Abstract
Very recent experimental information obtained from the Belle experiment, along with that accumulated by the BABAR and LHCb experiments, has shown the existence of anomalies in the ratios $R(D)$ and $R(D^{*})$ associated with the charged-current transition $b \to c \tau \bar{\nu}_\tau$. Although the Belle measurements are in agreement with the standard model (SM) predictions, the new experimental world averages still exhibit a tension. In addition, the $D^\ast$ longitudinal polarization $F_L(D^\ast)$ related with the channel $B \to D^\ast \tau \bar{\nu}_\tau$ observed by the Belle Collaboration and the ratio $R(J/\psi)$ measured by the LHCb Collaboration also show discrepancies with their corresponding SM estimations. We present a model-independent study based on the most general effective Lagrangian that yields a tree-level effective contribution to the transition $b \to c \tau \bar{\nu}_\tau$ induced by a general $W^\prime$ boson. Instead of considering any specific new physics (NP) realization, we perform an analysis by considering all of the different chiral charges to the charm-bottom and $\tau$-$\nu_{\tau}$ interaction terms with a charged $W^\prime$ boson that explain the anomalies. We present a phenomenological study of parameter space allowed by the new experimental $b \to c \tau \bar{\nu}_\tau$ data and with the mono-tau signature $pp \to \tau_h X + \rm{MET}$ at the LHC. For comparison, we include some of the $W^\prime$ boson NP realizations that have already been studied in the literature.
Highlights
The B meson system has constituted a good scenario for studying, on both theoretical and experimental levels, the standard model (SM) as well as for exploring new physics (NP) effects at low-energy scales
Motivated by the new Heavy Flavor Averaging Group (HFLAV) world average values on the ratios RðDðÃÞÞ, due to the recent Belle measurements, we addressed the anomalies RðDðÃÞÞ related to the chargedcurrent transition b → cτντ within a general W0 boson scenario
In order to provide a robust analysis, we considered in addition the available experimental information on all of the charged transition b → cτντ observables—namely, the ratios RðJ=ψÞ, RðXcÞ and the polarizations PτðDÃÞ, FLðDÃÞ, as well as the upper limit BRðB−c → τ−ντÞ < 10%
Summary
The B meson system has constituted a good scenario for studying, on both theoretical and experimental levels, the standard model (SM) as well as for exploring new physics (NP) effects at low-energy scales. We present a phenomenological analysis of parameter space allowed by the experimental data, and for comparison, we include some of the W0 boson NP realizations that have already been studied in the literature [95,100,101,104,105,106,108,109,110] Most of these models were implemented by considering the previous HFLAV averages and, in addition, not all of them considered the polarization observables PτðDÃÞ and FLðDÃÞ; we explore which of these benchmark models are still favored (or disfavored) by the new b → cτντ data.
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