |
 +| 520    | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z \gamma \gamma \to {\ell}^{-} {\ell}^{+} 
 +\gamma \gamma$     | :::        |
 +| 521    | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z \gamma \gamma \to \nu_{\ell} \bar{\nu}_{\ell} 
 +\gamma \gamma$     | :::        |
 +| 530    | $p \overset{\mbox{\tiny{(--)}}}{p} \to \gamma \gamma \gamma$     | :::        |
 +
 +\\
 +
 +== Double vector boson production in association with a hadronic jet ==
 +
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 610    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to W^{-} \gamma j \to \ell^{-} \bar \nu_{\ell} \gamma j$     | anomalous couplings        |
 +| 620    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to W^{+} \gamma j  \to \ell^{+} \nu_{\ell} \gamma j$     | :::        |
 +| 630    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to W^{-} Z j \to \ell_{1}^{-} \bar \nu_{\ell_1} \ell_{2}^{-} \ell_{2}^{+} j$     | :::        |
 +| 640    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to W^{+} Z j \to  \ell_{1}^{+}\nu_{\ell_1} \ell_{2}^{-}\ell_{2}^{+}j$     | :::        |
 +
 +\\
 +
 +== Triple vector boson production in association with a hadronic jet ==
 +
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 800    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to W^{+} \gamma \gamma j  \to \ell^{+} \nu_{\ell} \gamma \gamma j$     | ---      | 
 +| 810    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to W^{-} \gamma \gamma j \to \ell^{-} \bar \nu_{\ell} \gamma \gamma j$     |     :::        |
 +
 +\\
 +
 +== Higgs boson production plus two jets via Gluon Fusion ==
 +
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 4100    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj$     | MSSM, general 2HDM        |
 +| 4101    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to \gamma\gamma \, jj$     | MSSM        |
 +| 4102    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to \mu^+\mu^- \, jj$     | :::        |
 +| 4103    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to \tau^+\tau^- \, jj$     | :::        |
 +| 4104    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to b\bar{b} \, jj$     | :::        |
 +| 4105    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to W^{+}W^{-} \, jj\to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^- 
 +\bar{\nu}_{\ell_{2}} \, jj$     | :::        |
 +| 4106    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \ell_{2}^+ 
 +\ell_{2}^- \, jj$     | :::        |
 +| 4107    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}}  
 +\bar{\nu}_{\ell_{2}} \, jj$     | :::        |
 +
 +
 +\\
 +
 +== Gluon-induced diboson production ==
 +
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 4300    | $gg \to W^{+}W^{-} \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{-}\bar{\nu}_{\ell_{2}}$     | Anomalous HVV couplings        |
 +| 4330    | $gg \to ZZ \to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+}\ell_{2}^{-}$     | :::      |
 +| 4360    | $gg \to Z\gamma \to \ell_{1}^{+} \ell_{1}^{-} \gamma$     | :::        |
 +| 4370    | $gg \to \gamma\gamma $     | :::        |
 +
 +
 +\\