Processes
  1. VBF Production Processes
  2. Single/Double/Triple boson
  3. Single/Double/Triple boson + 1 jet
  4. Gluon Fusion
  1. Vector Boson Fusion Production Processes
    • 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 \(p \stackrel{(-)}{p} \to H \gamma \, jj\to ZZ \gamma \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \gamma \,jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \)
  2. Single, Double and triple vector boson production
    • 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 \(p \stackrel{(-)}{p} \to \gamma \gamma \gamma \) \(\checkmark\) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \)
  3. 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 \(p \stackrel{(-)}{p} \to W^{-} \gamma \gamma j \to \ell^{-} \bar \nu_{\ell} \gamma \gamma j \) \(-\) \(\checkmark\) \(-\) \(-\) \(-\) \(-\) \(-\)
  4. 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 \(p \stackrel{(-)}{p} \to Z\gamma \, jj\to \nu_{\ell} \bar{\nu}_{\ell} \gamma\, jj\) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \) \( - \)
  5. 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 \(p \stackrel{(-)}{p} \to W^{+}W^{-} j \to \ell^{+} \nu_{\ell} q\bar{q} j \) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\) \(-\)