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arxiv: 2605.07586 · v1 · submitted 2026-05-08 · ✦ hep-ex

Recognition: 2 theorem links

· Lean Theorem

Evidence for the decay B⁰_stoφη'

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. 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 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. 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 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 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 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 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 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 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 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 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 2026-05-11 02:24 UTC · model grok-4.3

classification ✦ hep-ex
keywords B_s meson decaybranching fractionrare decayphi eta primeinvariant mass fitproton-proton collisionshadron collider
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The pith

Evidence is found for the decay of the neutral strange B meson into a phi and an eta-prime meson at 3.5 sigma significance.

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

The paper reports a search for the decay B_s^0 to phi eta-prime using proton-proton collision data corresponding to 9 inverse femtobarns of integrated luminosity. It establishes evidence for this mode at 3.5 sigma and determines its branching fraction relative to the reference decay B_s^0 to phi phi. A sympathetic reader would care because rare B meson decays like this one test the Standard Model description of quark transitions and can reveal deviations that point to new physics. The measurement adds a new data point to the pattern of observed branching fractions in the B_s system.

Core claim

Using proton-proton collision data, evidence is found for the decay B^0_s to phi eta-prime with 3.5 sigma significance. The branching ratio relative to B^0_s to phi phi is measured to be R = (3.56 ± 0.79 ± 0.18 ± 0.06) × 10^{-2}. This corresponds to an absolute branching fraction B(B^0_s to phi eta-prime) = (0.66 ± 0.15 ± 0.03 ± 0.02) × 10^{-6}, where the uncertainties are statistical, systematic, and from external inputs respectively.

What carries the argument

The relative branching fraction R extracted from an invariant-mass fit to selected B candidate decays, normalized to the reference channel B_s^0 to phi phi.

If this is right

  • The measured branching fraction provides a new experimental input for testing theoretical calculations of non-leptonic B_s decays.
  • This decay channel can be used in future studies to compare the rate of eta-prime production against predictions from QCD models.
  • The result constrains the size of possible contributions from penguin amplitudes or other mechanisms in the decay amplitude.
  • Larger future datasets can reduce the uncertainty on this branching fraction and enable searches for CP violation or other asymmetries in the same final state.

Where Pith is reading between the lines

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

  • The observation opens the possibility of measuring the lifetime or mixing parameters of the B_s^0 in this specific decay mode with higher statistics.
  • Comparison of this rate to the related B_s^0 to phi eta decay could test isospin or SU(3) flavor symmetry relations in the final state.
  • If the measured value deviates from updated Standard Model predictions, it would motivate targeted searches for new physics in b to s transitions.

Load-bearing premise

The parametric shapes used for the signal peak and the various background components in the invariant mass fit correctly describe the observed data without large unaccounted contributions from other B decays.

What would settle it

An independent re-analysis of the same or larger dataset that finds the fitted signal yield in the B_s^0 to phi eta-prime mass window consistent with zero would falsify the 3.5 sigma evidence claim.

Figures

Figures reproduced from arXiv: 2605.07586 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. Saitta, B. Schmidt, B. Sciascia, B. Sevilla Sanjuan, B. Shi, B. Souza De Paula, B. Urbach, B. Vivacqua, B. Wang, C.A. Aidala, C. 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Figure 1
Figure 1. Figure 1: Feynman diagram for the B0 s → ϕη′ decay. 1The symbols ϕ and η ′ indicate the ϕ(1020) and η ′ (958) mesons throughout. 1 [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: Distribution of the K+K−η ′ invariant-mass for the complete dataset, summing over the four categories. The result of the simultaneous fit described in the text is also shown, with the signal component represented in yellow [PITH_FULL_IMAGE:figures/full_fig_p007_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: The K+K−K+K− invariant-mass distribution for the normalisation mode for the complete dataset, summing over the four categories. The simultaneous fit result is shown. The impact of the B0 s → ϕη′ fit model choice on the yield is evaluated using pseudoex￾periments, where an alternative model is selected instead. Specifically, the signal shape is described by a skewed Student’s t-distribution, and the combina… view at source ↗
Figure 4
Figure 4. Figure 4: Ratio of branching fraction R for each of the categories and their weighted average, compared to the upper limit at 90% (red dashed line) and 95% (cyan dashed line) confidence level previously obtained with the Run 1 dataset [9]. The shaded area on the error bar represents the statistical, while the full error bar represents the total uncertainty. The green band shows the average value in this analysis. 6 … view at source ↗
read the original abstract

Using a dataset corresponding to an integrated luminosity of $9 \,\textrm{fb}^{-1}$ collected in proton-proton collisions between 2011 and 2018 by the LHCb experiment, evidence is found for the decay $B^0_s\to\phi\eta'$ with $3.5 \sigma$ significance. The branching ratio relative to the $B^0_s\to\phi\phi$ decay is determined to be $R=(3.56 \pm 0.79\pm 0.18\pm 0.06)\times10^{-2}$. This corresponds to a branching fraction, $B(B^0_s\to\phi\eta')=(0.66 \pm 0.15 \pm 0.03 \pm 0.02) \times 10^{-6}$ where, in both cases, the first uncertainty is statistical, the second systematic, and the third due to external branching fractions.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 2 minor

Summary. The manuscript reports evidence at 3.5σ significance for the decay B_s^0 → ϕη' in a dataset of 9 fb^{-1} collected by LHCb in pp collisions from 2011–2018. The branching ratio relative to the normalization channel B_s^0 → ϕϕ is measured as R = (3.56 ± 0.79 ± 0.18 ± 0.06) × 10^{-2}, corresponding to an absolute branching fraction B(B_s^0 → ϕη') = (0.66 ± 0.15 ± 0.03 ± 0.02) × 10^{-6}, with uncertainties statistical, systematic, and from external inputs, respectively.

Significance. If the result holds, it provides the first evidence for this decay mode, adding a new measurement in the B_s sector that can test theoretical predictions involving penguin amplitudes and η' mixing. Normalizing to the well-measured B_s^0 → ϕϕ mode is a strength that reduces absolute efficiency uncertainties. The moderate significance is consistent with a rare decay and does not undermine the claim provided the fit procedure is robust.

major comments (1)
  1. [Invariant mass fit] The central 3.5σ significance is extracted from an unbinned maximum-likelihood fit to the B-candidate invariant mass; the weakest assumption is that the chosen parametric shapes for signal (typically Crystal Ball or Gaussian) and background (exponential or polynomial) accurately describe the data without significant unaccounted peaking backgrounds from other B decays. More explicit validation of fit stability, including pull distributions and alternative background models, is needed to confirm the yield is not biased.
minor comments (2)
  1. [Abstract] The abstract clearly states the result but could briefly note the fit model and efficiency ratio determination for improved readability.
  2. [Systematic uncertainties] A dedicated table or section breaking down the systematic uncertainties (currently quoted as a single ±0.18 term) would allow readers to assess their individual contributions more precisely.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for the positive assessment of our manuscript and the recommendation for minor revision. We address the single major comment on the invariant mass fit validation in the point-by-point response below.

read point-by-point responses
  1. Referee: The central 3.5σ significance is extracted from an unbinned maximum-likelihood fit to the B-candidate invariant mass; the weakest assumption is that the chosen parametric shapes for signal (typically Crystal Ball or Gaussian) and background (exponential or polynomial) accurately describe the data without significant unaccounted peaking backgrounds from other B decays. More explicit validation of fit stability, including pull distributions and alternative background models, is needed to confirm the yield is not biased.

    Authors: We thank the referee for this constructive comment. In the analysis, the signal is modeled with a Crystal Ball function whose parameters are determined from simulation, and the combinatorial background with an exponential function. The manuscript already reports the fit results and the 3.5σ significance obtained from the likelihood ratio test. To strengthen the validation as suggested, we will add in the revised version: (i) pull distributions from the fit and from pseudo-experiments, (ii) results using an alternative background model (second-order polynomial), and (iii) a dedicated study of possible peaking backgrounds from other B decays (such as B^0 → ϕη or B_s^0 → ϕη) showing their contribution is negligible within the selected mass window. These will be included either in the main text or as supplementary material to demonstrate that the extracted yield is robust and unbiased. revision: yes

Circularity Check

0 steps flagged

No significant circularity: direct experimental measurement

full rationale

The paper reports a standard LHCb branching-fraction measurement. Event yields for the signal mode B_s^0 → ϕη' and the normalization mode B_s^0 → ϕϕ are extracted from unbinned maximum-likelihood fits to the invariant-mass distribution. The relative branching ratio is obtained from the yield ratio after correction by the ratio of selection efficiencies (determined from simulation and data-driven methods). The absolute branching fraction is then scaled by the external world-average value of B(B_s^0 → ϕϕ). No equation or step reduces the reported result to a fitted parameter by construction, no ansatz is smuggled via self-citation, and no uniqueness theorem or self-referential definition is invoked. The analysis chain is externally falsifiable and relies on independent inputs (data, simulation, external branching fractions).

Axiom & Free-Parameter Ledger

2 free parameters · 2 axioms · 0 invented entities

The measurement depends on standard LHCb reconstruction efficiencies, background parametrizations in the mass fit, and external branching fractions for the normalization channel; these are treated as inputs rather than derived within the paper.

free parameters (2)
  • signal and background yields in mass fit
    Fitted directly from the data distribution to extract the raw signal count.
  • efficiency ratio between signal and normalization channels
    Determined from simulation and corrected with data-driven methods; value not stated in abstract.
axioms (2)
  • domain assumption The invariant-mass distributions of signal and background are adequately described by the chosen parametric forms
    Invoked when performing the unbinned maximum-likelihood fit to extract the yield.
  • domain assumption External branching fraction of B_s^0 to phi phi is known to sufficient precision
    Used to convert the relative ratio into an absolute branching fraction.

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uses
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40 extracted references · 40 canonical work pages · 1 internal anchor

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