Processes
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Vector Boson Fusion Production Processes
- Higgs boson production plus two jets via Vector Boson Fusion
- Higgs boson production plus three 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
- Vector boson pair production plus two jets via Vector Boson Fusion
- VBF production of a spin-2 particle
- Higgs boson production with a photon and two jets via Vector Boson Fusion
- Single, Double and triple vector boson production
- Single, double and triple vector boson production plus one jet
- Gluon Fusion Processes
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Vector Boson Fusion Production Processes
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Higgs boson production plus two jets via Vector Boson Fusion
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 100 \(p \stackrel{(-)}{p} \rightarrow H j j\) \( \checkmark \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) \( \checkmark \) 101 \(p \stackrel{(-)}{p} \rightarrow H j j \rightarrow \gamma \gamma j j\) \( - \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) \( \checkmark \) 102 \(p \stackrel{(-)}{p} \rightarrow H j j \rightarrow \mu^{+} \mu^{-} j j\) \( - \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) \( \checkmark \) 103 \(p \stackrel{(-)}{p} \rightarrow H j j \rightarrow \tau^{+} \tau^{-} j j\) \( - \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) \( \checkmark \) 104 \(p \stackrel{(-)}{p} \rightarrow H j j \rightarrow b \bar{b} j j\) \( - \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) \( \checkmark \) 105 \(p \stackrel{(-)}{p} \rightarrow H j j \rightarrow W^{+} W^{-} jj \rightarrow \ell_1^{+}\nu_{\ell_1} \ell_2^{-} \bar{\nu}_{\ell_2} j j \) \( - \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) \( \checkmark \) 106 \(p \stackrel{(-)}{p} \rightarrow H j j \rightarrow ZZjj \rightarrow \ell_1^+ \ell_1^- \ell_2^+ \ell_2^- jj\) \( - \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) \( \checkmark \) 107 \(p \stackrel{(-)}{p} \rightarrow H j j \rightarrow ZZjj \rightarrow \ell_1^+ \ell_1^- \nu_{\ell_2} \bar{\nu}_{\ell_2} j j\) \( - \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) \( \checkmark \) 108 \(p \stackrel{(-)}{p} \rightarrow H j j \rightarrow W^+ W^- j j \rightarrow q \bar{q} \ell^- \bar{\nu}_\ell j j\) \( - \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) \( \checkmark \) 109 \(p \stackrel{(-)}{p} \rightarrow H j j \rightarrow W^+ W^- j j \rightarrow \ell^+ \nu_{\ell} q \bar{q} j j\) \( - \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) \( \checkmark \) 1010 \(p \stackrel{(-)}{p} \rightarrow H j j \rightarrow ZZ j j \rightarrow q \bar{q} \ell^+ \ell^- j j\) \( - \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) \( \checkmark \) -
Higgs boson production plus three jets via Vector Boson
Fusion
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 110 \(p \stackrel{(-)}{p} \rightarrow H j j j\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 111 \(p \stackrel{(-)}{p} \rightarrow H j j j \rightarrow \gamma \gamma j j j\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 112 \(p \stackrel{(-)}{p} \rightarrow H j j j \rightarrow \mu^{+} \mu^{-} j j j \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 113 \(p \stackrel{(-)}{p} \rightarrow H j j j\rightarrow \tau^{+} \tau^{-} j j j\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 114 \(p \stackrel{(-)}{p} \rightarrow H j j j \rightarrow b \bar{b} j j j \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 115 \(p \stackrel{(-)}{p} \rightarrow H j j j \rightarrow W^{+} W^{-} jj j \rightarrow \ell_1^{+}\nu_{\ell_1} \ell_2^{-} \bar{\nu}_{\ell_2} j j j \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 116 \(p \stackrel{(-)}{p} \rightarrow H j jj \rightarrow ZZjjj \rightarrow \ell_1^+ \ell_1^- \ell_2^+ \ell_2^- jjj\) \( - \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) \( \checkmark \) 117 \(p \stackrel{(-)}{p} \rightarrow H j j j \rightarrow ZZjjj \rightarrow \ell_1^+ \ell_1^- \nu_{\ell_2} \bar{\nu}_{\ell_2} j j j\) \( - \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) \( \checkmark \) -
Single vector boson production plus two jets via Vector Boson
Fusion
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 120 \(p \stackrel{(-)}{p} \to Z \, jj \to \ell^{+} \ell^{-} \, jj\) \( \checkmark \) \( \checkmark \) \( - \) \( - \) \( - \) \( - \) \( - \) 121 \(p \stackrel{(-)}{p} \to Z \, jj \to \nu_\ell \bar{\nu}_\ell \, jj\) \( \checkmark \) \( \checkmark \) \( - \) \( - \) \( - \) \( - \) \( - \) 130 \(p \stackrel{(-)}{p} \to W^{+} \, jj \to \ell^{+} \nu_\ell \, jj\) \( \checkmark \) \( \checkmark \) \( - \) \( - \) \( - \) \( - \) \( - \) 140 \(p \stackrel{(-)}{p} \to W^{-} \, jj \to \ell^{-} \bar{\nu}_\ell \, jj\) \( \checkmark \) \( \checkmark \) \( - \) \( - \) \( - \) \( - \) \( - \) 150 \(p \stackrel{(-)}{p} \to \gamma \, jj\) \( \checkmark \) \( \checkmark \) \( - \) \( - \) \( - \) \( - \) \( - \) -
VBF production of two Higgs bosons and two jets
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 160 \(p \stackrel{(-)}{p} \to HH \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 161 \(p \stackrel{(-)}{p} \to HH \, jj \to b\bar{b}\tau^+\tau^- \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 162 \(p \stackrel{(-)}{p} \to HH \, jj \to b\bar{b}\gamma\gamma \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) -
VBF production of a spin-2 particle
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 191 \(p \stackrel{(-)}{p} \to S_{2} \, jj \to \gamma \gamma \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( \checkmark \) \( - \) 195 \(p \stackrel{(-)}{p} \to S_{2} \, jj \to W^{+}W^{-} \, jj \to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^- \bar{\nu}_{\ell_{2}} \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( \checkmark \) \( - \) 196 \(p \stackrel{(-)}{p} \to S_{2} \, jj \to ZZ \, jj \to \ell_{1}^+ \ell_{1}^- \ell_{2}^+ \ell_{2}^- \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( \checkmark \) \( - \) 197 \(p \stackrel{(-)}{p} \to S_{2} \, jj \to ZZ \, jj \to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( \checkmark \) \( - \) -
Vector boson pair production plus two jets via Vector Boson
Fusion
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 200 \(p \stackrel{(-)}{p} \to W^{+}W^{-} \, jj \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} \, jj\) \( \checkmark \) \( \checkmark \) \( - \) \( \checkmark \) \( \checkmark \) \( \checkmark \) \( - \) 201 \(p \stackrel{(-)}{p} \to W^{+}W^{-} \, jj \to q \bar{q} \, \ell^{-} \bar{\nu}_{\ell} \, jj\) \( - \) \( \checkmark \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) 202 \(p \stackrel{(-)}{p} \to W^{+}W^{-} \, jj\to \ell^{+} \nu_\ell \, q \bar{q} \, jj\) \( - \) \( \checkmark \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) 210 \(p \stackrel{(-)}{p} \to ZZ \, jj\to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \ell_{2}^{-} \, jj\) \( \checkmark \) \( \checkmark \) \( - \) \( \checkmark \) \( \checkmark \) \( \checkmark \) \( - \) 211 \(p \stackrel{(-)}{p} \to ZZ \, jj\to \ell_{1}^{+} \ell_{1}^{-} \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \, jj\) \( \checkmark \) \( \checkmark \) \( - \) \( \checkmark \) \( \checkmark \) \( \checkmark \) \( - \) 212 \(p \stackrel{(-)}{p} \to ZZ \, jj\to q \bar{q} \, \ell^{+} \ell^{-} \, jj\) \( - \) \( \checkmark \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) 220 \(p \stackrel{(-)}{p} \to W^{+}Z \, jj\to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{+} \ell_{2}^{-} \, jj\) \( \checkmark \) \( \checkmark \) \( - \) \( \checkmark \) \( \checkmark \) \( \checkmark \) \( - \) 221 \(p \stackrel{(-)}{p} \to W^{+}Z \, jj\to q \bar{q} \, \ell^{+} \ell^{-} \, jj\) \( - \) \( \checkmark \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) 222 \(p \stackrel{(-)}{p} \to W^{+}Z \, jj\to \ell^{+} \nu_{\ell} \, q \bar{q} \, jj\) \( - \) \( \checkmark \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) 230 \(p \stackrel{(-)}{p} \to W^{-}Z \, jj\to \ell_{1}^{-} \bar{\nu}_{\ell _{1}} \ell_{2}^{+} \ell_{2}^{-} \, jj\) \( \checkmark \) \( \checkmark \) \( - \) \( \checkmark \) \( \checkmark \) \( \checkmark \) \( - \) 231 \(p \stackrel{(-)}{p} \to W^{-}Z \, jj\to q \bar{q} \, \ell^{+} \ell^{-} \, jj\) \( - \) \( \checkmark \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) 232 \(p \stackrel{(-)}{p} \to W^{-}Z \, jj\to \ell^{-} \bar{\nu}_{\ell} \, q \bar{q} \, jj\) \( - \) \( \checkmark \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) 240 \(p \stackrel{(-)}{p} \to \gamma\gamma \, jj\) \( \checkmark \) \( \checkmark \) \( - \) \( - \) \( - \) \( - \) \( - \) 250 \(p \stackrel{(-)}{p} \to W^{+}W^{+} \, jj\to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{+} \nu_{\ell_{2}} \, jj\) \( \checkmark \) \( \checkmark \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) 251 \(p \stackrel{(-)}{p} \to W^{+}W^{+} \, jj\to q \bar{q} \, \ell^{+} \nu_{\ell} \, jj\) \( - \) \( \checkmark \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) 260 \(p \stackrel{(-)}{p} \to W^{-}W^{-} \, jj\to \ell_{1}^{-} \bar{\nu}_{\ell_{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} \, jj\) \( \checkmark \) \( \checkmark \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) 261 \(p \stackrel{(-)}{p} \to W^{-}W^{-} \, jj\to q \bar{q} \, \ell^{-} \bar{\nu}_{\ell} \, jj\) \( - \) \( \checkmark \) \( - \) \( \checkmark \) \( - \) \( - \) \( - \) 270 \(p \stackrel{(-)}{p} \to W^{+}\gamma \, jj\to \ell^{+} \nu_{\ell} \gamma \, jj\) \( \checkmark \) \( \checkmark \) \( - \) \( - \) \( - \) \( - \) \( - \) 280 \(p \stackrel{(-)}{p} \to W^{-}\gamma \, jj\to \ell^{-} \bar{\nu}_{\ell} \gamma \, jj\) \( \checkmark \) \( \checkmark \) \( - \) \( - \) \( - \) \( - \) \( - \) 290 \(p \stackrel{(-)}{p} \to Z\gamma \, jj\to \ell^{+} \ell^{-} \gamma \, jj\) \( \checkmark \) \( \checkmark \) \( - \) \( - \) \( - \) \( - \) \( - \) 291 \(p \stackrel{(-)}{p} \to Z\gamma \, jj\to \nu_{\ell}\bar{\nu}_{\ell} \gamma \, jj\) \( \checkmark \) \( \checkmark \) \( - \) \( - \) \( - \) \( - \) \( - \) -
Higgs boson production with a photon and two jets via Vector
Boson Fusion
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 2100 \(p \stackrel{(-)}{p} \to H \gamma \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 2101 \(p \stackrel{(-)}{p} \to H \gamma \, jj\to \gamma\gamma \gamma \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 2102 \(p \stackrel{(-)}{p} \to H \gamma \, jj\to \mu^+\mu^- \gamma \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 2103 \(p \stackrel{(-)}{p} \to H \gamma \, jj\to \tau^+\tau^- \gamma \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 2104 \(p \stackrel{(-)}{p} \to H \gamma \, jj\to b\bar{b} \gamma \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 2105 \(p \stackrel{(-)}{p} \to H \gamma \, jj\to W^+W^- \gamma \, jj\to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^- \bar{\nu}_{\ell_{2}} \gamma \,jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 2106 \(p \stackrel{(-)}{p} \to H \gamma \, jj\to ZZ \gamma \, jj\to \ell_{1}^+ \ell_{1}^- \ell_{2}^+ \ell_{2}^- \gamma \,jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 2107 \(p \stackrel{(-)}{p} \to H \gamma \, jj\to ZZ \gamma \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \gamma \,jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \)
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Higgs boson production plus two jets via Vector Boson Fusion
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Single, Double and triple vector boson production
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W production
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 1330 \(p \stackrel{(-)}{p} \to W^+ \to \ell^+\nu_{\ell}\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 1340 \(p \stackrel{(-)}{p} \to W^- \to \ell^- \bar{\nu}_{\ell}\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) -
WH production
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 1300 \(p \stackrel{(-)}{p} \to W^+ H \to \ell^+\nu_{\ell} H \) \(-\) \( \checkmark \) \(-\) \(-\) \(-\) \(-\) \(-\) 1301 \(p \stackrel{(-)}{p} \to W^+ H \to \ell^+\nu_{\ell} \gamma\gamma \) \(-\) \( \checkmark \) \(-\) \(-\) \(-\) \(-\) \(-\) 1302 \(p \stackrel{(-)}{p} \to W^+ H \to \ell^+\nu_{\ell} \mu^+\mu^- \) \(-\) \( \checkmark \) \(-\) \(-\) \(-\) \(-\) \(-\) 1303 \(p \stackrel{(-)}{p} \to W^+ H \to \ell^+\nu_{\ell} \tau^+\tau^- \) \(-\) \( \checkmark \) \(-\) \(-\) \(-\) \(-\) \(-\) 1304 \(p \stackrel{(-)}{p} \to W^+ H \to \ell^+\nu_{\ell} b\bar{b} \) \(-\) \( \checkmark \) \(-\) \(-\) \(-\) \(-\) \(-\) 1305 \(p \stackrel{(-)}{p} \to W^+ H \to W^+ W^{+}W^{-} \to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^+\nu_{\ell_{2}} \ell_{3}^- \bar{\nu}_{\ell_{3}} \) \(-\) \( \checkmark \) \(-\) \(-\) \(-\) \(-\) \(-\) 1306 \(p \stackrel{(-)}{p} \to W^+ H \to W^+ ZZ \to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \ell_{3}^+ \ell_{3}^- \) \(-\) \( \checkmark \) \(-\) \(-\) \(-\) \(-\) \(-\) 1307 \(p \stackrel{(-)}{p} \to W^+ H \to W^+ ZZ \to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \nu_{\ell_{3}} \bar{\nu}_{\ell_{3}} \) \(-\) \( \checkmark \) \(-\) \(-\) \(-\) \(-\) \(-\) 1310 \(p \stackrel{(-)}{p} \to W^- H \to \ell^- \bar{\nu}_{\ell} H \) \(-\) \( \checkmark \) \(-\) \(-\) \(-\) \(-\) \(-\) 1311 \(p \stackrel{(-)}{p} \to W^- H \to \ell^- \bar{\nu}_{\ell} \gamma\gamma \) \(-\) \( \checkmark \) \(-\) \(-\) \(-\) \(-\) \(-\) 1312 \(p \stackrel{(-)}{p} \to W^- H \to \ell^- \bar{\nu}_{\ell} \mu^+\mu^- \) \(-\) \( \checkmark \) \(-\) \(-\) \(-\) \(-\) \(-\) 1313 \(p \stackrel{(-)}{p} \to W^- H \to \ell^- \bar{\nu}_{\ell} \tau^+\tau^- \) \(-\) \( \checkmark \) \(-\) \(-\) \(-\) \(-\) \(-\) 1314 \(p \stackrel{(-)}{p} \to W^- H \to \ell^- \bar{\nu}_{\ell} b\bar{b} \) \(-\) \( \checkmark \) \(-\) \(-\) \(-\) \(-\) \(-\) 1315 \(p \stackrel{(-)}{p} \to W^- H \to W^- W^{+}W^{-} \to \ell_{1}^-\bar{\nu}_{\ell_{1}} \ell_{2}^+\nu_{\ell_{2}} \ell_{3}^- \bar{\nu}_{\ell_{3}}\) \(-\) \( \checkmark \) \(-\) \(-\) \(-\) \(-\) \(-\) 1316 \(p \stackrel{(-)}{p} \to W^- H \to W^- ZZ \to \ell_{1}^-\bar{\nu}_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \ell_{3}^+ \ell_{3}^-\) \(-\) \( \checkmark \) \(-\) \(-\) \(-\) \(-\) \(-\) 1317 \(p \stackrel{(-)}{p} \to W^- H \to W^- ZZ \to \ell_{1}^-\bar{\nu}_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \nu_{\ell_{3}} \bar{\nu}_{\ell_{3}}\) \(-\) \( \checkmark \) \(-\) \(-\) \(-\) \(-\) \(-\) -
Diboson production
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 300 \(p \stackrel{(-)}{p} \to W^{+}W^{-} \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{-}\bar{\nu}_{\ell_{2}} \) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) 301 \(p \stackrel{(-)}{p} \to W^{+}W^{-} \to q \bar{q} \, \ell^{-}\bar{\nu}_{\ell} \) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) 302 \(p \stackrel{(-)}{p} \to W^{+}W^{-} \to \ell^{+} \nu_{\ell} \, q \bar{q} \) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) 310 \(p \stackrel{(-)}{p} \to W^{+}Z \to \ell_{1}^{+} \nu_{\ell_1} \ell_{2}^{+} \ell_{2}^{-} \) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) 312 \(p \stackrel{(-)}{p} \to W^{+}Z \to q \bar{q} \, \ell^{+} \ell^{-} \) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) 313 \(p \stackrel{(-)}{p} \to W^{+}Z \to \ell^{+} \nu_{\ell} \, q \bar{q} \) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) 320 \(p \stackrel{(-)}{p} \to W^{-}Z \to \ell_{1}^{-} \bar{\nu}_{\ell_{1}} \ell_{2}^{+} \ell_{2}^{-} \) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) 322 \(p \stackrel{(-)}{p} \to W^{-}Z \to q \bar{q} \, \ell^{+} \ell^{-} \) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) 323 \(p \stackrel{(-)}{p} \to W^{-}Z \to \ell^{-} \bar{\nu}_{\ell} \, q \bar{q} \) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) 330 \(p \stackrel{(-)}{p} \to ZZ \to \ell_{1}^{-} \ell_{1}^{+} \ell_{2}^{-} \ell_{2}^{+} \) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) 331 \(p \stackrel{(-)}{p} \to ZZ \to q \bar{q} \, \ell^{-} \ell^{+} \) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) 340 \(p \stackrel{(-)}{p} \to W^{+}\gamma \to \ell_{1}^{+} \nu_{\ell_1} \gamma \) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) 350 \(p \stackrel{(-)}{p} \to W^{-}\gamma \to \ell_{1}^{-} \bar{\nu}_{\ell_{1}} \gamma \) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) 360 \(p \stackrel{(-)}{p} \to Z\gamma \to \ell_{1}^{-} \ell_{1}^{+} \gamma \) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) 370 \(p \stackrel{(-)}{p} \to \gamma\gamma \) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) -
Triple vector boson production
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 400 \(p \stackrel{(-)}{p} \to W^{+}W^{-}Z \to \ell_{1}^{+}\nu_{\ell_{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} \ell_{3}^{+} \ell_{3}^{-} \) \(\checkmark\) \(\checkmark\) \( - \) \( - \) \(\checkmark\) \( - \) \( - \) 401 \(p \stackrel{(-)}{p} \to W^{+}W^{-}Z \to q \bar{q} \, \ell_{1}^{-} \bar{\nu}_{\ell_{1}} \ell_{2}^{+} \ell_{2}^{-} \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 402 \(p \stackrel{(-)}{p} \to W^{+}W^{-}Z \to \ell_{1}^{+}\nu_{\ell_{1}} \, q \bar{q} \, \ell_{2}^{+} \ell_{2}^{-} \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 403 \(p \stackrel{(-)}{p} \to W^{+}W^{-}Z \to \ell_{1}^{+}\nu_{\ell_{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} \, q \bar{q} \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 410 \(p \stackrel{(-)}{p} \to ZZW^{+} \to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \ell_{2}^{-} \ell_{3}^{+} \nu_{\ell_{3}} \) \(\checkmark\) \(\checkmark\) \( - \) \( - \) \(\checkmark\) \( - \) \( - \) 411 \(p \stackrel{(-)}{p} \to ZZW^{+} \to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \ell_{2}^{-} \, q \bar{q} \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 412 \(p \stackrel{(-)}{p} \to ZZW^{+} \to q \bar{q} \, \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \nu_{\ell_{2}} \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 420 \(p \stackrel{(-)}{p} \to ZZW^{-} \to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \ell_{2}^{-} \ell_{3}^{-} \bar{\nu}_{\ell_{3}}\) \(\checkmark\) \(\checkmark\) \( - \) \( - \) \(\checkmark\) \( - \) \( - \) 421 \(p \stackrel{(-)}{p} \to ZZW^{-} \to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \ell_{2}^{-} \, q \bar{q} \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 422 \(p \stackrel{(-)}{p} \to ZZW^{-} \to q \bar{q} \, \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{-} \bar{\nu}_{\ell_{2}}\) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 430 \(p \stackrel{(-)}{p} \to W^{+}W^{-}W^{+} \to \ell_{1}^{+}\nu_{\ell_1} \ell_{2}^{-} \bar{\nu}_{\ell_2} \ell_{3}^{+}\nu_{\ell_{3}}\) \(\checkmark\) \(\checkmark\) \( - \) \( - \) \(\checkmark\) \( - \) \( - \) 431 \(p \stackrel{(-)}{p} \to W^{+}W^{-}W^{+} \to q \bar{q} \, \ell_{1}^{-} \bar{\nu}_{\ell_1} \ell_{2}^{+}\nu_{\ell_{2}}\) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 432 \(p \stackrel{(-)}{p} \to W^{+}W^{-}W^{+} \to \ell_{1}^{+}\nu_{\ell_1} \, q \bar{q} \, \ell_{2}^{+}\nu_{\ell_{2}}\) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 440 \(p \stackrel{(-)}{p} \to W^{-}W^{+}W^{-} \to \ell_{1}^{-} \bar{\nu}_{\ell_1}\ell_{2}^{+}\nu_{\ell_2} \ell_{3}^{-} \bar{\nu}_{\ell_{3}} \) \(\checkmark\) \(\checkmark\) \( - \) \( - \) \(\checkmark\) \( - \) \( - \) 441 \(p \stackrel{(-)}{p} \to W^{-}W^{+}W^{-} \to \ell_{1}^{-} \bar{\nu}_{\ell_1} \, q \bar{q} \, \ell_{2}^{-} \bar{\nu}_{\ell_{2}} \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 442 \(p \stackrel{(-)}{p} \to W^{-}W^{+}W^{-} \to q \bar{q} \, \ell_{1}^{+}\nu_{\ell_1} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 450 \(p \stackrel{(-)}{p} \to ZZZ \to \ell_{1}^{-} \ell_{1}^{+} \ell_{2}^{-} \ell_{2}^{+} \ell_{3}^{-} \ell_{3}^{+} \) \(\checkmark\) \(\checkmark\) \( - \) \( - \) \(\checkmark\) \( - \) \( - \) 451 \(p \stackrel{(-)}{p} \to ZZZ \to q \bar{q} \, \ell_{1}^{-} \ell_{1}^{+} \ell_{2}^{-} \ell_{2}^{+} \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 460 \(p \stackrel{(-)}{p} \to W^{-}W^{+} \gamma \to \ell_{1}^{-} \bar{\nu}_{\ell_1} \ell_{2}^{+}\nu_{\ell_2} \gamma\) \(\checkmark\) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 461 \(p \stackrel{(-)}{p} \to W^{+}W^{-} \gamma \to q \bar{q} \, \ell^{-}\bar{\nu}_{\ell} \gamma\) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 462 \(p \stackrel{(-)}{p} \to W^{+}W^{-} \gamma \to \ell^{+} \nu_{\ell} \, q \bar{q} \, \gamma\) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 470 \(p \stackrel{(-)}{p} \to Z Z \gamma \to \ell_{1}^{-} \ell_{1}^{+} \ell_{2}^{-} \ell_{2}^{+} \gamma\) \(\checkmark\) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 471 \(p \stackrel{(-)}{p} \to ZZ \gamma \to \ell^{-} \ell^{+} \, q \bar{q} \, \gamma\) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 472 \(p \stackrel{(-)}{p} \to ZZ \gamma \to \ell_{1}^{-} \ell_{1}^{+} \nu_{\ell_2} \bar{\nu}_{\ell_2} \gamma\) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 480 \(p \stackrel{(-)}{p} \to W^{+} Z \gamma \to \ell_{1}^{+}\nu_{\ell_1} \ell_{2}^{-} \ell_{2}^{+} \gamma\) \(\checkmark\) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 481 \(p \stackrel{(-)}{p} \to W^{+} Z \gamma \to q \bar{q} \, \ell^{-} \ell^{+} \gamma\) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 482 \(p \stackrel{(-)}{p} \to W^{+} Z \gamma \to \ell^{+}\nu_{\ell} \, q \bar{q} \, \gamma\) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 490 \(p \stackrel{(-)}{p} \to W^{-} Z \gamma \to \ell_{1}^{-} \bar{\nu}_{\ell_1} \ell_{2}^{-} \ell_{2}^{+} \gamma\) \(\checkmark\) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 491 \(p \stackrel{(-)}{p} \to W^{-} Z \gamma \to q \bar{q} \, \ell^{-} \ell^{+} \gamma\) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 492 \(p \stackrel{(-)}{p} \to W^{-} Z \gamma \to \ell^{-} \bar{\nu}_{\ell} \, q \bar{q} \, \gamma\) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 500 \(p \stackrel{(-)}{p} \to W^{+} \gamma \gamma \to {\ell}^{+}\nu_{\ell} \gamma \gamma\) \(\checkmark\) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 510 \(p \stackrel{(-)}{p} \to W^{-} \gamma \gamma \to {\ell}^{-} \bar{\nu}_{\ell} \gamma \gamma\) \(\checkmark\) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 520 \(p \stackrel{(-)}{p} \to Z \gamma \gamma \to {\ell}^{-} {\ell}^{+} \gamma \gamma\) \(\checkmark\) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 521 \(p \stackrel{(-)}{p} \to Z \gamma \gamma \to \nu_{\ell} \bar{\nu}_{\ell} \gamma \gamma\) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 530 \(p \stackrel{(-)}{p} \to \gamma \gamma \gamma \) \(\checkmark\) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \)
-
W production
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Single, double and triple vector boson production plus one jet
-
W production in association with a hadronic jet
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 1630 \(p \stackrel{(-)}{p} \to W^+ \, j \to \ell^+\nu_{\ell} \, j\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 1640 \(p \stackrel{(-)}{p} \to W^- \, j \to \ell^- \bar{\nu}_{\ell} \, j\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) -
Double vector boson production in association with a hadronic
jet
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 600 \(p \stackrel{(-)}{p} \to W^{+} W^{-} j \to \ell_{1}^{+}\nu_{\ell_1} \ell_{2}^{-} \bar{\nu}_{\ell_2} j \) \( - \) \( - \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) 601 \(p \stackrel{(-)}{p} \to W^{+} W^{-} j \to q\bar{q} \ell^{-} \bar{\nu}_{\ell} j \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 602 \(p \stackrel{(-)}{p} \to W^{+} W^{-} j \to \ell^{+}\nu_{\ell} q\bar{q} j \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 610 \(p \stackrel{(-)}{p} \to W^{-} \gamma j \to \ell^{-} \bar{\nu}_{\ell} \gamma j \) \( - \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) 620 \(p \stackrel{(-)}{p} \to W^{+} \gamma j \to \ell^{+} \nu_{\ell} \gamma j \) \( - \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) 630 \(p \stackrel{(-)}{p} \to W^{-} Z j \to \ell_{1}^{-} \bar{\nu}_{\ell_1} \ell_{2}^{-} \ell_{2}^{+} j\) \( - \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) 640 \(p \stackrel{(-)}{p} \to W^{+} Z j \to \ell_{1}^{+}\nu_{\ell_1} \ell_{2}^{-} \ell_{2}^{+}j \) \( - \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) 650 \(p \stackrel{(-)}{p} \to Z Z j \to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \ell_{2}^{-} j \) \( - \) \( - \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) -
WH production in association with a hadronic jet
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 1600 \(p \stackrel{(-)}{p} \to W^+ H \, j \to \ell^+\nu_{\ell} H \, j \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 1601 \(p \stackrel{(-)}{p} \to W^+ H \, j \to \ell^+\nu_{\ell} \gamma\gamma \, j \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 1602 \(p \stackrel{(-)}{p} \to W^+ H \, j \to \ell^+\nu_{\ell} \mu^+\mu^- \, j \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 1603 \(p \stackrel{(-)}{p} \to W^+ H \, j \to \ell^+\nu_{\ell} \tau^+\tau^- \, j \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 1604 \(p \stackrel{(-)}{p} \to W^+ H \, j \to \ell^+\nu_{\ell} b\bar{b} \, j \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 1605 \(p \stackrel{(-)}{p} \to W^+ H \, j \to W^+ W^{+}W^{-} \, j \to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^+\nu_{\ell_{2}} \ell_{3}^- \bar{\nu}_{\ell_{3}}\, j \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 1606 \(p \stackrel{(-)}{p} \to W^+ H \, j \to W^+ ZZ \, j \to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \ell_{3}^+ \ell_{3}^-\, j \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 1607 \(p \stackrel{(-)}{p} \to W^+ H \, j \to W^+ ZZ \, j \to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \nu_{\ell_{3}} \bar{\nu}_{\ell_{3}}\, j \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 1610 \(p \stackrel{(-)}{p} \to W^- H \, j \to \ell^- \bar{\nu}_{\ell} H \, j \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 1611 \(p \stackrel{(-)}{p} \to W^- H \, j \to \ell^- \bar{\nu}_{\ell} \gamma\gamma \, j \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 1612 \(p \stackrel{(-)}{p} \to W^- H \, j \to \ell^- \bar{\nu}_{\ell} \mu^+\mu^- \, j \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 1613 \(p \stackrel{(-)}{p} \to W^- H \, j \to \ell^- \bar{\nu}_{\ell} \tau^+\tau^- \, j \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 1614 \(p \stackrel{(-)}{p} \to W^- H \, j \to \ell^- \bar{\nu}_{\ell} b\bar{b} \, j \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 1615 \(p \stackrel{(-)}{p} \to W^- H \, j \to W^- W^{+}W^{-} \, j \to \ell_{1}^-\bar{\nu}_{\ell_{1}} \ell_{2}^+\nu_{\ell_{2}} \ell_{3}^- \bar{\nu}_{\ell_{3}}\, j \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 1616 \(p \stackrel{(-)}{p} \to W^- H \, j \to W^- ZZ \, j \to \ell_{1}^-\bar{\nu}_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \ell_{3}^+ \ell_{3}^-\, j \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) 1617 \(p \stackrel{(-)}{p} \to W^- H \, j \to W^- ZZ \, j \to \ell_{1}^-\bar{\nu}_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \nu_{\ell_{3}} \bar{\nu}_{\ell_{3}}\, j \) \( - \) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \) -
Triple vector boson production in association with a hadronic
jet
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 800 \(p \stackrel{(-)}{p} \to W^{+} \gamma \gamma j \to \ell^{+} \nu_{\ell} \gamma \gamma j \) \(-\) \(\checkmark\) \(-\) \(-\) \(-\) \(-\) \(-\) 810 \(p \stackrel{(-)}{p} \to W^{-} \gamma \gamma j \to \ell^{-} \bar \nu_{\ell} \gamma \gamma j \) \(-\) \(\checkmark\) \(-\) \(-\) \(-\) \(-\) \(-\)
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W production in association with a hadronic jet
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QCD induced processes
-
QCD indiced production of a vector boson in association with
two jets
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 3120 \(p \stackrel{(-)}{p} \to Z \, jj\to \ell^{+} \ell^{-} \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 3121 \(p \stackrel{(-)}{p} \to Z \, jj\to \nu_{\ell} \bar{\nu}_{\ell} \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 3130 \(p \stackrel{(-)}{p} \to W^{+} \, jj\to \ell^{+} \nu_\ell \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 3140 \(p \stackrel{(-)}{p} \to W^{-} \, jj\to \ell^{-} \bar{\nu}_\ell \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) -
QCD induced diboson production in association with two
jets
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 3210 \(p \stackrel{(-)}{p} \to ZZ \, jj\to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \ell_{2}^{-} \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 3211 \(p \stackrel{(-)}{p} \to ZZ \, jj\to \ell_{1}^{+} \ell_{1}^{-} \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 3220 \(p \stackrel{(-)}{p} \to W^{+}Z \, jj\to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{+} \ell_{2}^{-} \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 3230 \(p \stackrel{(-)}{p} \to W^{-}Z \, jj\to \ell_{1}^{-} \bar{\nu}_{\ell _{1}} \ell_{2}^{+} \ell_{2}^{-} \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 3240 \(p \stackrel{(-)}{p} \to \gamma\gamma \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 3250 \(p \stackrel{(-)}{p} \to W^{+}W^{+} \, jj\to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{+} \nu_{\ell_{2}} \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 3260 \(p \stackrel{(-)}{p} \to W^{-}W^{-} \, jj\to \ell_{1}^{-} \bar{\nu}_{\ell_{1}} \ell_{2}^{-} \bar{\nu}_{\ell_{2}} \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 3270 \(p \stackrel{(-)}{p} \to W^{+}\gamma \, jj\to \ell^{+} \nu_{\ell} \gamma \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 3280 \(p \stackrel{(-)}{p} \to W^{-}\gamma \, jj\to \ell^{-} \bar{\nu}_{\ell} \gamma \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 3290 \(p \stackrel{(-)}{p} \to Z\gamma \, jj\to \ell^{+} \ell^{-} \gamma \, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) 3291 \(p \stackrel{(-)}{p} \to Z\gamma \, jj\to \nu_{\ell} \bar{\nu}_{\ell} \gamma\, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \)
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QCD indiced production of a vector boson in association with
two jets
-
Gluon fusion processes
-
Higgs boson production pluts two jets
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 4100 \(p \stackrel{(-)}{p} \to H \, jj\) \(-\) \(-\) \(-\) \(\checkmark\) \(-\) \(-\) \(\checkmark\) 4101 \(p \stackrel{(-)}{p} \to H \, jj \to \gamma\gamma \, jj\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(\checkmark\) 4102 \(p \stackrel{(-)}{p} \to H \, jj \to \mu^+\mu^- \, jj\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(\checkmark\) 4103 \(p \stackrel{(-)}{p} \to H \, jj \to \tau^+\tau^- \, jj\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(\checkmark\) 4104 \(p \stackrel{(-)}{p} \to H \, jj \to b\bar{b} \, jj\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(\checkmark\) 4105 \(p \stackrel{(-)}{p} \to H \, jj\to W^{+}W^{-} \, jj\to \ell_{1}^+\nu_{\ell_{1}} \ell_{2}^- \bar{\nu}_{\ell_{2}} \,jj\) \(-\) \(-\) \(\checkmark\) \(\checkmark\) \(-\) \(-\) \(\checkmark\) 4106 \(p \stackrel{(-)}{p} \to H \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \ell_{2}^+ \ell_{2}^- \,jj\) \(-\) \(-\) \(\checkmark\) \(\checkmark\) \(-\) \(-\) \(\checkmark\) 4107 \(p \stackrel{(-)}{p} \to H \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \,jj\) \(-\) \(-\) \(\checkmark\) \(\checkmark\) \(-\) \(-\) \(\checkmark\) -
Higgs boson production pluts three jets
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 4200 \(p \stackrel{(-)}{p} \to H \, jjj \) \(-\) \(-\) \(-\) \(\checkmark\) \(-\) \(-\) \(\checkmark\) -
diboson production
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 4300 \(p \stackrel{(-)}{p} \to W^{+}W^{-} \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{-}\bar{\nu}_{\ell_{2}} \) \(-\) \(-\) \(\checkmark\) \(-\) \(-\) \(-\) \(-\) 4330 \(p \stackrel{(-)}{p} \to ZZ \to \ell_{1}^{-} \ell_{1}^{+} \ell_{2}^{-} \ell_{2}^{+} \) \(-\) \(-\) \(\checkmark\) \(-\) \(-\) \(-\) \(-\) 4360 \(p \stackrel{(-)}{p} \to Z\gamma \to \ell_{1}^{-} \ell_{1}^{+} \gamma \) \(-\) \(-\) \(\checkmark\) \(-\) \(-\) \(-\) \(-\) 4370 \(p \stackrel{(-)}{p} \to \gamma\gamma \) \(-\) \(-\) \(\checkmark\) \(-\) \(-\) \(-\) \(-\) 4301 \(p \stackrel{(-)}{p} \to W^{+}W^{-} \to q \bar{q} \, \ell^{-}\bar{\nu}_{\ell} \) \(-\) \(-\) \(\checkmark\) \(-\) \(-\) \(-\) \(-\) 4302 \(p \stackrel{(-)}{p} \to W^{+}W^{-} \to \ell^{+} \nu_{\ell} \, q \bar{q} \) \(-\) \(-\) \(\checkmark\) \(-\) \(-\) \(-\) \(-\) 4331 \(p \stackrel{(-)}{p} \to ZZ \to q \bar{q} \, \ell^{-} \ell^{+} \) \(-\) \(-\) \(\checkmark\) \(-\) \(-\) \(-\) \(-\) -
diboson production in association with a hadronic jet
ProcId Process BLHA anom. gauge couplings anom. Higgs couplings Two-Higgs model Kaluza-Klein model Spin-2 model MSSM 4600 \(p \stackrel{(-)}{p} \to W^{+}W^{-} j \to \ell_{1}^{+} \nu_{\ell_{1}} \ell_{2}^{-}\bar{\nu}_{\ell_{2}} j \) \(-\) \(-\) \(\checkmark\) \(-\) \(-\) \(-\) \(-\) 4650 \(p \stackrel{(-)}{p} \to ZZ j \to \ell_{1}^{-} \ell_{1}^{+} \ell_{2}^{-} \ell_{2}^{+} j \) \(-\) \(-\) \(\checkmark\) \(-\) \(-\) \(-\) \(-\) 4601 \(p \stackrel{(-)}{p} \to W^{+}W^{-} j \to q\bar{q} \ell^{-}\bar{\nu}_{\ell} j \) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) 4602 \(p \stackrel{(-)}{p} \to W^{+}W^{-} j \to \ell^{+} \nu_{\ell} q\bar{q} j \) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\)
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Higgs boson production pluts two jets