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 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.
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Higgs boson production plus two jets via Vector Boson Fusion
Higgs boson production plus three jets via Vector Boson Fusion
Higgs boson production with a photon and two jets via Vector Boson Fusion
Single vector boson production plus two jets via Vector Boson Fusion
VBF production of two Higgs bosons and two jets
VBF production of a spin-2 particle
Vector boson pair production plus two jets via Vector Boson Fusion
Diboson production
Triple vector boson production
Double vector boson production in association with a hadronic jet
Triple vector boson production in association with a hadronic jet
WH production
W production
WH production in association with a hadronic jet
W production in association with a hadronic jet
QCD induced production of a vector boson in association with two jets
QCD induced diboson production in association with two jets
Higgs boson production plus two jets via Gluon Fusion
Gluon-induced diboson production
Gluon-induced diboson production in association with a hadronic jet
Processes with fully leptonic decays:
| Process ID | Process | BSM Options |
|---|---|---|
| 100 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj$ | anomalous HVV couplings, MSSM |
| 101 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj\to \gamma\gamma \, jj$ | |
| 102 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj\to \mu^+\mu^- \, jj$ | |
| 103 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj\to \tau^+\tau^- \, jj$ | |
| 104 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj\to b\bar{b} \, jj$ | |
| 105 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj\to W^{+}W^{-} \, jj\to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^- \bar{\nu}_{\ell_{2}} \, jj$ | |
| 106 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \ell_{2}^+ \ell_{2}^- \, jj$ | |
| 107 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \, jj$ |
Processes with semi-leptonic decays:
| Process ID | Process | BSM Options |
|---|---|---|
| 108 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj\to W^{+}W^{-} \, jj\to q\bar{q} \, \ell^- \bar{\nu}_{\ell} \,jj$ | anomalous HVV couplings, MSSM |
| 109 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj\to W^{+}W^{-} \, jj\to \ell^+\nu_{\ell} \, q\bar{q} \,jj$ | |
| 1010 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj\to ZZ \, jj\to q\bar{q} \, \ell^+ \ell^- \,jj$ |
| Process ID | Process | BSM Options |
|---|---|---|
| 110 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jjj$ | — |
| 111 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jjj\to \gamma\gamma \, jjj$ | |
| 112 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jjj\to \mu^+\mu^- \, jjj$ | |
| 113 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jjj\to \tau^+\tau^- \, jjj$ | |
| 114 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jjj\to b\bar{b} \, jjj$ | |
| 115 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jjj\to W^{+}W^{-} \, jj\to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^- \bar{\nu}_{\ell_{2}} \, jjj$ | |
| 116 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jjj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \ell_{2}^+ \ell_{2}^- \, jjj$ | |
| 117 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jjj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \, jjj$ |
| Process ID | Process | BSM Options |
|---|---|---|
| 2100 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \gamma \, jj$ | — |
| 2101 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \gamma \, jj\to \gamma\gamma \gamma \, jj$ | |
| 2102 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \gamma \, jj\to \mu^+\mu^- \gamma \, jj$ | |
| 2103 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \gamma \, jj\to \tau^+\tau^- \gamma \, jj$ | |
| 2104 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \gamma \, jj\to b\bar{b} \gamma \, jj$ | |
| 2105 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \gamma \, jj\to W^{+}W^{-} \gamma \, jj\to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^- \bar{\nu}_{\ell_{2}} \gamma \, jj$ | |
| 2106 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \gamma \, jj\to ZZ \gamma \, jj\to \ell_{1}^+ \ell_{1}^- \ell_{2}^+ \ell_{2}^- \gamma \, jj$ | |
| 2107 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \gamma \, jj\to ZZ \gamma \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \gamma \, jj$ |
| Process ID | Process | BSM Options |
|---|---|---|
| 120 | $p \overset{\tiny{\mbox{(—)}}}{p} \to Z \, jj \to \ell^{+} \ell^{-} \, jj$ | Anomalous gauge couplings |
| 121 | $p \overset{\tiny{\mbox{(—)}}}{p} \to Z \, jj\to \nu_\ell \bar{\nu}_\ell \, jj$ | |
| 130 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+} \, jj\to \ell^{+} \nu_\ell \, jj$ | |
| 140 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-} \, jj\to \ell^{-} \bar{\nu}_\ell \, jj$ | |
| 150 | $p \overset{\tiny{\mbox{(—)}}}{p} \to \gamma \, jj$ |
| Process ID | Process | BSM Options |
|---|---|---|
| 160 | $p \overset{\tiny{\mbox{(—)}}}{p} \to HH \, jj$ | — |
| 161 | $p \overset{\tiny{\mbox{(—)}}}{p} \to HH \, jj \to b\bar{b}\tau^+\tau^- \, jj$ | |
| 162 | $p \overset{\tiny{\mbox{(—)}}}{p} \to HH \, jj \to b\bar{b}\gamma\gamma \, jj$ |
| Process ID | Process | BSM Options |
|---|---|---|
| 191 | $p \overset{\tiny{\mbox{(—)}}}{p} \to S_{2} \, jj\to \gamma\gamma \, jj$ | spin-2 resonant production |
| 195 | $p \overset{\tiny{\mbox{(—)}}}{p} \to S_{2} \, jj\to W^{+}W^{-} \, jj\to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^- \bar{\nu}_{\ell_{2}} \,jj$ | |
| 196 | $p \overset{\tiny{\mbox{(—)}}}{p} \to S_{2} \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \ell_{2}^+ \ell_{2}^- \,jj$ | |
| 197 | $p \overset{\tiny{\mbox{(—)}}}{p} \to S_{2} \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \,jj$ |
Processes with fully leptonic decays:
| Process ID | Process | BSM Options |
|---|---|---|
| 200 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}W^{-} \, jj \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} \, jj$ | anomalous gauge couplings, two-Higgs model, Kaluza-Klein models, spin-2 models |
| 210 | $p \overset{\tiny{\mbox{(—)}}}{p} \to ZZ \, jj\to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \ell_{2}^{-} \, jj$ | |
| 211 | $p \overset{\tiny{\mbox{(—)}}}{p} \to ZZ \, jj\to \ell_{1}^{+} \ell_{1}^{-} \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \, jj$ | |
| 220 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}Z \, jj\to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{+} \ell_{2}^{-} \, jj$ | |
| 230 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-}Z \, jj\to \ell_{1}^{-} \bar{\nu}_{\ell _{1}} \ell_{2}^{+} \ell_{2}^{-} \, jj$ | |
| 250 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}W^{+} \, jj\to \ell_{1}^{+} \nu_{\ell _{1}} \ell_{2}^{+} \nu_{\ell_{2}} \, jj$ | anomalous gauge couplings, two-Higgs model |
| 260 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-}W^{-} \, jj\to \ell_{1}^{-} \bar{\nu}_{\ell _{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} \, jj$ | |
| 270 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}\gamma \, jj\to \ell^{+} \nu_{\ell} \gamma \, jj$ | anomalous gauge couplings |
| 280 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-}\gamma \, jj\to \ell^{-} \bar{\nu}_{\ell} \gamma \, jj$ | |
| 290 | $p \overset{\tiny{\mbox{(—)}}}{p} \to Z\gamma \, jj\to \ell^{+} \ell^{-} \gamma \, jj$ | |
| 291 | $p \overset{\tiny{\mbox{(—)}}}{p} \to Z\gamma \, jj\to \nu_{\ell}\bar{\nu}_{\ell} \gamma \, jj$ |
Processes with semi-leptonic decays:
| Process ID | Process | BSM Options |
|---|---|---|
| 201 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}W^{-} \, jj \to q \bar{q} \, \ell^{-} \bar{\nu}_{\ell} \, jj$ | anomalous gauge couplings, two-Higgs model |
| 202 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}W^{-} \, jj\to \ell^{+} \nu_\ell \, q \bar{q} \, jj$ | |
| 212 | $p \overset{\tiny{\mbox{(—)}}}{p} \to ZZ \, jj\to q \bar{q} \, \ell^{+} \ell^{-} \, jj$ | |
| 221 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}Z \, jj\to q \bar{q} \, \ell^{+} \ell^{-} \, jj$ | |
| 222 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}Z \, jj\to \ell^{+} \nu_{\ell} \, q \bar{q} \, jj$ | |
| 231 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-}Z \, jj\to q \bar{q} \, \ell^{+} \ell^{-} \, jj$ | |
| 232 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-}Z \, jj\to \ell^{-} \bar{\nu}_{\ell} \, q \bar{q} \, jj$ | |
| 251 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}W^{+} \, jj\to q \bar{q} \, \ell^{+} \nu_{\ell} \, jj$ | |
| 261 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-}W^{-} \, jj\to q \bar{q} \, \ell^{-} \bar{\nu}_{\ell} \, jj$ |
Processes with fully leptonic decays:
| Process ID | Process | BSM Options |
|---|---|---|
| 300 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}W^{-} \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{-}\bar{\nu}_{\ell_{2}}$ | anomalous HVV and gauge couplings |
| 310 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}Z \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{+}\ell_{2}^{-}$ | anomalous gauge couplings |
| 320 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-}Z \to \ell_{1}^{-} \bar{\nu}_{\ell_{1}} \ell_{2}^{+}\ell_{2}^{-}$ | |
| 330 | $p \overset{\tiny{\mbox{(—)}}}{p} \to ZZ \to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+}\ell_{2}^{-}$ | anomalous HVV couplings |
| 340 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}\gamma \to \ell_{1}^{+} \nu_{\ell_{1}} \gamma$ | anomalous gauge couplings |
| 350 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-}\gamma \to \ell_{1}^{-} \bar{\nu}_{\ell_{1}} \gamma$ | |
| 360 | $p \overset{\tiny{\mbox{(—)}}}{p} \to Z\gamma \to \ell_{1}^{+} \ell_{1}^{-} \gamma$ | anomalous HVV couplings |
| 370 | $p \overset{\tiny{\mbox{(—)}}}{p} \to \gamma\gamma $ |
Processes with semi-leptonic decays:
| Process ID | Process | BSM Options |
|---|---|---|
| 301 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}W^{-} \to q \bar{q} \, \ell^{-}\bar{\nu}_{\ell} $ | anomalous HVV and gauge couplings |
| 302 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}W^{-} \to \ell^{+} \nu_{\ell} \, q \bar{q} $ | |
| 312 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}Z \to q \bar{q} \, \ell^{+} \ell^{-} $ | anomalous gauge couplings |
| 313 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}Z \to \ell^{+} \nu_{\ell} \, q \bar{q}$ | |
| 322 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-}Z \to q \bar{q} \, \ell^{+} \ell^{-}$ | |
| 323 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-}Z \to \ell^{-} \bar{\nu}_{\ell} \, q \bar{q}$ | |
| 331 | $p \overset{\tiny{\mbox{(—)}}}{p} \to ZZ \to q \bar{q} \, \ell^{-} \ell^{+}$ | anomalous HVV couplings |
Processes with fully leptonic decays:
| Process ID | Process | BSM Options |
|---|---|---|
| 400 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}W^{-}Z \to \ell_{1}^{+}\nu_{\ell_{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} {\ell_3}^{+} {\ell_3}^{-}$ | anomalous gauge couplings, Kaluza-Klein models |
| 410 | $p \overset{\tiny{\mbox{(—)}}}{p} \to ZZW^{+} \to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \ell_{2}^{-} {\ell_3}^{+} \nu_{\ell_3}$ | |
| 420 | $p \overset{\tiny{\mbox{(—)}}}{p} \to ZZW^{-} \to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \ell_{2}^{-} {\ell_3}^{-} \bar{\nu}_{\ell_3}$ | |
| 430 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}W^{-}W^{+} \to \ell_{1}^{+}\nu_{\ell_1} \ell_{2}^{-} \bar{\nu}_{\ell_2} {\ell_3}^{+}\nu_{\ell_3}$ | |
| 440 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-}W^{+}W^{-} \to \ell_{1}^{-} \bar{\nu}_{\ell_1}\ell_{2}^{+}\nu_{\ell_2} {\ell_3}^{-} \bar{\nu}_{\ell_3}$ | |
| 450 | $p \overset{\tiny{\mbox{(—)}}}{p} \to ZZZ \to \ell_{1}^{-} \ell_{1}^{+} \ell_{2}^{-} \ell_{2}^{+} {\ell_3}^{-} {\ell_3}^{+}$ | anomalous gauge couplings |
| 460 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-}W^{+} \gamma \to \ell_{1}^{-} \bar{\nu}_{\ell_1} \ell_{2}^{+}\nu_{\ell_2} \gamma$ | |
| 470 | $p \overset{\tiny{\mbox{(—)}}}{p} \to Z Z \gamma \to \ell_{1}^{-} \ell_{1}^{+} \ell_{2}^{-} \ell_{2}^{+} \gamma$ | |
| 480 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+} Z \gamma \to \ell_{1}^{+}\nu_{\ell_1} \ell_{2}^{-} \ell_{2}^{+} \gamma$ | |
| 490 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-} Z \gamma \to \ell_{1}^{-} \bar{\nu}_{\ell_1} \ell_{2}^{-} \ell_{2}^{+} \gamma$ | |
| 500 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+} \gamma \gamma \to {\ell}^{+}\nu_{\ell} \gamma \gamma$ | |
| 510 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-} \gamma \gamma \to {\ell}^{-} \bar{\nu}_{\ell} \gamma \gamma$ | |
| 520 | $p \overset{\tiny{\mbox{(—)}}}{p} \to Z \gamma \gamma \to {\ell}^{-} {\ell}^{+} \gamma \gamma$ | |
| 521 | $p \overset{\tiny{\mbox{(—)}}}{p} \to Z \gamma \gamma \to \nu_{\ell} \bar{\nu}_{\ell} \gamma \gamma$ | |
| 530 | $p \overset{\tiny{\mbox{(—)}}}{p} \to \gamma \gamma \gamma$ |
Processes with semi-leptonic decays:
| Process ID | Process | BSM Options |
|---|---|---|
| 401 | $p \overset{\tiny{\mbox{(—)}}}{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{\tiny{\mbox{(—)}}}{p} \to W^{+}W^{-}Z \to \ell_{1}^{+}\nu_{\ell_{1}} \, q \bar{q} \, \ell_{2}^{+} \ell_{2}^{-} $ | |
| 403 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}W^{-}Z \to \ell_{1}^{+}\nu_{\ell_{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} \, q \bar{q} $ | |
| 411 | $p \overset{\tiny{\mbox{(—)}}}{p} \to ZZW^{+} \to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \ell_{2}^{-} \, q \bar{q} $ | |
| 412 | $p \overset{\tiny{\mbox{(—)}}}{p} \to ZZW^{+} \to q \bar{q} \, \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \nu_{\ell_{2}} $ | |
| 421 | $p \overset{\tiny{\mbox{(—)}}}{p} \to ZZW^{-} \to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \ell_{2}^{-} \, q \bar{q} $ | |
| 422 | $p \overset{\tiny{\mbox{(—)}}}{p} \to ZZW^{-} \to q \bar{q} \, \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{-} \bar{\nu}_{\ell_{2}}$ | |
| 431 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}W^{-}W^{+} \to q \bar{q} \, \ell_{1}^{-} \bar{\nu}_{\ell_1} \ell_{2}^{+}\nu_{\ell_{2}}$ | |
| 432 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}W^{-}W^{+} \to \ell_{1}^{+}\nu_{\ell_1} \, q \bar{q} \, \ell_{2}^{+}\nu_{\ell_{2}}$ | |
| 441 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-}W^{+}W^{-} \to \ell_{1}^{-} \bar{\nu}_{\ell_1} \, q \bar{q} \, \ell_{2}^{-} \bar{\nu}_{\ell_{2}} $ | |
| 442 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-}W^{+}W^{-} \to q \bar{q} \, \ell_{1}^{+}\nu_{\ell_1} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} $ | |
| 451 | $p \overset{\tiny{\mbox{(—)}}}{p} \to ZZZ \to q \bar{q} \, \ell_{1}^{-} \ell_{1}^{+} \ell_{2}^{-} \ell_{2}^{+} $ | |
| 461 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}W^{-} \gamma \to q \bar{q} \, \ell^{-}\bar{\nu}_{\ell} \gamma$ | |
| 462 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}W^{-} \gamma \to \ell^{+} \nu_{\ell} \, q \bar{q} \, \gamma$ | |
| 471 | $p \overset{\tiny{\mbox{(—)}}}{p} \to Z Z \gamma \to \ell^{-} \ell^{+} \, q \bar{q} \, \gamma$ | |
| 481 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+} Z \gamma \to q \bar{q} \, \ell^{-} \ell^{+} \gamma$ | |
| 482 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+} Z \gamma \to \ell^{+}\nu_{\ell} \, q \bar{q} \, \gamma$ | |
| 491 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-} Z \gamma \to q \bar{q} \, \ell^{-} \ell^{+} \gamma$ | |
| 492 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-} Z \gamma \to \ell^{-} \bar{\nu}_{\ell} \, q \bar{q} \, \gamma$ |
| Process ID | Process | BSM Options |
|---|---|---|
| 600 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+} W^{-} j \to \ell_{1}^{+}\nu_{\ell_1} \ell_{2}^{-} \bar{\nu}_{\ell_2} j $ | anomalous HVV couplings |
| 610 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-} \gamma j \to \ell^{-} \bar \nu_{\ell} \gamma j$ | anomalous gauge couplings |
| 620 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+} \gamma j \to \ell^{+} \nu_{\ell} \gamma j$ | |
| 630 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-} Z j \to \ell_{1}^{-} \bar \nu_{\ell_1} \ell_{2}^{-} \ell_{2}^{+} j$ | |
| 640 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+} Z j \to \ell_{1}^{+}\nu_{\ell_1} \ell_{2}^{-}\ell_{2}^{+}j$ | |
| 650 | $p \overset{\tiny{\mbox{(—)}}}{p} \to Z Z j \to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \ell_{2}^{-} j $ | anomalous HVV couplings |
| Process ID | Process | BSM Options |
|---|---|---|
| 800 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+} \gamma \gamma j \to \ell^{+} \nu_{\ell} \gamma \gamma j$ | anomalous gauge couplings |
| 810 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-} \gamma \gamma j \to \ell^{-} \bar \nu_{\ell} \gamma \gamma j$ |
| Process ID | Process | BSM Options |
|---|---|---|
| 1300 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^+ H \to \ell^+\nu_{\ell} H $ | anomalous gauge couplings |
| 1301 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^+ H \to \ell^+\nu_{\ell} \gamma\gamma $ | |
| 1302 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^+ H \to \ell^+\nu_{\ell} \mu^+\mu^- $ | |
| 1303 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^+ H \to \ell^+\nu_{\ell} \tau^+\tau^- $ | |
| 1304 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^+ H \to \ell^+\nu_{\ell} b\bar{b} $ | |
| 1305 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^+ H \to W^+ W^{+}W^{-} \to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^+\nu_{\ell_{2}} \ell_{3}^- \bar{\nu}_{\ell_{3}}$ | |
| 1306 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^+ H \to W^+ ZZ \to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \ell_{3}^+ \ell_{3}^-$ | |
| 1307 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^+ H \to W^+ ZZ \to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \nu_{\ell_{3}} \bar{\nu}_{\ell_{3}}$ | |
| 1310 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^- H \to \ell^- \bar{\nu}_{\ell} H $ | |
| 1311 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^- H \to \ell^- \bar{\nu}_{\ell} \gamma\gamma $ | |
| 1312 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^- H \to \ell^- \bar{\nu}_{\ell} \mu^+\mu^- $ | |
| 1313 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^- H \to \ell^- \bar{\nu}_{\ell} \tau^+\tau^- $ | |
| 1314 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^- H \to \ell^- \bar{\nu}_{\ell} b\bar{b} $ | |
| 1315 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^- H \to W^- W^{+}W^{-} \to \ell_{1}^-\bar{\nu}_{\ell_{1}} \ell_{2}^+\nu_{\ell_{2}} \ell_{3}^- \bar{\nu}_{\ell_{3}}$ | |
| 1316 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^- H \to W^- ZZ \to \ell_{1}^-\bar{\nu}_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \ell_{3}^+ \ell_{3}^-$ | |
| 1317 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^- H \to W^- ZZ \to \ell_{1}^-\bar{\nu}_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \nu_{\ell_{3}} \bar{\nu}_{\ell_{3}}$ |
| Process ID | Process | BSM Options |
|---|---|---|
| 1330 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^+ \to \ell^+\nu_{\ell} $ | — |
| 1340 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^- \to \ell^- \bar{\nu}_{\ell} $ |
| Process ID | Process | BSM Options |
|---|---|---|
| 1600 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^+ H \, j \to \ell^+\nu_{\ell} H \, j $ | anomalous gauge couplings |
| 1601 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^+ H \, j \to \ell^+\nu_{\ell} \gamma\gamma \, j $ | |
| 1602 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^+ H \, j \to \ell^+\nu_{\ell} \mu^+\mu^- \, j $ | |
| 1603 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^+ H \, j \to \ell^+\nu_{\ell} \tau^+\tau^- \, j $ | |
| 1604 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^+ H \, j \to \ell^+\nu_{\ell} b\bar{b} \, j $ | |
| 1605 | $p \overset{\tiny{\mbox{(—)}}}{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{\tiny{\mbox{(—)}}}{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{\tiny{\mbox{(—)}}}{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{\tiny{\mbox{(—)}}}{p} \to W^- H \, j \to \ell^- \bar{\nu}_{\ell} H \, j $ | |
| 1611 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^- H \, j \to \ell^- \bar{\nu}_{\ell} \gamma\gamma \, j $ | |
| 1612 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^- H \, j \to \ell^- \bar{\nu}_{\ell} \mu^+\mu^- \, j $ | |
| 1613 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^- H \, j \to \ell^- \bar{\nu}_{\ell} \tau^+\tau^- \, j $ | |
| 1614 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^- H \, j \to \ell^- \bar{\nu}_{\ell} b\bar{b} \, j $ | |
| 1615 | $p \overset{\tiny{\mbox{(—)}}}{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{\tiny{\mbox{(—)}}}{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{\tiny{\mbox{(—)}}}{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 $ |
| Process ID | Process | BSM Options |
|---|---|---|
| 1630 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^+ \, j \to \ell^+\nu_{\ell} \, j $ | — |
| 1640 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^- \, j\to \ell^- \bar{\nu}_{\ell} \, j $ |
| Process ID | Process | BSM Options |
|---|---|---|
| 3120 | $p \overset{\tiny{\mbox{(—)}}}{p} \to Z \, jj\to \ell^{+} \ell^{-} \, jj$ | — |
| 3121 | $p \overset{\tiny{\mbox{(—)}}}{p} \to Z \, jj\to \nu_{\ell} \bar{\nu}_{\ell} \, jj$ | |
| 3130 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+} \, jj\to \ell^{+} \nu_\ell \, jj$ | |
| 3140 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-} \, jj\to \ell^{-} \bar{\nu}_\ell \, jj$ |
| Process ID | Process | BSM Options |
|---|---|---|
| 3210 | $p \overset{\tiny{\mbox{(—)}}}{p} \to ZZ \, jj\to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \ell_{2}^{-} \, jj$ | — |
| 3211 | $p \overset{\tiny{\mbox{(—)}}}{p} \to ZZ \, jj\to \ell_{1}^{+} \ell_{1}^{-} \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \, jj$ | |
| 3220 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}Z \, jj\to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{+} \ell_{2}^{-} \, jj$ | |
| 3230 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-}Z \, jj\to \ell_{1}^{-} \bar{\nu}_{\ell _{1}} \ell_{2}^{+} \ell_{2}^{-} \, jj$ | |
| 3250 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}W^{+} \, jj\to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{+} \nu_{\ell_{2}} \, jj$ | |
| 3260 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-}W^{-} \, jj\to \ell_{1}^{-} \bar{\nu}_{\ell_{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} \, jj$ | |
| 3270 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}\gamma \, jj\to \ell^{+} \nu_{\ell} \gamma \, jj$ | |
| 3280 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-}\gamma \, jj\to \ell^{-} \bar{\nu}_{\ell} \gamma \, jj$ | |
| 3290 | $p \overset{\tiny{\mbox{(—)}}}{p} \to Z\gamma \, jj\to \ell^{+} \ell^{-} \gamma \, jj$ | |
| 3291 | $p \overset{\tiny{\mbox{(—)}}}{p} \to Z\gamma \, jj\to \nu_{\ell} \bar{\nu}_{\ell} \gamma\, jj$ |
| Process ID | Process | BSM Options |
|---|---|---|
| 4100 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj$ | MSSM, general 2HDM |
| 4101 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj\to \gamma\gamma \, jj$ | MSSM |
| 4102 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj\to \mu^+\mu^- \, jj$ | |
| 4103 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj\to \tau^+\tau^- \, jj$ | |
| 4104 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj\to b\bar{b} \, jj$ | |
| 4105 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj\to W^{+}W^{-} \, jj\to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^- \bar{\nu}_{\ell_{2}} \, jj$ | MSSM, general 2HDM, anomalous HVV couplings |
| 4106 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \ell_{2}^+ \ell_{2}^- \, jj$ | |
| 4107 | $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \, jj$ |
Processes with fully leptonic decays:
| 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 $ |
Processes with semi-leptonic decays:
| 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^{+} $ |
| Process ID | Process | BSM Options |
|---|---|---|
| 4600 | $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{+}W^{-} j \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{-}\bar{\nu}_{\ell_{2}} j $ | anomalous HVV couplings |
| 4650 | $p \overset{\tiny{\mbox{(—)}}}{p} \to ZZ j \to \ell_{1}^{-} \ell_{1}^{+} \ell_{2}^{-} \ell_{2}^{+} j $ |