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arxiv: 2604.08396 · v1 · submitted 2026-04-09 · ✦ hep-ex

Recognition: unknown

Search for the lepton-flavour violating decays B^+ to π^+ μ^pm e^mp

LHCb collaboration: R. Aaij , M. Abdelfatah , A.S.W. Abdelmotteleb , C. Abellan Beteta , F. Abudin\'en , T. Ackernley , A. A. Adefisoye , B. Adeva
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M. Adinolfi P. Adlarson C. Agapopoulou C.A. Aidala S. Akar K. Akiba P. Albicocco J. Albrecht R. Aleksiejunas F. Alessio P. Alvarez Cartelle 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 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 Z. B. Bai 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. Baron S. Barsuk W. Barter J. Bartz S. Bashir B. Batsukh P. B. Battista A. Bavarchee A. Bay A. Beck M. Becker F. Bedeschi I.B. Bediaga N. A. Behling S. Belin A. Bellavista I. Belov I. Belyaev G. Bencivenni E. Ben-Haim J.L.M. Berkey R. Bernet 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 J.A. Boelhauve O. Boente Garcia T. Boettcher A. Bohare C. Bolognani R. Bolzonella R. B. Bonacci 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 C. Breitfeld J. Brodzicka J. Brown D. Brundu E. Buchanan M. Burgos Marcos C. Burr C. Buti J.S. Butter J. Buytaert W. Byczynski S. Cadeddu H. Cai Y. Cai A. Caillet R. Calabrese L. Calefice M. Calvi M. Calvo Gomez P. Camargo Magalhaes J. I. Cambon Bouzas P. Campana A. C. Campos A.F. Campoverde Quezada Y. Cao 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 M. Charles Ph. Charpentier E. Chatzianagnostou R. Cheaib M. Chefdeville C. Chen J. Chen S. Chen Z. Chen A. Chen Hu M. Cherif S. Chernyshenko X. Chiotopoulos G. Chizhik V. Chobanova M. Chrzaszcz V. Chulikov P. Ciambrone X. Cid Vidal 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 G. C. Costantino J. Cottee Meldrum B. Couturier D.C. Craik N. Crepet M. Cruz Torres M. Cubero Campos E. Curras Rivera R. Currie C.L. Da Silva X. Dai J. Dalseno C. D'Ambrosio 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. Debernardis D. Decamp S. Dekkers L. Del Buono B. Delaney J. Deng V. Denysenko O. Deschamps F. Dettori B. Dey P. Di Nezza S. Ding Y. Ding L. Dittmann A. D. Docheva A. Doheny C. Dong F. Dordei A.C. dos Reis A. D. Dowling L. Dreyfus W. Duan P. Duda L. Dufour V. Duk P. Durante M. M. Duras J.M. Durham O. D. Durmus K. Duwe A. Dziurda S. Easo E. Eckstein U. Egede S. Eisenhardt E. Ejopu L. Eklund M. Elashri D. Elizondo Blanco J. Ellbracht S. Ely A. Ene J. Eschle T. Evans F. Fabiano S. Faghih L.N. Falcao B. Fang R. Fantechi L. Fantini M. Faria K. Farmer F. Fassin D. Fazzini L. Felkowski C. Feng M. Feng A. Fernandez Casani M. Fernandez Gomez A.D. Fernez F. Ferrari F. Ferreira Rodrigues M. Ferrillo M. Ferro-Luzzi R.A. Fini M. Fiorini M. Firlej K.L. Fischer D.S. Fitzgerald C. Fitzpatrick T. Fiutowski F. Fleuret A. Fomin M. Fontana L. A. Foreman R. Forty D. Foulds-Holt V. Franco Lima M. Franco Sevilla M. Frank E. Franzoso G. Frau C. Frei D.A. Friday J. Fu Q. F\"uhring T. Fulghesu G. Galati M.D. Galati A. Gallas Torreira D. Galli S. Gambetta M. Gandelman P. Gandini B. Ganie H. Gao R. Gao T.Q. Gao Y. Gao L.M. Garcia Martin P. Garcia Moreno J. Garc\'ia Pardi\~nas P. Gardner L. Garrido C. Gaspar A. Gavrikov E. Gersabeck M. Gersabeck T. Gershon S. Ghizzo Z. Ghorbanimoghaddam F. I. Giasemis V. Gibson H.K. Giemza A.L. Gilman M. Giovannetti A. Giovent\`u L. Girardey M.A. Giza F.C. Glaser V.V. Gligorov C. G\"obel L. Golinka-Bezshyyko E. Golobardes A. Golutvin S. Gomez Fernandez W. Gomulka F. Goncalves Abrantes I. Gon\c{c}ales Vaz M. Goncerz G. Gong J. A. Gooding C. Gotti E. Govorkova J.P. Grabowski L.A. Granado Cardoso E. Graug\'es E. Graverini L. Grazette G. Graziani A. T. Grecu N.A. Grieser L. Grillo C. Gu M. Guarise L. Guerry A.-K. Guseinov Y. Guz T. Gys K. Habermann T. Hadavizadeh C. Hadjivasiliou G. Haefeli C. Haen S. Haken G. Hallett P.M. Hamilton Q. Han X. Han S. Hansmann-Menzemer N. Harnew T. J. Harris M. Hartmann S. Hashmi J. He N. Heatley A. Hedes F. Hemmer C. Henderson R. Henderson R.D.L. Henderson A.M. Hennequin K. Hennessy J. Herd P. Herrero Gascon J. Heuel A. Heyn A. Hicheur G. Hijano Mendizabal J. 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Lai A. Lampis D. Lancierini C. Landesa Gomez J.J. Lane G. Lanfranchi C. Langenbruch T. Latham F. Lazzari C. Lazzeroni R. Le Gac H. Lee R. Lef\`evre M. Lehuraux E. Lemos Cid O. Leroy T. Lesiak E. D. Lesser B. Leverington A. Li C. Li H. Li J. Li K. Li L. Li P. Li P.-R. Li Q. Li T. Li W. Li Y. Li Z. Lian Q. Liang X. Liang Z. Liang S. Libralon A. Lightbody T. Lin R. Lindner H. Linton R. Litvinov D. Liu F. L. Liu G. Liu K. Liu S. Liu W. Liu Y. Liu Y. L. Liu G. Loachamin Ordonez I. Lobo A. Lobo Salvia A. Loi T. Long F. C. L. Lopes J.H. Lopes A. Lopez Huertas C. Lopez Iribarnegaray Q. Lu C. Lucarelli D. Lucchesi M. Lucio Martinez Y. Luo A. Lupato M. Lupberger E. Luppi K. Lynch S. Lyu X.-R. Lyu H. Ma S. Maccolini F. Machefert F. Maciuc B. Mack I. Mackay L. M. Mackey L.R. Madhan Mohan M. J. Madurai D. Magdalinski J.J. Malczewski S. Malde L. Malentacca G. Manca G. Mancinelli C. Mancuso R. Manera Escalero A. Mangalasseri F. M. Manganella D. Manuzzi S. Mao D. Marangotto J.F. Marchand R. 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Nandakumar G. Napoletano I. Nasteva M. Needham N. Neri S. Neubert N. Neufeld J. Nicolini D. Nicotra E.M. Niel L. Nisi Q. Niu B. K. Njoki P. Nogarolli P. Nogga C. Normand J. Novoa Fernandez G. Nowak H. N. Nur A. Oblakowska-Mucha T. Oeser O. Okhrimenko R. Oldeman F. Oliva E. Olivart Pino M. Olocco R.H. O'Neil J.S. Ordonez Soto D. Osthues J.M. Otalora Goicochea P. Owen A. Oyanguren O. Ozcelik F. Paciolla A. Padee K.O. Padeken B. Pagare T. Pajero A. Palano L. Palini M. Palutan C. Pan X. Pan S. Panebianco S. Paniskaki L. Paolucci A. Papanestis M. Pappagallo L.L. Pappalardo C. Pappenheimer C. Parkes D. Parmar G. Passaleva D. Passaro A. Pastore M. Patel J. Patoc C. Patrignani A. Paul C.J. Pawley A. Pellegrino J. Peng X. Peng M. Pepe Altarelli S. Perazzini H. Pereira Da Costa M. Pereira Martinez A. Pereiro Castro C. Perez P. Perret A. Perrevoort A. Perro M.J. Peters K. Petridis A. Petrolini S. Pezzulo J. P. Pfaller H. Pham L. Pica M. Piccini L. Piccolo B. Pietrzyk R. N. Pilato D. Pinci F. Pisani M. Pizzichemi V. M. Placinta M. Plo Casasus T. Poeschl F. Polci M. Poli Lener A. Poluektov I. Polyakov E. Polycarpo S. Ponce D. Popov K. Popp K. Prasanth C. Prouve D. Provenzano V. Pugatch A. Puicercus Gomez G. Punzi J.R. Pybus Q. Qian W. Qian N. Qin R. Quagliani R.I. Rabadan Trejo B. Rachwal R. Racz J.H. Rademacker M. Rama M. Ram\'irez Garc\'ia V. Ramos De Oliveira M. Ramos Pernas M.S. Rangel G. Raven M. Rebollo De Miguel F. Redi J. Reich F. Reiss Z. Ren P.K. Resmi M. Ribalda Galvez R. Ribatti G. Ricart D. Riccardi S. Ricciardi K. Richardson M. Richardson-Slipper F. Riehn K. Rinnert P. Robbe G. Robertson E. Rodrigues A. Rodriguez Alvarez E. Rodriguez Fernandez J.A. Rodriguez Lopez E. Rodriguez Rodriguez J. Roensch A. Rogovskiy D.L. Rolf P. Roloff V. Romanovskiy A. Romero Vidal G. Romolini F. Ronchetti T. Rong M. Rotondo M.S. Rudolph M. Ruiz Diaz J. Ruiz Vidal J. J. Saavedra-Arias J.J. Saborido Silva S. E. R. Sacha Emile R. D. Sahoo N. Sahoo B. Saitta M. Salomoni I. 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Steinkamp F. Suljik J. Sun L. Sun M. Sun D. Sundfeld W. Sutcliffe P. Svihra V. Svintozelskyi K. Swientek F. Swystun A. Szabelski T. Szumlak Y. Tan Y. Tang Y. T. Tang M.D. Tat J. A. Teijeiro Jimenez 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 A. Upadhyay B. Urbach A. Usachov 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 K. Vos C. Vrahas J. Wagner J. Walsh N. Walter 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 R. Xu Z. Xu S. Yadav K. Yang X. Yang Y. Yang Z. Yang 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 S.H Zeng C. Zhang D. Zhang J. Zhang L. Zhang R. Zhang S. Zhang S. L. Zhang Y. Zhang Z. Zhang J. Zhao Y. Zhao A. Zhelezov S. Z. Zheng X. Z. Zheng Y. Zheng T. Zhou X. 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 2026-05-10 17:08 UTC · model grok-4.3

classification ✦ hep-ex
keywords lepton flavour violationB meson decaysLHCbrare decaysbranching fraction limitsb to d transitionsmuon electron final states
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The pith

No significant signal is observed for the lepton-flavour violating decay B⁺ → π⁺ μ± e∓, setting an upper limit of 1.8 × 10^{-9} at 90% confidence level.

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

The paper reports the first dedicated search for B⁺ decays to a charged pion plus a muon and electron of opposite charge signs, performed with proton-proton collision data recorded by LHCb. No excess above background appears in the reconstructed invariant-mass distribution, so the branching fraction is bounded from above at 1.8 × 10^{-9}. A sympathetic reader cares because this process is strictly forbidden by the Standard Model yet could arise in models that explain neutrino masses or other flavour anomalies; the result also supplies the first LHC bound on any lepton-flavour violating b to d quark transition and the tightest existing limit on b to d muon-electron final states.

Core claim

Using 9 fb^{-1} of data collected between 2011 and 2018, B⁺ → π⁺ μ± e∓ candidates are reconstructed and an unbinned maximum-likelihood fit is performed on their invariant mass. With no significant signal observed, the branching fraction is limited to less than 1.8 × 10^{-9} at the 90% confidence level. This constitutes the first constraint on lepton-flavour violating b → d transitions at the LHC and the most stringent upper limits to date on b → d μ± e∓ processes. Limits are additionally derived for left-handed and scalar operators in beyond-Standard-Model scenarios.

What carries the argument

The central mechanism is the maximum-likelihood fit to the invariant-mass distribution of selected candidates, with signal efficiency determined from simulation and background shapes constrained by data control samples.

If this is right

  • This supplies the first LHC constraint on lepton-flavour violating b to d quark transitions.
  • It improves the previous world-average limit on the branching fraction by two orders of magnitude.
  • Limits are placed on left-handed and scalar operators in specific beyond-Standard-Model scenarios.
  • The result provides a reference point for future searches with larger data samples.

Where Pith is reading between the lines

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

  • Additional data from later LHC runs could tighten the limit by a factor of several.
  • Parallel searches in other B-meson decay modes could give complementary bounds on the same new-physics operators.
  • The null result is consistent with Standard-Model expectations but leaves room for small effects that might appear in other channels or with higher statistics.

Load-bearing premise

Background modelling, detection efficiencies, and systematic uncertainties are correctly estimated from simulation and control samples, so that any real signal would appear as a distinct peak above background.

What would settle it

Observation of a statistically significant peak at the known B⁺ mass in the invariant-mass spectrum of a future dataset would falsify the null result and indicate a non-zero branching fraction.

Figures

Figures reproduced from arXiv: 2604.08396 by A. A. Adefisoye, A. Anelli, A. Balboni, A. Bavarchee, A. Bay, A. Beck, A. Bellavista, A. Bertolin, A. Biolchini, A. Bitadze, A. Bizzeti, A.B. Morris, A. Bohare, A. Bordelius, A. Boyer, A. Brea Rodriguez, A. Caillet, A. Carbone, A. Cardini, A. Casais Vidal, A. C. Campos, A.C. dos Reis, A. Chen Hu, A. Comerma-Montells, A. Contu, A. Correia, A. Davidson, A. D. Docheva, A. D. Dowling, A.D. Fernez, A. Doheny, A. Dziurda, 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. Iohner, A. Jawahery, A.J. Chadwick, A. Jelavic, A. John Rubesh Rajan, A. Kauniskangas, A.-K. Guseinov, A. Kleimenova, A. Konoplyannikov, A. Korchin, A. Kupsc, A. Lai, A. Lampis, A.L. Gilman, A. Li, A. Lightbody, A. Lobo Salvia, A. Loi, A. Lopez Huertas, A. Lupato, A. Mangalasseri, A. Martorell i Granollers, A. Massafferri, A. Mathad, A. Mauri, A. McNab, A. Merli, A.M. Hennequin, A. Minotti, A.M. Marshall, A. Modak, A. Morcillo Gomez, A. Moro, A. Oblakowska-Mucha, 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. Rogovskiy, A. Romero Vidal, A. R. Thomson-Strong, A.R. Wiederhold, A. Saputi, A. Sarnatskiy, A. Satta, A. Scarabotto, A. Schopper, A. Sciuccati, A. Sergi, A. Solomin, A.S.W. Abdelmotteleb, A. Szabelski, A. T. Grecu, A. Ukleja, A. Upadhyay, A. Usachov, 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. Khanji, B. K. Njoki, B. Kutsenko, B. Leverington, B. Mack, B. Meadows, B. Mitreska, B. Pagare, B. Pietrzyk, B. Rachwal, B. Saitta, B. Schmidt, B. Sciascia, B. Sevilla Sanjuan, B. Shi, B. Souza De Paula, B. Urbach, B. Vivacqua, B. Wang, C.A. 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Figure 1
Figure 1. Figure 1: Selection efficiency of B+→ π +µ ±e ∓ decays as a function of the squared invariant masses, m2 π+µ± and m2 π+e∓ . The efficiency varies across the Dalitz plane due to the applied selection requirements. The signal branching fraction B(B+→ π +µ ±e ∓) is determined relative to the normali￾sation mode using B(B+→ π +µ ±e ∓) = N(B+→ π +µ ±e ∓) · α , α ≡ B(B+→ J/ψ(→ µ +µ −)K+) ε (B+→ π +µ ±e ∓) ε (B+→ J/ψ(→ µ +… view at source ↗
Figure 2
Figure 2. Figure 2: (Left) Invariant-mass distribution of B+→ π +µ ±e ∓ candidates with the signal-plus￾background fit function also shown. (Right) Profile likelihood-ratio scan for B+→ π +µ ±e ∓ branching fraction with all nuisance parameters profiled for the baseline signal model fit to data, available at Ref. [41]. decays, respectively, resulting in uncertainties of up to 2.0% depending on the analysis category. The finite… view at source ↗
Figure 3
Figure 3. Figure 3: Upper limit on the branching fraction of the [PITH_FULL_IMAGE:figures/full_fig_p008_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: Profile likelihood-ratio scan for B+→ π +µ ±e ∓ branching fraction with all nuisance parameters profiled for (left) left-handed and (right) scalar signal model fit to data, available at Ref. [41]. 8 [PITH_FULL_IMAGE:figures/full_fig_p010_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: Upper limits on the branching fraction of the [PITH_FULL_IMAGE:figures/full_fig_p011_5.png] view at source ↗
read the original abstract

The first search for the lepton-flavour violating decays $B^+ \to \pi^+ \mu^{\pm} e^{\mp}$ in proton-proton collisions is presented, using data collected by the LHCb experiment between 2011 and 2018, corresponding to an integrated luminosity of 9 fb$^{-1}$. No significant signal is observed and an upper limit on the branching fraction is set at $\mathcal{B}(B^+ \to \pi^+ \mu^{\pm} e^{\mp}) < 1.8 \times 10^{-9}$ at the $90\%$ confidence level, two orders of magnitude more restrictive than the current world average. This is the first constraint on lepton-flavour violating $b \to d$ quark transitions at the LHC and also sets the most stringent upper limits to date on $b \to d \mu^{\pm} e^{\mp}$ transitions. Limits on left-handed and scalar scenarios beyond the Standard Model are also reported.

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 / 1 minor

Summary. The manuscript reports the first search for the lepton-flavour violating decay B⁺ → π⁺ μ± e∓ using 9 fb⁻¹ of LHCb proton-proton collision data collected between 2011 and 2018. No significant signal is observed in the B⁺ candidate invariant-mass distribution. An upper limit is set on the branching fraction of ℬ(B⁺ → π⁺ μ± e∓) < 1.8 × 10^{-9} at 90% confidence level, representing a two-order-of-magnitude improvement over the previous world average. The result also provides the first LHC constraint on lepton-flavour violating b → d transitions and the most stringent limits to date on b → d μ± e∓ processes, together with derived limits on left-handed and scalar beyond-Standard-Model scenarios.

Significance. If the analysis is sound, the result is significant for rare-decay phenomenology. It delivers the first direct LHC bound on LFV b → d transitions and tightens constraints on new-physics models that generate such processes. The reported sensitivity gain is consistent with the increase in integrated luminosity and the performance of the LHCb detector for this final state; the use of a standard unbinned maximum-likelihood fit with simulation-validated efficiencies and background modeling supports the reliability of the quoted limit.

minor comments (1)
  1. The abstract states that limits on left-handed and scalar BSM scenarios are reported but does not indicate the specific effective operators or the procedure used to translate the branching-fraction limit into those constraints; a short clarifying sentence would improve readability.

Simulated Author's Rebuttal

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We thank the referee for their positive assessment of the manuscript, recognition of its significance as the first LHC search for lepton-flavour violating b → d transitions, and recommendation to accept. No major comments were raised.

Circularity Check

0 steps flagged

No significant circularity in experimental upper-limit result

full rationale

This is a standard LHCb experimental search paper reporting a null result for B+ → π+ μ± e∓. The central claim (upper limit < 1.8 × 10^{-9} at 90% CL) is obtained from an unbinned maximum-likelihood fit to the B candidate invariant-mass distribution in 9 fb^{-1} of data, with signal efficiency from Monte Carlo simulation and background shapes from simulation plus control samples. No theoretical derivation exists, no quantity is defined in terms of a fitted parameter that is then called a prediction, and no self-citation chain is load-bearing for the result. The analysis is self-contained against external benchmarks (prior world-average limits) and uses standard, externally falsifiable procedures.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

The result rests on standard assumptions of background estimation from sidebands and simulation, efficiency determination from data-driven methods, and conventional statistical limit setting; no new free parameters, axioms, or invented entities are introduced beyond those common to LHCb rare-decay analyses.

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    hep-ex 2026-04 unverdicted novelty 5.0

    LHCb reports first searches and the most stringent limits to date on rare decays such as b to s tau+ tau- and tau to three muons.

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