What can a heavy $U(1)_{\rm B-L}$ $Z^\prime$ boson do to the muon $(g-2)_\mu$ anomaly and to a new Higgs boson mass?
Ant\'onio P. Morais, Roman Pasechnik, J. Pedro Rodrigues

TL;DR
The paper examines whether a heavy $U(1)_{B-L}$ $Z'$ boson can explain the muon $(g-2)_$ anomaly and influence the Higgs boson mass, concluding it cannot resolve the anomaly with current constraints.
Contribution
It provides a phenomenological analysis of the $U(1)_{B-L}$ extension, showing the heavy $Z'$ boson cannot account for the muon $(g-2)_$ anomaly within experimental bounds.
Findings
The $Z'$ contribution to muon $(g-2)_$ is at most $8.9 imes 10^{-12}$.
Heavy $Z'$ boson mass range is 6.3 to 6.5 TeV, within future LHC reach.
Minimal Higgs mass is around 400 GeV with heavy $Z'$ boson.
Abstract
The minimal extension of the Standard Model (B-L-SM) offers an explanation for neutrino mass generation via a seesaw mechanism as well as contains two new physics states such as an extra Higgs boson and a new gauge boson. The emergence of a second Higgs particle as well as a new gauge boson, both linked to the breaking of a local symmetry, makes the B-L-SM rather constrained by direct searches at the Large Hadron Collider (LHC) experiments. We investigate the phenomenological status of the B-L-SM by confronting the new physics predictions with the LHC and electroweak precision data. Taking into account the current bounds from direct LHC searches, we demonstrate that the prediction for the muon anomaly in the B-L-SM yields at most a contribution of approximately which represents a tension of …
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