| 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 | \(p \stackrel{(-)}{p} \rightarrow H j j \rightarrow ZZ j j \rightarrow q \bar{q} \ell^+ \ell^- j j\) | \( - \) | \( - \) | \( \checkmark \) | \( - \) | \( - \) | \( - \) | \( \checkmark \) |
| 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 | \(p \stackrel{(-)}{p} \rightarrow H j j j \rightarrow ZZjjj \rightarrow \ell_1^+ \ell_1^- \nu_{\ell_2} \bar{\nu}_{\ell_2} j j j\) | \( - \) | \( - \) | \( \checkmark \) | \( - \) | \( - \) | \( - \) | \( \checkmark \) |
| 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 | \(p \stackrel{(-)}{p} \to \gamma \, jj\) | \( \checkmark \) | \( \checkmark \) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) |
| 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 | \(p \stackrel{(-)}{p} \to HH \, jj \to b\bar{b}\gamma\gamma \, jj\) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) |
| 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 | \(p \stackrel{(-)}{p} \to S_{2} \, jj \to ZZ \, jj \to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \, jj\) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) | \( \checkmark \) | \( - \) |
| 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 | \(p \stackrel{(-)}{p} \to Z\gamma \, jj\to \nu_{\ell}\bar{\nu}_{\ell} \gamma \, jj\) | \( \checkmark \) | \( \checkmark \) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) |
| 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 | \(p \stackrel{(-)}{p} \to H \gamma \, jj\to ZZ \gamma \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \gamma \,jj\) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) |
| 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 | \(p \stackrel{(-)}{p} \to W^- \to \ell^- \bar{\nu}_{\ell}\) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) |
| 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 | \(p \stackrel{(-)}{p} \to W^- H \to W^- ZZ \to \ell_{1}^-\bar{\nu}_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \nu_{\ell_{3}} \bar{\nu}_{\ell_{3}}\) | \(-\) | \( \checkmark \) | \(-\) | \(-\) | \(-\) | \(-\) | \(-\) |
| 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 | \(p \stackrel{(-)}{p} \to \gamma\gamma \) | \(-\) | \(-\) | \(-\) | \(-\) | \(-\) | \(-\) | \(-\) |
| 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 | \(p \stackrel{(-)}{p} \to \gamma \gamma \gamma \) | \(\checkmark\) | \(\checkmark\) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) |
| 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 | \(p \stackrel{(-)}{p} \to W^- \, j \to \ell^- \bar{\nu}_{\ell} \, j\) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) |
| 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 | \(p \stackrel{(-)}{p} \to Z Z j \to \ell_{1}^{+} \ell_{1}^{-} \ell_{2}^{+} \ell_{2}^{-} j \) | \( - \) | \( - \) | \( - \) | \(\checkmark\) | \( - \) | \( - \) | \( - \) |
| 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 | \(p \stackrel{(-)}{p} \to W^- H \, j \to W^- ZZ \, j \to \ell_{1}^-\bar{\nu}_{\ell_{1}} \ell_{2}^+ \ell_{2}^- \nu_{\ell_{3}} \bar{\nu}_{\ell_{3}}\, j \) | \( - \) | \(\checkmark\) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) |
| 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 | \(p \stackrel{(-)}{p} \to W^{-} \gamma \gamma j \to \ell^{-} \bar \nu_{\ell} \gamma \gamma j \) | \(-\) | \(\checkmark\) | \(-\) | \(-\) | \(-\) | \(-\) | \(-\) |
| 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 | \(p \stackrel{(-)}{p} \to W^{-} \, jj\to \ell^{-} \bar{\nu}_\ell \, jj\) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) |
| 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 | \(p \stackrel{(-)}{p} \to Z\gamma \, jj\to \nu_{\ell} \bar{\nu}_{\ell} \gamma\, jj\) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) | \( - \) |
| 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 | \(p \stackrel{(-)}{p} \to H \, jj\to ZZ \, jj\to \ell_{1}^+ \ell_{1}^- \nu_{\ell_{2}} \bar{\nu}_{\ell_{2}} \,jj\) | \(-\) | \(-\) | \(\checkmark\) | \(\checkmark\) | \(-\) | \(-\) | \(\checkmark\) |
| ProcId | Process | BLHA | anom. gauge couplings | anom. Higgs couplings | Two-Higgs model | Kaluza-Klein model | Spin-2 model | MSSM |
|---|---|---|---|---|---|---|---|---|
| 4200 | \(p \stackrel{(-)}{p} \to H \, jjj \) | \(-\) | \(-\) | \(-\) | \(\checkmark\) | \(-\) | \(-\) | \(\checkmark\) |
| 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 | \(p \stackrel{(-)}{p} \to ZZ \to q \bar{q} \, \ell^{-} \ell^{+} \) | \(-\) | \(-\) | \(\checkmark\) | \(-\) | \(-\) | \(-\) | \(-\) |
| 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 | \(p \stackrel{(-)}{p} \to W^{+}W^{-} j \to \ell^{+} \nu_{\ell} q\bar{q} j \) | \(-\) | \(-\) | \(-\) | \(-\) | \(-\) | \(-\) | \(-\) |