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arxiv: 2604.12706 · v1 · submitted 2026-04-14 · ✦ hep-ex

Recognition: unknown

Measurement of the W-boson production cross-sections in pp collisions at sqrt{s} = 13 TeV in the forward region

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 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 N. Crepet 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 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 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 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 14:17 UTC · model grok-4.3

classification ✦ hep-ex
keywords W boson productioncross section measurementLHCbforward region13 TeVmuon decayperturbative QCDproton-proton collisions
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The pith

LHCb measures the W+ and W- boson production cross sections in the forward region at 13 TeV to be 1754 pb and 1178 pb respectively, agreeing with NNLO predictions.

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

The paper performs a precision measurement of W boson production in proton-proton collisions at 13 TeV using the decay to muons, based on 5.1 inverse femtobarns of data collected by the LHCb experiment. The cross sections are extracted for muons with transverse momentum from 25 to 55 GeV and pseudorapidity from 2.0 to 4.5 in the forward detector region. The reported values match next-to-next-to-leading order perturbative QCD calculations within uncertainties and achieve substantially better precision than earlier results in the same kinematic range. This establishes a refined experimental benchmark for electroweak boson production at the LHC.

Core claim

The integrated production cross-sections are measured to be σ(W+ → μ+ν) = 1754.2 ± 1.5 ± 11.9 ± 35.1 pb and σ(W- → μ-ν̄) = 1178.1 ± 1.3 ± 9.7 ± 23.6 pb, where uncertainties are statistical, systematic, and due to luminosity, respectively. These values are obtained in the specified muon kinematic range and are found to be in good agreement with theoretical predictions at next-to-next-to-leading order in perturbative quantum chromodynamics, representing a significant improvement in precision over previous measurements in this regime.

What carries the argument

Selection and background subtraction of W → μν decays in the forward pseudorapidity acceptance of LHCb, normalized to the recorded integrated luminosity of 5.1 fb^{-1}.

If this is right

  • The measured values provide a more precise test of next-to-next-to-leading order perturbative QCD calculations for W boson production in forward kinematics.
  • They supply improved experimental constraints on parton distribution functions at low momentum fractions probed in the forward region.
  • The higher precision establishes a stronger reference point for comparing against future LHC data sets collected at the same or higher energies.
  • Agreement with theory supports the validity of Standard Model predictions for electroweak processes under these conditions.

Where Pith is reading between the lines

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

  • These forward-region results can be combined with central-rapidity measurements from ATLAS and CMS to tighten global constraints on proton parton densities across a broader kinematic range.
  • Any statistically significant deviation from the predicted cross sections in higher-luminosity data could indicate contributions from physics beyond the Standard Model.
  • The analysis methods developed for isolating the muon decay channel in the forward region may be adapted to measure associated production or other vector-boson processes at LHCb.

Load-bearing premise

The absolute scale of the cross sections depends on the accuracy of the luminosity determination for the data sample, so any overall bias in that normalization would scale both reported values directly.

What would settle it

An independent analysis or new data set that yields cross sections lying outside the combined total uncertainties of the quoted values while disagreeing with the NNLO predictions would falsify the claimed agreement.

Figures

Figures reproduced from arXiv: 2604.12706 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. 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. Lin, C. Lopez Iribarnegaray, C. Lucarelli, C. Mancuso, C. Marin Benito, C. Matteuzzi, C. Normand, C. Nunez, 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. Hutchcroft, D.J.D. Thompson, D. Johnson, D.J. Unverzagt, D. Kaminaris, D. 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Figure 1
Figure 1. Figure 1: Invariant-mass distributions of Z → µ +µ − candidates used in the momentum smearing fit, with the fit results also shown. The red and blue curves are simulated data. method from Ref. [82], which computes a normalized weighted average over the dilepton angular coordinates (θ, ϕ). The method evaluates a projection function in the numerator while normalizing to the unpolarized differential cross-section in th… view at source ↗
Figure 2
Figure 2. Figure 2: Distribution of the muon pT for selected (left) W+ and (right) W− bosons for the example interval 2.125 < ηµ < 2.250, with the fit results also shown. 6 Efficiencies The total reconstruction and selection efficiency for a given ηµ interval is defined as εW± = P reco W ωtrk,id,trg · ωsel · ωgen P true W ωgen , (9) where the numerator aggregates weights from events in the W-boson simulated samples passing al… view at source ↗
Figure 3
Figure 3. Figure 3: Data-to-simulation efficiency ratios for muon selection requirements, shown as functions [PITH_FULL_IMAGE:figures/full_fig_p011_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: Differential W → µν cross-sections, as a function of ηµ. The bands represent the data, with the inner region corresponding to the statistical uncertainty and the outer one to the total uncertainty. For theoretical predictions, the error bars incorporate both PDF and scale uncertainties. Acknowledgements We express our gratitude to our colleagues in the CERN accelerator departments for the excellent perform… view at source ↗
Figure 5
Figure 5. Figure 5: Total (top) W+→ µ +νµ and (bottom) W−→ µ −νµ cross-sections compared with theoretical predictions. The bands denote the measurements, with the inner region corresponding to the statistical and the outer one to the total uncertainty. For the theoretical predictions, the error bars incorporate both PDF and scale uncertainties. 14 [PITH_FULL_IMAGE:figures/full_fig_p016_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: Results for the (top) σW+→µ+ν/σZ→µ+µ− and (bottom) σW−→µ−ν/σZ→µ+µ− cross￾section ratios compared with theoretical predictions. The p µ T range used for the W (Z) cross￾section measurement is 25 < pµ T < 55 GeV (p µ T > 20 GeV). The bands denote the measurements, with the inner region corresponding to the statistical uncertainty and the outer region corre￾sponding to the statistical and systematic uncertain… view at source ↗
Figure 7
Figure 7. Figure 7: Integrated cross-sections measurements of (top) [PITH_FULL_IMAGE:figures/full_fig_p018_7.png] view at source ↗
read the original abstract

A precision measurement of the $W$-boson production cross-section is performed using the $W \to \mu\nu$ decay channel, based on a sample of proton-proton collision data collected by the LHCb experiment at $\sqrt{s}$ = 13 TeV and corresponding to an integrated luminosity of 5.1 $fb^{-1}$. The cross-section is measured for muons with transverse momentum between 25 and 55 GeV and pseudorapidity between 2.0 and 4.5. The integrated production cross-sections of $W$ bosons are measured to be $$ \begin{array}{lcl} \sigma_{W^+ \to \mu^+\nu} &=& 1754.2 \pm 1.5 \pm 11.9 \pm 35.1\text{ pb} \\ \sigma_{W^- \to \mu^-\bar{\nu}} &=& 1178.1 \pm 1.3 \pm 9.7 \pm 23.6\text{ pb} \end{array} $$ where uncertainties are statistical, systematic, and due to the luminosity determination, respectively. Results are in good agreement with theoretical predictions at next-to-next-to-leading order in perturbative quantum chromodynamics. This measurement is significantly more precise than previous results in this kinematic regime.

Editorial analysis

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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 paper presents a precision measurement of the W-boson production cross-sections in the forward region using the W → μν decay channel in pp collisions at √s = 13 TeV with the LHCb experiment. Based on 5.1 fb^{-1} of integrated luminosity, the fiducial cross-sections (25 < p_T < 55 GeV, 2.0 < η < 4.5) are reported as σ(W^+ → μ^+ν) = 1754.2 ± 1.5 ± 11.9 ± 35.1 pb and σ(W^- → μ^-ν̄) = 1178.1 ± 1.3 ± 9.7 ± 23.6 pb, where the uncertainties are statistical, systematic, and luminosity, respectively. The results are stated to agree with NNLO pQCD predictions and to be significantly more precise than previous measurements in this kinematic regime.

Significance. If the result holds, this provides a high-precision benchmark for NNLO pQCD calculations in the forward acceptance, where data are sensitive to parton distributions at large x. The explicit separation of statistical, systematic, and luminosity uncertainties, together with the direct comparison to theory evaluated in the identical fiducial volume, are strengths that enhance the result's utility for PDF constraints and theoretical validation. The measurement improves substantially on prior precision in this region.

minor comments (1)
  1. [Abstract] The cross-section results in the abstract are presented in an array; separate aligned equations would improve readability.

Simulated Author's Rebuttal

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We thank the referee for their positive assessment of the manuscript, the recognition of its precision and utility for PDF constraints, and the recommendation to accept. No major comments were raised in the report.

Circularity Check

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No significant circularity; direct experimental measurement

full rationale

This paper reports a standard fiducial cross-section measurement of W → μν production in the LHCb forward acceptance using 5.1 fb⁻¹ of 13 TeV pp data. The central results are obtained by selecting signal candidates, subtracting backgrounds, applying efficiency corrections (determined from simulation validated with data-driven methods), and normalizing to the measured integrated luminosity. No load-bearing step in the analysis chain reduces by construction to a fitted parameter, self-citation, or ansatz imported from prior work by the same authors. The quoted agreement with NNLO pQCD predictions is an external comparison performed after the measurement, not part of the derivation. The paper is self-contained against external benchmarks (luminosity, detector response) and exhibits none of the enumerated circularity patterns.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

No new free parameters or invented entities; relies on standard LHC luminosity calibration, muon identification efficiencies, and background subtraction procedures established in prior LHCb papers.

axioms (2)
  • domain assumption Standard model electroweak and QCD interactions govern W production and decay
    Invoked throughout to interpret the observed muon yields as W boson production.
  • domain assumption Detector response and efficiencies can be modeled from simulation and control samples
    Used to correct raw yields to cross-sections.

pith-pipeline@v0.9.0 · 11606 in / 1164 out tokens · 47977 ms · 2026-05-10T14:17:21.329568+00:00 · methodology

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Works this paper leans on

88 extracted references · 69 canonical work pages · 2 internal anchors

  1. [1]

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