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arxiv: 2512.09288 · v2 · submitted 2025-12-10 · ✦ hep-ex

Recognition: no theorem link

Precision measurement of CP violation and branching fractions in B^{pm} to K⁰_{S} h^{pm} (h = π, K) decays and search for the rare decay B_c^{pm} to K⁰_{S} K^{pm}

R. Aaij , A.S.W. Abdelmotteleb , C. Abellan Beteta , F. Abudin\'en , T. Ackernley , A. A. Adefisoye , B. Adeva , M. Adinolfi
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P. Adlarson C. Agapopoulou C.A. Aidala Z. Ajaltouni S. Akar K. Akiba M. Akthar P. Albicocco J. Albrecht R. Aleksiejunas F. Alessio P. Alvarez Cartelle R. Amalric S. Amato J.L. Amey Y. Amhis L. An L. Anderlini M. Andersson P. Andreola M. Andreotti S. Andres Estrada A. Anelli D. Ao C. Arata F. Archilli Z. Areg M. Argenton S. Arguedas Cuendis L. Arnone A. Artamonov M. Artuso E. Aslanides R. Ata\'ide Da Silva M. Atzeni B. Audurier J. A. Authier D. Bacher I. Bachiller Perea S. Bachmann M. Bachmayer J.J. Back P. Baladron Rodriguez V. Balagura A. Balboni W. Baldini Z. Baldwin L. Balzani H. Bao J. Baptista de Souza Leite C. Barbero Pretel M. Barbetti I. R. Barbosa R.J. Barlow M. Barnyakov S. Barsuk W. Barter J. Bartz S. Bashir B. Batsukh P. B. Battista A. Bay A. Beck M. Becker F. Bedeschi I.B. Bediaga N. A. Behling S. Belin A. Bellavista K. Belous I. Belov I. Belyaev G. Benane G. Bencivenni E. Ben-Haim A. Berezhnoy R. Bernet S. Bernet Andres A. Bertolin F. Betti J. Bex O. Bezshyyko S. Bhattacharya M.S. Bieker N.V. Biesuz A. Biolchini M. Birch F.C.R. Bishop A. Bitadze A. Bizzeti T. Blake F. Blanc J.E. Blank S. Blusk V. Bocharnikov J.A. Boelhauve O. Boente Garcia T. Boettcher A. Bohare A. Boldyrev C. Bolognani R. Bolzonella R. B. Bonacci N. Bondar A. Bordelius F. Borgato S. Borghi M. Borsato J.T. Borsuk E. Bottalico S.A. Bouchiba M. Bovill T.J.V. Bowcock A. Boyer C. Bozzi J. D. Brandenburg A. Brea Rodriguez N. Breer J. Brodzicka J. Brown D. Brundu E. Buchanan M. Burgos Marcos A.T. Burke C. Burr C. Buti J.S. Butter J. Buytaert W. Byczynski S. Cadeddu H. Cai Y. Cai A. Caillet R. Calabrese S. Calderon Ramirez L. Calefice M. Calvi M. Calvo Gomez P. Camargo Magalhaes J. I. Cambon Bouzas P. Campana A.F. Campoverde Quezada S. Capelli M. Caporale L. Capriotti R. Caravaca-Mora A. Carbone L. Carcedo Salgado R. Cardinale A. Cardini P. Carniti L. Carus A. Casais Vidal R. Caspary G. Casse M. Cattaneo G. Cavallero V. Cavallini S. Celani I. Celestino S. Cesare A.J. Chadwick I. Chahrour H. Chang M. Charles Ph. Charpentier E. Chatzianagnostou R. Cheaib M. Chefdeville C. Chen J. Chen S. Chen Z. Chen A. Chen Hu M. Cherif A. Chernov S. Chernyshenko X. Chiotopoulos V. Chobanova M. Chrzaszcz A. Chubykin V. Chulikov P. Ciambrone X. Cid Vidal G. Ciezarek P. Cifra P.E.L. Clarke M. Clemencic H.V. Cliff J. Closier C. Cocha Toapaxi V. Coco J. Cogan E. Cogneras L. Cojocariu S. Collaviti P. Collins T. Colombo M. Colonna A. Comerma-Montells L. Congedo J. Connaughton A. Contu N. Cooke G. Cordova C. Coronel I. Corredoira A. Correia G. Corti J. Cottee Meldrum B. Couturier D.C. Craik M. Cruz Torres M. Cubero Campos E. Curras Rivera R. Currie C.L. Da Silva S. Dadabaev X. Dai E. Dall'Occo J. Dalseno C. D'Ambrosio J. Daniel G. Darze A. Davidson J.E. Davies O. De Aguiar Francisco C. De Angelis F. De Benedetti J. de Boer K. De Bruyn S. De Capua M. De Cian U. De Freitas Carneiro Da Graca E. De Lucia J.M. De Miranda L. De Paula M. De Serio P. De Simone F. De Vellis J.A. de Vries F. 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Tan Y. Tang Y. T. Tang M.D. Tat J. A. Teijeiro Jimenez A. Terentev F. Terzuoli F. Teubert E. Thomas D.J.D. Thompson A. R. Thomson-Strong H. Tilquin V. Tisserand S. T'Jampens M. Tobin T. T. Todorov L. Tomassetti G. Tonani X. Tong T. Tork L. Toscano D.Y. Tou C. Trippl G. Tuci N. Tuning L.H. Uecker A. Ukleja D.J. Unverzagt A. Upadhyay B. Urbach A. Usachov A. Ustyuzhanin U. Uwer V. Vagnoni A. Vaitkevicius V. Valcarce Cadenas G. Valenti N. Valls Canudas J. van Eldik H. Van Hecke E. van Herwijnen C.B. Van Hulse R. Van Laak M. van Veghel G. Vasquez R. Vazquez Gomez P. Vazquez Regueiro C. V\'azquez Sierra S. Vecchi J. Velilla Serna J.J. Velthuis M. Veltri A. Venkateswaran M. Verdoglia M. Vesterinen W. Vetens D. Vico Benet P. Vidrier Villalba M. Vieites Diaz X. Vilasis-Cardona E. Vilella Figueras A. Villa P. Vincent B. Vivacqua F.C. Volle D. vom Bruch N. Voropaev K. Vos C. Vrahas J. Wagner J. Walsh E.J. Walton G. Wan A. Wang B. Wang C. Wang G. Wang H. Wang J. Wang M. Wang N. W. Wang R. Wang X. Wang X. W. Wang Y. Wang Y. H. Wang Z. Wang J.A. Ward M. Waterlaat N.K. Watson D. Websdale Y. Wei Z. Weida J. Wendel B.D.C. Westhenry C. White M. Whitehead E. Whiter A.R. Wiederhold D. Wiedner M. A. Wiegertjes C. Wild G. Wilkinson M.K. Wilkinson M. Williams M. J. Williams M.R.J. Williams R. Williams S. Williams Z. Williams F.F. Wilson M. Winn W. Wislicki M. Witek L. Witola T. Wolf E. Wood G. Wormser S.A. Wotton H. Wu J. Wu X. Wu Y. Wu Z. Wu K. Wyllie S. Xian Z. Xiang Y. Xie T. X. Xing A. Xu L. Xu M. Xu Z. Xu S. Yadav K. Yang X. Yang Y. Yang Z. Yang V. Yeroshenko H. Yeung H. Yin X. Yin C. Y. Yu J. Yu X. Yuan Y Yuan J. A. Zamora Saa M. Zavertyaev M. Zdybal F. Zenesini C. Zeng M. Zeng C. Zhang D. Zhang J. Zhang L. Zhang R. Zhang S. Zhang S. L. Zhang Y. Zhang Y. Z. Zhang Z. Zhang Y. Zhao A. Zhelezov S. Z. Zheng X. Z. Zheng Y. Zheng T. Zhou X. Zhou Y. Zhou V. Zhovkovska L. Z. Zhu X. Zhu Y. Zhu V. Zhukov J. Zhuo D. Zuliani G. Zunica
Authors on Pith no claims yet

Pith reviewed 2026-05-17 00:00 UTC · model grok-4.3

classification ✦ hep-ex
keywords CP violationB meson decaysbranching fractionsLHCbrare decaysasymmetriesB_c mesonflavor physics
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The pith

LHCb reports the most precise CP asymmetry measurements for B± to K0S π± and B± to K0S K± decays plus a branching ratio of 0.055 and an upper limit on the rare Bc decay.

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

The paper extracts CP asymmetries and a branching fraction ratio from 5.4 fb^{-1} of proton-proton collisions at 13 TeV. It finds the pion-mode asymmetry close to zero at -0.028 and the kaon-mode asymmetry at 0.118, with the ratio of the two modes measured to 0.055. These quantities test Standard Model predictions for b to s transitions in a channel expected to be theoretically clean. No evidence appears for the Bc to K0S K decay, yielding a tight upper limit on the product of its branching fraction and the fragmentation ratio fc/fu. The results tighten constraints on possible new physics contributions beyond the Standard Model.

Core claim

Using LHCb data corresponding to 5.4 fb^{-1} at 13 TeV, the CP asymmetries are determined to be A^CP(B± → K0S π±) = -0.028 ± 0.009 ± 0.009 and A^CP(B± → K0S K±) = 0.118 ± 0.062 ± 0.031, while the branching fraction ratio B(B± → K0S K±)/B(B± → K0S π±) = 0.055 ± 0.004 ± 0.002. No significant signal is observed for Bc± → K0S K±, and the upper limit on the product of the branching fraction ratio B(Bc± → K0S K±)/B(B± → K0S π±) and the fragmentation fraction ratio fc/fu is set to 0.015 (0.016) at 90% (95%) confidence level.

What carries the argument

Yield extraction from invariant-mass fits to reconstructed B± → K0S h± candidates, with efficiencies and backgrounds modeled from simulation and control samples to determine asymmetries and ratios.

If this is right

  • The near-zero asymmetry in the pion mode can be combined with other measurements to bound penguin contributions or new physics phases in b to s transitions.
  • The branching ratio of 0.055 quantifies the relative suppression of the strangeness-changing mode and can be compared directly to theoretical predictions.
  • The upper limit on the Bc decay constrains models of Bc production and decay and serves as a reference for searches in future LHC runs.
  • These values update the world averages and improve the precision of global fits to CKM parameters and flavor observables.

Where Pith is reading between the lines

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

  • The positive kaon-mode asymmetry suggests a measurable contribution from penguin amplitudes that could be further tested with larger samples.
  • Independent determinations of the fragmentation fraction fc/fu would allow conversion of the reported product limit into a pure branching-fraction bound.
  • The results demonstrate that current LHCb data already reach the precision where small Standard Model deviations or new physics effects could become visible in these channels.
  • Similar analysis techniques could be applied to other rare Bc decays to map out the landscape of heavy-flavor transitions.

Load-bearing premise

The analysis assumes that detector efficiencies, acceptances, and background shapes are accurately modeled by simulation and control samples.

What would settle it

A future analysis with substantially larger data that extracts a pion-mode CP asymmetry differing from -0.028 by more than 3 standard deviations combined would falsify the current central value.

Figures

Figures reproduced from arXiv: 2512.09288 by A. A. Adefisoye, A. Anelli, A. Artamonov, A. Balboni, 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. Boyer, A. Brea Rodriguez, A. Caillet, A. Carbone, A. Cardini, A. Casais Vidal, A.C. dos Reis, A. Chen Hu, A. Chernov, A. Chubykin, A. Comerma-Montells, A. Contu, A. Correia, A. Davidson, A. D. Docheva, A. D. Dowling, 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. Giovent\`u, A.G. Morris, A. Golutvin, A. Hedes, A. Heyn, A. Hicheur, A. Iniukhin, A. Iohner, A. Ishteev, A. Jawahery, A.J. Chadwick, A. John Rubesh Rajan, A. Kauniskangas, A.-K. Guseinov, A. Kharisova, A. Kleimenova, A. Konoplyannikov, A. Korchin, A. Kozachuk, A. Kupsc, A. Lai, A. Lampis, A. Leflat, A.L. Gilman, A. Li, A. Lightbody, A. Lobo Salvia, A. Loi, A. Lopez Huertas, A. Lupato, A. Malinin, A. Martorell i Granollers, A. Massafferri, A. Mathad, A. Mauri, A. McNab, A.M. Donohoe, A. Merli, A.M. Hennequin, A. Minotti, A.M. Marshall, A. Modak, A. Morcillo Gomez, A. Moro, A. Oblakowska-Mucha, A. Okhotnikov, A. Oyanguren, A. Padee, A. Palano, A. Papanestis, A. Pastore, A. Paul, A. Pellegrino, A. Pereiro Castro, A. Perrevoort, A. Perro, A. Petrolini, A. Poluektov, A. Puicercus Gomez, A. Rodriguez Alvarez, A. Rogachev, A. Rogovskiy, A. Romero Vidal, A. R. Thomson-Strong, A.R. Wiederhold, A. Saputi, A. Sarnatskiy, A. Satta, A. Scarabotto, A. Schopper, A. Sciuccati, A. Semennikov, A. Sergi, A. Seuthe, A. Solomin, A. Solovev, A.S.W. Abdelmotteleb, A. Szabelski, A.T. Burke, A. Terentev, A. T. Grecu, A. Ukleja, A. Upadhyay, A. Usachov, A. Ustyuzhanin, A. Vaitkevicius, A. Venkateswaran, A. Villa, A. Wang, A. Xu, A. Zhelezov, B. Adeva, B. Audurier, B. Batsukh, B. Couturier, B.D.C. Westhenry, B. Delaney, B. Dey, B. Fang, B. Ganie, B. Jost, B. 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Figure 1
Figure 1. Figure 1: Mass distributions of (top left) K0 S π +, (top right) K0 S π −, (bottom left) K0 SK+, and (bottom right) K0 SK− pairs. The results of the simultaneous fit are also shown. background is parameterized with a first-order polynomial function. In the fit to data, the signal peak positions and widths are treated as free parameters, shared between B+ and B−. The width of the B+ → K0 SK+ signal is scaled relative… view at source ↗
Figure 2
Figure 2. Figure 2: Mass distribution of selected B+ c → K0 SK+ candidates. The data points with error bars are shown together with the result of the fit (solid curve). 9 [PITH_FULL_IMAGE:figures/full_fig_p011_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Comparison of branching fraction ratios measured in this paper with results from [PITH_FULL_IMAGE:figures/full_fig_p012_3.png] view at source ↗
read the original abstract

The decay $B^{\pm} \to K^0_{\mathrm{S}} \pi^{\pm}$, with a $CP$ asymmetry expected to be close to zero in the Standard Model, is theoretically clean and sensitive to potential new physics. An analysis of the decays $B^{\pm} \to K^0_{\mathrm{S}} \pi^{\pm}$ and $B^{\pm} \to K^0_{\mathrm{S}} K^{\pm}$ is performed using proton-proton collision data collected by the LHCb experiment at a center-of-mass energy of $13\,\mathrm{TeV}$, corresponding to an integrated luminosity of $5.4\,\mathrm{fb}^{-1}$. The \CP asymmetries are determined to be ${\cal A}^{CP}(B^{\pm} \to K^0_{\mathrm{S}} \pi^{\pm})=-0.028\pm 0.009\pm 0.009$ and ${\cal A}^{CP}(B^{\pm} \to K^0_{\mathrm{S}} K^{\pm})=0.118\pm 0.062 \pm 0.031$, and the branching fraction ratio is measured to be ${\cal B}(B^{\pm} \to K^0_{\mathrm{S}} K^{\pm})/{\cal B}(B^{\pm} \to K^0_{\mathrm{S}} \pi^{\pm})=0.055\pm 0.004 \pm 0.002$, where the first uncertainties are statistical and the second are systematic. These results are the most precise measurements of these quantities to date. A search for the rare decay $B_c^{\pm} \to K^0_{\mathrm{S}} K^{\pm}$ is also performed. No significant signal is observed, and the upper limit on the product of the branching fraction ratio ${\cal B}(B_c^{\pm} \to K^0_{\mathrm{S}} K^{\pm})/{\cal B}(B^{\pm} \to K^0_{\mathrm{S}} \pi^{\pm})$ and the fragmentation-fraction ratio $f_c/f_u$ is set to be 0.015 (0.016) at the 90\% (95\%) confidence level.

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. The manuscript reports precision measurements of CP asymmetries in B± → K0S π± and B± → K0S K± decays, the branching-fraction ratio between these modes, and an upper limit on the rare Bc± → K0S K± decay, using 5.4 fb^{-1} of LHCb pp collision data at √s = 13 TeV. The central results are A^CP(B± → K0S π±) = −0.028 ± 0.009 ± 0.009, A^CP(B± → K0S K±) = 0.118 ± 0.062 ± 0.031, B(B± → K0S K±)/B(B± → K0S π±) = 0.055 ± 0.004 ± 0.002, and an upper limit of 0.015 (0.016) at 90 % (95 %) CL on the product of the Bc branching-fraction ratio and fc/fu.

Significance. If the results hold, they constitute the most precise determinations of these CP asymmetries and the branching-fraction ratio to date, providing a clean test of the Standard Model expectation that A^CP(B± → K0S π±) is near zero and supplying improved input for fragmentation-fraction studies. The upper limit on the rare Bc decay adds a useful constraint on Bc production and decay rates.

minor comments (2)
  1. [Abstract] Abstract: the statement that the results are 'the most precise measurements to date' would be strengthened by a brief quantitative comparison with the previous world averages or LHCb results in the text or a dedicated table.
  2. [Results] The treatment of the fragmentation fraction fc/fu in the Bc upper-limit calculation is only summarized; a short dedicated paragraph or appendix detailing the adopted value and its uncertainty would improve clarity.

Simulated Author's Rebuttal

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We thank the referee for the positive review and the recommendation to accept the manuscript. The referee's summary accurately captures the main results and their significance for Standard Model tests and fragmentation studies.

Circularity Check

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No significant circularity; results extracted from data fits with standard efficiency corrections

full rationale

The paper reports direct measurements of CP asymmetries and branching-fraction ratios extracted from fits to invariant-mass distributions in 5.4 fb^{-1} of LHCb data. No derivation reduces by construction to previously fitted parameters, self-defined quantities, or load-bearing self-citations whose validity depends on the present result. Efficiency modeling, background shapes, and the fc/fu fragmentation factor are taken from simulation and control samples whose assumptions are independent of the target observables; the quoted uncertainties already fold in the dominant systematics. This is a standard experimental extraction with no self-definitional, fitted-input-renamed-as-prediction, or uniqueness-theorem circularity. Minor self-citations to prior LHCb methodology papers exist but are not load-bearing for the central claims.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The central claims rest on standard experimental assumptions about detector response, background modeling, and simulation accuracy rather than new theoretical postulates.

axioms (2)
  • domain assumption Standard Model predicts CP asymmetry close to zero in B± → K0S π±
    Benchmark for interpreting the measured asymmetry as a test of the SM.
  • domain assumption LHCb detector efficiencies and background shapes are correctly modeled
    Required for extracting branching fractions and asymmetries from observed yields.

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