pith. machine review for the scientific record. sign in

arxiv: 2411.18639 · v2 · submitted 2024-11-25 · ✦ hep-ex

Recognition: 1 theorem link

· Lean Theorem

Averages of b-hadron, c-hadron, and τ-lepton properties as of 2023

Authors on Pith no claims yet

Pith reviewed 2026-05-16 22:27 UTC · model grok-4.3

classification ✦ hep-ex
keywords b-hadronc-hadrontau-leptonworld averagesbranching fractionslifetimesCKM matrixCP violation
0
0 comments X

The pith

This paper reports updated world averages for b-hadron, c-hadron, and tau-lepton properties from measurements before October 2023.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The Heavy Flavour Averaging Group has compiled world averages for a range of properties including branching fractions, lifetimes, neutral meson mixing, CP violation, semileptonic decays, and Cabibbo-Kobayashi-Maskawa matrix elements. Common input parameters from different experiments are rescaled to agreed reference values, and known correlations are incorporated into the averaging. These averages serve as the current standard reference for heavy flavor physics. A sympathetic reader cares because they provide the most precise constraints currently available on flavor-changing processes and CKM parameters.

Core claim

The paper reports world averages of measurements of b-hadron, c-hadron, and τ-lepton properties obtained by the Heavy Flavour Averaging Group using results available before October 2023. In rare cases, significant results obtained several months later are also used. For the averaging, common input parameters used in the various analyses are adjusted to common values, and known correlations are taken into account. The averages include branching fractions, lifetimes, neutral meson mixing parameters, CP violation parameters, parameters of semileptonic decays, and Cabibbo-Kobayashi-Maskawa matrix elements.

What carries the argument

The averaging procedure that rescales common input parameters to agreed reference values while accounting for correlations between experimental measurements.

Load-bearing premise

All relevant correlations between the input experimental measurements have been correctly identified and the rescaling of common parameters to agreed reference values does not introduce bias into the final averages.

What would settle it

A new independent analysis of the underlying experimental data that produces averages differing significantly from those reported here, for example in the tau lepton lifetime or a specific branching fraction, would indicate that the current world averages are not accurate.

read the original abstract

This paper reports world averages of measurements of $b$-hadron, $c$-hadron, and $\tau$-lepton properties obtained by the Heavy Flavour Averaging Group using results available before October 2023. In rare cases, significant results obtained several months later are also used. For the averaging, common input parameters used in the various analyses are adjusted (rescaled) to common values, and known correlations are taken into account. The averages include branching fractions, lifetimes, neutral meson mixing parameters, CP violation parameters, parameters of semileptonic decays, and Cabibbo-Kobayashi-Maskawa matrix elements.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

0 major / 2 minor

Summary. This paper reports world averages of b-hadron, c-hadron, and τ-lepton properties compiled by the Heavy Flavour Averaging Group from experimental results available before October 2023 (with rare later inclusions). Common input parameters are rescaled to agreed reference values and known correlations are incorporated. The averages cover branching fractions, lifetimes, neutral meson mixing and CP violation parameters, semileptonic decay parameters, and CKM matrix elements.

Significance. If the input measurements and correlations are faithfully represented, these averages constitute an essential, regularly updated reference for the flavor physics community. They enable consistent inputs for precision tests of the Standard Model, CKM fits, and new-physics searches, building directly on the long-established HFAG methodology of rescaling shared parameters and accounting for correlations.

minor comments (2)
  1. The abstract states that 'in rare cases, significant results obtained several months later are also used'; a brief footnote or sentence in §1 identifying the specific results and the cutoff date would improve transparency without altering the central claim.
  2. Tables listing the final averages would benefit from an explicit column or footnote indicating the number of input measurements and the dominant correlation sources for each entry, to allow readers to assess the robustness of the quoted uncertainties at a glance.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for the careful review and for recommending acceptance of the manuscript. The referee's summary accurately reflects the scope, methodology, and importance of the HFAG world averages.

Circularity Check

0 steps flagged

No significant circularity in the averaging procedure

full rationale

The paper compiles world averages from independent experimental measurements of b-hadron, c-hadron, and τ-lepton properties. It adjusts common input parameters to agreed external reference values and incorporates reported correlations using established HFAG statistical procedures. No derivation step reduces by construction to a fitted parameter, self-defined quantity, or load-bearing self-citation; the inputs are external data and the output is a weighted average that does not presuppose its own results. The procedure is self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central output consists of statistical combinations of existing measurements; the paper relies on the correctness of the input experimental results and on the validity of the correlation estimates supplied by the original analyses.

axioms (1)
  • domain assumption Input measurements are unbiased and their reported uncertainties and correlations are accurate.
    Standard assumption for any world-average compilation; invoked when combining results from different experiments.

pith-pipeline@v0.9.0 · 5597 in / 1255 out tokens · 37909 ms · 2026-05-16T22:27:43.382701+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

What do these tags mean?
matches
The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
The paper's claim conflicts with a theorem or certificate in the canon.
unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Forward citations

Cited by 18 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Evidence for the decay $B^0_s\to\phi\eta'$

    hep-ex 2026-05 conditional novelty 8.0

    First evidence for B_s^0 to phi eta-prime decay with relative branching ratio (3.56 ± 0.79 ± 0.18 ± 0.06) x 10^{-2} and absolute branching fraction (0.66 ± 0.15 ± 0.03 ± 0.02) x 10^{-6}.

  2. First evidence of the $B_s^0\rightarrow K^-\pi^+\gamma$ decay

    hep-ex 2026-01 accept novelty 8.0

    LHCb reports the first experimental evidence for the Bs0 to K- pi+ gamma decay with 3.5 sigma significance and measures its branching fraction ratio to the B0 decay in two mass ranges.

  3. Unbinned extraction of $\gamma$ from $B\to DK$ with normalizing flows

    hep-ph 2026-05 unverdicted novelty 7.0

    Normalizing flows trained on D decay data create a continuous unbinned model of Dalitz plot amplitudes, allowing extraction of gamma from B decay data with successful recovery of injected values in Monte Carlo tests.

  4. Precise measurement of the CKM angle $\gamma$ with a novel approach

    hep-ex 2026-04 unverdicted novelty 7.0

    A joint fit to LHCb B to D h decays and BESIII quantum-correlated D Dbar data yields gamma = 71.3 plus or minus 5.0 degrees, the most precise measurement to date.

  5. Measurement of the CKM angle $\gamma$ in $B^{\pm} \rightarrow D(\rightarrow K^{0}_{\rm S} h^{\prime+}h^{\prime-})h^{\pm}$ decays with a novel approach

    hep-ex 2026-04 unverdicted novelty 7.0

    A novel model-independent approach with per-event phase-space weights on combined BESIII and LHCb data measures the CKM angle γ as (71.3 ± 5.0)° in B± → D(→ K0S h'+h'-) h± decays.

  6. Probing New Physics and CP Violation in $\nu_\tau n \to \Lambda_c \tau^- (\pi^- \nu_\tau)$ and $\bar\nu_\tau p \to \Lambda \tau^+ (\pi^+ \bar\nu_\tau)$

    hep-ph 2026-01 conditional novelty 6.0

    An azimuthal asymmetry in the pion from tau decays in specific neutrino-hyperon processes provides a CP-odd signal for beyond-Standard-Model physics encoded in dimension-six operators.

  7. New Predictions for the Lifetimes of Doubly Heavy Baryons and the $B_c$ Meson

    hep-ph 2026-05 unverdicted novelty 5.0

    Updated lifetime predictions for doubly heavy baryons and B_c meson with NNLO and NLO corrections in MS-bar, kinetic, and Upsilon mass schemes, including new hierarchies for bc states.

  8. Real and Complex Singlet-Scalar Benchmarks with a Vector-Like Down Quark for $B\to X_s\gamma$ and $B_s-\bar B_s$ Mixing

    hep-ph 2026-05 unverdicted novelty 5.0

    In minimal benchmarks with a vector-like down quark D and singlet scalar, the new-physics contribution to B to X_s gamma is only 0.4 percent of the Standard Model value at TeV scales, while B_s mixing imposes stronger...

  9. New insights into the $b\rightarrow c \bar{u}q$ puzzle through Top-Bottom synergies

    hep-ph 2026-04 unverdicted novelty 5.0

    Anomalies in b to c u-bar q transitions remain puzzling as proposed new physics scenarios involving SU(2) doublets are not significantly relaxed by collider dilution or factorization breakdown.

  10. $\bar B\to D^{(*)}\ell\bar \nu$ Branching Ratios and Evidence for Isospin Breaking in $\Upsilon(4S)$ Decays

    hep-ph 2026-04 unverdicted novelty 5.0

    A combined fit to B to D(*) l nu data yields R^{±0}=1.062(19) as evidence for isospin violation in Υ(4S) decays and branching fractions up to 1.6σ larger than prior averages, addressing inconsistencies in V_cb extractions.

  11. $B_c$ meson decays into $S$-wave charmonium plus light meson pairs in the perturbative QCD approach

    hep-ph 2026-01 unverdicted novelty 5.0

    pQCD calculations predict ~90% longitudinal polarization in B_c to J/psi or psi(2S) plus rho or K* mediated light meson pairs, with one branching ratio ratio matching LHCb at 2.67 vs 2.80.

  12. $C\!P$ violation analysis of local and nonlocal amplitudes in the $\overline{B}^0 \to \overline{K}^{*0}\mu^+\mu^-$ decay

    hep-ex 2026-05 unverdicted novelty 4.0

    LHCb measures CP-violating Wilson coefficients in B0 -> K*0 mu+ mu- with higher precision than before and finds results consistent with the Standard Model.

  13. CP asymmetries in charged meson decay to two pions

    hep-ph 2026-05 unverdicted novelty 4.0

    CP asymmetries for B+ to pi+ pi0, D+ to pi+ pi0, and K+ to pi+ pi0 are estimated in the Standard Model at roughly 3 times 10 to the -3, 10 to the -5, and 10 to the -6 using a unified formalism for isospin violation.

  14. Closing the knowledge gap in semileptonic $B\rightarrow X_c\ell\nu$ decays

    hep-ph 2026-05 unverdicted novelty 4.0

    The unmeasured fraction of inclusive semileptonic B to charm decays is dominated by final states without D mesons, likely from baryons and Ds mesons.

  15. Measurement of the branching fractions and longitudinal polarisations of $B^0_{(s)} \to K^{*0} \kern 0.18em \overline{\kern -0.18em K}{}^{*0}$ decays

    hep-ex 2025-12 accept novelty 4.0

    LHCb measures f_L^d = 0.600 and f_L^s = 0.159 for B to K* Kbar* decays and reports a ratio L of 4.92 that confirms 4.4 sigma discrepancy with theory.

  16. Review of experimental studies of charmed meson decays at BESIII

    hep-ex 2026-04 unverdicted novelty 3.0

    A review of BESIII charmed meson decay studies presents the most precise averages for |V_cs|, |V_cd|, D and D_s decay constants, and several hadronic form factors from combined experimental results.

  17. Leptonic and semileptonic charm decays at BESIII

    hep-ex 2026-04 unverdicted novelty 3.0

    BESIII presents measurements of branching fractions, |V_cs|, |V_cd|, decay constants, form factors, and lepton flavor universality tests in charmed decays.

  18. Flavour Physics beyond the LHC

    hep-ex 2026-04 unverdicted novelty 2.0

    The next two decades of flavour physics will be dominated by LHCb and Belle II data, with an e+e- collider potentially adding precision through Z, W+W-, and ttbar runs.

Reference graph

Works this paper leans on

300 extracted references · 300 canonical work pages · cited by 18 Pith papers · 180 internal anchors

  1. [1]

    HFLAV collaboration, Y. S. Amhiset al., Averages of b-hadron, c-hadron, andτ-lepton properties as of 2021, Phys. Rev. D107 (2023) 052008, arXiv:2206.07501

  2. [2]

    Cabibbo,Unitary Symmetry and Leptonic Decays, Phys

    N. Cabibbo,Unitary Symmetry and Leptonic Decays, Phys. Rev. Lett.10 (1963) 531

  3. [3]

    Kobayashi and T

    M. Kobayashi and T. Maskawa,CP Violation in the Renormalizable Theory of Weak Interaction, Prog. Theor. Phys.49 (1973) 652

  4. [4]

    Combined results on b-hadron production rates, lifetimes, oscillations and semileptonic decays

    D. Abbaneoet al., Combined results onb-hadron production rates, lifetimes, oscillations and semileptonic decays, arXiv:hep-ex/0009052, CERN-EP-2000-096; D. Abbaneoet al., Combined results onb-hadron production rates and decay properties, arXiv:hep-ex/0112028, CERN-EP-2001-050

  5. [5]

    HFLAV web page, https://hflav.web.cern.ch

  6. [6]

    Schneider and H

    O. Schneider and H. Seywerd,COMBOS: a program to COMbine results from B OScillations analyses, https://gitlab.cern.ch/hflav/shared-material/-/blob/main/combos.pdf, 1999

  7. [7]

    Bertholet and T

    E. Bertholet and T. Kuhr,HFLAV averaging, https://gitlab.cern.ch/hflav/averaging,

  8. [8]

    doi: 10.5281/zenodo.6632075

  9. [9]

    A. C. Aitken,On least squares and linear combination of observations, Proc. R. Soc. Edinb55 (1936) 42

  10. [10]

    Particle Data Group, P. A. Zylaet al., Review of Particle Physics, PTEP2020 (2020) 083C01

  11. [11]

    Asymmetric Statistical Errors

    R. Barlow,Asymmetric statistical errors, arXiv:physics/0406120

  12. [12]

    CLEO collaboration, J. P. Alexanderet al., Measurement of the relative branching fraction of Υ (4S) to charged and neutralB meson pairs, Phys. Rev. Lett.86 (2001) 2737, arXiv:hep-ex/0006002

  13. [13]

    Measurement of Branching Fractions and Charge Asymmetries for Exclusive B Decays to Charmonium

    BABA Rcollaboration, B. Aubertet al., Measurement of branching fractions and charge asymmetries for exclusiveB decays to charmonium, Phys. Rev. Lett.94 (2005) 141801, arXiv:hep-ex/0412062

  14. [14]

    Choudhuryet al., Measurement of theB+/B0 production ratio ine+e− collisions at theΥ (4S) resonance using B → J/ψ(ℓℓ)K decays at Belle, Phys

    Belle collaboration, S. Choudhuryet al., Measurement of theB+/B0 production ratio ine+e− collisions at theΥ (4S) resonance using B → J/ψ(ℓℓ)K decays at Belle, Phys. Rev. D107 (2023) L031102, arXiv:2207.01194

  15. [15]

    CLEO collaboration, S. B. Atharet al., Measurement of the ratio of branching fractions of the Υ (4S) to charged and neutralB mesons, Phys. Rev.D66 (2002) 052003, arXiv:hep-ex/0202033

  16. [16]

    Belle collaboration, N. C. Hastingset al., Studies of B0 - B 0 mixing properties with inclusive dilepton events, Phys. Rev. D67 (2003) 052004, arXiv:hep-ex/0212033

  17. [17]

    Measurement of the Branching Fraction of Upsilon(4S) --> B0B0bar

    BABA Rcollaboration, B. Aubertet al., Measurement of the branching fraction of Υ (4S) → B0B 0 , Phys. Rev. Lett.95 (2005) 042001, arXiv:hep-ex/0504001

  18. [18]

    Barishet al., Measurements of theB semileptonic branching fraction with lepton tags, Phys

    CLEO collaboration, B. Barishet al., Measurements of theB semileptonic branching fraction with lepton tags, Phys. Rev. Lett.76 (1996) 1570. 430

  19. [19]

    Study of hadronic transitions between Y states and observation of Y(4S)-> eta Y(1S) decay

    BaBar collaboration, B. Aubertet al., Study of hadronic transitions between Upsilon states and observation ofΥ (4S) → ηΥ (1S) decay, Phys. Rev.D78 (2008) 112002, arXiv:0807.2014

  20. [20]

    Study of $\eta$ and dipion transitions in $\Upsilon(4S)$ decays to lower bottomonia

    Belle collaboration, E. Guidoet al., Study of η and dipion transitions inΥ (4S) decays to lower bottomonia, Phys. Rev.D96 (2017) 052005, arXiv:1707.04973

  21. [21]

    Observation of $\Upsilon(4S)\to \eta' \Upsilon(1S)$

    Belle collaboration, E. Guidoet al., Observation of Υ (4S) → η′Υ (1S), Phys. Rev. Lett.121 (2018) 062001, arXiv:1803.10303

  22. [22]

    First observation of the hadronic transition $ \Upsilon(4S) \to \eta h_{b}(1P)$ and new measurement of the $h_b(1P)$ and $\eta_b(1S)$ parameters

    Belle collaboration, U. Tamponiet al., First observation of the hadronic transition Υ (4S) → ηhb(1P ) and new measurement of thehb(1P ) and ηb(1S) parameters, Phys. Rev. Lett. 115 (2015) 142001, arXiv:1506.08914

  23. [23]

    J. Chay, H. Georgi, and B. Grinstein,Lepton energy distributions in heavy meson decays from QCD, Phys. Lett. B247 (1990) 399

  24. [24]

    Isospin in $B$ Decays and the $(B^0 \bar B^0)/(B^+ B^-)$ Production Ratio

    M. Gronau, Y. Grossman, and J. L. Rosner,Isospin in B decays and the (B0 anti-B0)/(B+ B-) production ratio, Phys. Rev. D73 (2006) 057501, arXiv:hep-ph/0601136

  25. [25]

    Branching ratio measurements and isospin violation in B-meson decays

    M. Jung,Branching ratio measurements and isospin violation in B-meson decays, Phys. Lett. B753 (2016) 187, arXiv:1510.03423

  26. [26]

    Bernlochneret al., Novel approaches to determineB± and B0 meson production fractions, arXiv:2306.04686

    F. Bernlochneret al., Novel approaches to determineB± and B0 meson production fractions, arXiv:2306.04686

  27. [27]

    A. E. Bondar, A. I. Milstein, R. V. Mizuk, and S. G. Salnikov,Effects of isospin violation in the e+e− → B(∗)B(∗) cross sections, JHEP05 (2022) 170, arXiv:2204.03961

  28. [28]

    Mizuket al., Measurement of the energy dependence of the e+e− → BB, BB∗ and B∗B∗ exclusive cross sections, JHEP06 (2021) 137, arXiv:2104.08371

    Belle collaboration, R. Mizuket al., Measurement of the energy dependence of the e+e− → BB, BB∗ and B∗B∗ exclusive cross sections, JHEP06 (2021) 137, arXiv:2104.08371

  29. [29]

    Measurement of the Mass Difference m(B0) - m(B+)

    BaBar collaboration, B. Aubertet al., Measurement of the Mass Difference m(B0) - m(B+), Phys. Rev. D78 (2008) 011103, arXiv:0805.0497

  30. [30]

    Adachiet al., Measurement of the energy dependence of the e+e− → BB, BB ∗ , and B∗B ∗ cross sections at Belle II, JHEP10 (2024) 114, arXiv:2405.18928

    Belle-II collaboration, I. Adachiet al., Measurement of the energy dependence of the e+e− → BB, BB ∗ , and B∗B ∗ cross sections at Belle II, JHEP10 (2024) 114, arXiv:2405.18928

  31. [31]

    Study of e+e- => B(*) B(*)-bar pi+- at sqrt(s)=10.866 GeV

    Belle collaboration, A. Garmashet al., Observation of Zb(10610) and Zb(10650) Decaying to B Mesons, Phys. Rev. Lett.116 (2016) 212001, arXiv:1512.07419

  32. [32]

    Drutskoyet al., Measurement of Υ(5S) decays toB0 and B+ mesons, Phys

    Belle collaboration, A. Drutskoyet al., Measurement of Υ(5S) decays toB0 and B+ mesons, Phys. Rev. D81 (2010) 112003, arXiv:1003.5885

  33. [33]

    Precise measurement of the branching fractions for Bs->Ds(*)+ Ds(*)- and first measurement of the Ds*+ Ds*- polarization using e+e- collisions

    Belle collaboration, S. Esenet al., Precise measurement of the branching fractions for Bs → D(∗)+ s D(∗)− s and first measurement of theD∗+ s D∗− s polarization using e+e− collisions, Phys. Rev. D87 (2013) 031101, arXiv:1208.0323

  34. [34]

    Belle collaboration, V. Zhukovaet al., Measurement of thee+e− → B0 s B0 sX cross section in the energy range from10.63 to 11.02 GeV using inclusive D+ s and D0 production, JHEP08 (2023) 131, arXiv:2305.10098

  35. [35]

    Wanget al., Measurement of B(Bs → DsX) with Bs semileptonic tagging, Phys

    Belle collaboration, B. Wanget al., Measurement of B(Bs → DsX) with Bs semileptonic tagging, Phys. Rev. D105 (2022) 012004, arXiv:2106.11265. 431

  36. [36]

    CLEO collaboration, G. S. Huanget al., Measurement of B(Υ (5S) → B(∗) s B (∗) s ) using ϕ mesons, Phys. Rev.D75 (2007) 012002, arXiv:hep-ex/0610035

  37. [37]

    BABA Rcollaboration, J. P. Leeset al., A measurement of the semileptonic branching fraction of the B0 s meson, Phys. Rev.D85 (2012) 011101, arXiv:1110.5600

  38. [38]

    Amplitude analysis of e+e- => Y(nS)pi+pi- at sqrt(s)=10.865 GeV

    Belle collaboration, A. Garmashet al., Amplitude analysis ofe+e− → Υ (nS)π+π− at√s = 10.865 GeV, Phys. Rev.D91 (2015) 072003, arXiv:1403.0992

  39. [39]

    First Observation of the Zb0(10610) in a Dalitz Analysis of Y(5S) -> Y(nS) pi0 pi0

    Belle collaboration, P. Krokovnyet al., First observation of theZb(10610)0 in a Dalitz analysis of Υ(10860) → Υ(nS)π0π0, Phys. Rev.D88 (2013) 052016, arXiv:1308.2646

  40. [40]

    First observation of the P-wave spin-singlet bottomonium states h_b(1P) and h_b(2P)

    Belle collaboration, I. Adachiet al., First observation of theP-wave spin-singlet bottomonium states hb(1P ) and hb(2P ), Phys. Rev. Lett.108 (2012) 032001, arXiv:1103.3419

  41. [41]

    Belle collaboration, X. H. Heet al., Observation of e+e− → π+π−π0χbJ and Search for Xb → ωΥ (1S) at √s = 10.867 GeV, Phys. Rev. Lett.113 (2014) 142001, arXiv:1408.0504

  42. [42]

    Inclusive study of bottomonium production in association with an $\eta$ meson in $e^+e^-$ annihilations near $\Upsilon(5S)$

    Belle collaboration, U. Tamponiet al., Inclusive study of bottomonium production in association with anη meson in e+e− annihilations near Υ (5S), Eur. Phys. J.C78 (2018) 633, arXiv:1803.03225

  43. [43]

    Louvot,Study of Bs meson production and measurement ofBs decays into aD(∗)− s and a light meson ine+e− collisions at √s = 10.87 GeV, PhD thesis #5213, EPFL, Lausanne, 2012

    R. Louvot,Study of Bs meson production and measurement ofBs decays into aD(∗)− s and a light meson ine+e− collisions at √s = 10.87 GeV, PhD thesis #5213, EPFL, Lausanne, 2012

  44. [44]

    HFLAV collaboration, Y. S. Amhiset al., Averages of b-hadron, c-hadron, and τ-lepton properties as of 2018, Eur. Phys. J.C81 (2021) 226, arXiv:1909.12524

  45. [45]

    M. A. Shifman and M. B. Voloshin,Hierarchy of lifetimes of charmed and beautiful hadrons, Sov. Phys. JETP64 (1986) 698

  46. [46]

    I. I. Bigi, N. G. Uraltsev, and A. I. Vainshtein,Nonperturbative corrections to inclusive beauty and charm decays: QCD versus phenomenological models, Phys. Lett.B293 (1992) 430, arXiv:hep-ph/9207214, Erratum ibid.B297 (1992) 477

  47. [47]

    K. G. Wilson,Nonlagrangian models of current algebra, Phys. Rev.179 (1969) 1499

  48. [48]

    Albrecht, F

    J. Albrecht, F. Bernlochner, A. Lenz, and A. Rusov,Lifetimes of b-hadrons and mixing of neutral B-mesons: theoretical and experimental status, Eur. Phys. J. ST233 (2024) 359, arXiv:2402.04224

  49. [49]

    Lenz,Lifetimes and heavy quark expansion, Int

    A. Lenz,Lifetimes and heavy quark expansion, Int. J. Mod. Phys.A30 (2015) 1543005, arXiv:1405.3601

  50. [50]

    M. A. Shifman,Quark-hadron duality, At The Frontier of Particle Physics (2001) 1447

  51. [51]

    I. I. Y. Bigi and N. Uraltsev,A Vademecum on quark hadron duality, Int. J. Mod. Phys.A16 (2001) 5201, arXiv:hep-ph/0106346

  52. [52]

    T. Jubb, M. Kirk, A. Lenz, and G. Tetlalmatzi-Xolocotzi,On the ultimate precision of meson mixing observables, Nucl. Phys.B915 (2017) 431, arXiv:1603.07770. 432

  53. [53]

    M. B. Voloshin,Relations between inclusive decay rates of heavy baryons, Phys. Rept.320 (1999) 275, arXiv:hep-ph/9901445; B. Guberina, B. Melic, and H. Stefancic,Enhancement of preasymptotic effects in inclusive beauty decays, Phys. Lett.B469 (1999) 253, arXiv:hep-ph/9907468; M. Neubert and C. T. Sachrajda,Spectator effects in inclusive decays of beauty h...

  54. [54]

    Spectator effects and lifetimes of heavy hadrons

    F. Gabbiani, A. I. Onishchenko, and A. A. Petrov,Spectator effects and lifetimes of heavy hadrons, Phys. Rev. D70 (2004) 094031, arXiv:hep-ph/0407004

  55. [55]

    Numerical updates of lifetimes and mixing parameters of B mesons

    A. Lenz and U. Nierste,Numerical updates of lifetimes and mixing parameters ofB mesons, arXiv:1102.4274

  56. [56]

    Theoretical update of Bs-Bs-bar mixing

    A. Lenz and U. Nierste,Theoretical update ofBs − Bs mixing, JHEP06 (2007) 072, arXiv:hep-ph/0612167

  57. [57]

    The B^+ B_d^0 Lifetime Difference Beyond Leading Logarithms

    M. Benekeet al., The B+ − B0 d lifetime difference beyond leading logarithms, Nucl. Phys.B639 (2002) 389, arXiv:hep-ph/0202106

  58. [58]

    Lifetime Ratios of Beauty Hadrons at the Next-to-Leading Order in QCD

    E. Franco, V. Lubicz, F. Mescia, and C. Tarantino,Lifetime ratios of beauty hadrons at the next-to-leading order in QCD, Nucl. Phys.B633 (2002) 212, arXiv:hep-ph/0203089

  59. [59]

    D-meson lifetimes within the heavy quark expansion

    A. Lenz and T. Rauh,D-meson lifetimes within the heavy quark expansion, Phys. Rev. D88 (2013) 034004, arXiv:1305.3588

  60. [60]

    Mannel, D

    T. Mannel, D. Moreno, and A. Pivovarov,Heavy quark expansion for heavy hadron lifetimes: completing the 1/m3 b corrections, JHEP08 (2020) 089, arXiv:2004.09485

  61. [61]

    A. Lenz, M. L. Piscopo, and A. V. Rusov,Contribution of the Darwin operator to non-leptonic decays of heavy quarks, JHEP12 (2020) 199, arXiv:2004.09527

  62. [62]

    Finauri and P

    G. Finauri and P. Gambino,The q2 moments in inclusive semileptonic B decays, JHEP02 (2024) 206, arXiv:2310.20324

  63. [63]

    Bordone, B

    M. Bordone, B. Capdevila, and P. Gambino,Three loop calculations and inclusive Vcb, Phys. Lett. B822 (2021) 136679, arXiv:2107.00604

  64. [64]

    Bernlochneret al., First extraction of inclusive Vcb from q2 moments, JHEP10 (2022) 068, arXiv:2205.10274

    F. Bernlochneret al., First extraction of inclusive Vcb from q2 moments, JHEP10 (2022) 068, arXiv:2205.10274

  65. [65]

    M. Kirk, A. Lenz, and T. Rauh,Dimension-six matrix elements for meson mixing and lifetimes from sum rules, JHEP12 (2017) 068, arXiv:1711.02100, [Erratum: JHEP 06, 162 (2020)]

  66. [66]

    D. King, A. Lenz, and T. Rauh,SU(3) breaking effects in B and D meson lifetimes, JHEP06 (202210.1007/JHEP06(2022)134) 134, arXiv:2112.03691

  67. [67]

    Gratrexet al., Quark-hadron duality at work: lifetimes of bottom baryons, JHEP04 (2023) 034, arXiv:2301.07698

    J. Gratrexet al., Quark-hadron duality at work: lifetimes of bottom baryons, JHEP04 (2023) 034, arXiv:2301.07698

  68. [68]

    A. Lenz, M. L. Piscopo, and A. V. Rusov,Disintegration of beauty: a precision study, JHEP 01 (2023) 004, arXiv:2208.02643

  69. [69]

    Blacket al., Using Gradient Flow to Renormalise Matrix Elements for Meson Mixing and Lifetimes, PoSLATTICE2023(2024) 263, arXiv:2310.18059

    M. Blacket al., Using Gradient Flow to Renormalise Matrix Elements for Meson Mixing and Lifetimes, PoSLATTICE2023(2024) 263, arXiv:2310.18059. 433

  70. [70]

    J. Lin, W. Detmold, and S. Meinel,Lattice Study of Spectator Effects inb-hadron Decays, PoS LATTICE2022(2023) 417, arXiv:2212.09275

  71. [71]

    Kinget al., Revisiting inclusive decay widths of charmed mesons, JHEP08 (2022) 241, arXiv:2109.13219

    D. Kinget al., Revisiting inclusive decay widths of charmed mesons, JHEP08 (2022) 241, arXiv:2109.13219

  72. [72]

    A Precise Measurement of the B+, B0 and Mean b-hadron Lifetime with the DELPHI Detector at LEP I

    DELPHI collaboration, J. Abdallahet al., A precise measurement of theB+, B0 and mean b-hadron lifetime with the DELPHI detector at LEP1, Eur. Phys. J.C33 (2004) 307, arXiv:hep-ex/0401025

  73. [73]

    Measurement of the Bbar0 and B- Meson Lifetimes

    ALEPH collaboration, R. Barateet al., Measurement of theB 0 and B− meson lifetimes, Phys. Lett.B492 (2000) 275, arXiv:hep-ex/0008016

  74. [74]

    Buskulicet al., Improved measurement of theB 0 and B− meson lifetimes, Z

    ALEPH collaboration, D. Buskulicet al., Improved measurement of theB 0 and B− meson lifetimes, Z. Phys.C71 (1996) 31

  75. [75]

    Abreuet al., A measurement ofB+ and B0 lifetimes using Dℓ+ events, Z

    DELPHI collaboration, P. Abreuet al., A measurement ofB+ and B0 lifetimes using Dℓ+ events, Z. Phys.C68 (1995) 13

  76. [76]

    Adamet al., Lifetimes of charged and neutralB hadrons using event topology, Z

    DELPHI collaboration, W. Adamet al., Lifetimes of charged and neutralB hadrons using event topology, Z. Phys.C68 (1995) 363

  77. [77]

    Abreuet al., A precise measurement of theB0 d meson lifetime using a new technique, Z

    DELPHI collaboration, P. Abreuet al., A precise measurement of theB0 d meson lifetime using a new technique, Z. Phys.C74 (1997) 19, Erratum ibid.C75 (1997) 579

  78. [78]

    Acciarriet al., Upper limit on the lifetime difference of shortlived and longlived B0 s mesons, Phys

    L3 collaboration, M. Acciarriet al., Upper limit on the lifetime difference of shortlived and longlived B0 s mesons, Phys. Lett.B438 (1998) 417

  79. [79]

    Akerset al., Improved measurements of theB0 and B+ meson lifetimes, Z

    OPAL collaboration, R. Akerset al., Improved measurements of theB0 and B+ meson lifetimes, Z. Phys.C67 (1995) 379

  80. [80]

    Measurement of the B+ and B0 Lifetimes and Search for CP(T) Violation using Reconstructed Secondary Vertices

    OPAL collaboration, G. Abbiendiet al., Measurement of theB+ and B0 lifetimes and search for C P(T) violation using reconstructed secondary vertices, Eur. Phys. J.C12 (2000) 609, arXiv:hep-ex/9901017

Showing first 80 references.