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The triplet vector boson (TVB) is a simplified new physics model involvingmassive vector bosons transforming as a weak triplet vector. Such a model hasbeen proposed as a combined explanation of the anomalous $b \to s\mu^+\mu^-$and $b \to c \tau\bar{\nu}_\tau$ data (the so-called $B$ meson anomalies). Inthis work, we carry out an updated view of the TVB model by incorporating themost recent 2022 and 2023 LHCb measurements on the lepton flavor universalityratios $R(D^{(\ast)}) = {\rm BR}(B \to D^{(\ast)}\tau \bar{\nu}_\tau)/{\rmBR}(B \to D^{(\ast)}\ell^\prime \bar{\nu}_{\ell^\prime})$, $R(\Lambda_c) = {\rmBR}(\Lambda_b \to \Lambda_c\tau\bar{\nu}_\tau)/{\rm BR}(\Lambda_b \to\Lambda_c\mu\bar{\nu}_\mu)$, and $R_{K^{(\ast)}} = {\rm BR}(B \toK^{(\ast)}\mu^+\mu^-)/{\rm BR}(B \to K^{(\ast)}e^+e^-)$. We perform a globalfit to explore the allowed parameter space by the new data and all relevantlow-energy flavor observables. Our results are confronted with the recenthigh-mass dilepton searches at the Large Hadron Collider (LHC). We find thatfor a heavy TVB mass of 1 TeV a common explanation of the $B$ meson anomaliesis possible for all data with the recent LHCb measurements on $R(D^{(\ast)})$,in consistency with LHC constraints. However, this framework is in strongtension with LHC bounds when one considers all data along with the worldaverage values (BABAR, Belle, and LHCb) on $R(D^{(\ast)})$. Future measurementswill be required in order to clarify such a situation. In the end, theimplications of our phenomenological analysis of the TVB model to some knownflavor parametrizations are also discussed.

$B$ meson anomalies within the triplet vector boson model to the light of recent measurements from LHCb