VBFNLO - A parton level Monte Carlo for processes with electroweak bosons
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documentation:proclist [2012/07/23 10:29]
sophy 		documentation:proclist [2015/08/05 15:04]
Michael Rauch update
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 The complete list of implemented production processes and decay modes in VBFNLO is summarized in the following. 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 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.+without Higgs decay 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. 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.
  
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 [[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#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#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 two Higgs bosons and two jets|VBF production of two Higgs bosons and two jets]]\\
 [[documentation:proclist#VBF production of a spin-2 particle|VBF production of a spin-2 particle]]\\ [[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#Vector boson pair production plus two jets via Vector Boson Fusion|Vector boson pair production plus two jets via Vector Boson Fusion]]\\
Line 17: Line 18:
 [[documentation:proclist#Double vector boson production in association with a hadronic jet|Double vector boson production in association with a hadronic jet]]\\ [[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#Triple vector boson production in association with a hadronic jet|Triple vector boson production in association with a hadronic jet]]\\
 +[[documentation:proclist#WH production|WH production]]\\
 +[[documentation:proclist#W production|W production]]\\
 +[[documentation:proclist#WH production in association with a hadronic jet|WH production in association with a hadronic jet]]\\
 +[[documentation:proclist#W production in association with a hadronic jet|W production in association with a hadronic jet]]\\
 +[[documentation:proclist#QCD induced production of a vector boson in association with two jets|QCD induced production of a vector boson in association with two jets]]\\
 +[[documentation:proclist#QCD induced diboson production in association with two jets|QCD induced diboson production in association with two jets]]\\
 [[documentation:proclist#Higgs boson production plus two jets via Gluon Fusion|Higgs boson production plus two jets via Gluon Fusion]]\\ [[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]]+[[documentation:proclist#Gluon-induced diboson production|Gluon-induced diboson production]]\\ 
 +[[documentation:proclist#Gluon-induced diboson production in association with a hadronic jet|Gluon-induced diboson production in association with a hadronic jet]]
  
 \\ \\
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 == Higgs boson production plus two jets via Vector Boson Fusion == == Higgs boson production plus two jets via Vector Boson Fusion ==
  
 +Processes with fully leptonic decays:
 +
 +|< 100% 12% 53% 35%>|
 ^ Process ID     ^ Process       ^ BSM Options          ^ ^ Process ID     ^ Process       ^ BSM Options          ^
 | 100    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj$     | anomalous HVV couplings, MSSM        | | 100    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj$     | anomalous HVV couplings, MSSM        |
Line 36: Line 47:
 | 107    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}}   | 107    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}}  
 \bar{\nu}_{\ell_{2}} \, jj$     | :::        | \bar{\nu}_{\ell_{2}} \, jj$     | :::        |
 +
 +Processes with semi-leptonic decays:
 +
 +|< 100% 12% 53% 35%>|
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 108    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to W^{+}W^{-} \, jj\to q\bar{q} \, \ell^- 
 +\bar{\nu}_{\ell} \,jj$     | anomalous HVV couplings, MSSM        |
 +| 109    |$p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to W^{+}W^{-} \, jj\to \ell^+\nu_{\ell} \,
 +q\bar{q}  \,jj$     | :::        |
 +| 1010    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to ZZ \, jj\to q\bar{q} \, \ell^+ \ell^- \,jj$     | :::        |
  
 \\ \\
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 == Higgs boson production plus three jets via Vector Boson Fusion == == Higgs boson production plus three jets via Vector Boson Fusion ==
  
 +|< 100% 12% 53% 35%>|
 ^ Process ID     ^ Process       ^ BSM Options          ^ ^ Process ID     ^ Process       ^ BSM Options          ^
 | 110    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jjj$     | ---        | | 110    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jjj$     | ---        |
Line 58: Line 80:
 == 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 ==
  
 +|< 100% 12% 53% 35%>|
 ^ Process ID     ^ Process       ^ BSM Options          ^ ^ Process ID     ^ Process       ^ BSM Options          ^
 | 2100    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \gamma \, jj$     | ---        | | 2100    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \gamma \, jj$     | ---        |
Line 74: Line 97:
 == Single vector boson production plus two jets via Vector Boson Fusion == == Single vector boson production plus two jets via Vector Boson Fusion ==
  
 +|< 100% 12% 53% 35%>|
 ^ Process ID     ^ Process       ^ BSM Options          ^ ^ Process ID     ^ Process       ^ BSM Options          ^
-| 120    | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z \, jj \to \ell^{+} \ell^{-} \, jj$     | Anomalous VVV couplings        |+| 120    | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z \, jj \to \ell^{+} \ell^{-} \, jj$     | Anomalous gauge couplings        |
 | 121    | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z  \, jj\to \nu_\ell \bar{\nu}_\ell \, jj$     | :::        | | 121    | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z  \, jj\to \nu_\ell \bar{\nu}_\ell \, jj$     | :::        |
 | 130    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+} \,  jj\to \ell^{+} \nu_\ell \, jj$     | :::        | | 130    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+} \,  jj\to \ell^{+} \nu_\ell \, jj$     | :::        |
 | 140    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-} \, jj\to \ell^{-} \bar{\nu}_\ell  \, jj$     | :::        | | 140    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-} \, jj\to \ell^{-} \bar{\nu}_\ell  \, jj$     | :::        |
 | 150    | $p \overset{\mbox{\tiny{(--)}}}{p} \to \gamma \, jj$     | :::        | | 150    | $p \overset{\mbox{\tiny{(--)}}}{p} \to \gamma \, jj$     | :::        |
 +
 +\\
 +
 +== VBF production of two Higgs bosons and two jets ==
 +
 +|< 100% 12% 53% 35%>|
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 160    | $p \overset{\mbox{\tiny{(--)}}}{p} \to HH \,  jj$ | ---        |
 +| 161    | $p \overset{\mbox{\tiny{(--)}}}{p} \to HH \,  jj \to b\bar{b}\tau^+\tau^- \, jj$ | :::        |
 +| 162    | $p \overset{\mbox{\tiny{(--)}}}{p} \to HH \,  jj \to b\bar{b}\gamma\gamma \, jj$ | :::        |
  
 \\ \\
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 == VBF production of a spin-2 particle == == VBF production of a spin-2 particle ==
  
 +|< 100% 12% 53% 35%>|
 ^ Process ID     ^ Process       ^ BSM Options          ^ ^ Process ID     ^ Process       ^ BSM Options          ^
-| 191    | $p \overset{\mbox{\tiny{(--)}}}{p} \to S_{2} \, jj\to \gamma\gamma \, jj$     | only spin-2 resonant production        |+| 191    | $p \overset{\mbox{\tiny{(--)}}}{p} \to S_{2} \, jj\to \gamma\gamma \, jj$     | spin-2 resonant production        | 
 +| 195    | $p \overset{\mbox{\tiny{(--)}}}{p} \to S_{2}  \, jj\to W^{+}W^{-} \, jj\to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^-  
 +\bar{\nu}_{\ell_{2}} \,jj$      | :::  | 
 +| 196    | $p \overset{\mbox{\tiny{(--)}}}{p} \to S_{2}  \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \ell_{2}^+  
 +\ell_{2}^- \,jj$     | :::  | 
 +| 197    | $p \overset{\mbox{\tiny{(--)}}}{p} \to S_{2}  \, jj\to  ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}}   
 +\bar{\nu}_{\ell_{2}} \,jj$     | :::  |
  
  
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 == Vector boson pair production plus two jets via Vector Boson Fusion == == Vector boson pair production plus two jets via Vector Boson Fusion ==
  
 +Processes with fully leptonic decays:
 +
 +|< 100% 12% 53% 35%>|
 ^ Process ID     ^ Process       ^ BSM Options          ^ ^ 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        | +| 200    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-} \, jj \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} \, jj$     | anomalous gauge couplings, two-Higgs model, 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        |+| 210    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZ  \, jj\to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \ell_{2}^{-} \, jj$ | :::    |
 | 211    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZ  \, jj\to \ell_{1}^{+} \ell_{1}^{-} \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \, jj$     | :::        | | 211    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZ  \, jj\to \ell_{1}^{+} \ell_{1}^{-} \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \, jj$     | :::        |
 | 220    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}Z \,  jj\to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{+} \ell_{2}^{-} \, jj$     | :::        | | 220    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}Z \,  jj\to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{+} \ell_{2}^{-} \, jj$     | :::        |
 | 230    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}Z \, jj\to \ell_{1}^{-} \bar{\nu}_{\ell _{1}} \ell_{2}^{+} \ell_{2}^{-} \, jj$     | :::        | | 230    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}Z \, jj\to \ell_{1}^{-} \bar{\nu}_{\ell _{1}} \ell_{2}^{+} \ell_{2}^{-} \, jj$     | :::        |
-| 250    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{+} \, jj\to \ell_{1}^{+} \nu_{\ell _{1}} \ell_{2}^{+} \nu_{\ell_{2}} \, jj$     | ---        |+| 250    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{+} \, jj\to \ell_{1}^{+} \nu_{\ell _{1}} \ell_{2}^{+} \nu_{\ell_{2}} \, jj$     | anomalous gauge couplings, two-Higgs model  |
 | 260    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}W^{-} \, jj\to \ell_{1}^{-} \bar{\nu}_{\ell _{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} \, jj$     | :::        | | 260    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}W^{-} \, jj\to \ell_{1}^{-} \bar{\nu}_{\ell _{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} \, jj$     | :::        |
 +| 270    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}\gamma \, jj\to \ell^{+} \nu_{\ell} \gamma \, jj$     | anomalous gauge couplings  |
 +| 280    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}\gamma \, jj\to \ell^{-} \bar{\nu}_{\ell} \gamma \, jj$     | :::        |
 +| 290    | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z\gamma \, jj\to \ell^{+} \ell^{-} \gamma \, jj$ | :::        |
 +| 291    | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z\gamma \, jj\to \nu_{\ell}\bar{\nu}_{\ell} \gamma \, jj$ | :::        |
  
 +Processes with semi-leptonic decays:
 +
 +|< 100% 12% 53% 35%>|
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 201    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-} \, jj \to q \bar{q} \, \ell^{-}
 +\bar{\nu}_{\ell} \, jj$     | anomalous gauge couplings, two-Higgs model   |
 +| 202    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-}  \, jj\to \ell^{+} \nu_\ell \, q \bar{q} \, jj$ | :::    |
 +| 212    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZ  \, jj\to q \bar{q} \, \ell^{+} \ell^{-} \, jj$ | :::    |
 +| 221    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}Z \,  jj\to q \bar{q} \, \ell^{+} \ell^{-} \, jj$ | :::    |
 +| 222    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}Z \,  jj\to \ell^{+} \nu_{\ell} \, q \bar{q} \, jj$ | :::    |
 +| 231    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}Z \, jj\to q \bar{q} \, \ell^{+} \ell^{-} \, jj$ | :::    |
 +| 232    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}Z \, jj\to \ell^{-} \bar{\nu}_{\ell} \, q \bar{q} \, jj$ | :::    |
 +| 251    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{+} \,  jj\to q \bar{q} \, \ell^{+} \nu_{\ell} \, jj$ | :::    |
 +| 261    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}W^{-} \,  jj\to q \bar{q} \, \ell^{-} \bar{\nu}_{\ell} \, jj$ | :::    |
  
 \\ \\
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 == Diboson production == == Diboson production ==
  
 +Processes with fully leptonic decays:
 +
 +|< 100% 12% 53% 35%>|
 ^ Process ID     ^ Process       ^ BSM Options          ^ ^ 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        | +| 300    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-} \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{-}\bar{\nu}_{\ell_{2}}$     | anomalous HVV and gauge couplings        | 
-| 310    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}Z \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{+}\ell_{2}^{-}$     | Anomalous VVV couplings        |+| 310    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}Z \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{+}\ell_{2}^{-}$     | anomalous gauge couplings        |
 | 320    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}Z \to \ell_{1}^{-} \bar{\nu}_{\ell_{1}} \ell_{2}^{+}\ell_{2}^{-}$     | :::       | | 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        | +| 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        |+| 340    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}\gamma \to \ell_{1}^{+} \nu_{\ell_{1}} \gamma$     | anomalous gauge couplings        |
 | 350    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}\gamma \to \ell_{1}^{-} \bar{\nu}_{\ell_{1}} \gamma$     | :::       | | 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        |+| 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 $     | :::        | | 370    | $p \overset{\mbox{\tiny{(--)}}}{p} \to \gamma\gamma $     | :::        |
 +
 +Processes with semi-leptonic decays:
 +
 +|< 100% 12% 53% 35%>|
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 301    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-} \to q \bar{q} \, \ell^{-}\bar{\nu}_{\ell} $ | anomalous HVV and gauge couplings |
 +| 302    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-} \to \ell^{+} \nu_{\ell} \, q \bar{q} $ | :::       |
 +| 312    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}Z \to  q \bar{q} \, \ell^{+} \ell^{-} $ | anomalous gauge couplings         |
 +| 313    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}Z \to  \ell^{+} \nu_{\ell} \, q \bar{q}$ | :::       |
 +| 322    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}Z \to q \bar{q} \, \ell^{+} \ell^{-}$ | :::       |
 +| 323    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}Z \to \ell^{-} \bar{\nu}_{\ell} \, q \bar{q}$ | :::       |
 +| 331    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZ \to q \bar{q} \, \ell^{-} \ell^{+}$ | anomalous HVV couplings        |
  
 \\ \\
Line 121: Line 198:
 == Triple vector boson production == == Triple vector boson production ==
  
 +Processes with fully leptonic decays:
 +
 +|< 100% 12% 53% 35%>|
 ^ Process ID     ^ Process       ^ BSM Options          ^ ^ 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        |+| 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 gauge couplings, Kaluza-Klein models        |
 | 410    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZW^{+} \to  \ell_{1}^{+} \ell_{1}^{-}  \ell_{2}^{+} \ell_{2}^{-}  | 410    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZW^{+} \to  \ell_{1}^{+} \ell_{1}^{-}  \ell_{2}^{+} \ell_{2}^{-} 
  {\ell_3}^{+} \nu_{\ell_3}$     | :::        |  {\ell_3}^{+} \nu_{\ell_3}$     | :::        |
Line 132: Line 212:
 {\ell_3}^{-} \bar{\nu}_{\ell_3}$     | :::        | {\ell_3}^{-} \bar{\nu}_{\ell_3}$     | :::        |
 | 450    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZZ \to \ell_{1}^{-} \ell_{1}^{+} \ell_{2}^{-} | 450    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZZ \to \ell_{1}^{-} \ell_{1}^{+} \ell_{2}^{-}
-\ell_{2}^{+} {\ell_3}^{-} {\ell_3}^{+}$     | ---        |+\ell_{2}^{+} {\ell_3}^{-} {\ell_3}^{+}$     | anomalous gauge couplings        |
 | 460    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}W^{+} \gamma \to \ell_{1}^{-} \bar{\nu}_{\ell_1} | 460    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}W^{+} \gamma \to \ell_{1}^{-} \bar{\nu}_{\ell_1}
 \ell_{2}^{+}\nu_{\ell_2} \gamma$     | :::        | \ell_{2}^{+}\nu_{\ell_2} \gamma$     | :::        |
Line 150: Line 230:
 \gamma \gamma$     | :::        | \gamma \gamma$     | :::        |
 | 530    | $p \overset{\mbox{\tiny{(--)}}}{p} \to \gamma \gamma \gamma$     | :::        | | 530    | $p \overset{\mbox{\tiny{(--)}}}{p} \to \gamma \gamma \gamma$     | :::        |
 +
 +Processes with semi-leptonic decays:
 +
 +|< 100% 12% 53% 35%>|
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 401    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-}Z \to q \bar{q} \, \ell_{1}^{-} \bar{\nu}_{\ell_{1}} 
 +\ell_{2}^{+} \ell_{2}^{-} $ | anomalous gauge couplings |
 +| 402    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-}Z \to \ell_{1}^{+}\nu_{\ell_{1}} \, q \bar{q} \,
 +\ell_{2}^{+} \ell_{2}^{-} $ | ::: |
 +| 403    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-}Z \to \ell_{1}^{+}\nu_{\ell_{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} \,
 +q \bar{q} $ | ::: |
 +| 411    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZW^{+} \to  \ell_{1}^{+} \ell_{1}^{-}  \ell_{2}^{+} \ell_{2}^{-} 
 + \, q \bar{q} $  | ::: |
 +| 412    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZW^{+} \to  q \bar{q} \, \ell_{1}^{+} \ell_{1}^{-}
 + \ell_{2}^{+} \nu_{\ell_{2}} $ | ::: |
 +| 421    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZW^{-} \to \ell_{1}^{+} \ell_{1}^{-}  \ell_{2}^{+} \ell_{2}^{-} 
 + \, q \bar{q} $ | ::: |
 +| 422    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZW^{-} \to q \bar{q} \, \ell_{1}^{+} \ell_{1}^{-}
 + \ell_{2}^{-}  \bar{\nu}_{\ell_{2}}$ | ::: |
 +| 431    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-}W^{+} \to  q \bar{q} \, \ell_{1}^{-}
 +\bar{\nu}_{\ell_1} \ell_{2}^{+}\nu_{\ell_{2}}$ | ::: |
 +| 432    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-}W^{+} \to \ell_{1}^{+}\nu_{\ell_1} \, q \bar{q} \,
 + \ell_{2}^{+}\nu_{\ell_{2}}$ | ::: |
 +| 441    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}W^{+}W^{-} \to \ell_{1}^{-} \bar{\nu}_{\ell_1} \, q \bar{q} \,
 +\ell_{2}^{-} \bar{\nu}_{\ell_{2}} $  | ::: |
 +| 442    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}W^{+}W^{-} \to  q \bar{q} \, \ell_{1}^{+}\nu_{\ell_1}
 +\ell_{2}^{-} \bar{\nu}_{\ell_{2}} $ | ::: |
 +| 451    | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZZ \to  q \bar{q} \, \ell_{1}^{-} \ell_{1}^{+} \ell_{2}^{-}
 +\ell_{2}^{+}  $ | ::: |
 +| 461    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-} \gamma \to  q \bar{q} \,
 +\ell^{-}\bar{\nu}_{\ell} \gamma$ | ::: |
 +| 462    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-} \gamma \to \ell^{+} \nu_{\ell}
 +\, q \bar{q} \, \gamma$ | ::: |
 +| 471    | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z Z \gamma \to \ell^{-} \ell^{+} \, q \bar{q} \, \gamma$ | ::: |
 +| 481    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+} Z \gamma \to  q \bar{q} \, \ell^{-}
 +\ell^{+} \gamma$ | ::: |
 +| 482    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+} Z \gamma \to \ell^{+}\nu_{\ell} \, q \bar{q} \, \gamma$ | ::: |
 +| 491    |$p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-} Z \gamma \to  q \bar{q} \, \ell^{-}
 +\ell^{+} \gamma$  | ::: |
 +| 492    | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-} Z \gamma \to \ell^{-} \bar{\nu}_{\ell} \, q \bar{q} \, \gamma$ | ::: |
 +
  
 \\ \\
Line 155: Line 276:
 == Double vector boson production in association with a hadronic jet == == Double vector boson production in association with a hadronic jet ==
  
 +|< 100% 12% 53% 35%>|
 ^ Process ID     ^ Process       ^ BSM Options          ^ ^ Process ID     ^ Process       ^ BSM Options          ^
-| 610    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to W^{-} \gamma j \to \ell^{-} \bar \nu_{\ell} \gamma j$     | anomalous couplings        |+| 600    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to W^{+} W^{-} j \to \ell_{1}^{+}\nu_{\ell_1} \ell_{2}^{-} \bar{\nu}_{\ell_2} j $ | anomalous HVV couplings        | 
 +| 610    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to W^{-} \gamma j \to \ell^{-} \bar \nu_{\ell} \gamma j$     | anomalous gauge couplings        |
 | 620    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to W^{+} \gamma j  \to \ell^{+} \nu_{\ell} \gamma j$     | :::        | | 620    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to W^{+} \gamma j  \to \ell^{+} \nu_{\ell} \gamma j$     | :::        |
 | 630    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to W^{-} Z j \to \ell_{1}^{-} \bar \nu_{\ell_1} \ell_{2}^{-} \ell_{2}^{+} j$     | :::        | | 630    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to W^{-} Z j \to \ell_{1}^{-} \bar \nu_{\ell_1} \ell_{2}^{-} \ell_{2}^{+} j$     | :::        |
 | 640    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to W^{+} Z j \to  \ell_{1}^{+}\nu_{\ell_1} \ell_{2}^{-}\ell_{2}^{+}j$     | :::        | | 640    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to W^{+} Z j \to  \ell_{1}^{+}\nu_{\ell_1} \ell_{2}^{-}\ell_{2}^{+}j$     | :::        |
 +| 650    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to Z Z j \to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \ell_{2}^{-} j $ | anomalous HVV couplings        |
  
 \\ \\
Line 165: Line 289:
 == Triple vector boson production in association with a hadronic jet == == Triple vector boson production in association with a hadronic jet ==
  
 +|< 100% 12% 53% 35%>|
 ^ Process ID     ^ Process       ^ BSM Options          ^ ^ Process ID     ^ Process       ^ BSM Options          ^
-| 800    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to W^{+} \gamma \gamma j  \to \ell^{+} \nu_{\ell} \gamma \gamma j$     | ---      | +| 800    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to W^{+} \gamma \gamma j  \to \ell^{+} \nu_{\ell} \gamma \gamma j$     | anomalous gauge couplings      | 
 | 810    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to W^{-} \gamma \gamma j \to \ell^{-} \bar \nu_{\ell} \gamma \gamma j$     |     :::        | | 810    | $p \overset{\mbox{\tiny{(--)}}}{p}  \to W^{-} \gamma \gamma j \to \ell^{-} \bar \nu_{\ell} \gamma \gamma j$     |     :::        |
  
 \\ \\
 +
 +
 +== WH production ==
 +
 +|< 100% 12% 53% 35%>|
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 1300 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^+ H \to \ell^+\nu_{\ell} H $ | anomalous gauge couplings |
 +| 1301 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^+ H \to \ell^+\nu_{\ell} \gamma\gamma $ | ::: |
 +| 1302 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^+ H \to \ell^+\nu_{\ell} \mu^+\mu^- $ | ::: |
 +| 1303 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^+ H \to \ell^+\nu_{\ell} \tau^+\tau^- $ | ::: |
 +| 1304 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^+ H \to \ell^+\nu_{\ell} b\bar{b} $ | ::: |
 +| 1305 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^+ H \to W^+ W^{+}W^{-} \to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^+\nu_{\ell_{2}} \ell_{3}^- \bar{\nu}_{\ell_{3}}$ | ::: |
 +| 1306 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^+ H \to W^+ ZZ \to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \ell_{3}^+ \ell_{3}^-$ | ::: |
 +| 1307 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^+ H \to W^+ ZZ \to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \nu_{\ell_{3}}  \bar{\nu}_{\ell_{3}}$ | ::: |
 +| 1310 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^- H \to \ell^- \bar{\nu}_{\ell} H $ | ::: |
 +| 1311 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^- H \to \ell^- \bar{\nu}_{\ell} \gamma\gamma $ | ::: |
 +| 1312 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^- H \to \ell^- \bar{\nu}_{\ell} \mu^+\mu^- $ | ::: |
 +| 1313 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^- H \to \ell^- \bar{\nu}_{\ell} \tau^+\tau^- $ | ::: |
 +| 1314 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^- H \to \ell^- \bar{\nu}_{\ell} b\bar{b} $ | ::: |
 +| 1315 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^- H \to W^- W^{+}W^{-} \to \ell_{1}^-\bar{\nu}_{\ell_{1}} \ell_{2}^+\nu_{\ell_{2}} \ell_{3}^- \bar{\nu}_{\ell_{3}}$ | ::: |
 +| 1316 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^- H \to W^- ZZ \to \ell_{1}^-\bar{\nu}_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \ell_{3}^+ \ell_{3}^-$ | ::: |
 +| 1317 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^- H \to W^- ZZ \to \ell_{1}^-\bar{\nu}_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \nu_{\ell_{3}}  \bar{\nu}_{\ell_{3}}$ | ::: |
 +
 +\\
 +
 +
 +== W production ==
 +
 +|< 100% 12% 53% 35%>|
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 1330 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^+ \to \ell^+\nu_{\ell} $  | --- |
 +| 1340 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^- \to \ell^- \bar{\nu}_{\ell} $ | ::: |
 +
 +\\
 +
 +
 +== WH production in association with a hadronic jet ==
 +
 +|< 100% 12% 53% 35%>|
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 1600 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^+ H \, j \to \ell^+\nu_{\ell} H \, j $ | anomalous gauge couplings |
 +| 1601 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^+ H \, j \to \ell^+\nu_{\ell} \gamma\gamma \, j $ | ::: |
 +| 1602 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^+ H \, j \to \ell^+\nu_{\ell} \mu^+\mu^- \, j $ | ::: |
 +| 1603 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^+ H \, j \to \ell^+\nu_{\ell} \tau^+\tau^- \, j $ | ::: |
 +| 1604 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^+ H \, j \to \ell^+\nu_{\ell} b\bar{b} \, j $ | ::: |
 +| 1605 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^+ H \, j \to W^+ W^{+}W^{-} \, j \to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^+\nu_{\ell_{2}} \ell_{3}^- \bar{\nu}_{\ell_{3}}\, j $ | ::: |
 +| 1606 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^+ H \, j \to W^+ ZZ \, j \to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \ell_{3}^+ \ell_{3}^-\, j $ | ::: |
 +| 1607 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^+ H \, j \to W^+ ZZ \, j \to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \nu_{\ell_{3}}  \bar{\nu}_{\ell_{3}}\, j $ | ::: |
 +| 1610 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^- H \, j \to \ell^- \bar{\nu}_{\ell} H \, j $ | ::: |
 +| 1611 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^- H \, j \to \ell^- \bar{\nu}_{\ell} \gamma\gamma \, j $ | ::: |
 +| 1612 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^- H \, j \to \ell^- \bar{\nu}_{\ell} \mu^+\mu^- \, j $ | ::: |
 +| 1613 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^- H \, j \to \ell^- \bar{\nu}_{\ell} \tau^+\tau^- \, j $ | ::: |
 +| 1614 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^- H \, j \to \ell^- \bar{\nu}_{\ell} b\bar{b} \, j $ | ::: |
 +| 1615 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^- H \, j \to W^- W^{+}W^{-} \, j \to \ell_{1}^-\bar{\nu}_{\ell_{1}} \ell_{2}^+\nu_{\ell_{2}} \ell_{3}^- \bar{\nu}_{\ell_{3}}\, j $ | ::: |
 +| 1616 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^- H \, j \to W^- ZZ \, j \to \ell_{1}^-\bar{\nu}_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \ell_{3}^+ \ell_{3}^-\, j $ | ::: |
 +| 1617 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^- H \, j \to W^- ZZ \, j \to \ell_{1}^-\bar{\nu}_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \nu_{\ell_{3}}  \bar{\nu}_{\ell_{3}}\, j $ | ::: |
 +
 +\\
 +
 +
 +== W production in association with a hadronic jet ==
 +
 +|< 100% 12% 53% 35%>|
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 1630 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^+ \, j \to \ell^+\nu_{\ell} \, j $  | --- |
 +| 1640 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^- \, j\to \ell^- \bar{\nu}_{\ell} \, j $ | ::: |
 +
 +\\
 +
 +
 +== QCD induced production of a vector boson in association with two jets ==
 +
 +|< 100% 12% 53% 35%>|
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 3120 | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z \,  jj\to \ell^{+} \ell^{-} \, jj$  | --- |
 +| 3121 | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z \,  jj\to \nu_{\ell} \bar{\nu}_{\ell} \, jj$ | ::: |
 +| 3130 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+} \,  jj\to \ell^{+} \nu_\ell \, jj$ | ::: |
 +| 3140 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-} \, jj\to \ell^{-} \bar{\nu}_\ell  \, jj$| ::: |
 +
 +\\
 +
 +
 +== QCD induced diboson production in association with two jets ==
 +
 +|< 100% 12% 53% 35%>|
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 3210 | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZ \,  jj\to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \ell_{2}^{-} \, jj$   | --- |
 +| 3211 | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZ \,  jj\to \ell_{1}^{+} \ell_{1}^{-} \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \, jj$  | ::: |
 +| 3220 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}Z \,  jj\to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{+} \ell_{2}^{-} \, jj$  | ::: |
 +| 3230 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}Z \, jj\to \ell_{1}^{-} \bar{\nu}_{\ell _{1}} \ell_{2}^{+} \ell_{2}^{-} \, jj$  | ::: |
 +| 3250 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{+} \,  jj\to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{+} \nu_{\ell_{2}} \, jj$ | ::: |
 +| 3260 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}W^{-} \,  jj\to \ell_{1}^{-} \bar{\nu}_{\ell_{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} \, jj$ | ::: |
 +| 3270 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}\gamma \,  jj\to \ell^{+} \nu_{\ell} \gamma \, jj$  | ::: |
 +| 3280 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}\gamma \, jj\to \ell^{-} \bar{\nu}_{\ell} \gamma \, jj$  | ::: |
 +| 3290 | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z\gamma \,  jj\to \ell^{+} \ell^{-} \gamma \, jj$  | ::: |
 +| 3291 | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z\gamma \,  jj\to \nu_{\ell} \bar{\nu}_{\ell} \gamma\, jj$ | ::: |
 +
 +\\
 +
  
 == Higgs boson production plus two jets via Gluon Fusion == == Higgs boson production plus two jets via Gluon Fusion ==
  
 +|< 100% 12% 53% 35%>|
 ^ Process ID     ^ Process       ^ BSM Options          ^ ^ Process ID     ^ Process       ^ BSM Options          ^
 | 4100    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj$     | MSSM, general 2HDM        | | 4100    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj$     | MSSM, general 2HDM        |
Line 180: Line 405:
 | 4104    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to b\bar{b} \, jj$     | :::        | | 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}^-  | 4105    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to W^{+}W^{-} \, jj\to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^- 
-\bar{\nu}_{\ell_{2}} \, jj$     | :::        |+\bar{\nu}_{\ell_{2}} \, jj$     | MSSM, general 2HDM, anomalous HVV couplings   |
 | 4106    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \ell_{2}^+  | 4106    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \ell_{2}^+ 
 \ell_{2}^- \, jj$     | :::        | \ell_{2}^- \, jj$     | :::        |
 | 4107    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}}   | 4107    | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}}  
 \bar{\nu}_{\ell_{2}} \, jj$     | :::        | \bar{\nu}_{\ell_{2}} \, jj$     | :::        |
- 
  
 \\ \\
Line 191: Line 415:
 == Gluon-induced diboson production == == Gluon-induced diboson production ==
  
 +Processes with fully leptonic decays:
 +
 +|< 100% 12% 53% 35%>|
 ^ Process ID     ^ Process       ^ BSM Options          ^ ^ 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        |+| 4300    | $gg \to W^{+}W^{-} \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{-}\bar{\nu}_{\ell_{2}}$     | anomalous HVV couplings        |
 | 4330    | $gg \to ZZ \to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+}\ell_{2}^{-}$     | :::      | | 4330    | $gg \to ZZ \to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+}\ell_{2}^{-}$     | :::      |
 | 4360    | $gg \to Z\gamma \to \ell_{1}^{+} \ell_{1}^{-} \gamma$     | :::        | | 4360    | $gg \to Z\gamma \to \ell_{1}^{+} \ell_{1}^{-} \gamma$     | :::        |
 | 4370    | $gg \to \gamma\gamma $     | :::        | | 4370    | $gg \to \gamma\gamma $     | :::        |
  
 +Processes with semi-leptonic decays:
 +
 +|< 100% 12% 53% 35%>|
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 4301    | $gg \to W^{+}W^{-} \to q \bar{q} \, \ell^{-}\bar{\nu}_{\ell} $ | anomalous HVV couplings        |
 +| 4332    | $gg \to W^{+}W^{-} \to \ell^{+} \nu_{\ell} \, q \bar{q} $ | :::      |
 +| 4331    | $gg \to ZZ \to q \bar{q} \, \ell^{-} \ell^{+} $ | :::      |
  
 \\ \\
 +
 +== Gluon-induced diboson production in association with a hadronic jet ==
 +
 +|< 100% 12% 53% 35%>|
 +^ Process ID     ^ Process       ^ BSM Options          ^
 +| 4600 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-} j \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{-}\bar{\nu}_{\ell_{2}} j $ | anomalous HVV couplings        |
 +| 4650 | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZ j \to \ell_{1}^{-} \ell_{1}^{+}  \ell_{2}^{-} \ell_{2}^{+} j $ | ::: |
 +
 +\\
 +