Recognition: unknown
Extracting production fractions of b hadrons from exclusive semi-leptonic decays
Pith reviewed 2026-05-09 20:02 UTC · model grok-4.3
The pith
Ratios of exclusive semi-leptonic decays extract b-hadron production fractions like fs/fd with large uncertainty cancellations.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
The central claim is that the production fraction ratio fs/fd can be extracted from the ratio of branching fractions for the decays bar B_s to D_s star ell bar nu over bar B to D star ell bar nu, multiplied by a calculable theoretical correction factor near unity. Because the semileptonic modes share very similar dynamics, most form-factor and efficiency uncertainties cancel, leaving a cleaner determination than methods based on hadronic final states.
What carries the argument
The ratio of branching fractions for the exclusive semileptonic decays bar B_(s) to D_(s)^(*) ell bar nu, which performs the cancellations of common experimental and theoretical uncertainties.
If this is right
- The uncertainty on fs/fd is currently 7 percent and dominated by experimental statistics rather than theory inputs.
- The method supplies an independent cross-check that does not rely on assumptions about hadronic decay branching fractions.
- The same ratios can be measured for production fractions of heavier b hadrons such as Bc and Lambda_b.
- Any beyond-Standard-Model contributions to the semileptonic decays largely cancel in the ratio, preserving the extraction.
Where Pith is reading between the lines
- This approach could become the preferred input for reducing systematic uncertainties in Bs CP-violation and mixing measurements at the LHC.
- With larger data sets the precision on these production fractions could reach the percent level or better.
- Analogous ratios in other heavy-flavor systems might help constrain production mechanisms where direct tagging is difficult.
Load-bearing premise
The small differences in decay dynamics between the B and Bs systems can be predicted accurately enough from theory that they do not dominate the final uncertainty on the extracted production fractions.
What would settle it
A high-precision measurement of the branching-fraction ratio for Bs to Ds l nu over Bd to D l nu that deviates from the theoretical expectation by more than the combined errors, while independent determinations of fs/fd remain unchanged, would show that the assumed cancellations have failed.
read the original abstract
Ratios of production fractions of $b$ hadrons are a dominant source of uncertainty in many LHC analyses, in particular in measurements with $B_s$ mesons. The currently used value for $f_s/f_d$ is based on a combination of hadronic and semi-inclusive semi-leptonic decays, and relies in part on assumptions about the underlying decays that are hard to quantify. We propose an independent alternative method to obtain this quantity by measuring ratios of the exclusive semi-leptonic decays $\bar B_{(s)} \to D_{(s)}^{(*)} \ell \bar\nu$. This method benefits from significant cancellations of both experimental and theoretical uncertainties, as well as robustness against potential contamination from heavy physics beyond the Standard Model. As a proof of principle, we show that current measurements constrain $f_s/f_d$ with an uncertainty of $7\%$, dominated by present experimental uncertainties. This method can also be applied to other ratios of production fractions involving heavier $b$ hadrons, such as $B_c$ or $\Lambda_b$.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript proposes an alternative method to determine the b-hadron production fraction ratio f_s/f_d from ratios of branching fractions in exclusive semi-leptonic decays B_{(s)} → D_{(s)}^{(*)} ℓ ν̄. It emphasizes cancellations of experimental efficiencies and theoretical form-factor uncertainties, plus robustness to potential BSM contributions that affect numerator and denominator similarly. As a proof of principle, existing measurements are shown to yield a 7% uncertainty on f_s/f_d, dominated by experimental inputs; the approach is also outlined for other ratios such as those involving B_c or Λ_b.
Significance. If the cancellations and numerical result hold, the method supplies an independent, data-driven route to f_s/f_d that avoids some of the hard-to-quantify assumptions in current hadronic plus semi-inclusive combinations. This would directly benefit precision LHC analyses involving B_s mesons by reducing a leading systematic. The BSM-robustness argument and the demonstration that theory uncertainties remain sub-dominant are genuine strengths of the proposal.
major comments (1)
- [Section deriving the numerical result] The central 7% uncertainty claim (abstract and the section deriving the numerical result) is presented only as a summary statement. No table or explicit list of the input branching fractions, their experimental uncertainties, the form-factor ratios used, or the uncertainty propagation is provided, preventing verification that the claimed cancellations actually reduce the total uncertainty to the stated level and that theory contributions are sub-dominant.
minor comments (1)
- Notation for the production fractions (f_s, f_d) and the decay modes should be defined once at first use and used consistently thereafter.
Simulated Author's Rebuttal
We thank the referee for the positive assessment of our manuscript and for the constructive comment. We address the point below and will incorporate the suggested changes in the revised version.
read point-by-point responses
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Referee: [Section deriving the numerical result] The central 7% uncertainty claim (abstract and the section deriving the numerical result) is presented only as a summary statement. No table or explicit list of the input branching fractions, their experimental uncertainties, the form-factor ratios used, or the uncertainty propagation is provided, preventing verification that the claimed cancellations actually reduce the total uncertainty to the stated level and that theory contributions are sub-dominant.
Authors: We agree that the numerical derivation requires more explicit documentation to allow independent verification of the uncertainty cancellations and the sub-dominance of theory contributions. In the revised manuscript we will add a new table (or expanded subsection) that lists: (i) the input branching-fraction measurements and their experimental uncertainties, (ii) the form-factor ratios and their uncertainties, (iii) the explicit propagation steps, and (iv) the breakdown of the final 7% uncertainty into experimental and theoretical components. This will make the cancellations transparent and confirm that theory uncertainties remain sub-dominant as stated. revision: yes
Circularity Check
No significant circularity
full rationale
The paper presents a data-driven extraction of fs/fd (and similar ratios) from measured branching-fraction ratios of exclusive semi-leptonic decays, relying on external experimental inputs and external theoretical form-factor ratios. The central numerical result is obtained by combining published measurements rather than by any internal derivation or fit that reduces to the paper's own equations by construction. No self-definitional steps, fitted-input-as-prediction, or load-bearing self-citation chains appear in the described method; the claimed cancellations are explicit ratios of independent quantities and the 7 % uncertainty is stated to be dominated by present experimental errors.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Standard Model framework for exclusive semi-leptonic b to c transitions
Forward citations
Cited by 1 Pith paper
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Closing the knowledge gap in semileptonic $B\rightarrow X_c\ell\nu$ decays
The unmeasured fraction of inclusive semileptonic B to charm decays is dominated by final states without D mesons, likely from baryons and Ds mesons.
Reference graph
Works this paper leans on
-
[1]
F. Bernlochner, M. Jung, M. Khan, G. Landsberg and Z. Ligeti,Novel approaches to determineB ± andB 0 meson production fractions,Phys. Rev. D110(2024) 014007, [2306.04686]
-
[2]
M. Jung and S. Schacht, ¯B→D (∗)ℓ¯νBranching Ratios and Evidence for Isospin Breaking in Υ(4S)Decays,2604.08391. [4]LHCbcollaboration, R. Aaij et al.,Precise measurement of thef s/fd ratio of fragmentation fractions and ofB 0 s decay branching fractions,Phys. Rev. D104(2021) 032005, [2103.06810]. [5]CMScollaboration, A. Tumasyan et al.,Measurement of theB...
work page internal anchor Pith review Pith/arXiv arXiv 2021
-
[3]
Isgur and M
N. Isgur and M. B. Wise,Weak Decays of Heavy Mesons in the Static Quark Approximation, Phys. Lett. B232(1989) 113–117
1989
-
[4]
Isgur and M
N. Isgur and M. B. Wise,Weak transition form factors between heavy mesons,Phys. Lett. B 237(1990) 527–530
1990
-
[5]
Kobach,Continuity and SemileptonicB (s) →D (s) Form Factors,Phys
A. Kobach,Continuity and SemileptonicB (s) →D (s) Form Factors,Phys. Lett. B809 (2020) 135708, [1910.13024]. – 17 – [10]LHCbcollaboration, R. Aaij et al.,Measurement of the fragmentation fraction ratiof s/fd and its dependence onBmeson kinematics,JHEP04(2013) 001, [1301.5286]. [11]LHCbcollaboration, R. Aaij et al.,Measurement of the branching fraction of ...
-
[6]
M. Jung and S. Schacht,Standard model predictions and new physics sensitivity inB→DD decays,Phys. Rev. D91(2015) 034027, [1410.8396]
-
[7]
J. Davies, M. Jung and S. Schacht, B→ DDdecays and the extraction of f d/fu at hadron colliders,JHEP01(2024) 191, [2311.16952]. [18]CMScollaboration, A. Tumasyan et al.,Measurement of the dependence of the hadron production fraction ratiof s/fu andf d/fu on B meson kinematic variables in proton-proton collisions at √s= 13 TeV,Phys. Rev. Lett.131(2023) 121...
-
[8]
R. Fleischer, N. Serra and N. Tuning,A New Strategy forB s Branching Ratio Measurements and the Search for New Physics inB 0 s →µ +µ−,Phys. Rev. D82(2010) 034038, [1004.3982]
-
[9]
M. Beneke, G. Buchalla, M. Neubert and C. T. Sachrajda,QCD factorization for exclusive, nonleptonic B meson decays: General arguments and the case of heavy light final states, Nucl. Phys. B591(2000) 313–418, [hep-ph/0006124]
work page Pith review arXiv 2000
- [10]
-
[11]
M. Bordone, N. Gubernari, T. Huber, M. Jung and D. van Dyk,A puzzle in ¯B0 (s) →D (∗)+ (s) {π−, K−}decays and extraction of thef s/fd fragmentation fraction,Eur. Phys. J. C80(2020) 951, [2007.10338]. [24]Bellecollaboration, N. C. Hastings et al.,Studies ofB 0 − ¯B0 mixing properties with inclusive dilepton events,Phys. Rev. D67(2003) 052004, [hep-ex/0212033]
- [12]
-
[13]
Finauri,Kinematic moments of B→X cℓνℓ to orderO Λ5 QCD/m5 b ,JHEP04(2025) 112, [2501.09090]
G. Finauri,Kinematic moments of B→X cℓνℓ to orderO Λ5 QCD/m5 b ,JHEP04(2025) 112, [2501.09090]
-
[14]
The𝑞2 moments in inclusive semileptonic𝑏decays, 2024
G. Finauri and P. Gambino,The q 2 moments in inclusive semileptonic B decays,JHEP02 (2024) 206, [2310.20324]. – 18 –
-
[15]
F. Bernlochner, M. Fael, K. Olschewsky, E. Persson, R. van Tonder, K. K. Vos et al.,First extraction of inclusive V cb from q2 moments,JHEP10(2022) 068, [2205.10274]
-
[16]
A. Carvunis, G. Finauri, P. Gambino, M. Jung and S. M¨ achler,New Physics in inclusive semileptonic B decays,JHEP01(2026) 037, [2507.22123]
-
[17]
P. Gambino, S. Hashimoto, S. M¨ achler, M. Panero, F. Sanfilippo, S. Simula et al.,Lattice QCD study of inclusive semileptonic decays of heavy mesons,JHEP07(2022) 083, [2203.11762]
-
[18]
P. Gambino, S. Hashimoto, S. M¨ achler, M. Panero, F. Sanfilippo, S. Simula et al.,On the study of inclusive semileptonic decays of Bs-meson from lattice QCD⋆,Nuovo Cim. C47 (2024) 92, [2311.09892]
-
[19]
A. De Santis et al.,Inclusive semileptonic decays of the Ds meson: A first-principles lattice QCD calculation,Phys. Rev. D112(2025) 054503, [2504.06063]
-
[20]
A. De Santis et al.,Inclusive Semileptonic Decays of the Ds Meson: Lattice QCD Confronts Experiments,Phys. Rev. Lett.135(2025) 121901, [2504.06064]
-
[21]
M. Bordone and P. Gambino,The semileptonicB s andΛ b widths,PoSCKM2021(2023) 055, [2203.13107]
- [22]
- [23]
-
[24]
M. Rudolph,An experimentalist’s guide to the semileptonic bottom to charm branching fractions,Int. J. Mod. Phys. A33(2018) 1850176, [1805.05659]
-
[25]
van Tonder, F
R. van Tonder, F. Herren, in progress
-
[26]
On the simulated kinematic distributions of heavy meson decays
F. Herren and R. van Tonder,On the simulated kinematic distributions of semileptonicB decays,2602.18378. [40]CLEOcollaboration, R. Fulton et al.,Exclusive and inclusive semileptonic decays of B mesons to D mesons,Phys. Rev. D43(1991) 651–663. [41]BaBarcollaboration, B. Aubert et al.,Measurement of the relative branching fractions of ¯B→D/D ∗/D∗∗ℓ−¯νℓ deca...
work page internal anchor Pith review Pith/arXiv arXiv 1991
- [27]
-
[28]
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]
- [29]
- [30]
-
[31]
C. G. Boyd, B. Grinstein and R. F. Lebed,Model independent determinations of ¯B→Dℓ, D ∗ℓ¯νform-factors,Nucl. Phys. B461(1996) 493–511, [hep-ph/9508211]
work page internal anchor Pith review arXiv 1996
-
[32]
I. Caprini and M. Neubert,Improved bounds for the slope and curvature of ¯B→D (∗) lepton anti-neutrino form-factors,Phys. Lett. B380(1996) 376–384, [hep-ph/9603414]
-
[33]
N. Gubernari, M. Reboud, D. van Dyk and J. Virto,Dispersive analysis ofB→K (∗) and Bs →ϕform factors,JHEP12(2023) 153, [2305.06301]
- [34]
-
[35]
A. Gopal and N. Gubernari,Unitarity bounds with subthreshold and anomalous cuts for b-hadron decays,Phys. Rev. D111(2025) L031501, [2412.04388]
- [36]
-
[37]
Harrison,b¯csusceptibilities from fully relativistic lattice QCD,Phys
J. Harrison,b¯csusceptibilities from fully relativistic lattice QCD,Phys. Rev. D110(2024) 054506, [2405.01390]
-
[38]
Godfrey,Spectroscopy ofB c mesons in the relativized quark model,Phys
S. Godfrey,Spectroscopy ofB c mesons in the relativized quark model,Phys. Rev. D70 (2004) 054017, [hep-ph/0406228]
-
[39]
R. J. Dowdall, C. T. H. Davies, T. C. Hammant and R. R. Horgan,Precise heavy-light meson masses and hyperfine splittings from lattice QCD including charm quarks in the sea, Phys. Rev. D86(2012) 094510, [1207.5149]. [59]CMScollaboration, A. M. Sirunyan et al.,Observation of Two Excited B + c States and Measurement of the B + c (2S) Mass in pp Collisions at...
-
[40]
D. van Dyk, M. Reboud, M. Kirk, N. Gubernari, P. L¨ ughausen, D. Leljak et al.,EOSversion 1.0.20, 2026. 10.5281/zenodo.19852912
-
[41]
Higson, W
E. Higson, W. Handley, M. Hobson and A. Lasenby,Dynamic nested sampling: an improved algorithm for parameter estimation and evidence calculation,Statistics and Computing29 (dec, 2018) 891–913
2018
-
[42]
J. S. Speagle,dynesty: a dynamic nested sampling package for estimating Bayesian posteriors and evidences,Monthly Notices of the Royal Astronomical Society493(feb, 2020) 3132–3158. – 20 –
2020
-
[43]
S. Koposov, J. Speagle, K. Barbary, G. Ashton, E. Bennett, J. Buchner et al.,dynesty version 2.0.3, Dec., 2022. 10.5281/zenodo.7388523
-
[44]
Bolognani, M
C. Bolognani, M. Jung, M. Reboud and K. K. Vos,EOS/DATA-2026-02: Supplementary material forEOS/ANALYSIS-2024-03, Apr., 2026
2026
-
[45]
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]
-
[46]
M. Bordone and A. Juttner,New strategies for probingB→D ∗ℓ¯νℓ lattice and experimental data,Eur. Phys. J. C85(2025) 129, [2406.10074]
- [47]
-
[48]
I. Ray and S. Nandi,Test of new physics effects in B→ D(∗), π ℓ−νℓ decays with heavy and light leptons,JHEP01(2024) 022, [2305.11855]. [71]LHCbcollaboration, R. Aaij et al.,Measurement of|V cb|withB 0 s →D (∗)− s µ+νµ decays, Phys. Rev. D101(2020) 072004, [2001.03225]. [72]LHCbcollaboration, R. Aaij et al.,Measurement of the shape of theB 0 s →D ∗− s µ+νµ...
-
[49]
The role of right-handed neutrinos in b→cτ¯νanomalies,
R. Mandal, C. Murgui, A. Pe˜ nuelas and A. Pich,The role of right-handed neutrinos in b→cτ¯νanomalies,JHEP08(2020) 022, [2004.06726]
-
[50]
J. Aebischer, A. Crivellin, M. Fael and C. Greub,Matching of gauge invariant dimension-six operators forb→sandb→ctransitions,JHEP05(2016) 037, [1512.02830]
-
[51]
D. Beˇ cirevi´ c, N. Koˇ snik and A. Tayduganov,¯B→Dτ¯ν τ vs. ¯B→Dµ¯ν µ,Phys. Lett. B716 (2012) 208–213, [1206.4977]
-
[52]
M. Duraisamy and A. Datta,The FullB→D ∗τ − ¯ντ Angular Distribution and CP violating Triple Products,JHEP09(2013) 059, [1302.7031]. [77]LHCbcollaboration, R. Aaij et al.,Measurement of theb-quark production cross-section in 7 and 13 TeVppcollisions,Phys. Rev. Lett.118(2017) 052002, [1612.05140]. [78]Bellecollaboration, P. Urquijo et al.,Moments of the ele...
-
[53]
M. Bordone, A. Khodjamirian and T. Mannel,New sum rules for theB c →J/ψform factors,JHEP01(2023) 032, [2209.08851]. [85]LHCbcollaboration, R. Aaij et al.,Observation of the decayΛ 0 b →Λ + c τ −ντ,Phys. Rev. Lett. 128(2022) 191803, [2201.03497]. [86]LHCbcollaboration, R. Aaij et al.,Determination of the quark coupling strength|V ub|using baryonic decays,N...
-
[54]
Λb→pℓ−¯νℓand Λb→Λcℓ−¯νℓform factors from lattice QCD with rela- tivistic heavy quarks,
W. Detmold, C. Lehner and S. Meinel, Λ b →pℓ −¯νℓ andΛ b →Λ cℓ−¯νℓ form factors from lattice QCD with relativistic heavy quarks,Phys. Rev. D92(2015) 034503, [1503.01421]. [88]HPQCDcollaboration, H. Na, C. M. Bouchard, G. P. Lepage, C. Monahan and J. Shigemitsu,B→Dℓνform factors at nonzero recoil and extraction of|V cb|,Phys. Rev. D 92(2015) 054510, [1505....
-
[55]
E. McLean, C. T. H. Davies, J. Koponen and A. T. Lytle,B s →D sℓνForm Factors for the fullq 2 range from Lattice QCD with non-perturbatively normalized currents,Phys. Rev. D 101(2020) 074513, [1906.00701]. [91]Fermilab Lattice, MILCcollaboration, A. Bazavov et al.,Semileptonic form factors for B→D ∗ℓνat nonzero recoil from2 + 1-flavor lattice QCD: Fermila...
-
[56]
N. Gubernari, A. Kokulu and D. van Dyk,B→PandB→VForm Factors fromB-Meson Light-Cone Sum Rules beyond Leading Twist,JHEP01(2019) 150, [1811.00983]
-
[57]
M. Bordone, N. Gubernari, D. van Dyk and M. Jung,Heavy-Quark expansion for ¯Bs →D (∗) s form factors and unitarity bounds beyond theSU(3) F limit,Eur. Phys. J. C80(2020) 347, [1912.09335]. – 22 –
discussion (0)
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