pith. sign in

arxiv: 2512.08902 · v2 · submitted 2025-12-09 · ✦ hep-ph

Update of the nonlocal sub-leading {O}₁-{O}₇ contribution to bar B to X_s γ at LO

Pith reviewed 2026-05-16 23:58 UTC · model grok-4.3

classification ✦ hep-ph
keywords B to Xs gammanon-local contributionssub-leading correctionspenguin operatorsVoloshin termrare B decaysflavor physicselectroweak penguins
0
0 comments X

The pith

Complete non-local calculation revises the range for the O1-O7 contribution to B to Xs gamma

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

The paper updates previous calculations of the non-local sub-leading contribution to the inclusive penguin decay of B mesons to strange quarks plus a photon. Earlier analyses subtracted the local Voloshin term from the interference of operators O1 and O7, but this work computes the full non-local piece while incorporating the strong correlations between the uncertainties of the local and non-local terms. The resulting range for the non-local contribution changes substantially. This matters for refining theoretical predictions ahead of next-to-leading-order work at order alpha_s.

Core claim

The complete non-local contribution, evaluated without subtracting the local Voloshin term and with explicit use of the high correlation between local and non-local uncertainties, produces a revised numerical range that differs markedly from earlier subtracted results.

What carries the argument

The full non-local sub-leading O1^c-O7gamma interference term in the effective weak Hamiltonian for b to s gamma transitions, computed at leading order while retaining the correlated uncertainties with the local Voloshin term.

If this is right

  • The estimated range for the non-local contribution is updated to reflect the full term.
  • The new range supplies an improved input for the ongoing analysis at order alpha_s.
  • The total theoretical prediction for the branching ratio incorporates this revised non-local piece.

Where Pith is reading between the lines

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

  • The revised range may tighten or loosen constraints on new physics from measured B decay rates.
  • Similar correlation handling could be applied to other rare decays involving operator interferences.
  • Experimental analyses of the photon spectrum might now use the updated range as a benchmark.

Load-bearing premise

The uncertainties of the local Voloshin term and the non-local term are sufficiently correlated that their joint treatment yields a reliable revised range.

What would settle it

An independent leading-order calculation of the same non-local contribution or a future precision measurement of the photon energy spectrum in B to Xs gamma that lies outside the newly quoted range would test the result.

read the original abstract

In all previous calculations of the non-local sub-leading contribution to the inclusive penguin decay $\bar B \to X_s \gamma$ due to the interference of the electroweak operators ${O}_1^c$ - ${O}_{7\gamma}$ the local Voloshin term was subtracted. In view of the ongoing analysis at order $\alpha_s$, we present a calculation of the complete non-local contribution which takes into account the high correlation between the uncertainties of the local Voloshin and the non-local term of the previous analyses. The new calculation has a high impact on the range of the non-local contribution.

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

1 major / 1 minor

Summary. The manuscript updates the leading-order calculation of the non-local sub-leading O1-O7 contribution to the inclusive decay B̄ → Xsγ. Previous works subtracted the local Voloshin term from the non-local piece arising from O1c–O7γ interference; the present work instead retains the local term and recomputes the complete non-local contribution by explicitly incorporating the high correlation between the uncertainties of the local Voloshin term and the non-local term, yielding a revised numerical range for the full non-local piece.

Significance. If the revised range holds, the result tightens the theoretical uncertainty on a numerically relevant piece of the B̄ → Xsγ branching ratio. Because this contribution enters the ongoing O(αs) analysis, a more consistent treatment of the local–non-local correlation directly improves the precision of Standard-Model predictions used to constrain new-physics scenarios in rare B decays.

major comments (1)
  1. The central numerical claim rests on the statement that the correlation between the local Voloshin term and the non-local term is 'high' and is used to determine the revised range. The manuscript does not provide the explicit correlation coefficient, the covariance matrix, or the formula by which the combined uncertainty is obtained; without this information the quoted range cannot be reproduced or verified.
minor comments (1)
  1. The abstract and introduction should state the numerical value of the new range (central value and uncertainty) already in the opening paragraph so that the impact can be assessed without reading the full text.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the careful reading of our manuscript and for the constructive comment. We address the major point below and will incorporate the requested details in the revised version.

read point-by-point responses
  1. Referee: The central numerical claim rests on the statement that the correlation between the local Voloshin term and the non-local term is 'high' and is used to determine the revised range. The manuscript does not provide the explicit correlation coefficient, the covariance matrix, or the formula by which the combined uncertainty is obtained; without this information the quoted range cannot be reproduced or verified.

    Authors: We agree that the manuscript would be improved by providing the explicit correlation coefficient and the formula for the combined uncertainty. The correlation is high because the local Voloshin term and the non-local O1-O7 contribution share the dominant sources of theoretical uncertainty, namely the same non-perturbative matrix elements and the variation of the renormalization scale. In the revised manuscript we will add a short paragraph (or subsection) that states the correlation coefficient used, supplies the covariance matrix elements, and gives the explicit formula employed to obtain the revised numerical range for the complete non-local contribution. This addition will make the central result fully reproducible. revision: yes

Circularity Check

0 steps flagged

No significant circularity

full rationale

The paper updates the non-local O1-O7 contribution by retaining the local Voloshin term (instead of subtracting it) and explicitly incorporating the correlation between its uncertainty and that of the non-local piece. This is presented as a direct recalculation at leading order to address the prior subtraction procedure, with no equations or steps shown that reduce the claimed result to a fitted input, self-defined quantity, or load-bearing self-citation by construction. The derivation chain remains independent of the target numerical range.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Only the abstract is available; no specific free parameters, axioms, or invented entities can be identified from the provided information. The work relies on standard perturbative QCD and effective field theory techniques typical for this decay.

pith-pipeline@v0.9.0 · 5414 in / 997 out tokens · 105901 ms · 2026-05-16T23:58:43.206658+00:00 · methodology

discussion (0)

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

Reference graph

Works this paper leans on

24 extracted references · 24 canonical work pages · 14 internal anchors

  1. [1]

    Enhanced Non-local Power Corrections to the B->X_s+gamma Decay Rate

    S. J. Lee, M. Neubert and G. Paz, “Enhanced Non-local Power Corrections to the ¯B→X sγDecay Rate,” Phys. Rev. D75, 114005 (2007) [arXiv:hep-ph/0609224]

  2. [2]

    Factorization at Subleading Power and Irreducible Uncertainties in $\bar B\to X_s\gamma$ Decay

    M. Benzke, S. J. Lee, M. Neubert and G. Paz, “Factorization at Subleading Power and Irreducible Uncertainties in ¯B→X sγDecay,” JHEP1008(2010) 099 [arXiv:1003.5012 [hep-ph]]

  3. [3]

    Long-Distance Dominance of the CP Asymmetry in B->X_{s,d}+gamma Decays

    M. Benzke, S. J. Lee, M. Neubert and G. Paz, “Long-Distance Dominance of the CP Asymmetry in ¯B→X s,dγDecays,” Phys. Rev. Lett.106(2011) 141801 [arXiv:1012.3167 [hep-ph]]

  4. [4]

    Resolved Power Corrections to the Inclusive Decay $\bar B \to X_s \ell^+\ell^-$

    T. Hurth, M. Fickinger, S. Turczyk and M. Benzke, “Resolved Power Corrections to the Inclusive Decay ¯B→X sℓ+ℓ−,” Nucl. Part. Phys. Proc.285-286(2017) 57 [arXiv:1711.01162 [hep-ph]]

  5. [5]

    Subleading Power Factorization in $\bar B \to X_s \ell^+\ell^-$

    M. Benzke, T. Hurth and S. Turczyk, “Subleading power factorization in ¯B→ Xsℓ+ℓ−,” JHEP1710(2017) 031 [arXiv:1705.10366 [hep-ph]]

  6. [6]

    Updated NNLO QCD predictions for the weak radiative B-meson decays

    M. Misiaket al., “Updated NNLO QCD predictions for the weak radiativeB-meson decays,” Phys. Rev. Lett.114(2015) no.22, 221801 [arXiv:1503.01789 [hep-ph]]

  7. [7]

    Inclusive B -> X_s l^+ l^-: Complete angular analysis and a thorough study of collinear photons

    T. Huber, T. Hurth and E. Lunghi, “Inclusive ¯B→X sℓ+ℓ− : complete angu- lar analysis and a thorough study of collinear photons,” JHEP1506(2015) 176 [arXiv:1503.04849 [hep-ph]]

  8. [8]

    Long distance effects in inclusive rareBdecays and phenomenology of ¯B→X dℓ+ℓ−,

    T. Huber, T. Hurth, J. Jenkins, E. Lunghi, Q. Qin and K. K. Vos, “Long distance effects in inclusive rareBdecays and phenomenology of ¯B→X dℓ+ℓ−,” JHEP1910 (2019) 228 [arXiv:1908.07507 [hep-ph]]

  9. [9]

    Resolved 1/m b contributions to ¯B→X s,dℓ+ℓ− and ¯B→ Xsγ,

    M. Benzke and T. Hurth, “Resolved 1/m b contributions to ¯B→X s,dℓ+ℓ− and ¯B→ Xsγ,” Phys. Rev. D102, 114024 (2020) [arXiv:2006.00624 [hep-ph]]

  10. [10]

    Refactorisation in subleading ¯B→X sγ,

    T. Hurth and R. Szafron, “Refactorisation in subleading ¯B→X sγ,” [arXiv:2301.01739 [hep-ph]]

  11. [11]

    Factorization at subleading power and endpoint-divergent convolutions inh→γγdecay,

    Z. L. Liu and M. Neubert, “Factorization at subleading power and endpoint-divergent convolutions inh→γγdecay,” JHEP04, 033 (2020) [arXiv:1912.08818 [hep-ph]]

  12. [12]

    Factorization at subleading power and endpoint divergences inh→γγdecay. Part II. Renormalization and scale evo- lution,

    Z. L. Liu, B. Mecaj, M. Neubert and X. Wang, “Factorization at subleading power and endpoint divergences inh→γγdecay. Part II. Renormalization and scale evo- lution,” JHEP01, 077 (2021) [arXiv:2009.06779 [hep-ph]]

  13. [13]

    Next-to-leading power endpoint factorization and resummation for off- diagonal “gluon

    M. Beneke, M. Garny, S. Jaskiewicz, J. Strohm, R. Szafron, L. Vernazza and J. Wang, “Next-to-leading power endpoint factorization and resummation for off- diagonal “gluon” thrust,” JHEP07, 144 (2022) [arXiv:2205.04479 [hep-ph]]

  14. [14]

    Reevaluating uncertainties in B→X sγdecay,

    A. Gunawardana and G. Paz, “Reevaluating uncertainties in B→X sγdecay,” JHEP 11(2019), 141 [arXiv:1908.02812 [hep-ph]]

  15. [15]

    On HQET and NRQCD Operators of Dimension 8 and Above

    A. Gunawardana and G. Paz, “On HQET and NRQCD Operators of Dimension 8 and Above,” JHEP1707(2017) 137 [arXiv:1702.08904 [hep-ph]]. 8

  16. [16]

    Renormalisation group evolution of the shape function g17 in B→X sγand B→X sℓ+ℓ− at subleading power,

    R. Bartocci, P. B¨ oer and T. Hurth, “Renormalisation group evolution of the shape function g17 in B→X sγand B→X sℓ+ℓ− at subleading power,” JHEP04(2025), 066 [arXiv:2411.16634 [hep-ph]]

  17. [17]

    NLO analysis of the subleading-powerQc 1 −Q 7γ interference in ¯B→X sγat large photon energies,

    R. Bartocci, P. B¨ oer and T. Hurth, “NLO analysis of the subleading-powerQc 1 −Q 7γ interference in ¯B→X sγat large photon energies,” [arXiv:2510.18811 [hep-ph]]

  18. [18]

    Treating the b quark distribution function with reliable uncertainties

    Z. Ligeti, I. W. Stewart and F. J. Tackmann, “Treating the b quark distribution func- tion with reliable uncertainties,” Phys. Rev. D78(2008), 114014 [arXiv:0807.1926 [hep-ph]]

  19. [19]

    Nonperturbative m_X cut effects in B -> Xs l+ l- observables

    K. S. M. Lee and F. J. Tackmann, “Nonperturbativem X cut effects inB→X sl+l− observables,” Phys. Rev. D79(2009), 114021 [arXiv:0812.0001 [hep-ph]]

  20. [20]

    Precision Global Determination of theB→X sγ Decay Rate,

    F. U. Bernlochneret al.[SIMBA], “Precision Global Determination of theB→X sγ Decay Rate,” [arXiv:2007.04320 [hep-ph]]

  21. [21]

    $O(m_c^{-2})$ nonperturbative corrections to the inclusive rate of the decay $B \to X_s \gamma$

    M. B. Voloshin, “LargeO(m −2 c ) non-perturbative correction to the inclusive rate of the decayB→X sγ,” Phys. Lett. B397, 275 (1997) [arXiv:hep-ph/9612483]

  22. [22]

    Comment on nonperturbative effects in $B\to X_s\gamma$

    Z. Ligeti, L. Randall and M. B. Wise, “Comment on non-perturbative effects in ¯B→X sγ,” Phys. Lett. B402, 178 (1997) [arXiv:hep-ph/9702322]

  23. [23]

    Comment On Nonperturbative O(1/m_c^2) Corrections to B -> X_s gamma

    A. K. Grant, A. G. Morgan, S. Nussinov and R. D. Peccei, “Comment on non- perturbativeO(1/m 2 c) corrections to Γ( ¯B→X sγ),” Phys. Rev. D56, 3151 (1997) [arXiv:hep-ph/9702380]

  24. [24]

    Corrections of Order $\Lambda^2_{QCD}/m^2_c$ to Inclusive Rare B Decays

    G. Buchalla, G. Isidori and S. J. Rey, “Corrections of order Λ 2 QCD/m2 c to inclusive rareBdecays,” Nucl. Phys. B511, 594 (1998) [arXiv:hep-ph/9705253]. 9