Simplified Limits on New LHC Resonances
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![Figure 1. Left: The experimental ATLAS [12] upper limits (solid red curves) and expected limits (dashed bluecurves) yield these upper bounds on the branching ratio product [BR(R → WLZL)]2 assuming production of an s-channel resonance R via vector boson fus](https://thumb-us.123doks.com/thumbv2/123dok_us/8148857.1358765/6.482.46.439.79.246/figure-experimental-expected-bluecurves-branching-assuming-production-resonance.webp)
![Figure 2. Left: The experimental ATLAS [12] upper limits and expected limits on the production cross-sectionfor WZ → R → WZ yield these upper bounds on ζ assuming production of the s-channel resonance R via vectorboson fusion alone](https://thumb-us.123doks.com/thumbv2/123dok_us/8148857.1358765/7.482.46.439.80.247/experimental-expected-production-sectionfor-assuming-production-resonance-vectorboson.webp)
![Figure 3. Experimental observed (solid red) and expected (dashed blue) upper bounds [35] on ζ for productionof an s-channel resonance R via photon fusion and subsequent decay to diphotons](https://thumb-us.123doks.com/thumbv2/123dok_us/8148857.1358765/8.482.44.440.342.505/experimental-observed-expected-productionof-channel-resonance-subsequent-diphotons.webp)
![Figure 4. Experimental observed (solid red) and expected (dashed blue) upper bounds [35] on ζ for productionof an s-channel resonance R via gluon fusion and subsequent decay to diphotons](https://thumb-us.123doks.com/thumbv2/123dok_us/8148857.1358765/10.482.45.440.80.248/experimental-observed-expected-productionof-channel-resonance-subsequent-diphotons.webp)
![Figure 5. In these plots in the ζ vs. resonance mass plane, the shaded region corresponds to values of ζ consistentwith upper bounds on branching ratios as described in [4] (1 for the upper left pane and 1/4 for the other panes) andΓ/M ≤ 10%](https://thumb-us.123doks.com/thumbv2/123dok_us/8148857.1358765/11.482.49.431.76.415/figure-resonance-region-corresponds-values-consistentwith-branching-described.webp)
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