Last update on 01.08.2026
This web page contains the averages of the ratios of Branching Fractions
R(D*)=BF(B→D*τντ)/BF(B→D* l νl)
and R(D)=BF(B→Dτντ)/BF(B→D l νl).
In addition to the traditional 2-Dimensional (R(D), R(D*)) average, a 3D average of R(D), R(D*) and tau polarisation Pτ(D*) is also reported.
In the present average we consider the following measurements:
The preliminary BaBar result using semileptonic tagging sample presented at Moriond 2026 [talk] is not included in our nominal averages, as the systematic uncertainties and checks are still being finalised by the Collaboration ([talk at ICHEP 2026]). However we report also averages including the result for completeness. The poor quality of these averages reflects the incompatibility of the inputs (contributions to the chi2 of the average and compatibility of each measurement with the average are included for the 2D average).
In the average we assume 100% correlation for the systematic uncertainties associated with the B→D(*) form factors, the D** composition and shapes, and the τ branching fractions. The other uncertainties are considered uncorrelated between the various experiments. The average is obtained using the the CoCo averaging tool.| Experiment | R(D*) | R(D) | Rescaled Correlation (stat/total) |
Pτ(D*) | Correlation (R(D*),Pτ(D*)) (stat/total) |
Inputs | Remarks |
|---|---|---|---|---|---|---|---|
| BaBar | 0.332 ± 0.024 ± 0.018 | 0.440 ± 0.058 ± 0.042 | -0.45/-0.27 | - | - | input | Phys.Rev.Lett. 109,101802 (2012) arXiv:1205.5442_[hep-ex] Phys.Rev.D 88, 072012 (2013) arXiv:1303.0571_[hep-ex] |
| BELLEa | 0.293 ± 0.038 ± 0.015 | 0.375 ± 0.064 ± 0.026 | -0.56/-0.49 | - | - | input, input2D | Phys.Rev.D 92, 072014 (2015) arXiv:1507.03233 [hep-ex] |
| BELLEb | 0.270 ± 0.035 + 0.028-0.025 | - | - | -0.38 ± 0.51 + 0.21-0.16 | 0.29/0.33 | input | Phys.Rev.Lett.118,211801 (2017) arXiv:1612.00529 [hep-ex] Phys.Rev.D 97, 012004 (2018) arXiv:1709.00129_[hep-ex] |
| BELLEc | 0.283 ± 0.018 ± 0.014 | 0.307 ± 0.037 ± 0.016 | -0.53/-0.51 | - | - | input | Phys.Rev.Lett. 124 (2020) 16, 161803 arXiv:1910.05864 [hep-ex] |
| LHCba | 0.281 ± 0.018 ± 0.024 | 0.441 ± 0.060 ± 0.066 | -0.49/-0.43 | - | - | input | Phys. Rev. Lett. 131, 111802 [arXiv:2302.02886] |
| LHCbb | 0.267 ± 0.012 ± 0.019 | - | - | - | - | input | Phys. Rev. D 108, 012018 [arXiv:2305.01463] |
| LHCbc | 0.402 ± 0.081 ± 0.085 | 0.249 ± 0.043 ± 0.047 | -0.48/-0.39 | - | - | input | Phys. Rev. Lett. 134, 061801 (2025) [arXiv:2406.03387] |
| Belle IIb | 0.306 ± 0.034 ± 0.018 | 0.418 ± 0.074 ± 0.051 | -0.27/-0.22 | - | - | input | Phys. Rev. D 112 (2025) 3, 032010 [arXiv:2504.11220] |
| Belle IIa | 0.242 ± 0.019 ± 0.016 | 0.439 ± 0.055 ± 0.046 | -0.40/-0.20 | - | - | input | Presented at CKM 2025 [talk] |
| Belle IIc | 0.222 ± 0.041 ± 0.030 | - | - | -0.33 ± 1.15 ± 0.65 | 0.25 (prelim.) | input, input2D | Presented at ICHEP 2026 [talk] |
| 2D Average
(R(D),R(D*)) logfile.txt |
0.280 ± 0.011 | 0.359 ± 0.024 | -0.37 | - | - | chi2/dof = 17.656/15 (CL = 0.28) |
R(D)-R(D*), 68% C.L. contours rdrds.pdf
chi2 contributions chi2contributions.pdf and compatibility (in number of σ) of each measurement with the average nsigma.pdf R(D) .pdf R(D*) .pdf |
| 3D Average
(R(D),R(D*),Pτ(D*)) logfile.txt |
0.280 ± 0.011 | 0.359 ± 0.024 | -0.37 | -0.298 ± 0.481 | 0.10 (Corr (Pτ(D*),R(D*))) -0.03 (Corr (Pτ(D*),R(D))) |
chi2/dof = 17.72/16 (CL = 0.34) | Pτ(D*)-R(D*), 68% C.L. contours ptaurds.pdf
Pτ(D*)-R(D), 68% C.L. contours ptaurd.pdf R(D)-R(D*), 68% C.L. contours rdrds.pdf |
| BaBarb | 0.226 ± 0.022 ± 0.012 | 0.316 ± 0.062 ± 0.019 | -0.94/-0.82 | - | - | input | Presented at Moriond 2026 [talk] |
| 2D Average
(R(D),R(D*)) (including BaBarb)) logfile.txt |
0.262 ± 0.010 | 0.337 ± 0.022 | -0.51 | - | - | chi2/dof = 33.406/17 (CL = 0.01) |
R(D)-R(D*), 68% C.L. contours rdrds.pdf
chi2 contributions chi2contributions.pdf and compatibility (in number of σ) of each measurement with the average nsigma.pdf |
| 3D Average
(R(D),R(D*),Pτ(D*)) (including BaBarb)) logfile.txt |
0.262 ± 0.010 | 0.337 ± 0.022 | -0.51 | -0.388 ± 0.480 | 0.09 (Corr (Pτ(D*),R(D*))) -0.04 (Corr (Pτ(D*),R(D))) |
chi2/dof = 33.454/18 (CL = 0.01) |
SM predictions for R(D) based on following Lattice calculations:
The SM prediction for R(D*) widely used for many HFLAV reports was:
In 2021 FNAL/MILC released the first unquenched Lattice calculation of B→D*l ν form factors at non-zero recoil,
A.Bazavov et al. [Eur. Phys. J. C 82, 1141 (2022)] ,
predicting a value of R(D*)=0.265 ± 0.013, using only Lattice inputs.
In addition, since 2023, two indipendent lattice calculations at non-zero recoil are available: from HPQCD arXiv:2304.03137[hep-lat] (R(D*)=0.273 ± 0.015), and JLQCD arXiv:2306.05657[hep-lat] (R(D*)=0.252 ± 0.022), have been released.
Various indipendent analyses of these three lattice data has been performed by various groups. The first were performed by G. Martinelli et al. [Eur. Phys. J. C 84 (2024) 400] and I.Ray et al. [JHEP 01 (2024) 022], and the results reported in the table below. In these papers result combined with experimental inputs from Belle and Belle II on B→D*l ν are reported along with results based on lattice only calculations.
In the following table SM predictions are reported along with the compatibility of the current 2D (R(D),R(D*)) HFLAV average with each of them. The correlation between R(D) and R(D*) theory prediction has been used when avaialable in the publication.
| R(D) | R(D*) | Compatibility in σ | |
|---|---|---|---|
| D.Bigi, P.Gambino, Phys.Rev. D94 (2016) no.9, 094008 [arXiv:1606.08030 [hep-ph]] | 0.299 ± 0.003 | 2.48 | |
| M.Bordone, M.Jung, Danny van Dyk, Eur.Phy.J.C 80 (2020) 2, 74 [arXiv:1908.09398 [hep-ph]] | 0.298 ± 0.003 | 0.247 ± 0.006 | 4.07 |
| G. Martinelli, S. Simula, L. Vittorio, Phys.RevD 105 (2022) 3, 034503 [arXiv:2105.08674 [hep-ph]] | 0.296 ± 0.008 | 2.49 | |
| F. U. Bernlochner, Z. Ligeti, M. Papucci, M. T. Prim, D. J. Robinson, C. Xiong, Phys. Rev. D 106 (2022) 096015 [arXiv:2206.11281 [hep-ph]] | 0.288 ± 0.004 | 0.249 ± 0.003 | 4.61 |
| I.Ray, S.Nandi, JHEP 01 (2024) 022 [arXiv:2305.11855 [hep-lat]] | 0.304 ± 0.003 | 0.258 ± 0.012 | 2.55 |
| FLAG Collaboration, [arXiv:2411.04268 [hep-lat]] | 0.2938 ± 0.0054 | 2.65 | |
| BaBar Collaboration, Phys.Rev.Lett. 123 (2019) 9, 091801 [arXiv:1903.10002 [hep-ex]] | 0.253 ± 0.005 | 2.27 | |
| P.Gambino, M.Jung, S.Schacht, Phys.Lett.B795 (2019) 386 [arXiv:1905.08209 [hep-ph]] | 0.254 + 0.007 − 0.006 | 2.06 | |
| G. Martinelli, S. Simula, L. Vittorio, Eur. Phys. J. C 84 (2024) 400 [arXiv:2310.03680 [hep-ph]] | 0.262 ± 0.009 | 1.27 | |
| Arithmetic average | 0.296 ± 0.004 | 0.254 ± 0.005 | 3.73 |
| FLAG Collaboration, R(D*) Nf=2+1 [arXiv:2411.04268 [hep-lat]] | 0.2938 ± 0.0054 | 0.2582 ± 0.0051 | 3.47 |
| FLAG Collaboration, R(D*) Nf=2+1+1 [arXiv:2411.04268 [hep-lat]] | 0.2938 ± 0.0054 | 0.275 ± 0.015 | 2.31 |
| FLAG Collaboration, R(D*) G. Martinelli et. al. [arXiv:2411.04268 [hep-lat], arXiv:2310.03680 [hep-ph]] | 0.2938 ± 0.0054 | 0.262 ± 0.009 | 2.94 |
R(D) and R(D*) exceed the SM predictions (arithmetic average) given above, by 2.6σ and 2.2σ respectively. Considering the R(D)-R(D*)) correlation of -0.371, the resulting combined χ2 is 17.15 for 2 degree of freedom, corresponding to a p-value of 1.89 x 10-4. The difference with the SM predictions reported above, corresponds to about 3.7σ.
In the following table SM predictions are reported along with the compatibility of the current 3D (R(D),R(D*),Pτ(D*)) HFLAV average with each of them. The correlation between R(D) and R(D*) theory prediction has been used when avaialable in the publication. The SM prediction for the tau polarisation Pτ(D*)= -0.497 ± 0.007 (Phys. Rev. D 871,202 034028 (2013)) has been considered.
| R(D) | R(D*) | Compatibility in σ | |
|---|---|---|---|
| D.Bigi, P.Gambino, Phys.Rev. D94 (2016) no.9, 094008 [arXiv:1606.08030 [hep-ph]] | 0.299 ± 0.003 | 2.48 | |
| M.Bordone, M.Jung, Danny van Dyk, Eur.Phy.J.C 80 (2020) 2, 74 [arXiv:1908.09398 [hep-ph]] | 0.298 ± 0.003 | 0.247 ± 0.006 | 3.75 |
| G. Martinelli, S. Simula, L. Vittorio, Phys.RevD 105 (2022) 3, 034503 [arXiv:2105.08674 [hep-ph]] | 0.296 ± 0.008 | 2.49 | |
| F. U. Bernlochner, Z. Ligeti, M. Papucci, M. T. Prim, D. J. Robinson, C. Xiong, Phys. Rev. D 106 (2022) 096015 [arXiv:2206.11281 [hep-ph]] | 0.288 ± 0.004 | 0.249 ± 0.003 | 4.30 |
| I.Ray, S.Nandi, JHEP 01 (2024) 022 [arXiv:2305.11855 [hep-lat]] | 0.304 ± 0.003 | 0.258 ± 0.012 | 2.22 |
| FLAG Collaboration, [arXiv:2411.04268 [hep-lat]] | 0.2938 ± 0.0054 | 2.65 | |
| BaBar Collaboration, Phys.Rev.Lett. 123 (2019) 9, 091801 [arXiv:1903.10002 [hep-ex]] | 0.253 ± 0.005 | 2.27 | |
| P.Gambino, M.Jung, S.Schacht, Phys.Lett.B795 (2019) 386 [arXiv:1905.08209 [hep-ph]] | 0.254 + 0.007 − 0.006 | 2.06 | |
| G. Martinelli, S. Simula, L. Vittorio, Eur. Phys. J. C 84 (2024) 400 [arXiv:2310.03680 [hep-ph]] | 0.262 ± 0.009 | 1.27 | |
| Arithmetic average | 0.296 ± 0.004 | 0.254 ± 0.005 | 3.41 |
| FLAG Collaboration, R(D*) Nf=2+1 [arXiv:2411.04268 [hep-lat]] | 0.2938 ± 0.0054 | 0.2582 ± 0.0051 | 3.14 |
| FLAG Collaboration, R(D*) Nf=2+1+1 [arXiv:2411.04268 [hep-lat]] | 0.2938 ± 0.0054 | 0.275 ± 0.015 | 1.98 |
| FLAG Collaboration, R(D*) G. Martinelli et. al. [arXiv:2411.04268 [hep-lat], arXiv:2310.03680 [hep-ph]] | 0.2938 ± 0.0054 | 0.262 ± 0.009 | 2.60 |
When including the latest preliminary BaBar result (BaBarb), the compatibility with the SM (HFLAV aritmetic average) is of about 1.99σ for the 2D (R(D),R(D*)) average, and 1.63 σ for the 3D (R(D),R(D*),Pτ(D*)) average.