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Constraints on exclusive branching fractions $BF_i(B^+\to X_c^il^+ν)$ from moment measurements in inclusive $B\to X_clν$ decays

As an alternative to direct measurements, we extract exclusive branching fractions of semileptonic B-meson decays to charmed mesons, $BF_i(B\to X_c^ilν)$ with $X_c^i = D, D^*, D_0, D'_1, D_1, D_2, D', D'^*$ and non-resonant final states $(D^{(*)}π)_{nr}$, from a fit to electron energy, hadronic mass and combined hadronic mass-energy moments measured in inclusive $B\to X_clν$ decays. The fit is performed by constraining the sum of exclusive branching fractions to the measured value of $BF(B\to X_clν)$, and with different sets of additional constraining terms for the directly measured branching fractions. There is no fit scenario in which a single branching fraction alone is enhanced to close the gap between $BF(B\to X_clν)$ and the sum of known branching fractions $BF_i(B\to X_c^ilν)$. The fitted $BF(B\to D^*lν)$ is 5% to 10% larger than the direct measurement depending on whether or not $BF(B\to D^*lν)$ is constrained to its direct measurement. $BF(B\to Dlν)$ values are in good agreement with the direct measurement unless $BF(B\to D^*lν)$ is constrained, which results in a higher $BF(B\to Dlν)$ value. Within large uncertainties, $BF(B\to D'_1lν)$ agrees with direct measurements. Depending on the fit scenario, $BF(B\to D_0lν)$ is consistent with or larger than its direct measurement. The fit is not able to easily disentangle $B\to D_1lν$ and $B\to D_2lν$, and tends to increase the sum of these two branching fractions. $BF(B\to (D^{(*)}π)_{nr}lν)$ with non-resonant $(D^{(*)}π)_{nr}$ final states is found to be 0.2-0.4%, consistent with $B\to D^{(*)}πlν$ and $B\to D^{**}(D^{(*)}π)lν$ measurements. No indication is found for significant contributions from so far unmeasured $B\to D'^{(*)}lν$ decays assuming that the $D'$ and $D'^*$ can be identified with the observed $D(2550)$, respectively, $D^*(2600)$ state.