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arxiv: 2604.21987 · v1 · submitted 2026-04-23 · ✦ hep-ex

Recognition: unknown

Angular analysis of the B^+toπ^+μ^+μ^- decay

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 M.F. Cicala 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 Y. 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 R. Grande Quartieri 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 L. Hartman 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. Horswill R. Hou Y. Hou D.C. Houston N. Howarth W. Hu X. Hu W. Hulsbergen R.J. Hunter D. Hurley D. Hutchcroft M. Idzik P. Ilten A. Iohner H. Jage S.J. Jaimes Elles S. Jakobsen T. Jakoubek E. Jans A. Jawahery C. Jayaweera A. Jelavic V. Jevtic Z. Jia E. Jiang X. Jiang Y. Jiang Y. J. Jiang E. Jimenez Moya N. Jindal M. John A. John Rubesh Rajan D. Johnson C.R. Jones S. Joshi B. Jost J. Juan Castella N. Jurik I. Juszczak K. Kalecinska D. Kaminaris S. Kandybei M. Kane Y. Kang C. Kar M. Karacson A. Kauniskangas J.W. Kautz M.K. Kazanecki F. Keizer M. Kenzie T. Ketel B. Khanji S. Kholodenko G. Khreich F. Kiraz T. Kirn V.S. Kirsebom N. Kleijne A. Kleimenova D. K. Klekots K. Klimaszewski M.R. Kmiec T. Knospe R. Kolb S. Koliiev L. Kolk A. Konoplyannikov P. Kopciewicz P. Koppenburg A. Korchin I. Kostiuk O. Kot S. Kotriakhova E. Kowalczyk O. Kravcov M. Kreps W. Krupa W. Krzemien O. Kshyvanskyi S. Kubis M. Kucharczyk A. Kupsc V. Kushnir B. Kutsenko J. Kvapil I. Kyryllin D. Lacarrere P. Laguarta Gonzalez A. 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. Marchevski U. Marconi E. Mariani S. Mariani C. Marin Benito J. Marks A.M. Marshall L. Martel G. Martelli G. Martellotti L. Martinazzoli M. Martinelli C. Martinez D. Martinez Gomez D. Martinez Santos F. Martinez Vidal A. Martorell i Granollers A. Massafferri R. Matev A. Mathad C. Matteuzzi K.R. Mattioli A. Mauri E. Maurice J. Mauricio P. Mayencourt J. Mazorra de Cos M. Mazurek D. Mazzanti Tarancon M. McCann N.T. McHugh A. McNab R. McNulty B. Meadows D. Melnychuk D. Mendoza Granada P. Menendez Valdes Perez F. M. Meng M. Merk A. Merli L. Meyer Garcia D. Miao H. Miao M. Mikhasenko D.A. Milanes A. Minotti E. Minucci B. Mitreska D.S. Mitzel R. Mocanu A. Modak L. Moeser R.D. Moise E. F. Molina Cardenas T. Momb\"acher M. Monk T. Monnard S. Monteil A. Morcillo Gomez G. Morello M.J. Morello M.P. Morgenthaler A. Moro J. Moron W. Morren A.B. Morris A.G. Morris R. Mountain Z. Mu N. Muangkod E. Muhammad F. Muheim M. Mulder K. M\"uller F. Mu\~noz-Rojas R. Murta V. Mytrochenko P. Naik T. Nakada R. 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. Sanderswood R. Santacesaria C. Santamarina Rios M. Santimaria L. Santoro E. Santovetti A. Saputi A. Sarnatskiy G. Sarpis M. Sarpis C. Satriano A. Satta M. Saur H. Sazak F. Sborzacchi A. Scarabotto S. Schael S. Scherl M. Schiller H. Schindler M. Schmelling B. Schmidt N. Schmidt S. Schmitt H. Schmitz O. Schneider A. Schopper N. Schulte M.H. Schune G. Schwering B. Sciascia A. Sciuccati G. Scriven I. Segal S. Sellam M. Senghi Soares A. Sergi N. Serra L. Sestini B. Sevilla Sanjuan Y. Shang D.M. Shangase R. S. Sharma L. Shchutska T. Shears J. Shen Z. Shen S. Sheng B. Shi J. Shi Q. Shi W. S. Shi E. Shmanin R. Silva Coutinho G. Simi S. Simone M. Singha I. Siral N. Skidmore T. Skwarnicki M.W. Slater E. Smith M. Smith L. Soares Lavra M.D. Sokoloff F.J.P. Soler A. Solomin K. Solovieva N. S. Sommerfeld R. Song Y. Song Y. S. Song F.L. Souza De Almeida B. Souza De Paula K.M. Sowa E. Spadaro Norella E. Spedicato J.G. Speer P. Spradlin F. Stagni M. Stahl S. Stahl S. Stanislaus M. Stefaniak O. 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 2026-05-08 13:11 UTC · model grok-4.3

classification ✦ hep-ex
keywords B meson decayrare decayangular distributionforward-backward asymmetryflat termdimuon massStandard Model testflavor changing neutral current
0
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The pith

The first measurement of forward-backward asymmetry and flat term in the B+ to pi+ mu+ mu- decay finds Standard Model predictions inside the reported confidence intervals.

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

The paper reports the initial extraction of two angular observables that describe how the muons are distributed in the decay of a charged B meson to a pion and a muon pair. These observables are measured separately in a low-mass region and a high-mass region of the muon pair, each chosen to avoid the narrow resonances from charmonium states. The extracted values place the Standard Model expectations inside the 68 percent interval for the higher-mass data and inside the 99 percent interval for the lower-mass data. A sympathetic reader would see this as a direct test of whether the rare flavor-changing transition proceeds exactly as the Standard Model predicts, with any future deviation potentially pointing to additional particles or interactions.

Core claim

The angular distribution of the B+ to pi+ mu+ mu- decay is described by the forward-backward asymmetry AFB and the flat term FH. Using proton-proton collision data corresponding to 9 inverse femtobarns, the first determination of these parameters in two dimuon-mass intervals yields results consistent with Standard Model calculations, lying within the 68 percent confidence level interval in the high-mass region and within the 99 percent interval in the low-mass region.

What carries the argument

The forward-backward asymmetry AFB and flat term FH, which together parameterize the angular distribution of the two muons in the dimuon rest frame.

Load-bearing premise

The analysis assumes that background contributions, detector efficiencies, and acceptance corrections are accurately modeled and do not introduce significant biases in the extracted angular parameters.

What would settle it

A statistically significant measurement of either AFB or FH lying outside the quoted confidence intervals in the high-mass or low-mass region would show a discrepancy with the Standard Model.

Figures

Figures reproduced from arXiv: 2604.21987 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. Aidala, C. Abellan Beteta, C. Agapopoulou, C. Arata, C. Barbero Pretel, C. Bolognani, C. Bozzi, C. Breitfeld, C. Burr, C. Buti, C.B. Van Hulse, C. Chen, C. Cocha Toapaxi, C. Coronel, C. D'Ambrosio, C. De Angelis, C. Dong, C. Feng, C. Fitzpatrick, C. Frei, C. Gaspar, C. G\"obel, C. Gotti, C. Gu, C. Hadjivasiliou, C. Haen, C. Henderson, C. Jayaweera, C.J. Pawley, C. Kar, C. Landesa Gomez, C. Langenbruch, C. Lazzeroni, C.L. Da Silva, C. Li, C. Lopez Iribarnegaray, C. Lucarelli, C. Mancuso, C. Marin Benito, C. Martinez, C. Matteuzzi, C. Normand, C. Pan, C. Pappenheimer, C. Parkes, C. Patrignani, C. Perez, C. Prouve, C.R. Jones, C. Santamarina Rios, C. Satriano, C. Trippl, C. V\'azquez Sierra, C. Vrahas, C. Wang, C. White, C. Wild, C. Y. Yu, C. Zeng, C. Zhang, D.A. Friday, D.A. Milanes, D. Ao, D. Bacher, D. Brundu, D.C. Craik, D.C. Houston, D. Decamp, D. Elizondo Blanco, D. Fazzini, D. Foulds-Holt, D. Galli, D. Hurley, D. Hutchcroft, D.J.D. Thompson, D. Johnson, D. Kaminaris, D. K. Klekots, D. Lacarrere, D. Lancierini, D. Liu, D.L. Rolf, D. Lucchesi, D. Magdalinski, D. Manuzzi, D. Marangotto, D. Martinez Gomez, D. Martinez Santos, D. Mazzanti Tarancon, D. Melnychuk, D. Mendoza Granada, D. Miao, D.M. Shangase, D. Nicotra, D. Osthues, D. Parmar, D. Passaro, D. Pinci, D. Popov, D. Provenzano, D. Riccardi, D. Sahoo, D.S. Fitzgerald, D.S. Mitzel, D. Sundfeld, D. Vico Benet, D. vom Bruch, D. Websdale, D. Wiedner, D.Y. Tou, D. Zhang, D. Zuliani, E. Aslanides, E. Ben-Haim, E. Bottalico, E. Buchanan, E. Chatzianagnostou, E. Cogneras, E. Curras Rivera, E. De Lucia, E. D. Lesser, E. Eckstein, E. Ejopu, E. F. Molina Cardenas, E. Franzoso, E. Gersabeck, E. Golobardes, E. Govorkova, E. Graug\'es, E. Graverini, E. Jans, E. Jiang, E. Jimenez Moya, E.J. Walton, E. Kowalczyk, E. Lemos Cid, E. Luppi, E. Mariani, E. Maurice, E. Minucci, E.M. Niel, E. Muhammad, E. Olivart Pino, E. Polycarpo, E. Rodrigues, E. Rodriguez Fernandez, E. Rodriguez Rodriguez, E. Santovetti, E. Shmanin, E. Smith, E. Spadaro Norella, E. Spedicato, E. Thomas, E. van Herwijnen, E. Vilella Figueras, E. Whiter, E. Wood, F. Abudin\'en, F. Alessio, F. Archilli, F. Bedeschi, F. Betti, F. Blanc, F. Borgato, F.C. Glaser, F. C. L. Lopes, F.C.R. Bishop, F.C. Volle, F. De Benedetti, F. Debernardis, F. Dettori, F. De Vellis, F. Dordei, F. Fabiano, F. Fassin, F. Ferrari, F. Ferreira Rodrigues, F. Fleuret, F.F. Wilson, F. Goncalves Abrantes, F. Hemmer, F. I. Giasemis, F.J.P. Soler, F. Keizer, F. Kiraz, F. Lazzari, F. L. Liu, F.L. Souza De Almeida, F. Machefert, F. Maciuc, F. Martinez Vidal, F. M. Manganella, F. M. Meng, F. Muheim, F. Mu\~noz-Rojas, F. Oliva, F. Paciolla, F. Pisani, F. Polci, F. Redi, F. Reiss, F. Riehn, F. Ronchetti, F. Sborzacchi, F. Stagni, F. Suljik, F. Swystun, F. Terzuoli, F. Teubert, F. Zenesini, G. Bencivenni, G. Casse, G. Cavallero, G. C. Costantino, G. Chizhik, G. Cordova, G. Corti, G. Darze, G. Frau, G. Galati, G. Gong, G. Graziani, G. Haefeli, G. Hallett, G. 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Shchutska, L. Soares Lavra, L. Sun, L. Tomassetti, L. Toscano, L. Witola, L. Xu, L. Zhang, L. Z. Zhu, M. Abdelfatah, M. Adinolfi, M.A. Giza, M. Andersson, M. Andreotti, M. Argenton, M. Artuso, M. Atzeni, M. A. Wiegertjes, M. Bachmayer, M. Barbetti, M. Barnyakov, M. Becker, M. Birch, M. Borsato, M. Bovill, M. Burgos Marcos, M. Calvi, M. Calvo Gomez, M. Caporale, M. Cattaneo, M. Charles, M. Chefdeville, M. Cherif, M. Chrzaszcz, M. Clemencic, M. Colonna, M. Cruz Torres, M. Cubero Campos, M. De Cian, M. De Serio, M.D. Galati, M.D. Sokoloff, M.D. Tat, M. Elashri, M. Faria, M.F. Cicala, M. Feng, M. Fernandez Gomez, M. Ferrillo, M. Ferro-Luzzi, M. Fiorini, M. Firlej, M. Fontana, M. Franco Sevilla, M. Frank, M. Gandelman, M. Gersabeck, M. Giovannetti, M. Goncerz, M. Guarise, M. Hartmann, M.H. Schune, M. Idzik, M. J. Madurai, M.J. Morello, M. John, M.J. Peters, M. J. Williams, M. Kane, M. Karacson, M. Kenzie, M.K. Kazanecki, M. Kreps, M. Kucharczyk, M.K. Wilkinson, M. Lehuraux, M. 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Figure 1
Figure 1. Figure 1: Leading-order Feynman diagrams for the B+→ π +µ +µ − decay in the SM. 1The inclusion of charge-conjugate processes is implied throughout this paper unless explicitly stated. 1 view at source ↗
Figure 2
Figure 2. Figure 2: Illustration of the B+→ π +µ +µ − decay in the rest frame of (left) the B+ meson and (right) the dimuon system. The angle θl is defined as the angle between the direction of the µ + and the direction opposite the pion in the dimuon rest frame. and 15.0 < q2 < 22.0 GeV2 /c4 . While no measurements have previously been made of the angular distribution of the B+→ π +µ +µ − decay, the BaBar, Belle, CDF, CMS an… view at source ↗
Figure 3
Figure 3. Figure 3: Efficiency as a function of cos θl for B+→ π +µ +µ − decays in simulation in the q 2 regions (left) 1.1 < q2 < 6.0 GeV2 /c4 and (right) 15.0 < q2 < 22.0 GeV2 /c4 . The projections of fits using a fourth-order polynomial parameterisation, containing only even terms, are superimposed, with the uncertainty on the obtained efficiency function shown as a band. is assigned view at source ↗
Figure 4
Figure 4. Figure 4: Distribution of (left) the π +µ +µ − mass and (right) cos θl for selected B+→ J/ψπ+ candidates. The data are superimposed on the result of the fit described in the text. the two signal q 2 regions. The data are described well by the fit results. The discontinuity in cos θl (visible in the 1.1 < q2 < 6.0 GeV2 /c4 range) arises from the J/ψ veto. The observed signal yields are 89 ± 13 and 135 ± 15 in the low… view at source ↗
Figure 8
Figure 8. Figure 8: At low q 2 , the data show a nonzero AFB value and a large value of FH that are not consistent with the SM point within 95% confidence level (CL), but are consistent within 99% CL. At high q 2 , the data show values of AFB and FH that are consistent with the SM point within 68% CL. The stability of the results is tested by imposing alternative selection criteria on the output of the boosted-decision-tree b… view at source ↗
Figure 5
Figure 5. Figure 5: Distribution of (left) the π +µ +µ − mass and (right) cos θl for selected B+→ π +µ +µ − candidates in the range (top) 1.1 < q2 < 6.0 GeV2 /c4 and (bottom) 15.0 < q2 < 22.0 GeV2 /c4 . The data are superimposed on the result of the fit described in the text. −1 −0.5 0 0.5 1 l cos θ 0 10 20 30 Candidates per 0.1 Data Total fit − µ + µ + → π + B − µ + µ + → K + B Combinatorial LHCb −1 9 fb 2 ) < 5300 MeV/c − µ… view at source ↗
Figure 6
Figure 6. Figure 6: Distribution of cos θl for selected B+→ π +µ +µ − candidates in the range (left) 1.1 < q2 < 6.0 GeV2 /c4 and (right) 15.0 < q2 < 22.0 GeV2 /c4 . The candidates are re￾quired to be within the mass interval 5260 < m(π +µ +µ −) < 5300 MeV/c 2 , corresponding to a window of approximately twice the π +µ +µ − mass resolution around the known B+ meson mass. The data are superimposed on the result of the fit descr… view at source ↗
Figure 7
Figure 7. Figure 7: Obtained results for (left) FH and (right) AFB in bins of dimuon mass squared, q 2 . The markers indicate the best-fit values from the likelihood fit. The boxes represent the 68% CL intervals as determined using the Feldman–Cousins construction. The outer bars represent the total uncertainties, obtained by adding in quadrature the contribution arising from systematic uncertainties. −0.4 −0.2 0 0.2 0.4 AFB … view at source ↗
Figure 8
Figure 8. Figure 8: Two-dimensional CL regions obtained with the Feldman–Cousins procedure for view at source ↗
read the original abstract

This paper presents the first measurement of the forward-backward asymmetry, $A_{\rm FB}$, and the flat term, $F_{H}$, that parameterise the angular distribution of the $B^+\to\pi^+\mu^+\mu^-$ decay. The proton-proton collision dataset used in the analysis corresponds to an integrated luminosity of 9 fb$^{-1}$, collected with the LHCb experiment between 2011 and 2018. The analysis is performed in two intervals of dimuon mass squared, one above and one below the region containing the $J\mskip -3mu/\mskip -2mu\psi$ and $\psi(2S)$ narrow charmonium resonances. The Standard Model predictions lie within the obtained $68\%$ confidence level interval in the high-mass and within the $99\%$ interval in the low-mass region.

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 / 1 minor

Summary. The paper reports the first measurement of the forward-backward asymmetry A_FB and the flat term F_H parameterizing the angular distribution of the rare decay B^+ → π^+ μ^+ μ^-. Using 9 fb^{-1} of LHCb proton-proton collision data collected 2011-2018, the analysis is performed in two intervals of dimuon mass squared (q^2), one above and one below the narrow charmonium resonances J/ψ and ψ(2S). The central result is that Standard Model predictions lie within the obtained 68% CL interval in the high-mass region and within the 99% CL interval in the low-mass region.

Significance. If the result holds, this supplies the first experimental constraints on these angular observables in a b→d transition, adding a new data point to tests of the Standard Model and searches for new physics in flavor-changing neutral currents. The choice of a large LHCb dataset and the explicit avoidance of resonance regions are appropriate and strengthen the analysis; the direct extraction of A_FB and F_H from data (rather than derived quantities) is a methodological strength.

major comments (2)
  1. [Abstract] Abstract: the claim that SM predictions lie within the 68% CL (high-mass) and 99% CL (low-mass) intervals is central to the paper, yet no numerical values for the measured A_FB and F_H, their uncertainties, or the SM reference values are supplied, preventing verification of the stated consistency.
  2. [Analysis] The extraction of unbiased A_FB and F_H requires accurate modeling of backgrounds, efficiencies, and acceptance corrections (especially near the excluded resonance regions). The manuscript provides no quantitative information on systematic uncertainty budgets, fit stability tests, or validation with control samples, which directly affects the reliability of the reported CL intervals.
minor comments (1)
  1. The integrated luminosity is stated as 9 fb^{-1}; confirm that the exact value and its uncertainty are reported consistently in the main text and tables.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful review of our manuscript and the positive recommendation for minor revision. The comments are constructive and we address each major point below.

read point-by-point responses
  1. Referee: [Abstract] Abstract: the claim that SM predictions lie within the 68% CL (high-mass) and 99% CL (low-mass) intervals is central to the paper, yet no numerical values for the measured A_FB and F_H, their uncertainties, or the SM reference values are supplied, preventing verification of the stated consistency.

    Authors: We agree that the abstract would benefit from explicit numerical values to allow immediate verification. In the revised manuscript we will augment the abstract with the measured A_FB and F_H values (including uncertainties) in both q^2 intervals together with the corresponding Standard Model predictions. revision: yes

  2. Referee: [Analysis] The extraction of unbiased A_FB and F_H requires accurate modeling of backgrounds, efficiencies, and acceptance corrections (especially near the excluded resonance regions). The manuscript provides no quantitative information on systematic uncertainty budgets, fit stability tests, or validation with control samples, which directly affects the reliability of the reported CL intervals.

    Authors: The manuscript already contains dedicated sections describing the background model, efficiency and acceptance corrections, and the angular fit procedure. Nevertheless, we accept that a consolidated quantitative summary would strengthen the presentation. We will add an explicit systematic uncertainty budget (with individual contributions tabulated), results of fit stability tests, and validation studies performed on control samples such as B^+ → J/ψ K^+ decays. revision: yes

Circularity Check

0 steps flagged

No significant circularity in experimental measurement

full rationale

The paper reports a direct experimental extraction of the angular observables A_FB and F_H from LHCb collision data in two dimuon mass-squared intervals, after standard background subtraction, efficiency, and acceptance corrections. The central result is a comparison of these fitted values to independent Standard Model predictions, with the SM lying inside the reported confidence intervals. No derivation chain is claimed that reduces by the paper's own equations to quantities defined in terms of the fitted parameters themselves, nor does any load-bearing step rely on self-citation of an unverified uniqueness theorem or ansatz. The analysis is self-contained against external benchmarks (data-driven control samples and simulation validation), yielding a normal non-finding of circularity.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The measurement rests on standard LHCb detector calibration, background modeling, and efficiency corrections that are not derived in the paper itself; no new free parameters or invented entities are introduced beyond conventional fit parameters for the angular coefficients.

free parameters (1)
  • A_FB and F_H fit parameters
    Extracted from data in each dimuon-mass interval; values are the central result rather than inputs.
axioms (1)
  • domain assumption Standard Model angular distribution form for b→sℓℓ decays
    Used to compare measured coefficients against theoretical predictions.

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