Processes
  1. Vector Boson Fusion Production Processes
  2. Single, Double and triple vector boson production
  3. Single, double and triple vector boson production plus one jet
  4. Gluon Fusion Processes
  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 \(p \stackrel{(-)}{p} \to \gamma \gamma \gamma \) \(\checkmark\) \(\checkmark\) \( - \) \( - \) \( - \) \( - \) \( - \)
  • Single, double and triple vector boson production plus one jet
  • QCD induced processes
  • Gluon fusion processes