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arxiv: 2604.08631 · v1 · submitted 2026-04-09 · ✦ hep-ex

Recognition: unknown

Test of lepton flavour universality with B⁰to K^{*0}ell^+ell^- decays at large dilepton invariant mass

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 Z. Ajaltouni S. Akar K. Akiba 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 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 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. Bavarchee A. Bay A. Beck M. Becker F. Bedeschi I.B. Bediaga N. A. Behling S. Belin A. Bellavista I. Belov I. Belyaev G. Benane G. Bencivenni E. Ben-Haim 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 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 G. Chizhik V. Chobanova M. Chrzaszcz 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 G. C. Costantino J. Cottee Meldrum B. Couturier D.C. Craik M. Cruz Torres M. Cubero Campos E. Curras Rivera R. Currie C.L. Da Silva 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. 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 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 L.L. Gerken 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. Horswill R. Hou Y. Hou D.C. Houston N. Howarth W. Hu X. Hu W. Hulsbergen R.J. Hunter 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 S. Klaver 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 J. Langer 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 Y. Li Z. Lian Q. Liang X. Liang Z. Liang S. Libralon A. Lightbody C. Lin 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 G. M. Ma 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 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 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 E. Muhammad F. Muheim M. Mulder K. M\"uller F. Mu\~noz-Rojas 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 C. Nunez 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 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 R.A. Ruiz Fernandez 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 T. Senger 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 Y. Su F. Suljik J. Sun L. 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 D.J. Unverzagt 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 Y. Z. Zhang Z. Zhang 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 16:55 UTC · model grok-4.3

classification ✦ hep-ex
keywords lepton flavour universalityB0 to K*0 dilepton decaysbranching fraction ratiohigh dilepton massrare B decaysLHCb measurementStandard Model test
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The pith

LHCb measures the muon-to-electron branching fraction ratio R_K*0 at 1.08 in B0 to K*0 dilepton decays above 14 GeV2/c4, consistent with the Standard Model.

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

This paper tests lepton flavour universality by measuring the ratio of branching fractions for B0 to K*0 mu mu versus B0 to K*0 e e decays in the region of high dilepton invariant mass squared. Using proton-proton collision data recorded by the LHCb detector, the analysis finds the ratio equals 1.08 with statistical uncertainty of +0.14/-0.12 and systematic uncertainty of 0.07, agreeing with the Standard Model expectation that the two lepton species should behave identically after phase-space corrections. A reader cares because this ratio cancels many experimental effects and provides a clean probe for whether new forces or particles might treat muons differently from electrons. The result is the most precise measurement available in this kinematic region and the first obtained at a hadron collider.

Core claim

The paper measures the lepton flavour universality ratio R_K*0 in B0 to K*0 ell+ ell- decays for dilepton invariant mass squared above 14.0 GeV2/c4. With 9 fb-1 of data collected at center-of-mass energies of 7, 8, and 13 TeV, the ratio of branching fractions between the muon and electron channels is determined to be 1.08^{+0.14}_{-0.12} (stat) ± 0.07 (syst). This value is consistent with the Standard Model prediction of approximately one.

What carries the argument

The ratio R_K*0 of branching fractions for the muon and electron modes in the high dilepton-mass region, chosen because many reconstruction and efficiency effects cancel between the two channels.

If this is right

  • The measured ratio agrees with the Standard Model expectation of equal rates for the two lepton species.
  • No evidence for lepton flavour non-universality appears in this high-mass kinematic region.
  • The precision sets a reference point for future tests of the same observable with additional data.

Where Pith is reading between the lines

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

  • The high-mass result provides a contrast point for lower-mass measurements in related B decays where tensions have been noted elsewhere.
  • Additional data from future LHC runs could shrink the uncertainties and test for smaller possible deviations from unity.
  • The ratio method used here can be applied to other rare decays to perform similar universality tests at hadron colliders.

Load-bearing premise

Detector efficiencies, background shapes, and reconstruction effects for muons and electrons are assumed to be modeled correctly so that differences cancel in the ratio; any uncancelled bias would shift the measured value.

What would settle it

An independent analysis or larger dataset that yields a ratio value lying outside the quoted uncertainty range after identical selection and efficiency corrections would indicate the consistency with the Standard Model does not hold.

Figures

Figures reproduced from arXiv: 2604.08631 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. Chernov, 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. 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: Invariant-mass distributions of the B0→ K∗0 ℓ +ℓ − candidates in the high-q 2 region for the (a) muon and (b) electron channel with the fit results also shown. The left-side cutoff of the combinatorial background distribution arises from the kinematic boundaries of the accessible phase space. contributing 0.1–0.8% to the uncertainty on the measured ratios. The overall uncertainty related to efficiencies su… view at source ↗
Figure 2
Figure 2. Figure 2: Log-likelihood profile of RK∗0 with (red solid) and without (blue dashed) systematic uncertainties [PITH_FULL_IMAGE:figures/full_fig_p010_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Summary of the measurement of RK∗0 from this work (blue square point), the LHCb measurements in the lower q 2 region [31] (green dot points) and the SM prediction (dashed line). The vertical error bars represent the total uncertainties. 9 [PITH_FULL_IMAGE:figures/full_fig_p011_3.png] view at source ↗
read the original abstract

Muon-electron universality is tested in $B^0 \to K^{*0} \ \ell^+ \ell^-$ decays, in the dilepton-invariant-mass region above the $\psi(2S)$ resonance. The analysis uses beauty mesons produced in proton-proton collisions recorded by the LHCb detector at center-of-mass energies of 7, 8, and 13 $\text{TeV}$, corresponding to an integrated luminosity of 9 $\text{fb}^{-1}$. The ratio of branching fractions between the muon and electron channels, $R_{K^{*0}}$, is measured to be $1.08\,^{+0.14}_{-0.12}\text{(stat)} \ \pm 0.07\text{(syst)}$ for a dilepton-invariant-mass squared above 14.0 $\text{GeV}^{2}/\text{c}^{4}$, consistent with the Standard Model prediction. This result represents the most precise measurement of $R_{K^{*0}}$ in this region and the first such measurement performed at a hadron collider.

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 paper reports a measurement of the lepton flavour universality ratio R_{K^{*0}} in B^0 → K^{*0} ℓ⁺ℓ⁻ decays for dilepton invariant mass squared q² > 14 GeV²/c⁴. Using 9 fb⁻¹ of LHCb pp collision data at 7, 8 and 13 TeV, the ratio of branching fractions between the muon and electron channels is found to be 1.08^{+0.14}_{-0.12}(stat) ± 0.07(syst), consistent with the Standard Model prediction. The result is presented as the most precise measurement in this kinematic region and the first performed at a hadron collider.

Significance. If the central result holds after full verification of efficiency corrections and background modeling, the measurement provides a valuable high-q² test of lepton flavour universality in b → sℓℓ transitions. It complements lower-q² results and demonstrates that a competitive ratio measurement can be performed at a hadron collider with data-driven cancellation of many systematic effects. The absence of free parameters in the final quoted ratio and the direct use of collision data for the observable are strengths.

minor comments (2)
  1. The abstract states the result is 'consistent with the Standard Model prediction' but does not quote the numerical SM expectation or its uncertainty; adding this value would improve clarity for readers.
  2. The integrated luminosity is given as 9 fb⁻¹ without breakdown by centre-of-mass energy; a short table or sentence in §2 or §3 would help assess the relative weight of the 13 TeV sample.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for the positive summary, significance assessment, and recommendation to accept the manuscript. We appreciate the recognition of the measurement's value as a high-q² test of lepton flavour universality in b → sℓℓ transitions and its complementarity to lower-q² results.

Circularity Check

0 steps flagged

No significant circularity: direct experimental ratio measurement

full rationale

The paper reports a direct measurement of the branching-fraction ratio R_{K^{*0}} from proton-proton collision data recorded by LHCb. The central result is obtained by counting signal candidates in the muon and electron channels after applying selection criteria, efficiency corrections, and background subtraction; the ratio is formed explicitly from these observed yields and correction factors. No derivation chain is present that reduces the reported value to a fitted parameter, self-citation, or ansatz by construction. Detector efficiencies and reconstruction effects are modeled with simulation and control samples, but these steps are external to the final ratio and do not create a self-referential loop within the paper's equations. The measurement is therefore self-contained against external benchmarks (collision data) and receives the lowest circularity score.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The central claim rests on the experimental measurement and its comparison to the Standard Model expectation; no new free parameters, axioms beyond standard particle physics assumptions, or invented entities are introduced in the abstract.

axioms (1)
  • domain assumption Standard Model branching fraction ratio equals unity in the absence of new physics
    The consistency statement relies on this SM prediction for the ratio.

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Works this paper leans on

55 extracted references · 47 canonical work pages · 1 internal anchor

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