Process List

Higgs boson production plus two jets via Vector Boson Fusion

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 $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj\to ZZ \, jj\to q\bar{q} \, \ell^+ \ell^- \,jj$


Higgs boson production plus three jets via Vector Boson Fusion
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 $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jjj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \, jjj$


Higgs boson production with a photon and two jets via Vector Boson Fusion
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 $p \overset{\tiny{\mbox{(—)}}}{p} \to H \gamma \, jj\to ZZ \gamma \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \gamma \, jj$


Single vector boson production plus two jets via Vector Boson Fusion
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 $p \overset{\tiny{\mbox{(—)}}}{p} \to \gamma \, jj$


VBF production of two Higgs bosons and two jets
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 $p \overset{\tiny{\mbox{(—)}}}{p} \to HH \, jj \to b\bar{b}\gamma\gamma \, jj$


VBF production of a spin-2 particle
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 $p \overset{\tiny{\mbox{(—)}}}{p} \to S_{2} \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \,jj$


Vector boson pair production plus two jets via Vector Boson Fusion

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 $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-}W^{-} \, jj\to q \bar{q} \, \ell^{-} \bar{\nu}_{\ell} \, jj$


Diboson production

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


Triple vector boson production

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 $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-} Z \gamma \to \ell^{-} \bar{\nu}_{\ell} \, q \bar{q} \, \gamma$


Double vector boson production in association with a hadronic jet
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


Triple vector boson production in association with a hadronic jet
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 $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-} \gamma \gamma j \to \ell^{-} \bar \nu_{\ell} \gamma \gamma j$


WH production
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 $p \overset{\tiny{\mbox{(—)}}}{p} \to W^- H \to W^- ZZ \to \ell_{1}^-\bar{\nu}_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \nu_{\ell_{3}} \bar{\nu}_{\ell_{3}}$


W production
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} $


WH production in association with a hadronic jet
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 $


W production in association with a hadronic jet
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 $


QCD induced production of a vector boson in association with two jets
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 $p \overset{\tiny{\mbox{(—)}}}{p} \to W^{-} \, jj\to \ell^{-} \bar{\nu}_\ell \, jj$


QCD induced diboson production in association with two jets
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 $p \overset{\tiny{\mbox{(—)}}}{p} \to Z\gamma \, jj\to \nu_{\ell} \bar{\nu}_{\ell} \gamma\, jj$


Higgs boson production plus two jets via Gluon Fusion
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 $p \overset{\tiny{\mbox{(—)}}}{p} \to H \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \, jj$


Gluon-induced diboson production

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^{+} $


Gluon-induced diboson production in association with a hadronic jet
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 $


Last modified:: 2017/08/22 11:30