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documentation:proclist [2012/07/23 10:29] sophy |
documentation:proclist [2014/04/15 16:06] Michael Rauch |
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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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== 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 | ^ Process ID ^ Process | ||
| 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 | | ||
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| 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 | ||
+ | | 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} | ||
+ | | 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 | ^ Process ID ^ Process | ||
| 110 | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jjj$ | --- | | | 110 | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \, jjj$ | --- | | ||
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== 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 | ^ Process ID ^ Process | ||
| 2100 | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \gamma \, jj$ | --- | | | 2100 | $p \overset{\mbox{\tiny{(--)}}}{p} \to H \gamma \, jj$ | --- | | ||
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== 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 | ^ Process ID ^ Process | ||
- | | 120 | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z \, jj \to \ell^{+} \ell^{-} \, jj$ | Anomalous | + | | 120 | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z \, jj \to \ell^{+} \ell^{-} \, jj$ | Anomalous |
| 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 | | 140 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-} \, jj\to \ell^{-} \bar{\nu}_\ell | ||
| 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 | ||
+ | | 160 | $p \overset{\mbox{\tiny{(--)}}}{p} \to HH \, jj$ | --- | | ||
\\ | \\ | ||
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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 | ^ Process ID ^ Process | ||
- | | 191 | $p \overset{\mbox{\tiny{(--)}}}{p} \to S_{2} \, jj\to \gamma\gamma \, jj$ | + | | 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 | ^ Process ID ^ Process | ||
- | | 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 |
- | | 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 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{+} \, jj\to \ell_{1}^{+} \nu_{\ell _{1}} \ell_{2}^{+} \nu_{\ell_{2}} \, jj$ |
| 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 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}\gamma \, jj\to \ell^{-} \bar{\nu}_{\ell} \gamma \, jj$ | ::: | | ||
+ | Processes with semi-leptonic decays: | ||
+ | |||
+ | |< 100% 12% 53% 35%>| | ||
+ | ^ Process ID ^ Process | ||
+ | | 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^{-} | ||
+ | | 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 | ^ Process ID ^ Process | ||
- | | 300 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-} \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{-}\bar{\nu}_{\ell_{2}}$ | + | | 300 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-} \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{-}\bar{\nu}_{\ell_{2}}$ |
- | | 310 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}Z \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{+}\ell_{2}^{-}$ | + | | 310 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}Z \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{+}\ell_{2}^{-}$ |
| 320 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}Z \to \ell_{1}^{-} \bar{\nu}_{\ell_{1}} \ell_{2}^{+}\ell_{2}^{-}$ | | 320 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}Z \to \ell_{1}^{-} \bar{\nu}_{\ell_{1}} \ell_{2}^{+}\ell_{2}^{-}$ | ||
- | | 330 | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZ \to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+}\ell_{2}^{-}$ | + | | 330 | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZ \to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+}\ell_{2}^{-}$ |
- | | 340 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}\gamma \to \ell_{1}^{+} \nu_{\ell_{1}} \gamma$ | + | | 340 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}\gamma \to \ell_{1}^{+} \nu_{\ell_{1}} \gamma$ |
| 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 | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z\gamma \to \ell_{1}^{+} \ell_{1}^{-} \gamma$ | + | | 360 | $p \overset{\mbox{\tiny{(--)}}}{p} \to Z\gamma \to \ell_{1}^{+} \ell_{1}^{-} \gamma$ |
| 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 | ||
+ | | 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 | ||
\\ | \\ | ||
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== Triple vector boson production == | == Triple vector boson production == | ||
+ | Processes with fully leptonic decays: | ||
+ | |||
+ | |< 100% 12% 53% 35%>| | ||
^ Process ID ^ Process | ^ Process ID ^ Process | ||
- | | 400 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-}Z \to \ell_{1}^{+}\nu_{\ell_{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} {\ell_3}^{+} {\ell_3}^{-}$ | + | | 400 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{+}W^{-}Z \to \ell_{1}^{+}\nu_{\ell_{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} {\ell_3}^{+} {\ell_3}^{-}$ |
| 410 | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZW^{+} \to \ell_{1}^{+} \ell_{1}^{-} | | 410 | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZW^{+} \to \ell_{1}^{+} \ell_{1}^{-} | ||
| | ||
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{\ell_3}^{-} \bar{\nu}_{\ell_3}$ | {\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}^{+}$ |
| 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$ | ||
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\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 | ||
+ | | 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}^{-} | ||
+ | \, q \bar{q} $ | ::: | | ||
+ | | 412 | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZW^{+} \to q \bar{q} \, \ell_{1}^{+} \ell_{1}^{-} | ||
+ | | ||
+ | | 421 | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZW^{-} \to \ell_{1}^{+} \ell_{1}^{-} | ||
+ | \, q \bar{q} $ | ::: | | ||
+ | | 422 | $p \overset{\mbox{\tiny{(--)}}}{p} \to ZZW^{-} \to q \bar{q} \, \ell_{1}^{+} \ell_{1}^{-} | ||
+ | | ||
+ | | 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} \, | ||
+ | | ||
+ | | 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 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-} Z \gamma \to \ell^{-} \bar{\nu}_{\ell} \, q \bar{q} \, \gamma$ | ::: | | ||
+ | |||
\\ | \\ | ||
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== 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 | ^ Process ID ^ Process | ||
- | | 610 | $p \overset{\mbox{\tiny{(--)}}}{p} | + | | 610 | $p \overset{\mbox{\tiny{(--)}}}{p} |
| 620 | $p \overset{\mbox{\tiny{(--)}}}{p} | | 620 | $p \overset{\mbox{\tiny{(--)}}}{p} | ||
| 630 | $p \overset{\mbox{\tiny{(--)}}}{p} | | 630 | $p \overset{\mbox{\tiny{(--)}}}{p} | ||
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== 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 | ^ Process ID ^ Process | ||
- | | 800 | $p \overset{\mbox{\tiny{(--)}}}{p} | + | | 800 | $p \overset{\mbox{\tiny{(--)}}}{p} |
| 810 | $p \overset{\mbox{\tiny{(--)}}}{p} | | 810 | $p \overset{\mbox{\tiny{(--)}}}{p} | ||
\\ | \\ | ||
+ | |||
+ | |||
+ | == WH production == | ||
+ | |||
+ | |< 100% 12% 53% 35%>| | ||
+ | ^ Process ID ^ Process | ||
+ | | 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}} | ||
+ | | 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}} | ||
+ | |||
+ | \\ | ||
+ | |||
+ | |||
+ | == W production == | ||
+ | |||
+ | |< 100% 12% 53% 35%>| | ||
+ | ^ Process ID ^ Process | ||
+ | | 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 | ||
+ | | 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}}\, | ||
+ | | 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}^-\, | ||
+ | | 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}} | ||
+ | | 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}}\, | ||
+ | | 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}^-\, | ||
+ | | 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}} | ||
+ | |||
+ | \\ | ||
+ | |||
+ | |||
+ | == W production in association with a hadronic jet == | ||
+ | |||
+ | |< 100% 12% 53% 35%>| | ||
+ | ^ Process ID ^ Process | ||
+ | | 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 | ||
+ | | 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 | ||
+ | |||
+ | \\ | ||
+ | |||
+ | |||
+ | == QCD induced diboson production in association with two jets == | ||
+ | |||
+ | |< 100% 12% 53% 35%>| | ||
+ | ^ Process ID ^ Process | ||
+ | | 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 | $p \overset{\mbox{\tiny{(--)}}}{p} \to W^{-}\gamma \, jj\to \ell^{-} \bar{\nu}_{\ell} \gamma \, jj$ | ::: | | ||
+ | |||
+ | \\ | ||
+ | |||
== 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 | ^ Process ID ^ Process | ||
| 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 392: | ||
| 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$ |
| 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 402: | ||
== Gluon-induced diboson production == | == Gluon-induced diboson production == | ||
+ | Processes with fully leptonic decays: | ||
+ | |||
+ | |< 100% 12% 53% 35%>| | ||
^ Process ID ^ Process | ^ Process ID ^ Process | ||
- | | 4300 | $gg \to W^{+}W^{-} \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{-}\bar{\nu}_{\ell_{2}}$ | + | | 4300 | $gg \to W^{+}W^{-} \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{-}\bar{\nu}_{\ell_{2}}$ |
| 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 | ||
+ | | 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^{+} $ | ::: | | ||
\\ | \\ | ||
+ |