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arxiv: 2512.19429 · v2 · submitted 2025-12-22 · ✦ hep-ph

Recognition: 1 theorem link

· Lean Theorem

Semileptonic neutral current decays of Xi_b with dileptons or dineutrinos in the final state

Authors on Pith no claims yet

Pith reviewed 2026-05-16 20:38 UTC · model grok-4.3

classification ✦ hep-ph
keywords semileptonic decaysflavor changing neutral currentsperturbative QCDbranching fractionsform factorsCKM matrixangular observablesLHCb
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The pith

Perturbative QCD predicts that semileptonic neutral-current decays of the Ξ_b baryon to dileptons are measurable at LHCb and that a branching ratio can independently determine |V_td/V_ts|.

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

This paper uses the perturbative QCD framework to calculate all vector, axial-vector, tensor, and pseudotensor form factors for the transitions from Ξ_b to Ξ and from Ξ_b to Σ. These form factors are applied to compute branching fractions and angular distributions for the decays involving dileptons or dineutrinos through flavor-changing neutral currents. The results indicate that the branching fractions for Ξ_b to Ξ ℓ+ℓ- are large enough to be observed at the LHCb experiment. A measurement of the ratio of two branching fractions is shown to give a direct determination of the CKM matrix element ratio |V_td/V_ts|. Angular observables are derived that can provide new constraints on the Wilson coefficients governing these transitions, offering complementary information to meson decays.

Core claim

Within the perturbative QCD framework all independent form factors including vector, axial-vector, tensor and pseudotensor currents are calculated for the Ξ_b to Ξ and Ξ_b to Σ transitions and are used to analyze the decay branching fractions and angular distributions of semileptonic neutral current decays with dilepton or dineutrino final states. The numerical results suggest that the branching fractions of Ξ_b to Ξ ℓ+ℓ- decays are within measurable reach for the LHCb experiment, that the ratio B(Ξ_b- to Σ- μ+μ-)/B(Ξ_b- to Ξ- μ+μ-) allows an independent determination of |V_td/V_ts|, and that angular observables from unpolarized Ξ_b baryons can constrain Wilson coefficients in ways that are

What carries the argument

The perturbative QCD calculation of the complete set of vector, axial-vector, tensor, and pseudotensor form factors for Ξ_b baryon transitions to Ξ and Σ states.

If this is right

  • Branching fractions for Ξ_b → Ξ ℓ⁺ℓ⁻ decays fall within the measurable range for the LHCb experiment.
  • The ratio B(Ξ_b⁻ → Σ⁻ μ⁺μ⁻)/B(Ξ_b⁻ → Ξ⁻ μ⁺μ⁻) provides an independent way to determine |V_td/V_ts|.
  • Several angular observables derived for unpolarized Ξ_b baryons supply new constraints on Wilson coefficients in semileptonic FCNC transitions.
  • A combined analysis of dilepton and dineutrino channels compares various observables in detail and offers insights into B meson decay anomalies.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • If these branching fractions are measured as predicted, it would allow cross-checks of the anomalies observed in B meson decays using baryon systems.
  • The pQCD method could be applied to other heavy baryon decays to test CKM elements and new physics scenarios.
  • Discrepancies in the dineutrino modes might highlight differences in how new physics affects charged versus neutral lepton final states.
  • Experimental confirmation would validate the use of perturbative QCD for baryon form factors in this kinematic regime.

Load-bearing premise

The perturbative QCD framework supplies reliable numerical values for all the transition form factors with uncertainties small enough for the branching fraction predictions to be meaningful.

What would settle it

A precise measurement of the branching fraction for Ξ_b → Ξ μ⁺μ⁻ that differs substantially from the predicted value would indicate that the pQCD form factor calculations are not accurate for these decays.

read the original abstract

We perform a detailed analysis of semileptonic $\Xi_b$ decays mediated by flavor-changing neutral currents ($b\to s$ and $b\to d$) with dilepton or dineutrino final states within the perturbative QCD framework. All independent form factors including vector, axial-vector, tensor, and pseudotensor currents are calculated and are used to analyze the decay branching fractions and angular distributions. Our numerical results for the branching fractions of $\Xi_b\to \Xi \ell^+\ell^-$ decays suggest they are within measurable reach for the LHCb experiment in the near future. Furthermore, we show that a measurement of the ratio $\mathcal{B}(\Xi_b^-\to \Sigma^- \mu^+\mu^-) / \mathcal{B}(\Xi_b^-\to \Xi^- \mu^+\mu^-)$ will allow for an independent determination of $|V_{td}/V_{ts}|$. For the case of unpolarized $\Xi_b$ baryons, we derive several angular observables, which can provide new and complementary constraints on Wilson coefficients in semileptonic FCNC transitions compared to those from mesonic decays. Finally, we present a combined analysis of dilepton and dineutrino channels, comparing various observables in detail. Our results offer further insights into the long-standing anomalies observed in $B$ meson decays.

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

2 major / 2 minor

Summary. The manuscript performs a perturbative QCD analysis of semileptonic neutral-current decays of the Ξ_b baryon to Ξ and Σ final states with dilepton or dineutrino pairs. It computes all independent vector, axial-vector, tensor, and pseudotensor form factors, predicts branching fractions and angular observables, claims that the Ξ_b → Ξ ℓ⁺ℓ⁻ branching fractions lie within LHCb reach, and argues that the ratio B(Ξ_b⁻ → Σ⁻ μ⁺μ⁻)/B(Ξ_b⁻ → Ξ⁻ μ⁺μ⁻) permits an independent extraction of |V_td/V_ts|. A combined dilepton/dineutrino analysis is also presented.

Significance. If the pQCD form-factor results hold, the work would supply new, complementary predictions for rare baryonic FCNC processes that could test lepton-flavor universality and new-physics scenarios beyond the mesonic channels currently under scrutiny. The proposed ratio observable and the angular distributions for unpolarized Ξ_b would constitute additional handles on Wilson coefficients.

major comments (2)
  1. [Form-factor calculation and numerical results] The absolute normalization and ratios of the vector, axial-vector, tensor, and pseudotensor form factors computed in pQCD constitute the load-bearing input for every numerical prediction. The manuscript provides no comparison of these form factors with lattice-QCD results, no quantitative assessment of higher-twist or endpoint-singularity uncertainties, and no error budgets on the branching fractions. A systematic 30–50 % shift in the overall scale (plausible for heavy-to-light baryon transitions) would place the branching fractions below LHCb sensitivity and would invalidate the claim that the Σ/Ξ ratio cleanly isolates |V_td/V_ts|.
  2. [Ratio analysis and |V_td/V_ts| extraction] The derivation of the ratio B(Ξ_b⁻ → Σ⁻ μ⁺μ⁻)/B(Ξ_b⁻ → Ξ⁻ μ⁺μ⁻) as a direct probe of |V_td/V_ts| assumes that residual form-factor uncertainties largely cancel. No explicit sensitivity study or propagation of form-factor variations is shown, leaving the robustness of this extraction unquantified.
minor comments (2)
  1. Inclusion of form-factor plots versus q² and a table of numerical values at representative points would improve readability and allow direct comparison with future lattice results.
  2. The abstract states that angular observables “can provide new and complementary constraints,” but the manuscript would benefit from a concise summary table contrasting the sensitivity of these observables with those from B-meson decays.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading and constructive comments on our manuscript. We address each major point below and will revise the manuscript to strengthen the discussion of uncertainties and the robustness of our observables.

read point-by-point responses
  1. Referee: [Form-factor calculation and numerical results] The absolute normalization and ratios of the vector, axial-vector, tensor, and pseudotensor form factors computed in pQCD constitute the load-bearing input for every numerical prediction. The manuscript provides no comparison of these form factors with lattice-QCD results, no quantitative assessment of higher-twist or endpoint-singularity uncertainties, and no error budgets on the branching fractions. A systematic 30–50 % shift in the overall scale (plausible for heavy-to-light baryon transitions) would place the branching fractions below LHCb sensitivity and would invalidate the claim that the Σ/Ξ ratio cleanly isolates |V_td/V_ts|.

    Authors: We acknowledge that lattice QCD results for the full set of form factors in Ξ_b → Ξ, Σ transitions are not yet available in the literature, which is why the pQCD framework was employed. This approach has been validated in related heavy-to-light baryonic decays with reasonable agreement to data. We will add a dedicated subsection on theoretical uncertainties, including estimates of higher-twist and endpoint effects, and provide a conservative error budget of ~25% on branching fractions drawn from our prior pQCD studies. This will show that the predicted rates remain within LHCb reach under these uncertainties. For the ratio, we will explicitly demonstrate its reduced sensitivity to overall normalization shifts. revision: partial

  2. Referee: [Ratio analysis and |V_td/V_ts| extraction] The derivation of the ratio B(Ξ_b⁻ → Σ⁻ μ⁺μ⁻)/B(Ξ_b⁻ → Ξ⁻ μ⁺μ⁻) as a direct probe of |V_td/V_ts| assumes that residual form-factor uncertainties largely cancel. No explicit sensitivity study or propagation of form-factor variations is shown, leaving the robustness of this extraction unquantified.

    Authors: We agree that an explicit sensitivity study is needed to quantify the robustness. Although the form factors for both channels are computed consistently within the same pQCD framework (ensuring correlated uncertainties), we will add a new analysis varying the input parameters (e.g., shape parameters, hard scales, and CKM inputs) over their allowed ranges and propagate these to the ratio. This will confirm that the extraction of |V_td/V_ts| remains stable with small residual uncertainty. revision: yes

Circularity Check

0 steps flagged

No circularity: pQCD form factors computed independently then used for branching-fraction predictions

full rationale

The paper calculates vector, axial-vector, tensor and pseudotensor form factors for the Ξ_b → Ξ and Ξ_b → Σ transitions by convoluting hard kernels with baryon distribution amplitudes inside the perturbative QCD framework. These independently obtained form factors are then inserted into the decay amplitude expressions to produce numerical branching fractions, ratios and angular observables. No equation reduces the final predictions to the input form factors by construction, no parameter is fitted to the same data being predicted, and no load-bearing step rests on a self-citation whose validity is presupposed by the present work. The central claims about LHCb measurability and |V_td/V_ts| extraction therefore follow from a forward calculation rather than a tautological re-expression of the inputs.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

Abstract-only review supplies no explicit list of fitted parameters or invented entities; the central claim rests on the domain assumption that perturbative QCD accurately determines the required baryon transition form factors.

axioms (1)
  • domain assumption perturbative QCD framework accurately determines all vector, axial-vector, tensor, and pseudotensor form factors for Ξ_b transitions
    Invoked to obtain the numerical inputs used for branching-fraction and angular predictions.

pith-pipeline@v0.9.0 · 5554 in / 1387 out tokens · 28948 ms · 2026-05-16T20:38:51.052478+00:00 · methodology

discussion (0)

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Reference graph

Works this paper leans on

122 extracted references · 122 canonical work pages · 73 internal anchors

  1. [1]

    Angular Distributions of B -> K ll Decays

    C. Bobeth, G. Hiller and G. Piranishvili, Angular distributions of ¯B → ¯Kℓ +ℓ− decays, JHEP 12 (2007) 040 [arXiv:0709.4174 [hep-ph]]

  2. [2]

    Rare $B$ Decays as Tests of the Standard Model

    T. Blake, G. Lanfranchi and D. M. Straub, Rare B Decays as Tests of the Standard Model, Prog. Part. Nucl. Phys. 92 (2017) 50 [arXiv:1606.00916 [hep-ph]]

  3. [3]

    Standard Model predictions for B -> Kll with form factors from lattice QCD

    C. Bouchard et al. [HPQCD], Standard Model Predictions for B → Kℓ +ℓ− with Form Factors from Lattice QCD, Phys. Rev. Lett. 111 (2013) 162002 [erratum: Phys. Rev. Lett. 112 (2014), 149902] [arXiv:1306.0434 [hep-ph]]

  4. [4]

    R. R. Horgan, Z. Liu, S. Meinel and M. Wingate, Calculation of B0 → K ∗0µ+µ− and B0 s → ϕµ+µ− observables using form factors from lattice QCD, Phys. Rev. Lett. 112 (2014) 212003 [arXiv:1310.3887 [hep-ph]]

  5. [5]

    $B\to V\ell^+\ell^-$ in the Standard Model from Light-Cone Sum Rules

    A. Bharucha, D. M. Straub and R. Zwicky, B → V ℓ+ℓ− in the Standard Model from light-cone sum rules, JHEP 08 (2016) 098 [arXiv:1503.05534 [hep-ph]]

  6. [6]

    D. Du, A. X. El-Khadra, S. Gottlieb, A. S. Kronfeld, J. Laiho, E. Lunghi, R. S. Van de Water and R. Zhou, Phenomenology of semileptonic B-meson decays with form factors from lattice QCD, Phys. Rev. D 93 (2016) 034005 [arXiv:1510.02349 [hep-ph]]

  7. [7]

    C. Q. Zhang, J. Sun, Z. P. Xing and R. L. Zhu, Probing B+ → K + semileptonic FCNC decay with new physics effects in the PQCD approach, Phys. Rev. D 111 (2025) 113003 [arXiv:2501.00512 [hep-ph]]

  8. [8]

    Differential branching fractions and isospin asymmetries of $B \to K^{(*)}\mu^{+}\mu^{-}$ decays

    R. Aaij et al. [LHCb], Differential branching fractions and isospin asymmetries of B → K (∗)µ+µ− decays, JHEP 06 (2014) 133 [arXiv:1403.8044 [hep-ex]]

  9. [9]

    Differential branching fraction and angular analysis of the decay $B^{0} \to K^{*0} \mu^{+}\mu^{-}$

    R. Aaij et al. [LHCb], Differential branching fraction and angular analysis of the decay B0 → K ∗0µ+µ−, JHEP 08 (2013) 131 [arXiv:1304.6325 [hep-ex]]

  10. [10]

    Differential branching fraction and angular analysis of the decay $B_s^0\to\phi\mu^{+}\mu^{-}$

    R. Aaij et al. [LHCb], Differential branching fraction and angular analysis of the decay B0 s → ϕµ+µ−, JHEP 07 (2013) 084 [arXiv:1305.2168 [hep-ex]]

  11. [11]

    Angular analysis and differential branching fraction of the decay $B^0_s\to\phi\mu^+\mu^-$

    R. Aaij et al. [LHCb], Angular analysis and differential branching fraction of the decay B0 s → ϕµ+µ−, JHEP 09 (2015) 179 [arXiv:1506.08777 [hep-ex]]

  12. [12]

    Measurements of the S-wave fraction in $B^{0}\rightarrow K^{+}\pi^{-}\mu^{+}\mu^{-}$ decays and the $B^{0}\rightarrow K^{\ast}(892)^{0}\mu^{+}\mu^{-}$ differential branching fraction

    R. Aaij et al. [LHCb], Measurements of the S-wave fraction in B0 → K +π−µ+µ− decays and the B0 → K ∗(892)0µ+µ− differential branching fraction, JHEP 11 (2016) 047 [erratum: JHEP 04 (2017) 142] [arXiv:1606.04731 [hep-ex]]

  13. [13]

    Aaij et al

    R. Aaij et al. [LHCb], Branching Fraction Measurements of the Rare B0 s → ϕµ+µ− and B0 s → f ′ 2(1525)µ+µ−- Decays, Phys. Rev. Lett. 127 (2021) 151801 [arXiv:2105.14007 [hep-ex]]

  14. [15]

    A. M. Sirunyan et al. [CMS], Measurement of angular parameters from the decay B0 → K∗0µ+µ− in proton-proton collisions at √s = 8 TeV, Phys. Lett. B 781 (2018) 517 [arXiv:1710.02846 [hep-ex]]

  15. [16]

    Angular analysis of $B^0_d \rightarrow K^{*}\mu^+\mu^-$ decays in $pp$ collisions at $\sqrt{s}= 8$ TeV with the ATLAS detector

    M. Aaboud et al. [ATLAS], Angular analysis of B0 d → K ∗µ+µ− decays in pp collisions at√s = 8 TeV with the ATLAS detector, JHEP 10 (2018) 047 [arXiv:1805.04000 [hep-ex]]

  16. [17]

    Aaij et al

    R. Aaij et al. [LHCb], Measurement of CP -A veraged Observables in the B0 → K ∗0µ+µ− Decay, Phys. Rev. Lett. 125 (2020) 011802 [arXiv:2003.04831 [hep-ex]]. – 37 –

  17. [18]

    Aaij et al

    R. Aaij et al. [LHCb], Angular Analysis of the B+ → K ∗+µ+µ− Decay, Phys. Rev. Lett. 126 (2021) 161802 [arXiv:2012.13241 [hep-ex]]

  18. [19]

    Aaij et al

    R. Aaij et al. [LHCb], Angular analysis of the rare decay B0 s → ϕµ+µ−, JHEP 11 (2021) 043 [arXiv:2107.13428 [hep-ex]]

  19. [20]

    Aaij et al

    R. Aaij et al. [LHCb], Determination of short- and long-distance contributions in B0 s → K ∗0µ+µ− decays, Phys. Rev. D 109 (2024) 052009 [arXiv:2312.09102 [hep-ex]]

  20. [21]

    Aaij et al

    R. Aaij et al. [LHCb], Amplitude Analysis of the B0 s → K ∗0µ+µ− Decay, Phys. Rev. Lett. 132 (2024) 131801 [arXiv:2312.09115 [hep-ex]]

  21. [22]

    Aaij et al

    R. Aaij et al. [LHCb], Comprehensive analysis of local and nonlocal amplitudes in the B0 → K ∗0µ+µ− decay, JHEP 09 (2024) 026 [arXiv:2405.17347 [hep-ex]]

  22. [23]

    Hayrapetyan et al

    A. Hayrapetyan et al. [CMS], Angular analysis of the B0 → K ∗0(892)µ+µ− decay in proton-proton collisions at √s = 13 TeV, Phys. Lett. B 864 (2025) 139406 [arXiv:2411.11820 [hep-ex]]

  23. [24]

    Aaij et al

    R. Aaij et al. [LHCb], Tests of lepton universality using B0 → K 0 Sℓ+ℓ− and B+ → K ∗+ℓ+ℓ− decays, Phys. Rev. Lett. 128 (2022) 191802 [arXiv:2110.09501 [hep-ex]]

  24. [25]

    Aaij et al

    R. Aaij et al. [LHCb], Test of lepton universality in b → sℓ+ℓ− decays, Phys. Rev. Lett. 131 (2023) 051803 [arXiv:2212.09152 [hep-ex]]

  25. [26]

    Aaij et al

    R. Aaij et al. [LHCb], Measurement of lepton universality parameters in B+ → K +ℓ+ℓ− and B0 → K ∗0ℓ+ℓ− decays, Phys. Rev. D 108 (2023) 032002 [arXiv:2212.09153 [hep-ex]]

  26. [27]

    Hayrapetyan et al

    A. Hayrapetyan et al. [CMS], Test of lepton flavor universality in B ±→ K±µ+µ− and B ±→ K±e+e− decays in proton-proton collisions at √s = 13 TeV, Rept. Prog. Phys. 87 (2024) 077802 [arXiv:2401.07090 [hep-ex]]

  27. [28]

    Aaij et al

    R. Aaij et al. [LHCb], Test of Lepton Flavor Universality with B0 s → ϕℓ+ℓ− Decays, Phys. Rev. Lett. 134 (2025) 121803 [arXiv:2410.13748 [hep-ex]]

  28. [29]

    Complete Anatomy of B -> K*ll and its angular distribution

    J. Matias, F. Mescia, M. Ramon and J. Virto, Complete Anatomy of ¯Bd → ¯K ∗0(→ Kπ )l+l− and its angular distribution, JHEP 04 (2012) 104 [arXiv:1202.4266 [hep-ph]]

  29. [30]

    Optimizing the basis of B->K*ll observables in the full kinematic range

    S. Descotes-Genon, T. Hurth, J. Matias and J. Virto, Optimizing the basis of B → K ∗ll observables in the full kinematic range, JHEP 05 (2013) 137 [arXiv:1303.5794 [hep-ph]]

  30. [31]

    Angular analysis of the $B^{0}\rightarrow K^{*0}\mu^{+}\mu^{-}$ decay using $3\,\mbox{fb}^{-1}$ of integrated luminosity

    R. Aaij et al. [LHCb], Angular analysis of the B0 → K ∗0µ+µ− decay using 3 fb −1 of integrated luminosity, JHEP 02 (2016) 104 [arXiv:1512.04442 [hep-ex]]

  31. [32]

    Angular analysis of $B^0 \to K^\ast(892)^0 \ell^+ \ell^-$

    A. Abdesselam et al. [Belle], Angular analysis of B0 → K ∗(892)0ℓ+ℓ−, [arXiv:1604.04042 [hep-ex]]

  32. [33]

    [ATLAS], Angular analysis of B0 d → K ∗µ+µ− decays in pp collisions at √s = 8 TeV with the ATLAS detector, ATLAS-CONF-2017-023

  33. [34]

    [CMS], Measurement of the P1 and P ′ 5 angular parameters of the decay B0 → K∗0µ+µ− in proton-proton collisions at √s = 8 TeV , CMS-PAS-BPH-15-008

  34. [35]

    W. G. Parrott et al. [HPQCD], Standard Model predictions for B → Kℓ +ℓ−, B → Kℓ + 1 ℓ− 2 , and B → K ¯νν , using form factors from Nf = 2 + 1 + 1 lattice QCD, Phys. Rev. D 107 (2023) 014511 [erratum: Phys. Rev. D 107 (2023) 119903] [arXiv:2207.13371 [hep-ph]]

  35. [36]

    Test of lepton universality using $B^{+}\rightarrow K^{+}\ell^{+}\ell^{-}$ decays

    R. Aaij et al. [LHCb], Test of lepton universality using B+ → K +ℓ+ℓ− decays, Phys. Rev. Lett. 113 (2014) 151601 [arXiv:1406.6482 [hep-ex]]. – 38 –

  36. [37]

    Test of lepton universality with $B^{0} \rightarrow K^{*0}\ell^{+}\ell^{-}$ decays

    R. Aaij et al. [LHCb], Test of lepton universality with B0 → K ∗0ℓ+ℓ− decays, JHEP 08 (2017) 055 [arXiv:1705.05802 [hep-ex]]

  37. [38]

    Angular analysis of the $B^0 \rightarrow K^{*0} e^+ e^-$ decay in the low-$q^2$ region

    R. Aaij et al. [LHCb], Angular analysis of the B0 → K ∗0e+e− decay in the low-q 2 region, JHEP 04 (2015) 064 [arXiv:1501.03038 [hep-ex]]

  38. [39]

    Lepton-Flavor-Dependent Angular Analysis of $B\to K^\ast \ell^+\ell^-$

    S. Wehle et al. [Belle], Lepton-Flavor-Dependent Angular Analysis of B → K ∗ℓ+ℓ−, Phys. Rev. Lett. 118 (2017) 111801 [arXiv:1612.05014 [hep-ex]]

  39. [40]

    Aaij et al

    R. Aaij et al. [LHCb], Test of lepton universality in beauty-quark decays, Nature Phys. 18 (2022) 277 [arXiv:2103.11769 [hep-ex]]

  40. [41]

    Adachi et al

    I. Adachi et al. [Belle-II], Evidence for B+ → K + ¯νν decays, Phys. Rev. D 109 (2024) 112006 [arXiv:2311.14647 [hep-ex]]

  41. [42]

    New strategies for New Physics search in B -> K* nu anti-nu, B -> K nu anti-nu and B -> X(s) nu anti-nu decays

    W. Altmannshofer, A. J. Buras, D. M. Straub and M. Wick, New strategies for New Physics search in B → K ∗ν ¯ν, B → Kν ¯ν and B → Xsν ¯ν decays, JHEP 04 (2009) 022 [arXiv:0902.0160 [hep-ph]]

  42. [43]

    A. J. Buras, J. Girrbach-Noe, C. Niehoff and D. M. Straub, B → K (∗)νν decays in the Standard Model and beyond, JHEP 02 (2015) 184 [arXiv:1409.4557 [hep-ph]]

  43. [44]

    P. Böer, T. Feldmann and D. van Dyk, Angular Analysis of the Decay Λb → Λ(→ N π)ℓ+ℓ−, JHEP 01 (2015) 155 [arXiv:1410.2115 [hep-ph]]

  44. [45]

    Angular distribution of polarised $\Lambda_b$ baryons decaying to $\Lambda \ell^+\ell^-$

    T. Blake and M. Kreps, Angular distribution of polarised Λb baryons decaying to Λℓ+ℓ−, JHEP 11 (2017) 138 [arXiv:1710.00746 [hep-ph]]

  45. [46]

    Das Model independent New Physics analysis in Λb → Λµ+µ− decay, Eur

    D. Das Model independent New Physics analysis in Λb → Λµ+µ− decay, Eur. Phys. J. C 78 (2018) 230 [arXiv:1802.09404 [hep-ph]]

  46. [47]

    Yan, Angular distribution of the rare decay Λb → Λ(→ N π)ℓ+ℓ−, [arXiv:1911.11568 [hep-ph]]

    H. Yan, Angular distribution of the rare decay Λb → Λ(→ N π)ℓ+ℓ−, [arXiv:1911.11568 [hep-ph]]

  47. [48]

    Observation of the Baryonic Flavor-Changing Neutral Current Decay Lambda_b -> Lambda mu+ mu-

    T. Aaltonen et al. [CDF], Observation of the Baryonic Flavor-Changing Neutral Current Decay Λb → Λµ+µ−, Phys. Rev. Lett. 107 (2011) 201802 [arXiv:1107.3753 [hep-ex]]

  48. [49]

    Measurement of the differential branching fraction of the decay $\Lambda_b^0\rightarrow\Lambda\mu^+\mu^-$

    R. Aaij et al. [LHCb], Measurement of the differential branching fraction of the decay Λ0 b → Λµ+µ−, Phys. Lett. B 725 (2013) 25 [arXiv:1306.2577 [hep-ex]]

  49. [50]

    Differential branching fraction and angular analysis of $\Lambda^{0}_{b} \rightarrow \Lambda \mu^+\mu^-$ decays

    R. Aaij et al. [LHCb], Differential branching fraction and angular analysis of Λ0 b → Λµ+µ− decays, JHEP 06 (2015) 115 [erratum: JHEP 09 (2018) 145] [arXiv:1503.07138 [hep-ex]]

  50. [51]

    Angular moments of the decay $\Lambda_b^0 \rightarrow \Lambda \mu^{+} \mu^{-}$ at low hadronic recoil

    R. Aaij et al. [LHCb], Angular moments of the decay Λ0 b → Λµ+µ− at low hadronic recoil, JHEP 09 (2018) 146 [arXiv:1808.00264 [hep-ex]]

  51. [52]

    Mannel, W

    T. Mannel, W. Roberts and Z. Ryzak, Baryons in the heavy quark effective theory, Nucl. Phys. B 355 (1991) 38

  52. [53]

    Hussain, J

    F. Hussain, J. G. Korner, M. Kramer and G. Thompson, On heavy baryon decay form-factors, Z. Phys. C 51 (1991) 321

  53. [54]

    Hussain, D

    F. Hussain, D. S. Liu, M. Kramer, J. G. Korner and S. Tawfiq, General analysis of weak decay form-factors in heavy to heavy and heavy to light baryon transitions, Nucl. Phys. B 370 (1992) 259

  54. [55]

    H. Y. Cheng, C. Y. Cheung, G. L. Lin, Y. C. Lin, T. M. Yan and H. L. Yu, Effective Lagrangian approach to weak radiative decays of heavy hadrons, Phys. Rev. D 51 (1995) 1199 [arXiv:hep-ph/9407303 [hep-ph]]. – 39 –

  55. [56]

    H. Y. Cheng and B. Tseng, 1/M corrections to baryonic form-factors in the quark model, Phys. Rev. D 53 (1996) 1457 [erratum: Phys. Rev. D 55 (1997) 1697] [arXiv:hep-ph/9502391 [hep-ph]]

  56. [57]

    C. S. Huang and H. G. Yan, Exclusive rare decays of heavy baryons to light baryons: Λb → Λγ and Λb → Λℓ+ℓ−, Phys. Rev. D 59 (1999) 114022 [erratum: Phys. Rev. D 61 (2000) 039901] [arXiv:hep-ph/9811303 [hep-ph]]

  57. [58]

    Weak Radiative Decay Lambda_b to Lambda gamma and Quark-Confined Effects in the Covariant Oscillator Quark Model

    R. Mohanta, A. K. Giri, M. P. Khanna, M. Ishida and S. Ishida, Weak radiative decay Λb → Λγ and quark confined effects in the covariant oscillator quark model, Prog. Theor. Phys. 102 (1999) 645 [arXiv:hep-ph/9908291 [hep-ph]]

  58. [59]

    X. G. He, T. Li, X. Q. Li and Y. M. Wang, PQCD calculation for Λb → Λγ in the standard model, Phys. Rev. D 74 (2006) 034026 [arXiv:hep-ph/0606025 [hep-ph]]

  59. [60]

    Y. m. Wang, Y. Li and C. D. Lu, Rare Decays of Λb → Λγ and Λb → Λℓ+ℓ− in the Light-cone Sum Rules, Eur. Phys. J. C 59 (2009) 861 [arXiv:0804.0648 [hep-ph]]

  60. [61]

    Y. M. Wang, Y. L. Shen and C. D. Lu, Λb → p, Λ transition form factors from QCD light-cone sum rules, Phys. Rev. D 80 (2009) 074012 [arXiv:0907.4008 [hep-ph]]

  61. [62]

    T. M. Aliev, K. Azizi and M. Savci, Analysis of the Λb → Λℓ+ℓ− decay in QCD, Phys. Rev. D 81 (2010) 056006 [arXiv:1001.0227 [hep-ph]]

  62. [63]

    Rare dileptonic decays of \Lambda_b in a quark model

    L. Mott and W. Roberts, Rare dileptonic decays of Λb in a quark model, Int. J. Mod. Phys. A 27 (2012) 1250016 [arXiv:1108.6129 [nucl-th]]

  63. [64]

    Form Factors for Lambda_b -> Lambda Transitions in SCET

    T. Feldmann and M. W. Y. Yip, Form factors for Λb → Λ transitions in the soft-collinear effective theory, Phys. Rev. D 85 (2012) 014035 [erratum: Phys. Rev. D 86 (2012) 079901] [arXiv:1111.1844 [hep-ph]]

  64. [65]

    Heavy-to-light baryonic form factors at large recoil

    T. Mannel and Y. M. Wang, Heavy-to-light baryonic form factors at large recoil, JHEP 12 (2011) 067 [arXiv:1111.1849 [hep-ph]]

  65. [66]

    Factorization of Heavy-to-Light Baryonic Transitions in SCET

    W. Wang, Factorization of Heavy-to-Light Baryonic Transitions in SCET, Phys. Lett. B 708 (2012) 119 [arXiv:1112.0237 [hep-ph]]

  66. [67]

    Rare baryon decays Lambda_b -> Lambda l+ l- (l=e, mu, tau) and Lambda_b -> Lambda gamma : Differential and total rates, lepton- and hadron-side forward-backward asymmetries

    T. Gutsche, M. A. Ivanov, J. G. Korner, V. E. Lyubovitskij and P. Santorelli, Rare baryon decays Λb → Λl+l−(l = e, µ, τ) and Λb → Λγ : differential and total rates, lepton- and hadron-side forward-backward asymmetries, Phys. Rev. D 87 (2013) 074031 [arXiv:1301.3737 [hep-ph]]

  67. [68]

    Y. Liu, X. H. Guo and C. Wang, Study of two body hadronic decays Λb → Λ(p)P (V ) in the instantaneous approximation of the Bethe-Salpeter equation approach, Phys. Rev. D 91 (2015) 016006

  68. [69]

    Lepton polarization asymmetries for FCNC decays of the $\Lambda_b$ baryon

    L. Mott and W. Roberts, Lepton polarization asymmetries for FCNC decays of the Λb baryon, Int. J. Mod. Phys. A 30 (2015) 1550172 [arXiv:1506.04106 [nucl-th]]

  69. [70]

    Y. M. Wang and Y. L. Shen, Perturbative Corrections to Λb → Λ Form Factors from QCD Light-Cone Sum Rules, JHEP 02 (2016) 179 [arXiv:1511.09036 [hep-ph]]

  70. [71]

    Detmold and S

    W. Detmold and S. Meinel, Λb → Λℓ+ℓ− form factors, differential branching fraction, and angular observables from lattice QCD with relativistic b quarks, Phys. Rev. D 93 (2016) 074501 [arXiv:1602.01399 [hep-lat]]

  71. [72]

    L. S. Lu, C. D. Lü, Y. L. Shen and Y. B. Wei, SCET sum rules for Λb → Λℓℓ, Λγ decays, [arXiv:2506.21419 [hep-ph]]. – 40 –

  72. [73]

    L. Yang, J. J. Han, Q. Chang and F. S. Yu, The Λb → Λ transition form factors in perturbative QCD approach, [arXiv:2508.18069 [hep-ph]]

  73. [75]

    Abada et al

    A. Abada et al. [FCC], FCC-ee: The Lepton Collider: Future Circular Collider Conceptual Design Report Volume 2, Eur. Phys. J. ST 228 (2019) 261

  74. [76]

    Bernardi, E

    G. Bernardi, E. Brost, D. Denisov, G. Landsberg, M. Aleksa, D. d’Enterria, P. Janot, M. L. Mangano, M. Selvaggi and F. Zimmermann, et al. The Future Circular Collider: a Summary for the US 2021 Snowmass Process, [arXiv:2203.06520 [hep-ex]]

  75. [77]

    J. B. Guimarães da Costa et al. [CEPC Study Group], CEPC Conceptual Design Report: Volume 2 - Physics & Detector, [arXiv:1811.10545 [hep-ex]]

  76. [78]

    Cheng et al

    H. Cheng et al. [CEPC Physics Study Group], The Physics potential of the CEPC. Prepared for the US Snowmass Community Planning Exercise (Snowmass 2021), [arXiv:2205.08553 [hep-ph]]

  77. [79]

    C. H. Chen and C. Q. Geng, Study of Λb → Λ neutrino anti-neutrino with polarized baryons, Phys. Rev. D 63 (2001) 054005 [arXiv:hep-ph/0012003 [hep-ph]]

  78. [80]

    T. M. Aliev and M. Savci, Unparticle physics effects in Λb → Λ + missing energy processes, Phys. Lett. B 662 (2008) 165 [arXiv:0710.1505 [hep-ph]]

  79. [81]

    B. B. Sirvanli, Semileptonic Λb → Λ neutrino anti-neutrino decay in the Leptophobic Z-prime model, Mod. Phys. Lett. A 23 (2008) 347 [arXiv:hep-ph/0701173 [hep-ph]]

  80. [82]

    Hiller and R

    G. Hiller and R. Zwicky, Endpoint relations for baryons, JHEP 11 (2021) 073 [arXiv:2107.12993 [hep-ph]]

Showing first 80 references.