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arxiv: 2604.05701 · v1 · submitted 2026-04-07 · ✦ hep-ex

Recognition: 2 theorem links

· Lean Theorem

Measurement of the CKM angle γ in B^{pm} rightarrow D(rightarrow K⁰_{rm S} h^{prime+}h^{prime-})h^{pm} decays with a novel approach

The BESIII , LHCb Collaborations: M. Ablikim , M. N. Achasov , P. Adlarson , X. C. Ai , C. S. Akondi , R. Aliberti , A. Amoroso
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Authors on Pith no claims yet

Pith reviewed 2026-05-10 18:23 UTC · model grok-4.3

classification ✦ hep-ex
keywords CKM angle gammaB to D h decaysCP violationmodel-independent analysisphase space weightingstrong phase parametersunitarity triangle
0
0 comments X

The pith

The CKM angle γ is measured to be 71.3 degrees with 5 degree uncertainty via a model-independent weighting method on combined collision data.

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

The paper establishes a new way to extract the CKM angle γ from B meson decays to a D meson that itself decays to three particles. Per-event weights are constructed from how the decay amplitude changes across the D decay phase space; these weights pull out the CP-violating observables while avoiding any assumption about the detailed strong-interaction phases inside the D decay. Data from electron-positron collisions totaling 8 inverse femtobarns and proton-proton collisions totaling 9 inverse femtobarns are analyzed together under this weighting scheme. A reader cares because γ is one of the three angles of the unitarity triangle, and its value directly tests whether the Standard Model accounts for all observed CP violation or whether new physics must be added.

Core claim

A joint fit to the weighted data yields the CKM angle γ = (71.3 ± 5.0)°, together with the associated strong-phase parameters. The fit is performed simultaneously on the two datasets and returns the most precise single determination of γ obtained so far.

What carries the argument

Per-event weights derived from the variation of the D-decay amplitude across phase space, which isolate the CP-violating observables in a model-independent manner.

If this is right

  • The result supplies the single most precise value of γ available from any one experiment or method.
  • Strong-phase parameters in the D decay are measured at the same time as γ.
  • The method can be applied directly to larger future data samples without new modeling assumptions.
  • The extracted γ can be inserted into global fits of the CKM matrix to test unitarity.

Where Pith is reading between the lines

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

  • The same weighting technique could be extended to other three-body D decays or to B decays with different final states to tighten the constraint on γ.
  • If future data reveal a persistent tension between this value and results from other methods, the discrepancy would point to either underestimated experimental effects or physics beyond the Standard Model.
  • The approach reduces the dominant systematic uncertainty that previously arose from modeling the D decay, thereby making the overall uncertainty budget more transparent for combination with other measurements.

Load-bearing premise

The per-event weights derived from the amplitude variation over the D-decay phase space correctly isolate CP-violating effects in a model-independent manner without introducing bias or residual model dependence.

What would settle it

An independent analysis of the identical decay modes that extracts a value of γ lying outside the quoted 5-degree uncertainty band when performed with an explicit amplitude model would show that the weighting procedure retains unaccounted model dependence.

Figures

Figures reproduced from arXiv: 2604.05701 by A. A. Adefisoye, A. Amoroso, A. Anelli, A. Artamonov, A. A. Zafar, A. Balboni, A. Bavarchee, A. Bay, A. Beck, A. Bellavista, A. Berezhnoy, A. Bertolin, A. Biolchini, A. Bitadze, A. Bizzeti, A.B. Morris, A. Bohare, A. Boldyrev, A. Bordelius, A. Bortone, A. Boyer, A. Brea Rodriguez, A. Brueggemann, A. Caillet, A. Calcaterra, A. Carbone, A. Cardini, A. Casais Vidal, A. C. Campos, A.C. dos Reis, A. Chen Hu, A. Chernov, A. Chubykin, A. Comerma-Montells, A. Contu, A. Correia, A. Davidson, A. Dbeyssi, A. D. Docheva, A. D. Dowling, A. Denig, A.D. Fernez, A. Doheny, A. Dziurda, A. Dzyuba, A. Egorychev, A. Ene, A.F. Campoverde Quezada, A. Fernandez Casani, A. Fomin, A. Gallas Torreira, A. Gavrikov, A. Gilman, A. Giovent\`u, A.G. Morris, A. Golutvin, A. Guskov, A. Hedes, A. Heyn, A. Hicheur, A. Iohner, A. Ishteev, A. Jawahery, A.J. Chadwick, A. Jelavic, A. John Rubesh Rajan, A. Kauniskangas, A.-K. Guseinov, A. Khoukaz, A. Kleimenova, A. 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Figure 1
Figure 1. Figure 1: Distributions of the strong-phase difference [PITH_FULL_IMAGE:figures/full_fig_p006_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: Distributions of the optimal weight w opt across the (left) D→ K0 S π +π − and (right) D→ K0 SK+K− Dalitz plots. They are obtained from amplitude models measured by the Belle and BaBar [30–32] experiments, and also take into account the effects of efficiency and background in the LHCb measurement [16]. The integrals of the weighting functions are normalized to unity. The weighted integrals of the B± decay … view at source ↗
Figure 3
Figure 3. Figure 3: Example fit results for the D→ K0 S/LK+K− channel at BESIII, where (top left) corresponds to the D→ K0 SKK vs. KK tag; (top right) the D→ K0 SKK vs. Ke[νe] tag; (bottom left) the D→ K0 S [K]K vs. D→ K0 S ππ tag; and (bottom right) the D→ [K0 L ]KK vs. KK tag. pions to be reconstructed in the vertex detector, and the second involves K0 S mesons that decay later such that track segments of the pions cannot b… view at source ↗
Figure 4
Figure 4. Figure 4: Mass distributions and fit results of the (left) [PITH_FULL_IMAGE:figures/full_fig_p014_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: Example efficiency distributions from BESIII simulation. For the Kπ tag mode, the plots correspond to the (top left) D→ K0 S π +π −, (top right) D→ K0 L π +π −, (bottom left) D→ K0 SK+K− and (bottom right) D→ K0 LK+K− signal modes. The average efficiencies over the Dalitz plot are scaled to unity [PITH_FULL_IMAGE:figures/full_fig_p015_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: Efficiency distributions of B±→ Dπ± decays with (top) D→ K0 S π +π − and (bottom) D→ K0 SK+K− decays for the (left) long and (right) downstream categories of the K0 S candidate. The average efficiencies over the Dalitz plot are scaled to unity. per-event weights from the phase space of both sides N s1s2 n1n2 = X i ({wn1,i1 ,wn1,i1 } /ϵi1 ) · ({wn2,i2 ,wn2,i2 } /ϵi2 ) , (17) where the first (second) set of … view at source ↗
Figure 7
Figure 7. Figure 7: Flavored parameters (left) P + n and (right) P − n of the D0→ K0 S π +π − decay from different tags. The total observables are obtained from combining those of all tags. The observables are normalized to P + 0 + P − 0 = 1. 0 1 2 3 4 n −0.2 0 0.2 0.4 0.6 0.8 + n P Total ± π ± K 0 π ± π ± K − π + π ± π ± K BESIII −1 8 fb 0 1 2 3 4 n 0 0.05 0.1 0.15 0.2 0.25 − n P Total ± π ± K 0 π ± π ± K − π + π ± π ± K BES… view at source ↗
Figure 8
Figure 8. Figure 8: Flavored parameters (left) P + n and (right) P − n of the D0→ K0 L π +π − decay from different tags. The total observables are obtained from combining those of all tags. The observables are normalized to P + 0 + P − 0 = 1. samples, covariances between CP-tag observables are computed by Eq. 18. Meanwhile, the correlations between self-conjugated tag observables are derived from pseudoexperiments with a much… view at source ↗
Figure 9
Figure 9. Figure 9: Observables from the (top) B±→ DK± and (bottom) B±→ Dπ± data sample with D→ K0 S π +π − decays in the downstream category. The CP-conjugated observable pairs, (left) N + n or N − n and (right) N − n or N + n , are plotted together to visualize CP asymmetries. where hDD = κNDD/(2NST f,1NST f,2 ) is the normalization factor. The factor κ ac￾counts for the different reconstruction methods between the two D me… view at source ↗
Figure 10
Figure 10. Figure 10: Results of CP observables from the joint fit. The contours correspond to 68% and 95% confidence levels of observable pairs, (left) (x DK + , yDK + ) in blue and (x DK − , yDK − ) in red, and (right) (x Dπ ξ , yDπ ξ ). from the joint fit, and those from systematic uncertainty studies as detailed in Sect. 7. The likelihood distributions are assumed to be Gaussian-like and were validated by the binned measur… view at source ↗
Figure 11
Figure 11. Figure 11: Strong-phase parameters of the (top) D→ K0 S/L π +π − and (bottom) D→ K0 S/LK+K− decays from BESIII data. measurements. The strong-phase parameters are obtained with the χ 2 test statistic as written in Eq. 25 and listed in [PITH_FULL_IMAGE:figures/full_fig_p022_11.png] view at source ↗
Figure 12
Figure 12. Figure 12: One-dimensional scan of the confidence level of the CKM angle [PITH_FULL_IMAGE:figures/full_fig_p029_12.png] view at source ↗
Figure 13
Figure 13. Figure 13: Two-dimensional confidence levels of the indicated parameter pairs from the [PITH_FULL_IMAGE:figures/full_fig_p030_13.png] view at source ↗
Figure 14
Figure 14. Figure 14: One-dimensional mass-fit results for the [PITH_FULL_IMAGE:figures/full_fig_p034_14.png] view at source ↗
Figure 15
Figure 15. Figure 15: One-dimensional mass-fit results for the [PITH_FULL_IMAGE:figures/full_fig_p035_15.png] view at source ↗
Figure 16
Figure 16. Figure 16: One-dimensional mass-fit results for the [PITH_FULL_IMAGE:figures/full_fig_p036_16.png] view at source ↗
read the original abstract

A measurement of the CKM angle $\gamma$ and related strong-phase parameters is performed using a novel, model-independent approach in ${B^{\pm}\rightarrow D(\rightarrow K^{0}_{\rm S} h^{\prime+}h^{\prime-}) h^{\pm}}$ decays, where $h^{(\prime)} \equiv \pi, K$. The analysis uses a joint data sample of electron-positron collisions collected by the BESIII experiment at the Beijing Electron-Positron Collider II during 2010--2011 and 2021--2022, corresponding to an integrated luminosity of 8 fb$^{-1}$, and proton-proton collisions collected by the LHCb experiment at the Large Hadron Collider during 2011--2018, corresponding to an integrated luminosity of 9 fb$^{-1}$. The two datasets are analyzed simultaneously by applying per-event weights based on the amplitude variation over the $D$-decay phase space to enhance the sensitivity to $C\!P$-violating observables. The CKM angle $\gamma$ is determined to be $\gamma = (71.3\pm 5.0)^{\circ}$, which constitutes the most precise single measurement to date.

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 / 2 minor

Summary. The manuscript presents a combined analysis of BESIII (8 fb^{-1}) and LHCb (9 fb^{-1}) data on B^{±} → D(→ K_S^0 h'^+ h'^- ) h^{±} decays (h,h' = π,K). A novel per-event weighting scheme based on the variation of the D-decay amplitude over phase space is applied to enhance sensitivity to CP-violating observables in a claimed model-independent manner. The CKM angle γ is extracted simultaneously with strong-phase parameters, yielding γ = (71.3 ± 5.0)° as the most precise single measurement to date.

Significance. If the weighting procedure is shown to be free of residual model dependence, the result would constitute a meaningful advance in precision for γ, tightening constraints on the CKM unitarity triangle and improving tests for physics beyond the Standard Model. The joint treatment of e^+e^- and pp datasets with this technique is innovative and could influence future multi-experiment analyses.

major comments (1)
  1. The central claim of model independence for the per-event weights (abstract and method description): the weights are constructed from the D → K_S^0 h^+ h^- amplitude variation and applied in the simultaneous fit. To support the absence of bias or correlation with the extracted γ, the paper must include explicit robustness tests using alternative D-decay amplitude parametrizations (e.g., different resonance content or isobar vs. dispersive models) and demonstrate that γ and the strong phases remain stable within the quoted uncertainties.
minor comments (2)
  1. The abstract states the result but does not separate statistical and systematic uncertainties on γ; this breakdown should be provided for clarity.
  2. Notation for the final-state particles (h and h') is compact but could be expanded on first use to aid readers outside the immediate B-physics community.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the careful reading of the manuscript and the constructive feedback. We appreciate the recognition of the innovative joint analysis and the potential of the per-event weighting technique. We address the major comment below.

read point-by-point responses
  1. Referee: The central claim of model independence for the per-event weights (abstract and method description): the weights are constructed from the D → K_S^0 h^+ h^- amplitude variation and applied in the simultaneous fit. To support the absence of bias or correlation with the extracted γ, the paper must include explicit robustness tests using alternative D-decay amplitude parametrizations (e.g., different resonance content or isobar vs. dispersive models) and demonstrate that γ and the strong phases remain stable within the quoted uncertainties.

    Authors: We agree that explicit robustness tests are required to substantiate the model-independence claim for the weighting procedure. Although the per-event weights are derived directly from the variation of the D-decay amplitude over phase space and the simultaneous fit extracts γ together with the strong-phase parameters without imposing a model on the B-decay amplitudes, additional validation against variations in the D-decay description is a valuable addition. In the revised manuscript we will include a new subsection that presents tests performed with alternative D-decay amplitude parametrizations, including changes to resonance content and comparisons between isobar and dispersive models. These tests show that the central value and uncertainty on γ, as well as the extracted strong phases, remain stable within the quoted uncertainties. We will also add a brief discussion of the implications for residual model dependence. revision: yes

Circularity Check

0 steps flagged

No circularity: direct experimental fit of γ from weighted data

full rationale

The analysis extracts γ via a simultaneous fit to the joint BESIII+LHCb dataset after applying per-event weights constructed from D-decay amplitude variation over phase space. No step reduces the extracted γ or strong-phase parameters to a quantity defined solely in terms of previously fitted inputs or self-citations by construction. The result is obtained from data likelihood maximization under the stated model-independent weighting; strong phases are free parameters in the same fit rather than inputs that force the γ value. This matches the default expectation for an experimental measurement paper whose central claim does not collapse to its own definitions or prior fitted quantities.

Axiom & Free-Parameter Ledger

2 free parameters · 1 axioms · 0 invented entities

The central claim rests on the validity of the model-independent weighting procedure and standard assumptions of particle physics data analysis; no new entities are postulated.

free parameters (2)
  • γ (CKM angle) = 71.3°
    Primary parameter extracted from the simultaneous fit to the weighted data.
  • strong-phase parameters
    Additional parameters determined together with γ in the same fit.
axioms (1)
  • domain assumption D-meson decay amplitudes vary over phase space in a manner that permits construction of per-event weights isolating CP-violating observables without model dependence.
    This assumption underpins the novel approach described in the abstract.

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Forward citations

Cited by 1 Pith paper

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

  1. Measurement of $\gamma$ using $B^{\pm}\rightarrow DK^{\pm}$ and $B^{\pm}\rightarrow D\pi^{\pm}$ decays with $D\rightarrow K_{\rm S}^{0}\pi^{+}\pi^{-}$ and $D\rightarrow K_{\rm S}^{0}K^{+}K^{-}$

    hep-ex 2026-05 unverdicted novelty 4.0

    The CKM angle γ is measured to be (68.1 ± 6.7)° from CP violation observed in the Dalitz plots of B± → DK± and B± → Dπ± decays with D → KS0π+π− and KS0K+K−.

Reference graph

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