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Search for a Heavy Resonance Decaying İnto a Z Boson and a Vector Boson in the νν¯¯¯qq¯¯¯ Final State

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Figure 1. Comparison of data and simulated events. Left: the corrected mass of the leading AK8 jet, interpreted as the hadronically decaying vector boson
Figure 2. Background yield prediction in the signal region obtained with the α method, in the low-purity (left) and high-purity (right) categories
Figure 3. Expected background shapes as a function of the transverse mass of the diboson can- can-didate obtained using the α method in the low-purity (left) and high-purity (right) categories, represented as colored areas bounded by smooth functions
Figure 4. The observed and expected limits on the product of the cross section and branching fraction σB(W 0 → W had Z inv ) for a spin-1 HVT signal hypothesis (left) and σB(G → Z had Z inv ) for

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