Angular Analysis of B to D^(*)ell bar{ν}_(ell) from Lattice and Experiment: |V_(cb)| and New Physics Constraints
Pith reviewed 2026-06-26 08:15 UTC · model grok-4.3
The pith
Combined lattice and experimental analysis determines |V_cb| = 0.03997(71) and excludes new physics mediated by scalar leptoquarks below 1 TeV.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The authors determine |V_cb| = 0.03997(71) in the massless lepton approximation using a joint fit to lattice form-factor data and experimental angular coefficients. They find no resolution of the exclusive-inclusive puzzle. At the 68% confidence level, new physics mediated by a scalar leptoquark is excluded at effective scales below 1.0 TeV and new physics mediated by a vector leptoquark or colourless scalar boson is excluded below 2.5 TeV.
What carries the argument
The Boyd-Grinstein-Lebed (BGL) ansatz for form-factor parameterization, with unitarity constraints as Bayesian priors, enabling a joint Bayesian fit of lattice data and experimental angular coefficients to extract |V_cb| and constrain Wilson coefficients.
If this is right
- The extracted |V_cb| value of 0.03997(71) does not resolve the exclusive-inclusive |V_cb| puzzle.
- Wilson coefficients for scalar and tensor currents are constrained by the joint fit.
- Scalar leptoquark new physics is excluded below an effective scale of 1.0 TeV at 68% CL.
- Vector leptoquark or colourless scalar boson new physics is excluded below 2.5 TeV at 68% CL.
- Renormalisation group evolution in SMEFT is used to connect the constraints to TeV-scale new physics.
Where Pith is reading between the lines
- The method of joint lattice-experiment fits with BGL priors could be extended to other semileptonic B decays to further test new physics scenarios.
- If future lattice calculations reduce uncertainties in form factors, the bounds on new physics scales could be strengthened.
- The lack of resolution in the |V_cb| puzzle suggests that either new physics affects both exclusive and inclusive channels similarly or the discrepancy arises from other sources.
- These constraints assume the validity of the SMEFT framework for running the Wilson coefficients down to low energies.
Load-bearing premise
The Boyd-Grinstein-Lebed ansatz with unitarity constraints imposed as Bayesian priors provides an accurate parameterization of the lattice form factors without residual systematic effects that bias the fit to the angular coefficients.
What would settle it
A new high-precision measurement of the angular coefficients in B to D* lepton neutrino that deviates from the predictions of the fitted form factors and |V_cb| value by more than the reported uncertainties.
read the original abstract
We present a combined angular analysis within and beyond the Standard Model (SM) of experimental measurements for the $B \to D^{*}\ell \bar{\nu}_{\ell}$ angular coefficients provided by the Belle collaboration, together with lattice-calculated hadronic form-factor data from the HPQCD, JLQCD, and FNAL/MILC collaborations. We focus on determining the CKM matrix element $|V_{cb}|$ and constraining a set of Wilson coefficients associated with new physics (NP) mediated by scalar and tensor currents. SM predictions for the angular coefficients are obtained using form-factor parameterisations based on the Boyd-Grinstein-Lebed (BGL) ansatz, with unitarity constraints imposed as Bayesian priors. Experimental and theoretical data are analysed jointly by considering the cases $\ell = e, \mu$ separately and comparing with the massless approximation. For the latter, we determine $|V_{cb}| = 0.03997(71)$, with no resolution of the exclusive-inclusive puzzle. Using the full expressions for the angular coefficients in the presence of scalar, vector, and tensor currents, the corresponding Wilson coefficients are constrained through a joint Bayesian fit to lattice and experimental data. By including the renormalisation group evolution of the Wilson coefficients in the SM effective field theory (SMEFT), these constraints translate into bounds on the effective scale of potential heavy NP at the TeV scale. We find, at the $68\%$ confidence level, that NP mediated by a scalar leptoquark and a vector leptoquark/colourless scalar boson are excluded at the effective scales 1.0 and 2.5 TeV, respectively.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript performs a joint Bayesian fit of lattice QCD form-factor data (HPQCD, JLQCD, FNAL/MILC) for B→D* transitions with Belle experimental angular coefficients in B→D*ℓνℓ, employing the BGL parameterization with unitarity constraints imposed as priors. In the SM it extracts |V_cb|=0.03997(71) (no resolution of the exclusive-inclusive tension) and, allowing scalar/vector/tensor NP operators, constrains the associated Wilson coefficients; after SMEFT RGE evolution these translate into 68% CL lower bounds of 1.0 TeV and 2.5 TeV on the effective scales of scalar-leptoquark and vector-leptoquark/colourless-scalar models, respectively.
Significance. If the BGL representation is shown to be free of appreciable residual truncation bias, the work supplies a statistically coherent extraction of |V_cb| from angular observables together with TeV-scale NP limits that incorporate full RGE running. The explicit use of unitarity as Bayesian priors and the separate treatment of e/μ channels are methodological strengths that improve upon purely phenomenological fits.
major comments (1)
- [Abstract] Abstract and the description of the form-factor parameterization: the central |V_cb| value and the derived NP scale bounds both rest on the assumption that the BGL series (truncated at a finite order) with unitarity priors supplies an unbiased representation of the lattice data over the full kinematic range. No numerical estimate of the residual truncation error after the priors are applied, nor a cross-check against an independent parameterization (BCL or z-expansion without unitarity priors), is reported; such a quantification is required to confirm that shape distortions do not shift the joint posterior for |V_cb| and the scalar/tensor Wilson coefficients.
minor comments (1)
- [Abstract] The abstract states that ℓ=e and ℓ=μ are analysed separately and compared with the massless limit, but the numerical impact of the lepton-mass terms on the extracted |V_cb| and Wilson-coefficient bounds is not quantified in the provided summary; a short table or sentence would clarify whether the difference is negligible.
Simulated Author's Rebuttal
We thank the referee for their careful reading of the manuscript and for highlighting this important methodological point. We address the comment below.
read point-by-point responses
-
Referee: [Abstract] Abstract and the description of the form-factor parameterization: the central |V_cb| value and the derived NP scale bounds both rest on the assumption that the BGL series (truncated at a finite order) with unitarity priors supplies an unbiased representation of the lattice data over the full kinematic range. No numerical estimate of the residual truncation error after the priors are applied, nor a cross-check against an independent parameterization (BCL or z-expansion without unitarity priors), is reported; such a quantification is required to confirm that shape distortions do not shift the joint posterior for |V_cb| and the scalar/tensor Wilson coefficients.
Authors: We agree that an explicit quantification of residual truncation effects would strengthen the robustness of the results. Although the unitarity priors are intended to regularize the series and penalize unphysical coefficient values, we did not report a dedicated numerical estimate of the remaining bias or a cross-validation against the BCL parameterization. In the revised manuscript we will add a dedicated subsection that (i) compares posterior results obtained with successive truncation orders of the BGL series and (ii) repeats the joint fit using the BCL z-expansion without unitarity priors, thereby providing a direct estimate of any truncation-induced shift in |V_cb| and the Wilson coefficients. revision: yes
Circularity Check
No significant circularity in joint lattice-experiment fit for |V_cb| and Wilson coefficients
full rationale
The paper performs a joint Bayesian fit of lattice form-factor data (from HPQCD, JLQCD, FNAL/MILC) and Belle experimental angular coefficients, using the external BGL parameterization with unitarity imposed only as priors. The reported |V_cb| = 0.03997(71) and NP scale bounds are explicitly presented as outputs of this fit to external datasets, not as independent predictions or derivations. No self-definitional steps, fitted inputs renamed as predictions, load-bearing self-citations, or ansatzes smuggled via author citations appear in the abstract or described method. The analysis is self-contained against the cited external lattice and experimental inputs.
Axiom & Free-Parameter Ledger
free parameters (2)
- |V_cb| =
0.03997(71)
- Wilson coefficients (scalar, vector, tensor)
axioms (3)
- domain assumption Boyd-Grinstein-Lebed (BGL) ansatz for form factor parameterization
- domain assumption Unitarity constraints imposed as Bayesian priors
- standard math SMEFT renormalization group evolution
invented entities (2)
-
scalar leptoquark
no independent evidence
-
vector leptoquark / colourless scalar boson
no independent evidence
Reference graph
Works this paper leans on
-
[1]
Cabibbo,Unitary Symmetry and Leptonic Decays,Phys
N. Cabibbo,Unitary Symmetry and Leptonic Decays,Phys. Rev. Lett.10(1963) 531
1963
-
[2]
M. Kobayashi and T. Maskawa,CP Violation in the Renormalizable Theory of Weak Interaction,Prog. Theor. Phys.49(1973) 652. [3]Flavour Lattice A veraging Group (FLAG)collaboration,FLAG review 2024,Phys. Rev. D113(2026) 014508 [2411.04268]. – 43 – [4]Particle Data Groupcollaboration,Review of particle physics,Phys. Rev. D110(2024) 030001. [5]Heavy Flavor A v...
Pith/arXiv arXiv 1973
-
[3]
J. de Blas et al.,Physics Briefing Book: Input for the 2026 update of the European Strategy for Particle Physics,2511.03883. [8]BaBarcollaboration,Evidence for an excess of ¯B→D (∗)τ −¯ντ decays,Phys. Rev. Lett. 109(2012) 101802 [1205.5442]. [9]BaBarcollaboration,Measurement of an Excess of ¯B→D (∗)τ −¯ντ Decays and Implications for Charged Higgs Bosons,P...
arXiv 2026
-
[4]
S. Fajfer, J.F. Kamenik and I. Nisandzic,On theB→D ∗τ¯ντ Sensitivity to New Physics, Phys. Rev. D85(2012) 094025 [1203.2654]
Pith/arXiv arXiv 2012
-
[5]
M. Duraisamy and A. Datta,The FullB→D ∗τ −¯ντ Angular Distribution and CP violating Triple Products,JHEP09(2013) 059 [1302.7031]
Pith/arXiv arXiv 2013
-
[6]
M.A. Ivanov, J.G. K¨ orner and C.-T. Tran,Analyzing new physics in the decays ¯B0 →D (∗)τ −¯ντ with form factors obtained from the covariant quark model,Phys. Rev. D 94(2016) 094028 [1607.02932]
Pith/arXiv arXiv 2016
-
[7]
P. Colangelo and F. De Fazio,Scrutinizing B→D ∗ (Dπ)ℓ −νℓ and B→D ∗ (Dγ)ℓ −νℓ in search of new physics footprints,JHEP06(2018) 082 [1801.10468]. – 44 –
Pith/arXiv arXiv 2018
-
[8]
M. Jung and D.M. Straub,Constraining new physics inb→cℓνtransitions,JHEP01 (2019) 009 [1801.01112]
Pith/arXiv arXiv 2019
-
[9]
M. Blanke, A. Crivellin, S. de Boer, T. Kitahara, M. Moscati, U. Nierste et al.,Impact of polarization observables andB c →τ νon new physics explanations of theb→cτ νanomaly, Phys. Rev. D99(2019) 075006 [1811.09603]
Pith/arXiv arXiv 2019
-
[10]
Impact of polarization observables andB c →τ νon new physics explanations of the b→cτ νanomaly
M. Blanke, A. Crivellin, T. Kitahara, M. Moscati, U. Nierste and I. Niˇ sandˇ zi´ c,Addendum to “Impact of polarization observables andB c →τ νon new physics explanations of the b→cτ νanomaly”,1905.08253
arXiv 1905
- [11]
- [12]
- [13]
- [14]
-
[15]
B. Bhattacharya, T.E. Browder, A. Datta, T. Kapoor, E. Kou and L. Mukherjee,New physics searches via angular distributions of B→D ∗ (→Dπ)τ(→ℓν τ νℓ) ντ decays,JHEP 04(2025) 135 [2411.09414]
Pith/arXiv arXiv 2025
-
[16]
Z.-R. Huang, F.M. Bhutta, N. Farooq, M.A. Paracha and Y. Li,Reinvestigating the semileptonicB→D (∗)τ¯ντ decays in the model independent scenarios and leptoquark models,Phys. Rev. D111(2025) 115035 [2501.03734]. [32]Bellecollaboration,Measurement of the CKM matrix element|V cb|fromB 0 →D ∗−ℓ+νℓ at Belle,Phys. Rev. D100(2019) 052007 [1809.03290]. [33]Bellec...
arXiv 2025
-
[17]
A. Bazavov, C.E. DeTar, D. Du, A.X. El-Khadra, E. G´ amiz, Z. Gelzer et al.,Semileptonic form factors forB→D ∗ℓνat nonzero recoil from2 + 1-flavor lattice QCD: Fermilab Lattice and MILC Collaborations,The European Physical Journal C82(2022) [2105.14019]
arXiv 2022
-
[18]
C.G. Boyd, B. Grinstein and R.F. Lebed,Constraints on form-factors for exclusive semileptonic heavy to light meson decays,Phys. Rev. Lett.74(1995) 4603 [hep-ph/9412324]
Pith/arXiv arXiv 1995
-
[19]
C.G. Boyd, B. Grinstein and R.F. Lebed,Model independent extraction of|V cb|using dispersion relations,Phys. Lett. B353(1995) 306 [hep-ph/9504235]
Pith/arXiv arXiv 1995
-
[20]
C.G. Boyd, B. Grinstein and R.F. Lebed,Model independent determinations of B→Dℓ ν, D∗ℓ νform-factors,Nucl. Phys. B461(1996) 493 [hep-ph/9508211]
Pith/arXiv arXiv 1996
-
[21]
C.G. Boyd, B. Grinstein and R.F. Lebed,Precision corrections to dispersive bounds on form factors,Physical Review D56(1997) 6895–6911
1997
-
[22]
N. Gubernari, D. van Dyk and J. Virto,Non-local matrix elements in B(s) → {K (∗), ϕ}ℓ+ℓ−,JHEP02(2021) 088 [2011.09813]
arXiv 2021
-
[23]
M. Di Carlo, G. Martinelli, M. Naviglio, F. Sanfilippo, S. Simula and L. Vittorio,Unitarity bounds for semileptonic decays in lattice QCD,Phys. Rev. D104(2021) 054502 [2105.02497]
arXiv 2021
- [24]
-
[25]
S. Simula and L. Vittorio,Multiple dispersive bounds. II. Subthreshold branch cuts,Phys. Rev. D113(2026) 074018 [2509.00412]
arXiv 2026
-
[26]
A. Gopal and N. Gubernari,Unitarity bounds with subthreshold and anomalous cuts for b-hadron decays,Phys. Rev. D111(2025) L031501 [2412.04388]
arXiv 2025
-
[27]
G. Martinelli, S. Simula and L. Vittorio,|V cb|andR(D (∗))using lattice QCD and unitarity, Phys. Rev. D105(2022) 034503 [2105.08674]
arXiv 2022
-
[28]
G. Martinelli, S. Simula and L. Vittorio,Exclusive determinations of|V cb|andR(D ∗) through unitarity,Eur. Phys. J. C82(2022) 1083 [2109.15248]
arXiv 2022
-
[29]
G. Martinelli, M. Naviglio, S. Simula and L. Vittorio,|V cb|, lepton flavor universality and SU(3) F symmetry breaking inB s →D (∗) s ℓνdecays through unitarity and lattice QCD, Phys. Rev. D106(2022) 093002 [2204.05925]
arXiv 2022
- [30]
-
[31]
G. Martinelli, S. Simula and L. Vittorio,Updates on the determination of|V cb|, R(D∗)and |Vub|/|Vcb|,Eur. Phys. J. C84(2024) 400 [2310.03680]
arXiv 2024
-
[32]
G. Martinelli, S. Simula and L. Vittorio,SemileptonicB→D ∗ decays from light toτ leptons: the extraction of the form factorF 2 from data,Eur. Phys. J. C85(2025) 242 [2410.17974]
arXiv 2025
-
[34]
S. Jaiswal, S. Nandi and S.K. Patra,Updates on extraction of|V cb|and SM prediction of R(D∗)inB→D ∗ℓνℓ decays,JHEP06(2020) 165 [2002.05726]
arXiv 2020
-
[35]
S. Iguro and R. Watanabe,Bayesian fit analysis to full distribution data of B→D (∗)ℓν:|V cb|determination and new physics constraints,JHEP08(2020) 006 [2004.10208]
arXiv 2020
-
[36]
M. Bordone and A. J¨ uttner,New strategies for probingB→D ∗ℓ¯νℓ lattice and experimental data,Eur. Phys. J. C85(2025) 129 [2406.10074]
arXiv 2025
-
[37]
W.-S. Fang, S. Iguro, X.-Q. Li, R. Sain, R. Watanabe and B.-L. Zhang,|V cb|determinations from ¯B→D (∗)ℓ¯νdecays within the SM and beyond,2606.17138. [62]Bellecollaboration, “Measurement of Angular Coefficients of ¯B→D ∗ℓ¯νℓ: Implications for |Vcb|and Tests of Lepton Flavor Universality.” HEPData (collection), 2024
Pith/arXiv arXiv 2024
- [38]
- [39]
-
[40]
F.U. Bernlochner, M. Fedele, T. Kretz, U. Nierste and M.T. Prim,Model independent bounds on heavy sterile neutrinos from the angular distribution of B→D ∗ℓνdecays,JHEP 01(2025) 040 [2410.11945]
arXiv 2025
-
[41]
P. Colangelo, F. De Fazio, F. Loparco and N. Losacco,New physics couplings from angular coefficient functions of ¯B→D ∗(Dπ)ℓ¯νℓ,Phys. Rev. D109(2024) 075047 [2401.12304]
arXiv 2024
-
[42]
Measurement of Differential Distributions ofB→D ∗ℓ¯νℓ and Implications on|V cb|
Belle Collaboration, “Measurement of Differential Distributions ofB→D ∗ℓ¯νℓ and Implications on|V cb|.” HEPData (collection), 2023
2023
-
[43]
Determination of|V cb|using B 0 →D ∗+ℓ−¯νℓ decays with Belle II
Belle-II Collaboration, “Determination of|V cb|using B 0 →D ∗+ℓ−¯νℓ decays with Belle II.” HEPData (collection), 2023
2023
-
[44]
K¨ orner, J. G. and Schuler, G. A.,Exclusive semileptonic heavy meson decays including lepton mass effects,Z. Phys. C46(1990) 93
1990
-
[45]
K¨ orner, J. G. and Schuler, G. A.,Lepton Mass Effects in SemileptonicBMeson Decays, Phys. Lett. B231(1989) 306
1989
-
[46]
Gilman and R.L
F.J. Gilman and R.L. Singleton,Analysis of Semileptonic Decays of Mesons Containing Heavy Quarks,Phys. Rev. D41(1990) 142
1990
-
[47]
Tanaka,Charged Higgs effects on exclusive semitauonicBdecays,Z
M. Tanaka,Charged Higgs effects on exclusive semitauonicBdecays,Z. Phys. C67(1995) 321 [hep-ph/9411405]. [73]BaBarcollaboration,Measurements of theB→D ∗ form-factors using the decay ¯B0 →D ∗+e−νe,Phys. Rev. D74(2006) 092004 [hep-ex/0602023]
Pith/arXiv arXiv 1995
-
[48]
M. Tanaka and R. Watanabe,New physics in the weak interaction of ¯B→D (∗)τ¯ν,Phys. Rev. D87(2013) 034028 [1212.1878]
Pith/arXiv arXiv 2013
-
[49]
P. Biancofiore, P. Colangelo and F. De Fazio,On the anomalous enhancement observed in B→D (∗)τ¯ντ decays,Phys. Rev. D87(2013) 074010 [1302.1042]
Pith/arXiv arXiv 2013
-
[50]
M. Duraisamy, P. Sharma and A. Datta,AzimuthalB→D ∗τ −¯ντ angular distribution with tensor operators,Phys. Rev. D90(2014) 074013 [1405.3719]. – 47 –
Pith/arXiv arXiv 2014
-
[51]
G. Martinelli, S. Simula and L. Vittorio,What we can learn from the angular differential rates from semileptonicB→D ∗ℓνℓ decays,Phys. Rev. D111(2025) 013005 [2409.10492]
arXiv 2025
-
[52]
Sirlin,Largem W ,m Z Behavior of theO(α)Corrections to Semileptonic Processes Mediated by W,Nucl
A. Sirlin,Largem W ,m Z Behavior of theO(α)Corrections to Semileptonic Processes Mediated by W,Nucl. Phys. B196(1982) 83
1982
-
[53]
Hagiwara, A.D
K. Hagiwara, A.D. Martin and M.F. Wade,Helicity Amplitude Analysis ofB→D ∗ℓν Decays,Phys. Lett. B228(1989) 144
1989
-
[54]
Bayesian Form factor Fit (BFF) library
A. J¨ uttner, “Bayesian Form factor Fit (BFF) library.” Available at: https://github.com/andreasjuettner/BFF,https://zenodo.org/records/7799543
-
[55]
Buchner, A
J. Buchner, A. Georgakakis, K. Nandra, L. Hsu, C. Rangel, M. Brightman et al.,X-ray spectral modelling of the AGN obscuring region in the CDFS: Bayesian model selection and catalogue,Astronomy & Astrophysics564(2014) A125
2014
-
[56]
Skilling,Nested Sampling,AIP Conf
J. Skilling,Nested Sampling,AIP Conf. Proc.735(2004) 395
2004
-
[57]
Feroz and M.P
F. Feroz and M.P. Hobson,Multimodal nested sampling: an efficient and robust alternative to Markov Chain Monte Carlo methods for astronomical data analyses: Multimodal nested sampling,Monthly Notices of the Royal Astronomical Society384(2008) 449–463
2008
-
[58]
Feroz, M.P
F. Feroz, M.P. Hobson and M. Bridges,MultiNest: an efficient and robust Bayesian inference tool for cosmology and particle physics,Monthly Notices of the Royal Astronomical Society398(2009) 1601–1614
2009
-
[59]
Feroz, M.P
F. Feroz, M.P. Hobson, E. Cameron and A.N. Pettitt,Importance Nested Sampling and the MultiNest Algorithm,The Open Journal of Astrophysics2(2019)
2019
- [60]
-
[61]
Jeffreys,The Theory of Probability, Oxford University Press (1998)
H. Jeffreys,The Theory of Probability, Oxford University Press (1998)
1998
-
[62]
Akaike,A new look at the statistical model identification,IEEE Trans
H. Akaike,A new look at the statistical model identification,IEEE Trans. Automatic Control19(1974) 716
1974
-
[63]
D’Agostini,On the use of the covariance matrix to fit correlated data,Nucl
G. D’Agostini,On the use of the covariance matrix to fit correlated data,Nucl. Instrum. Meth. A346(1994) 306
1994
-
[64]
M. Jung and S. Schacht, ¯B→D (∗)ℓ¯νBranching Ratios and Evidence for Isospin Breaking inΥ(4S)Decays,2604.08391. [91]Heavy Flavor A veraging Group (HFLA V)collaboration,Average of exclusive B→D ∗ℓν, July, 2024.doi:10.5281/zenodo.12696548
work page internal anchor Pith review Pith/arXiv arXiv doi:10.5281/zenodo.12696548 2024
- [65]
- [66]
-
[67]
P. Gambino and S. Hashimoto,Inclusive Semileptonic Decays from Lattice QCD,Phys. Rev. Lett.125(2020) 032001 [2005.13730]
arXiv 2020
- [68]
-
[69]
R. Kellermann, Z. Hu, A. Barone, A. Elgaziari, S. Hashimoto, T. Kaneko et al.,Inclusive semileptonic decays from lattice QCD: Analysis of systematic effects,Phys. Rev. D112 (2025) 014501 [2504.03358]
arXiv 2025
-
[70]
A. De Santis et al.,Inclusive semileptonic decays of theD s meson: A first-principles lattice QCD calculation,Phys. Rev. D112(2025) 054503 [2504.06063]
arXiv 2025
-
[71]
A. De Santis et al.,Inclusive Semileptonic Decays of theD s Meson: Lattice QCD Confronts Experiments,Phys. Rev. Lett.135(2025) 121901 [2504.06064]
arXiv 2025
-
[72]
J.T. Tsang and M. Della Morte,B-physics from lattice gauge theory,Eur. Phys. J. ST233 (2024) 253 [2310.02705]
arXiv 2024
-
[73]
Buchmuller and D
W. Buchmuller and D. Wyler,Effective Lagrangian Analysis of New Interactions and Flavor Conservation,Nucl. Phys. B268(1986) 621
1986
-
[74]
E.E. Jenkins, A.V. Manohar and P. Stoffer,Low-Energy Effective Field Theory below the Electroweak Scale: Operators and Matching,JHEP03(2018) 016 [1709.04486]
arXiv 2018
-
[75]
B. Grzadkowski, M. Iskrzynski, M. Misiak and J. Rosiek,Dimension-Six Terms in the Standard Model Lagrangian,JHEP10(2010) 085 [1008.4884]
Pith/arXiv arXiv 2010
-
[76]
I. Brivio and M. Trott,The Standard Model as an Effective Field Theory,Phys. Rept.793 (2019) 1 [1706.08945]
Pith/arXiv arXiv 2019
-
[77]
W. Altmannshofer, P. Ball, A. Bharucha, A.J. Buras, D.M. Straub and M. Wick, Symmetries and Asymmetries ofB→K ∗µ+µ− Decays in the Standard Model and Beyond, JHEP01(2009) 019 [0811.1214]
Pith/arXiv arXiv 2009
-
[78]
B. Bhattacharya, A. Datta, S. Kamali and D. London,CP Violation in ¯B0 →D ∗+µ−¯νµ, JHEP05(2019) 191 [1903.02567]
arXiv 2019
-
[79]
T. Kapoor, Z.-R. Huang and E. Kou,New physics search via angular distribution of B→D ∗ℓνℓ decay in the light of the new lattice data,JHEP02(2025) 053 [2401.11636]
arXiv 2025
-
[80]
M. Bordone, N. Gubernari, M. Jung and D. van Dyk,Challenging B(s) →D (∗) (s) form factors with the heavy quark expansion,JHEP11(2025) 051 [2507.03569]
arXiv 2025
-
[81]
O. Cat` a and M. Jung,Signatures of a nonstandard Higgs boson from flavor physics,Phys. Rev. D92(2015) 055018 [1505.05804]
Pith/arXiv arXiv 2015
discussion (0)
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