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No significant signal is observed, and upper limits are set on the branching fractions, ${\\cal B}(B^-\\to D^{+}\u03bc^-\u03bc^-) < 4.6 \\times 10^{-8}$ and ${\\cal B}(B^-\\to D^{*+}\u03bc^-\u03bc^-) < 5.9 \\times 10^{-8}$, at the 95% confidence level.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins3103133/1/csv","json":"https://www.hepdata.net/download/submission/ins3103133/1/json","root":"https://www.hepdata.net/download/submission/ins3103133/1/root","yaml":"https://www.hepdata.net/download/submission/ins3103133/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins3103133/1/yoda","yoda-h5":"https://www.hepdata.net/download/submission/ins3103133/1/yoda.h5"}},"analyses":[],"arxiv_id":"arXiv:2601.07657","authors":["Aaij, Roel","Abdelmotteleb, Ahmed Sameh Wagih","Abellan Beteta, Carlos","Abudin\u00e9n, Fernando Jesus","Ackernley, Thomas","Adefisoye, Ayomide Matthew","Adeva, Bernardo","Adinolfi, Marco","Adlarson, Patrik Harri","Agapopoulou, Christina"],"collaborations":["LHCb"],"control_number":"167818","creation_date":"2026-01-12","data":[{"abstract":"Binned efficiencies across the Dalitz plane for $B^- \\to D^{+} \\mu^- \\mu^-$ decay. Here $\\mu_1^-$ and $\\mu_2^-$ represent the two muons produced in the decay, and the index specifies their ordering in transverse momentum. Efficiencies are normalized to the average over the full simulated sample.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins3103133/Efficiencies of $B^- %5Cto D^{+} %5Cmu^- %5Cmu^-$ channel/csv","json":"https://www.hepdata.net/download/table/ins3103133/Efficiencies of $B^- %5Cto D^{+} %5Cmu^- %5Cmu^-$ channel/json","root":"https://www.hepdata.net/download/table/ins3103133/Efficiencies of $B^- %5Cto D^{+} %5Cmu^- %5Cmu^-$ channel/root","yaml":"https://www.hepdata.net/download/table/ins3103133/Efficiencies of $B^- %5Cto D^{+} %5Cmu^- %5Cmu^-$ channel/yaml","yoda":"https://www.hepdata.net/download/table/ins3103133/Efficiencies of $B^- %5Cto D^{+} %5Cmu^- %5Cmu^-$ channel/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins3103133/Efficiencies of $B^- %5Cto D^{+} %5Cmu^- %5Cmu^-$ channel/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"167849","creation_date":"2026-01-12","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["efficiency","simulation","Dalitz plane","phase space"],"reactions":["B- -> D+ mu- mu-"]},"date":"12 Jan 2026","doc_type":"datatable","doi":"10.17182/hepdata.167818.v1/t1","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":167849,"inspire_id":"3103133","journal_info":"LHCb-PAPER-2025-033","keywords":[{"name":"reactions","synonyms":"","value":"B- -> D+ mu- mu-"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"efficiency"},{"name":"phrases","synonyms":"","value":"simulation"},{"name":"phrases","synonyms":"","value":"phase space"},{"name":"phrases","synonyms":"","value":"Dalitz plane"}],"last_updated":"2026-01-23T14:36:06","parent_child_join":{"name":"child_datatable","parent":"167818"},"recid":167849,"related_publication":167818,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4131823?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4131824?landing_page=true"}],"title":"Efficiencies of $B^- \\to D^{+} \\mu^- \\mu^-$ channel","uuid":"05f7a063-54b9-45bf-aae9-a0bb1c75046b"},{"abstract":"Binned efficiencies across the Dalitz plane for $B^- \\to D^{*+} \\mu^- \\mu^-$ decay. Here $\\mu_1^-$ and $\\mu_2^-$ represent the two muons produced in the decay, and the index specifies their ordering in transverse momentum. Efficiencies are normalized to the average over the full simulated sample.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins3103133/Efficiencies of $B^- %5Cto D^{*+} %5Cmu^- %5Cmu^-$ channel/csv","json":"https://www.hepdata.net/download/table/ins3103133/Efficiencies of $B^- %5Cto D^{*+} %5Cmu^- %5Cmu^-$ channel/json","root":"https://www.hepdata.net/download/table/ins3103133/Efficiencies of $B^- %5Cto D^{*+} %5Cmu^- %5Cmu^-$ channel/root","yaml":"https://www.hepdata.net/download/table/ins3103133/Efficiencies of $B^- %5Cto D^{*+} %5Cmu^- %5Cmu^-$ channel/yaml","yoda":"https://www.hepdata.net/download/table/ins3103133/Efficiencies of $B^- %5Cto D^{*+} %5Cmu^- %5Cmu^-$ channel/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins3103133/Efficiencies of $B^- %5Cto D^{*+} %5Cmu^- %5Cmu^-$ channel/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"167850","creation_date":"2026-01-12","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["efficiency","simulation","Dalitz plane","phase space"],"reactions":["B- -> D*+ mu- mu-"]},"date":"12 Jan 2026","doc_type":"datatable","doi":"10.17182/hepdata.167818.v1/t2","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":167850,"inspire_id":"3103133","journal_info":"LHCb-PAPER-2025-033","keywords":[{"name":"reactions","synonyms":"","value":"B- -> D*+ mu- mu-"},{"name":"cmenergies","synonyms":"","value":"13000.0"},{"name":"phrases","synonyms":"","value":"efficiency"},{"name":"phrases","synonyms":"","value":"simulation"},{"name":"phrases","synonyms":"","value":"phase space"},{"name":"phrases","synonyms":"","value":"Dalitz plane"}],"last_updated":"2026-01-23T14:36:06","parent_child_join":{"name":"child_datatable","parent":"167818"},"recid":167850,"related_publication":167818,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/4131826?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/4131827?landing_page=true"}],"title":"Efficiencies of $B^- \\to D^{*+} \\mu^- \\mu^-$ channel","uuid":"f59538f5-8ee7-4e4a-ac3e-c455f39e4b12"}],"data_abstract":"The lepton-number-violating $B^- \\to D^{(*)+} \\mu^- \\mu^-$ decays are searched in this analysis. \nNo excessive signal is observed, and upper limits of their branching fractions are measured \nat a proton-proton centre-of-mass energy $\\sqrt{s} = 13\\,\\mathrm{TeV}$.\n\nSignal yields are normalized to the normalization channel $B^-\\to \\psi(\\mathrm{2S}) K^-$, and \nefficiency corrections are applied in the normalized based on Monte Carlo simulation. \nThe standard deviation of efficiencies arocess Dalitz plane is considered as the major\nsystematic uncertainty in the efficiency correction.\n\nThe efficiencies in each bin are provided in this HepData entry.\n","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["efficiency","simulation","Dalitz plane","phase space"],"reactions":["B- -> D+ mu- mu-","B- -> D*+ mu- mu-"]},"date":"12 Jan 2026","doc_type":"publication","doi":null,"first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"hepdata_doi":"10.17182/hepdata.167818","id":167818,"inspire_id":"3103133","journal_info":"LHCb-PAPER-2025-033","keywords":[],"last_updated":"2026-01-23T14:36:06","parent_child_join":{"name":"parent_publication"},"publication_date":"2026-01-23T00:00:00","recid":167818,"resources":[],"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},{"affiliation":"Warwick U.","full_name":"Abdelmotteleb, Ahmed Sameh Wagih"},{"affiliation":"Zurich U.","full_name":"Abellan Beteta, Carlos"},{"affiliation":"Warwick U.","full_name":"Abudin\u00e9n, Fernando Jesus"},{"affiliation":"Liverpool U.","full_name":"Ackernley, Thomas"},{"affiliation":"Syracuse U.","full_name":"Adefisoye, Ayomide Matthew"},{"affiliation":"U. 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Integrated over $p_\\mathrm{T}$, the measured cross-sections are \\begin{align*} \u03c3_{W^+ \\to \u03bc^+ \u03bd_\u03bc} &= 300.9 \\pm 2.4 \\pm 3.8 \\pm 6.0~\\text{pb}, \\\\ \u03c3_{W^- \\to \u03bc^- \\bar\u03bd_\u03bc} &= 236.9 \\pm 2.1 \\pm 2.7 \\pm 4.7~\\text{pb}, \\end{align*} where the first uncertainties are statistical, the second are systematic, and the third are associated with the luminosity calibration. These integrated results are consistent with theoretical predictions. This analysis introduces a new method to determine the $W$-boson mass using the measured differential cross-sections corrected for detector effects. The measurement is performed on this statistically limited dataset as a proof of principle and yields \\begin{align*} m_W = 80369 \\pm 130 \\pm 33~\\text{MeV}, \\end{align*} where the first uncertainty is experimental and the second is theoretical.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2972386/1/csv","json":"https://www.hepdata.net/download/submission/ins2972386/1/json","root":"https://www.hepdata.net/download/submission/ins2972386/1/root","yaml":"https://www.hepdata.net/download/submission/ins2972386/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2972386/1/yoda","yoda-h5":"https://www.hepdata.net/download/submission/ins2972386/1/yoda.h5"}},"analyses":[],"arxiv_id":"arXiv:2509.18817","authors":["Aaij, Roel","Abdelmotteleb, Ahmed Sameh Wagih","Abellan Beteta, Carlos","Abudin\u00e9n, Fernando Jesus","Ackernley, Thomas","Adefisoye, Ayomide Matthew","Adeva, Bernardo","Adinolfi, Marco","Adlarson, Patrik Harri","Agapopoulou, Christina"],"collaborations":["LHCb"],"control_number":"165429","creation_date":"2025-09-23","data":[{"abstract":"The measured differential cross sections ($d\\sigma/dp_T$) for $W^+$. 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To combine with $W^-$, use the rows and columns ordered as $W^+$ and then $W^-$. Assume no correlation in the statistical uncertainties between $W^+$ and $W^-$ (zero entries in the off-diagonal blocks).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2972386/Statistical correlation matrix for $W^+$/csv","json":"https://www.hepdata.net/download/table/ins2972386/Statistical correlation matrix for $W^+$/json","root":"https://www.hepdata.net/download/table/ins2972386/Statistical correlation matrix for $W^+$/root","yaml":"https://www.hepdata.net/download/table/ins2972386/Statistical correlation matrix for $W^+$/yaml","yoda":"https://www.hepdata.net/download/table/ins2972386/Statistical correlation matrix for $W^+$/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2972386/Statistical correlation matrix for $W^+$/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"165503","creation_date":"2025-09-23","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["SIG"],"phrases":["Cross Section","Differential Cross Section","W --> munu differential cross section","Fiducial cross section","Transverse momentum spectrum","Statistical uncertainty","dsigma/dpT","Proton-Proton Scattering","Inclusive W production differential cross section","W signal region cross section","W boson kinematic distribution","W boson yield vs. pT","Correlation matrix","W Production","Muon channel differential cross section","W boson production cross section","W production as a function of pT"],"reactions":["W+ --> mu+ nu"]},"date":"23 Sep 2025","doc_type":"datatable","doi":"10.17182/hepdata.165429.v1/t3","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":165503,"inspire_id":"2972386","journal_info":"LHCb-PAPER-2025-031","keywords":[{"name":"reactions","synonyms":"","value":"W+ --> mu+ nu"},{"name":"observables","synonyms":"","value":"SIG"},{"name":"cmenergies","synonyms":"","value":"5020"},{"name":"phrases","synonyms":"","value":"Statistical uncertainty"},{"name":"phrases","synonyms":"","value":"Correlation matrix"},{"name":"phrases","synonyms":"","value":"Differential Cross Section"},{"name":"phrases","synonyms":"","value":"Cross Section"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"W Production"},{"name":"phrases","synonyms":"","value":"dsigma/dpT"},{"name":"phrases","synonyms":"","value":"W boson production cross section"},{"name":"phrases","synonyms":"","value":"W --> munu differential cross section"},{"name":"phrases","synonyms":"","value":"Fiducial cross section"},{"name":"phrases","synonyms":"","value":"Transverse momentum spectrum"},{"name":"phrases","synonyms":"","value":"W production as a function of pT"},{"name":"phrases","synonyms":"","value":"Inclusive W production differential cross section"},{"name":"phrases","synonyms":"","value":"W boson yield vs. pT"},{"name":"phrases","synonyms":"","value":"Muon channel differential cross section"},{"name":"phrases","synonyms":"","value":"W signal region cross section"},{"name":"phrases","synonyms":"","value":"W boson kinematic distribution"}],"last_updated":"2025-09-24T20:00:34","parent_child_join":{"name":"child_datatable","parent":"165429"},"recid":165503,"related_publication":165429,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/3962749?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/3962750?landing_page=true"}],"title":"Statistical correlation matrix for $W^+$","uuid":"55c15228-ec4a-4f78-9e23-48e90923b924"},{"abstract":"The correlation matrix corresponding to the statistical uncertainties on the differential cross-section ($d\\sigma/dp_T$) fit results for $W^-$. To combine with $W^+$ results (Fig8a), use the rows and columns ordered as $W^+$ and then $W^-$. Assume no correlation in the statistical uncertainties between $W^+$ and $W^-$ (zero entries in the off-diagonal blocks).","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2972386/Statistical correlation matrix for $W^-$/csv","json":"https://www.hepdata.net/download/table/ins2972386/Statistical correlation matrix for $W^-$/json","root":"https://www.hepdata.net/download/table/ins2972386/Statistical correlation matrix for $W^-$/root","yaml":"https://www.hepdata.net/download/table/ins2972386/Statistical correlation matrix for $W^-$/yaml","yoda":"https://www.hepdata.net/download/table/ins2972386/Statistical correlation matrix for $W^-$/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2972386/Statistical correlation matrix for $W^-$/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"165504","creation_date":"2025-09-23","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["SIG"],"phrases":["Cross 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pT"},{"name":"phrases","synonyms":"","value":"Inclusive W production differential cross section"},{"name":"phrases","synonyms":"","value":"W boson yield vs. pT"}],"last_updated":"2025-09-24T20:00:34","parent_child_join":{"name":"child_datatable","parent":"165429"},"recid":165504,"related_publication":165429,"resources":[],"title":"Statistical correlation matrix for $W^-$","uuid":"9bf9cb63-b192-479e-a9be-2b8e60017557"},{"abstract":"The correlation matrix corresponding to all of the systematic uncertainties on the differential cross-section ($d\\sigma/dp_T$) fit results for $W^+$ and $W^-$ combined together, with rows and columns ordered as $W^+$ and then $W^-$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2972386/Systematic correlation matrix for $W^{%5Cpm}$ (combined)/csv","json":"https://www.hepdata.net/download/table/ins2972386/Systematic correlation matrix for $W^{%5Cpm}$ (combined)/json","root":"https://www.hepdata.net/download/table/ins2972386/Systematic correlation matrix for $W^{%5Cpm}$ (combined)/root","yaml":"https://www.hepdata.net/download/table/ins2972386/Systematic correlation matrix for $W^{%5Cpm}$ (combined)/yaml","yoda":"https://www.hepdata.net/download/table/ins2972386/Systematic correlation matrix for $W^{%5Cpm}$ (combined)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2972386/Systematic correlation matrix for $W^{%5Cpm}$ (combined)/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"165505","creation_date":"2025-09-23","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["SIG"],"phrases":["Cross Section","Differential Cross Section","W --> munu differential cross section","Fiducial cross section","Transverse momentum spectrum","dsigma/dpT","Proton-Proton Scattering","Inclusive W production differential cross section","W signal region cross section","W boson kinematic distribution","W boson yield vs. pT","Correlation matrix","W Production","Muon channel differential cross section","W boson production cross section","Systematic uncertainty","W production as a function of pT"],"reactions":["W --> mu nu"]},"date":"23 Sep 2025","doc_type":"datatable","doi":"10.17182/hepdata.165429.v1/t5","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":165505,"inspire_id":"2972386","journal_info":"LHCb-PAPER-2025-031","keywords":[{"name":"reactions","synonyms":"","value":"W --> mu nu"},{"name":"observables","synonyms":"","value":"SIG"},{"name":"cmenergies","synonyms":"","value":"5020"},{"name":"phrases","synonyms":"","value":"Systematic uncertainty"},{"name":"phrases","synonyms":"","value":"Correlation matrix"},{"name":"phrases","synonyms":"","value":"Differential Cross Section"},{"name":"phrases","synonyms":"","value":"Cross Section"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"W Production"},{"name":"phrases","synonyms":"","value":"dsigma/dpT"},{"name":"phrases","synonyms":"","value":"W boson production cross section"},{"name":"phrases","synonyms":"","value":"W --> munu differential cross section"},{"name":"phrases","synonyms":"","value":"Fiducial cross section"},{"name":"phrases","synonyms":"","value":"Transverse momentum spectrum"},{"name":"phrases","synonyms":"","value":"W production as a function of pT"},{"name":"phrases","synonyms":"","value":"Inclusive W production differential cross section"},{"name":"phrases","synonyms":"","value":"W boson yield vs. pT"},{"name":"phrases","synonyms":"","value":"Muon channel differential cross section"},{"name":"phrases","synonyms":"","value":"W signal region cross section"},{"name":"phrases","synonyms":"","value":"W boson kinematic distribution"}],"last_updated":"2025-09-24T20:00:34","parent_child_join":{"name":"child_datatable","parent":"165429"},"recid":165505,"related_publication":165429,"resources":[{"description":"Image file","type":"png","url":"https://www.hepdata.net/record/resource/3962753?landing_page=true"},{"description":"Thumbnail image file","type":"png","url":"https://www.hepdata.net/record/resource/3962754?landing_page=true"}],"title":"Systematic correlation matrix for $W^{\\pm}$ (combined)","uuid":"3d6b56c8-615a-430f-abda-b69c042a7e7c"}],"data_abstract":"The $pp \\to W^{\\pm}(\\to \\mu^{\\pm}\\nu_{\\mu})X$ cross-sections are measured at a\nproton-proton centre-of-mass energy $\\sqrt{s} = 5.02$ TeV using a dataset\ncorresponding to an integrated luminosity of $100\\,\\mathrm{pb}^{-1}$ recorded\nby the LHCb experiment.\n\nConsidering muons in the pseudorapidity range $2.2 < \\eta < 4.4$, the\ncross-sections are measured differentially in twelve intervals of muon\ntransverse momentum between $28 < p_{T} < 52$ GeV. Integrated over $p_{T}$,\nthe measured cross-sections are\n\n$$\n  \\sigma(W^+ \\to \\mu^+\\nu_{\\mu}) = 300.9 \\pm 2.4 \\,(\\mathrm{stat})\n  \\pm 3.8 \\,(\\mathrm{syst}) \\pm 6.0 \\,(\\mathrm{lumi})\\,\\mathrm{pb},\n$$\n\n$$\n  \\sigma(W^- \\to \\mu^-\\nu_{\\mu}) = 236.9 \\pm 2.1 \\,(\\mathrm{stat})\n  \\pm 2.7 \\,(\\mathrm{syst}) \\pm 4.7 \\,(\\mathrm{lumi})\\,\\mathrm{pb}.\n$$\n\nThese integrated results are consistent with theoretical predictions.\nThis analysis introduces a new method to determine the $W$ boson mass using the\nmeasured differential cross-sections corrected for detector effects. The\nmeasurement is performed on this statistically limited dataset as a proof of\nprinciple and yields\n\n$$\n  m_W = 80369 \\pm 130 \\,(\\mathrm{exp}) \\pm 33 \\,(\\mathrm{theo})\\,\\mathrm{MeV}.\n$$\n","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["SIG"],"phrases":["Differential Cross Section","Inclusive W production differential cross section","Proton-Proton Scattering","W boson kinematic distribution","W boson production cross section","Transverse momentum spectrum","Statistical uncertainty","W signal region cross section","W boson yield vs. pT","Muon channel differential cross section","Systematic uncertainty","W production as a function of pT","Cross Section","Fiducial cross section","W --> munu differential cross section","dsigma/dpT","Uncertainties","Correlation matrix","W Production"],"reactions":["W --> mu nu","W- --> mu- nu","W+ --> mu+ nu"]},"date":"23 Sep 2025","doc_type":"publication","doi":null,"first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"hepdata_doi":"10.17182/hepdata.165429","id":165429,"inspire_id":"2972386","journal_info":"LHCb-PAPER-2025-031","keywords":[],"last_updated":"2025-09-24T20:00:35","parent_child_join":{"name":"parent_publication"},"publication_date":"2025-10-01T00:00:00","recid":165429,"resources":[{"description":"wiki page","type":"html","url":"https://gitlab.cern.ch/LHCb-QEE/ew/ew-analyses/-/wikis/W-cross-section-and-mass-studies-with-5.02-TeV-data"}],"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},{"affiliation":"Warwick U.","full_name":"Abdelmotteleb, Ahmed Sameh Wagih"},{"affiliation":"Zurich U.","full_name":"Abellan Beteta, Carlos"},{"affiliation":"Warwick U.","full_name":"Abudin\u00e9n, Fernando Jesus"},{"affiliation":"Liverpool U.","full_name":"Ackernley, Thomas"},{"affiliation":"Syracuse U.","full_name":"Adefisoye, Ayomide Matthew"},{"affiliation":"U. Santiago de Compostela (main)","full_name":"Adeva, Bernardo"},{"affiliation":"Bristol U.","full_name":"Adinolfi, Marco"},{"affiliation":"","full_name":"Adlarson, Patrik Harri"},{"affiliation":"IJCLab, Orsay","full_name":"Agapopoulou, Christina"}],"title":"Measurement of the $W \\to \u03bc\u03bd_\u03bc$ cross-sections as a function of the muon transverse momentum in $pp$ collisions at 5.02 TeV","total_tables":5,"type":["article"],"uuid":"8cd70722-d769-4e40-8287-da34d0ca621e","version":1,"year":"2025"},{"abstract":"A study on the Bose-Einstein correlations for triplets of same-sign pions is presented. The analysis is performed using proton-proton collisions at a centre-of-mass energy of $\\sqrt{s}$ = 7 TeV, recorded by the LHCb experiment, corresponding to an integrated luminosity of 1.0 fb$^{-1}$. For the first time, the results are interpreted in the core-halo model. The parameters of the model are determined in regions of charged-particle multiplicity. This measurement provides insight into the nature of hadronisation in terms of coherence, showing a coherent emission of pions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2928684/1/csv","json":"https://www.hepdata.net/download/submission/ins2928684/1/json","root":"https://www.hepdata.net/download/submission/ins2928684/1/root","yaml":"https://www.hepdata.net/download/submission/ins2928684/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2928684/1/yoda","yoda-h5":"https://www.hepdata.net/download/submission/ins2928684/1/yoda.h5"}},"analyses":[],"arxiv_id":"arXiv:2506.03072","authors":["Aaij, Roel","Abdelmotteleb, Ahmed Sameh Wagih","Abellan Beteta, Carlos","Abudin\u00e9n, Fernando Jesus","Ackernley, Thomas","Adefisoye, A.A.","Adefisoye, Ayomide Matthew","Adeva, Bernardo","Adinolfi, Marco","Adlarson, Patrik Harri"],"collaborations":["LHCb"],"control_number":"160692","creation_date":"2025-06-03","data":[{"abstract":"Results of the fit to 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Carlos"},{"affiliation":"Warwick U.","full_name":"Abudin\u00e9n, Fernando Jesus"},{"affiliation":"Liverpool U.","full_name":"Ackernley, Thomas"},{"affiliation":"Syracuse U. (main)","full_name":"Adefisoye, A.A."},{"affiliation":"Syracuse U.","full_name":"Adefisoye, Ayomide Matthew"},{"affiliation":"U. Santiago de Compostela (main)","full_name":"Adeva, Bernardo"},{"affiliation":"Bristol U.","full_name":"Adinolfi, Marco"},{"affiliation":"Uppsala U.","full_name":"Adlarson, Patrik Harri"}],"title":"Three-pion Bose-Einstein correlations measured in proton-proton collisions","total_tables":3,"type":["article"],"uuid":"3502bb9f-de50-4174-933c-07e68ae994a7","version":1,"year":"2025"},{"abstract":"The LHCb collaboration presents a novel suite of heavy-flavour jet substructure measurements at forward rapidity in proton-proton collisions at a centre-of-mass energy of $\\sqrt{s} = 13$ TeV. The jet mass is a perturbatively calculable probe of the virtuality of hard-scattered quarks and gluons, connecting small-distance quantum chromodynamics (QCD) with long-distance experimental measurement. It becomes dominated by nonperturbative corrections at small values, presenting an excellent test of QCD across a broad range of energies. Measuring heavy-flavour jet mass with a theoretically unambiguous flavour definition for the first time probes the gluon splitting mechanism for heavy-flavour production and pushes tests of perturbative QCD to unprecedented theoretical precision. Utilising the soft drop jet-grooming technique to access the perturbative jet core further enhances constraints on first-principles theory. Measurements of the jet mass for jets containing fully reconstructed $B^\\pm$ hadrons are reported with and without grooming. 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Normalization is set to unity.\n$10 < p_{\\textrm{T,jet}} < 12$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 0/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 0/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 0/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 0/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 0/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 0/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160729","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t1","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160729,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160729,"related_publication":159893,"resources":[],"title":"Table 0","uuid":"ab6472c8-9c40-47d2-807d-42cac00b8090"},{"abstract":"Groomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet,gr}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data, without any WTA flavour requirement. Normalization is set to unity.\n$12 < p_{\\textrm{T,jet}} < 15$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 1/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 1/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 1/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 1/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 1/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 1/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160730","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t2","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160730,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160730,"related_publication":159893,"resources":[],"title":"Table 1","uuid":"2628f66b-a135-447c-a62d-47bcf177bd94"},{"abstract":"Groomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet,gr}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data, without any WTA flavour requirement. 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Normalization is set to unity.\n$30 < p_{\\textrm{T,jet}} < 50$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 4/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 4/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 4/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 4/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 4/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 4/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160733","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t5","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160733,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160733,"related_publication":159893,"resources":[],"title":"Table 4","uuid":"12793f3a-66ca-4347-8a8a-2a39270d25f3"},{"abstract":"Groomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet,gr}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data, without any WTA flavour requirement. 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Normalization is set to the soft drop tagging fraction, given by the number of groomed jets (without any WTA flavour requirement) to number of ungroomed jets (without any WTA flavour requirement).\n$12 < p_{\\textrm{T,jet}} < 15$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 7/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 7/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 7/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 7/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 7/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 7/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160736","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t8","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160736,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160736,"related_publication":159893,"resources":[],"title":"Table 7","uuid":"dcaff0f4-49f2-4536-9c0a-b7d763900aa6"},{"abstract":"Groomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet,gr}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data, without any WTA flavour requirement. Normalization is set to the soft drop tagging fraction, given by the number of groomed jets (without any WTA flavour requirement) to number of ungroomed jets (without any WTA flavour requirement).\n$15 < p_{\\textrm{T,jet}} < 20$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 8/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 8/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 8/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 8/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 8/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 8/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160737","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t9","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160737,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160737,"related_publication":159893,"resources":[],"title":"Table 8","uuid":"eb2b09d6-d3df-491a-bc54-f95c3b0e4215"},{"abstract":"Groomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet,gr}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data, without any WTA flavour requirement. Normalization is set to the soft drop tagging fraction, given by the number of groomed jets (without any WTA flavour requirement) to number of ungroomed jets (without any WTA flavour requirement).\n$20 < p_{\\textrm{T,jet}} < 30$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 9/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 9/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 9/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 9/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 9/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 9/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160738","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t10","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160738,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160738,"related_publication":159893,"resources":[],"title":"Table 9","uuid":"4fb2194d-63ba-4f15-b8d7-96a0eca534e7"},{"abstract":"Groomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet,gr}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data, without any WTA flavour requirement. Normalization is set to the soft drop tagging fraction, given by the number of groomed jets (without any WTA flavour requirement) to number of ungroomed jets (without any WTA flavour requirement).\n$30 < p_{\\textrm{T,jet}} < 50$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 10/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 10/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 10/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 10/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 10/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 10/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160739","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t11","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160739,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160739,"related_publication":159893,"resources":[],"title":"Table 10","uuid":"d9e799ef-8b18-4888-8fbb-83606004ee51"},{"abstract":"Groomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet,gr}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data, without any WTA flavour requirement. Normalization is set to the soft drop tagging fraction, given by the number of groomed jets (without any WTA flavour requirement) to number of ungroomed jets (without any WTA flavour requirement).\n$50 < p_{\\textrm{T,jet}} < 100$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 11/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 11/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 11/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 11/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 11/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 11/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160740","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t12","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160740,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160740,"related_publication":159893,"resources":[],"title":"Table 11","uuid":"03f4f8d5-4325-4388-8d42-1452f19a4e49"},{"abstract":"Ungroomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data, without any WTA flavour requirement. Normalization is set to unity.\n$10 < p_{\\textrm{T,jet}} < 12$ GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 12/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 12/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 12/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 12/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 12/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 12/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160741","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t13","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160741,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160741,"related_publication":159893,"resources":[],"title":"Table 12","uuid":"0e0121c8-9d6c-481a-8698-9ff74061352d"},{"abstract":"Ungroomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data, without any WTA flavour requirement. Normalization is set to unity.\n$12 < p_{\\textrm{T,jet}} < 15$ GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 13/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 13/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 13/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 13/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 13/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 13/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160742","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t14","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160742,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160742,"related_publication":159893,"resources":[],"title":"Table 13","uuid":"55c96387-549d-45a1-a47d-796ab10867c9"},{"abstract":"Ungroomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data, without any WTA flavour requirement. Normalization is set to unity.\n$15 < p_{\\textrm{T,jet}} < 20$ GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 14/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 14/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 14/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 14/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 14/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 14/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160743","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t15","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160743,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160743,"related_publication":159893,"resources":[],"title":"Table 14","uuid":"4be06624-34cf-4e9a-8b70-a68ecf382338"},{"abstract":"Ungroomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data, without any WTA flavour requirement. Normalization is set to unity.\n$20 < p_{\\textrm{T,jet}} < 30$ GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 15/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 15/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 15/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 15/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 15/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 15/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160744","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t16","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160744,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160744,"related_publication":159893,"resources":[],"title":"Table 15","uuid":"b2fc921b-1dd0-4067-bf9f-5ba50df7c841"},{"abstract":"Ungroomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data, without any WTA flavour requirement. Normalization is set to unity.\n$30 < p_{\\textrm{T,jet}} < 50$ GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 16/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 16/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 16/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 16/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 16/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 16/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160745","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t17","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160745,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160745,"related_publication":159893,"resources":[],"title":"Table 16","uuid":"3a61e43e-0d64-4724-b255-840ef3d4a881"},{"abstract":"Ungroomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data, without any WTA flavour requirement. Normalization is set to unity.\n$50 < p_{\\textrm{T,jet}} < 100$ GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 17/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 17/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 17/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 17/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 17/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 17/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160746","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t18","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160746,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160746,"related_publication":159893,"resources":[],"title":"Table 17","uuid":"5fc97e31-2030-4f5b-9d6b-094d408272c0"},{"abstract":"Groomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet,gr}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to the WTA tagging fraction, given by the number of (groomed) jets tagged with WTA flavour to number of (groomed) jets without WTA flavour tagging.\n$10 < p_{\\textrm{T,jet}} < 12$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 18/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 18/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 18/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 18/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 18/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 18/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160747","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t19","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160747,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160747,"related_publication":159893,"resources":[],"title":"Table 18","uuid":"c64d9425-dcd3-4e83-ab67-228df420b820"},{"abstract":"Groomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet,gr}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to the WTA tagging fraction, given by the number of (groomed) jets tagged with WTA flavour to number of (groomed) jets without WTA flavour tagging.\n$12 < p_{\\textrm{T,jet}} < 15$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 19/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 19/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 19/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 19/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 19/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 19/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160748","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t20","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160748,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160748,"related_publication":159893,"resources":[],"title":"Table 19","uuid":"96a38eba-298f-4b9f-a2ff-5a4cfb85ee00"},{"abstract":"Groomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet,gr}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to the WTA tagging fraction, given by the number of (groomed) jets tagged with WTA flavour to number of (groomed) jets without WTA flavour tagging.\n$15 < p_{\\textrm{T,jet}} < 20$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 20/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 20/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 20/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 20/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 20/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 20/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160749","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t21","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160749,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160749,"related_publication":159893,"resources":[],"title":"Table 20","uuid":"ac01868c-17c3-40be-8661-65e9b4e33ef6"},{"abstract":"Groomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet,gr}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to the WTA tagging fraction, given by the number of (groomed) jets tagged with WTA flavour to number of (groomed) jets without WTA flavour tagging.\n$20 < p_{\\textrm{T,jet}} < 30$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 21/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 21/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 21/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 21/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 21/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 21/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160750","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t22","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160750,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160750,"related_publication":159893,"resources":[],"title":"Table 21","uuid":"ad3eda9d-91c1-49c0-95c1-3da16c360320"},{"abstract":"Groomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet,gr}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to the WTA tagging fraction, given by the number of (groomed) jets tagged with WTA flavour to number of (groomed) jets without WTA flavour tagging.\n$30 < p_{\\textrm{T,jet}} < 50$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 22/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 22/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 22/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 22/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 22/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 22/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160751","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t23","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160751,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160751,"related_publication":159893,"resources":[],"title":"Table 22","uuid":"895d57fa-17a4-4e12-904a-ccada1c615c9"},{"abstract":"Groomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet,gr}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to the WTA tagging fraction, given by the number of (groomed) jets tagged with WTA flavour to number of (groomed) jets without WTA flavour tagging.\n$50 < p_{\\textrm{T,jet}} < 100$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 23/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 23/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 23/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 23/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 23/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 23/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160752","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t24","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160752,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160752,"related_publication":159893,"resources":[],"title":"Table 23","uuid":"7025f45d-3ea5-48c3-b106-b49af8890f83"},{"abstract":"Groomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet,gr}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to the soft drop tagging fraction, given by the number of groomed jets (tagged with WTA flavour) to number of ungroomed jets (tagged with WTA flavour).\n$10 < p_{\\textrm{T,jet}} < 12$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 24/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 24/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 24/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 24/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 24/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 24/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160753","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t25","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160753,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160753,"related_publication":159893,"resources":[],"title":"Table 24","uuid":"f0923693-b456-41da-a4b1-178439597092"},{"abstract":"Groomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet,gr}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to the soft drop tagging fraction, given by the number of groomed jets (tagged with WTA flavour) to number of ungroomed jets (tagged with WTA flavour).\n$12 < p_{\\textrm{T,jet}} < 15$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 25/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 25/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 25/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 25/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 25/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 25/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160754","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t26","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160754,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160754,"related_publication":159893,"resources":[],"title":"Table 25","uuid":"38c2a8c6-6ab6-440a-ae66-bb83a58f4ce8"},{"abstract":"Groomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet,gr}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to the soft drop tagging fraction, given by the number of groomed jets (tagged with WTA flavour) to number of ungroomed jets (tagged with WTA flavour).\n$15 < p_{\\textrm{T,jet}} < 20$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 26/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 26/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 26/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 26/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 26/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 26/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160755","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t27","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160755,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160755,"related_publication":159893,"resources":[],"title":"Table 26","uuid":"2f4e967b-e6b8-4f9b-9b19-c4fa9ae5d11c"},{"abstract":"Groomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet,gr}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to the soft drop tagging fraction, given by the number of groomed jets (tagged with WTA flavour) to number of ungroomed jets (tagged with WTA flavour).\n$20 < p_{\\textrm{T,jet}} < 30$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 27/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 27/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 27/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 27/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 27/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 27/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160756","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t28","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160756,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160756,"related_publication":159893,"resources":[],"title":"Table 27","uuid":"624021f0-1197-494a-a2c9-21901ff8cf87"},{"abstract":"Groomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet,gr}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to the soft drop tagging fraction, given by the number of groomed jets (tagged with WTA flavour) to number of ungroomed jets (tagged with WTA flavour).\n$30 < p_{\\textrm{T,jet}} < 50$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 28/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 28/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 28/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 28/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 28/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 28/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160757","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t29","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160757,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160757,"related_publication":159893,"resources":[],"title":"Table 28","uuid":"9f2240ae-8efb-4ae8-9d14-4dc0a37f8583"},{"abstract":"Groomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet,gr}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to the soft drop tagging fraction, given by the number of groomed jets (tagged with WTA flavour) to number of ungroomed jets (tagged with WTA flavour).\n$50 < p_{\\textrm{T,jet}} < 100$ GeV, soft drop $z_{\\textrm{cut}}=0.1, \\beta=0$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 29/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 29/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 29/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 29/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 29/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 29/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160758","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t30","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160758,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160758,"related_publication":159893,"resources":[],"title":"Table 29","uuid":"d0e73361-8e33-4c88-9c36-a4afe3b696cf"},{"abstract":"Ungroomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to the WTA tagging fraction, given by the number of (ungroomed) jets tagged with WTA flavour to number of (ungroomed) jets without WTA flavour tagging.\n$10 < p_{\\textrm{T,jet}} < 12$ GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 30/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 30/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 30/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 30/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 30/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 30/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160759","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t31","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160759,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160759,"related_publication":159893,"resources":[],"title":"Table 30","uuid":"7ccb0c44-1f61-4794-a5e8-dbab4ee90bc0"},{"abstract":"Ungroomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. 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Normalization is set to the WTA tagging fraction, given by the number of (ungroomed) jets tagged with WTA flavour to number of (ungroomed) jets without WTA flavour tagging.\n$15 < p_{\\textrm{T,jet}} < 20$ GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 32/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 32/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 32/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 32/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 32/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 32/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160761","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t33","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160761,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160761,"related_publication":159893,"resources":[],"title":"Table 32","uuid":"e72ae996-1a06-42d6-9379-f361b0ca1a12"},{"abstract":"Ungroomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to the WTA tagging fraction, given by the number of (ungroomed) jets tagged with WTA flavour to number of (ungroomed) jets without WTA flavour tagging.\n$20 < p_{\\textrm{T,jet}} < 30$ GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 33/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 33/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 33/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 33/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 33/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 33/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160762","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t34","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160762,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160762,"related_publication":159893,"resources":[],"title":"Table 33","uuid":"041b68f0-37a7-4495-9aa9-0a5367c0d8a5"},{"abstract":"Ungroomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to the WTA tagging fraction, given by the number of (ungroomed) jets tagged with WTA flavour to number of (ungroomed) jets without WTA flavour tagging.\n$30 < p_{\\textrm{T,jet}} < 50$ GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 34/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 34/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 34/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 34/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 34/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 34/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160763","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t35","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160763,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160763,"related_publication":159893,"resources":[],"title":"Table 34","uuid":"6063eb98-b948-4665-8746-fd89ff1edb02"},{"abstract":"Ungroomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to the WTA tagging fraction, given by the number of (ungroomed) jets tagged with WTA flavour to number of (ungroomed) jets without WTA flavour tagging.\n$50 < p_{\\textrm{T,jet}} < 100$ GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 35/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 35/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 35/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 35/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 35/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 35/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160764","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t36","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160764,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160764,"related_publication":159893,"resources":[],"title":"Table 35","uuid":"60f75e6e-a168-457f-9559-13d653e9b7b2"},{"abstract":"Ungroomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to unity.\n$10 < p_{\\textrm{T,jet}} < 12$ GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 36/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 36/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 36/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 36/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 36/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 36/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160765","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t37","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160765,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160765,"related_publication":159893,"resources":[],"title":"Table 36","uuid":"f950a3f3-43cf-48e3-a54a-8d048c2f9d68"},{"abstract":"Ungroomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to unity.\n$12 < p_{\\textrm{T,jet}} < 15$ GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 37/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 37/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 37/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 37/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 37/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 37/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160766","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t38","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160766,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160766,"related_publication":159893,"resources":[],"title":"Table 37","uuid":"b232cd0c-5936-4233-8b33-f2f893a794f1"},{"abstract":"Ungroomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to unity.\n$15 < p_{\\textrm{T,jet}} < 20$ GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 38/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 38/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 38/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 38/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 38/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 38/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160767","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t39","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160767,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160767,"related_publication":159893,"resources":[],"title":"Table 38","uuid":"d0a8a455-3e12-4513-aec4-de3e07205448"},{"abstract":"Ungroomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to unity.\n$20 < p_{\\textrm{T,jet}} < 30$ GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 39/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 39/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 39/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 39/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 39/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 39/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160768","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t40","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160768,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160768,"related_publication":159893,"resources":[],"title":"Table 39","uuid":"3813fcaf-9544-49a3-9837-5aac29c18274"},{"abstract":"Ungroomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to unity.\n$30 < p_{\\textrm{T,jet}} < 50$ GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 40/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 40/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 40/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 40/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 40/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 40/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160769","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t41","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160769,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160769,"related_publication":159893,"resources":[],"title":"Table 40","uuid":"958bb2cc-7aea-4b29-9f4c-7f12a88206f5"},{"abstract":"Ungroomed $B^\\pm$-tagged jet invariant mass $m_{\\textrm{jet}}/p_{\\textrm{T,jet}}$ for $R=0.5$ jets reconstructed in pp data tagged with WTA flavour. Normalization is set to unity.\n$50 < p_{\\textrm{T,jet}} < 100$ GeV.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2922449/Table 41/csv","json":"https://www.hepdata.net/download/table/ins2922449/Table 41/json","root":"https://www.hepdata.net/download/table/ins2922449/Table 41/root","yaml":"https://www.hepdata.net/download/table/ins2922449/Table 41/yaml","yoda":"https://www.hepdata.net/download/table/ins2922449/Table 41/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2922449/Table 41/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"160770","creation_date":"2025-05-17","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"datatable","doi":"10.17182/hepdata.159893.v1/t42","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":160770,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[{"name":"reactions","synonyms":"","value":"P P --> B+/B- jet X"},{"name":"cmenergies","synonyms":"","value":"13000."}],"last_updated":"2025-08-05T15:33:58","parent_child_join":{"name":"child_datatable","parent":"159893"},"recid":160770,"related_publication":159893,"resources":[],"title":"Table 41","uuid":"b789a279-75d0-45e1-866a-fb88b49953ec"}],"data_abstract":"","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"reactions":["P P --> B+/B- jet X"]},"date":"17 May 2025","doc_type":"publication","doi":"10.1016/j.physletb.2025.139854","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"hepdata_doi":"10.17182/hepdata.159893","id":159893,"inspire_id":"2922449","journal_info":"Phys.Lett.B 869 (2025) 139854","keywords":[],"last_updated":"2025-08-05T15:34:03","parent_child_join":{"name":"parent_publication"},"publication_date":"2025-11-06T00:00:00","recid":159893,"resources":[{"description":"web page with auxiliary material","type":"html","url":"https://lbfence.cern.ch/alcm/public/analysis/full-details/4555"},{"description":"Created with hepdata_lib 0.17.0","type":"zenodo","url":"https://doi.org/10.5281/zenodo.1217998"}],"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},{"affiliation":"Warwick U.","full_name":"Abdelmotteleb, Ahmed Sameh Wagih"},{"affiliation":"Zurich U.","full_name":"Abellan Beteta, Carlos"},{"affiliation":"Warwick U.","full_name":"Abudin\u00e9n, Fernando Jesus"},{"affiliation":"Liverpool U.","full_name":"Ackernley, Thomas"},{"affiliation":"Syracuse U.","full_name":"Adefisoye, Ayomide Matthew"},{"affiliation":"U. 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The integrated cross-section results are \\begin{equation*} \\sigma_{J/\\psi\\to\\mu^+\\mu^-}(2.0<y_{J/\\psi}<4.5,2.0<\\eta_{\\mu^\\pm} < 4.5) = 400 \\pm 2 \\pm 5 \\pm 12 \\,{\\rm pb}\\,, \\end{equation*}\\begin{equation*} \\sigma_{\\psi(2S)\\to\\mu^+\\mu^-}(2.0<y_{\\psi(2S)}<4.5,2.0<\\eta_{\\mu^\\pm} < 4.5) = 9.40 \\pm 0.15 \\pm 0.13 \\pm 0.27 \\,{\\rm pb}\\,, \\end{equation*} where the uncertainties are statistical, systematic and due to the luminosity determination. In addition, a measurement of the ratio of $\\psi(2S)$ and $J/\\psi$ cross-sections, at an average photon-proton centre-of-mass energy of 1 TeV, is performed, giving \\begin{equation*} \\frac{\\sigma_{\\psi(2S)}}{\\sigma_{J/\\psi}} = 0.1763 \\pm 0.0029 \\pm 0.0008 \\pm 0.0039 \\,, \\end{equation*} where the first uncertainty is statistical, the second systematic and the third due to the knowledge of the involved branching fractions. For the first time, the dependence of the $J/\\psi$ and $\\psi(2S)$ cross-sections on the total transverse momentum transfer is determined in $pp$ collisions and is found consistent with the behaviour observed in electron-proton collisions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2825384/1/csv","json":"https://www.hepdata.net/download/submission/ins2825384/1/json","root":"https://www.hepdata.net/download/submission/ins2825384/1/root","yaml":"https://www.hepdata.net/download/submission/ins2825384/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2825384/1/yoda","yoda-h5":"https://www.hepdata.net/download/submission/ins2825384/1/yoda.h5"}},"analyses":[],"arxiv_id":"arXiv:2409.03496","authors":["Aaij, Roel","Abdelmotteleb, Ahmed Sameh Wagih","Abellan Beteta, Carlos","Abudin\u00e9n, Fernando Jesus","Ackernley, Thomas","Adefisoye, Ayomide Matthew","Adeva, Bernardo","Adinolfi, Marco","Adlarson, Patrik Harri","Agapopoulou, Christina"],"collaborations":["LHCb"],"control_number":"167228","creation_date":"2024-09-05","data":[{"abstract":"Differential CEP $J/\\psi\\to\\mu^+\\mu^-$ cross-sections corrected for efficiency, acceptance and branching fraction. The systematic uncertainties are split between those uncorrelated across $y$ ranges, those that are 100% correlated and the luminosity uncertainty.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2825384/Table 4/csv","json":"https://www.hepdata.net/download/table/ins2825384/Table 4/json","root":"https://www.hepdata.net/download/table/ins2825384/Table 4/root","yaml":"https://www.hepdata.net/download/table/ins2825384/Table 4/yaml","yoda":"https://www.hepdata.net/download/table/ins2825384/Table 4/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2825384/Table 4/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"167811","creation_date":"2024-09-05","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Photoproduction","Central exclusive production","J/psi production"],"reactions":["P P --> JPSI <MU+ MU->"]},"date":"05 Sep 2024","doc_type":"datatable","doi":"10.17182/hepdata.167228.v1/t1","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":167811,"inspire_id":"2825384","journal_info":"SciPost Phys. 18 (2025) 071","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> JPSI <MU+ MU->"},{"name":"phrases","synonyms":"","value":"Central exclusive production"},{"name":"phrases","synonyms":"","value":"J/psi production"},{"name":"phrases","synonyms":"","value":"Photoproduction"}],"last_updated":"2026-01-15T12:36:39","parent_child_join":{"name":"child_datatable","parent":"167228"},"recid":167811,"related_publication":167228,"resources":[],"title":"Table 4","uuid":"ed204978-9e15-4d21-a2ac-a24e700e9880"},{"abstract":"Differential CEP $\\psi(2S)\\to\\mu^+\\mu^-$ cross-sections corrected for efficiency, acceptance and branching fraction. The systematic uncertainties are split between those uncorrelated across $y$ ranges, those that are 100% correlated and the luminosity uncertainty.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2825384/Table 5/csv","json":"https://www.hepdata.net/download/table/ins2825384/Table 5/json","root":"https://www.hepdata.net/download/table/ins2825384/Table 5/root","yaml":"https://www.hepdata.net/download/table/ins2825384/Table 5/yaml","yoda":"https://www.hepdata.net/download/table/ins2825384/Table 5/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2825384/Table 5/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"167812","creation_date":"2024-09-05","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["psi(2S) production","Photoproduction","Central exclusive production"],"reactions":["P P --> PSI(2S) <MU+ MU->"]},"date":"05 Sep 2024","doc_type":"datatable","doi":"10.17182/hepdata.167228.v1/t2","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":167812,"inspire_id":"2825384","journal_info":"SciPost Phys. 18 (2025) 071","keywords":[{"name":"cmenergies","synonyms":"","value":"13000"},{"name":"reactions","synonyms":"","value":"P P --> PSI(2S) <MU+ MU->"},{"name":"phrases","synonyms":"","value":"Central exclusive production"},{"name":"phrases","synonyms":"","value":"psi(2S) production"},{"name":"phrases","synonyms":"","value":"Photoproduction"}],"last_updated":"2026-01-15T12:36:39","parent_child_join":{"name":"child_datatable","parent":"167228"},"recid":167812,"related_publication":167228,"resources":[],"title":"Table 5","uuid":"3cd45828-1129-46bd-95df-0b5f5ab17ae9"},{"abstract":"Ratio of differential CEP $\\psi(2S)\\to\\mu^+\\mu^-$ to $J/\\psi\\to\\mu^+\\mu^-$ cross-sections corrected for efficiency, acceptance and branching fraction. The systematic uncertainties are split between those uncorrelated across $y$ ranges, those that are 100% correlated.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2825384/Table 6/csv","json":"https://www.hepdata.net/download/table/ins2825384/Table 6/json","root":"https://www.hepdata.net/download/table/ins2825384/Table 6/root","yaml":"https://www.hepdata.net/download/table/ins2825384/Table 6/yaml","yoda":"https://www.hepdata.net/download/table/ins2825384/Table 6/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2825384/Table 6/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"167813","creation_date":"2024-09-05","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["psi(2S) production","Photoproduction","Central exclusive production","J/psi production"],"reactions":["P P --> JPSI <MU+ MU->","P P --> PSI(2S) <MU+ MU->"]},"date":"05 Sep 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momentum squared","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2825384/Table 7(left)/csv","json":"https://www.hepdata.net/download/table/ins2825384/Table 7(left)/json","root":"https://www.hepdata.net/download/table/ins2825384/Table 7(left)/root","yaml":"https://www.hepdata.net/download/table/ins2825384/Table 7(left)/yaml","yoda":"https://www.hepdata.net/download/table/ins2825384/Table 7(left)/yoda","yoda-h5":"https://www.hepdata.net/download/table/ins2825384/Table 7(left)/yoda.h5"}},"authors":null,"collaborations":["LHCb"],"control_number":"167814","creation_date":"2024-09-05","data_keywords":{"cmenergies":[{"gte":13000.0,"lte":13000.0}],"phrases":["Photoproduction","Central exclusive production","J/psi production","Regge theory"],"reactions":["P P --> JPSI <MU+ MU->"]},"date":"05 Sep 2024","doc_type":"datatable","doi":"10.17182/hepdata.167228.v1/t4","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, 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The $\u03c7_{c0}(4500)$ state is observed with a significance over $6\u03c3$ and the $\u03c7_{c1}(4274)$ is confirmed with a significance of more than $4\u03c3$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2809344/1/csv","json":"https://www.hepdata.net/download/submission/ins2809344/1/json","root":"https://www.hepdata.net/download/submission/ins2809344/1/root","yaml":"https://www.hepdata.net/download/submission/ins2809344/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2809344/1/yoda","yoda-h5":"https://www.hepdata.net/download/submission/ins2809344/1/yoda.h5"}},"analyses":[],"arxiv_id":"arXiv:2407.14301","authors":["Aaij, Roel","Abdelmotteleb, Ahmed Sameh Wagih","Abellan Beteta, Carlos","Abudin\u00e9n, Fernando Jesus","Ackernley, Thomas","Adefisoye, A.A.","Adefisoye, Ayomide Matthew","Adeva, Bernardo","Adinolfi, Marco","Adlarson, Patrik 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The model used also accounts for nonlocal contributions from $B^{0}\\to K^{*0}\\left[\\tau^+\\tau^-\\to \\mu^+\\mu^-\\right]$ rescattering, resulting in the first direct measurement of the $b s\\tau\\tau$ vector effective-coupling $C_{9\\tau}$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2795535/1/csv","json":"https://www.hepdata.net/download/submission/ins2795535/1/json","root":"https://www.hepdata.net/download/submission/ins2795535/1/root","yaml":"https://www.hepdata.net/download/submission/ins2795535/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2795535/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2405.17347","authors":["Aaij, Roel","Abdelmotteleb, Ahmed Sameh Wagih","Abellan Beteta, Carlos","Abudin\u00e9n, Fernando Jesus","Ackernley, Thomas","Adefisoye, A.A.","Adeva, Bernardo","Adinolfi, Marco","Adlarson, Patrik Harri","Agapopoulou, Christina"],"collaborations":["LHCb"],"control_number":"161096","creation_date":"2024-05-27","data":[{"abstract":"Signal parameter results. 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The analysis is based on $pp$ collision data corresponding to an integrated luminosity of 8.4\\,$\\rm{fb}^{-1}$ collected by the LHCb experiment. This measurement employs for the first time a model of both one-particle and two-particle nonlocal amplitudes, and utilises the complete dimuon mass spectrum without any veto regions around the narrow charmonium resonances. In this way it is possible to explicitly isolate the local and nonlocal contributions and capture the interference between them. The results show that interference with nonlocal contributions, although larger than predicted, only has a minor impact on the Wilson Coefficients determined from the fit to the data. For the local contributions, the Wilson Coefficient $\\mathcal{C}_9$, responsible for vector dimuon currents, exhibits a $2.1\\sigma$ deviation from the Standard Model expectation. The Wilson Coefficients $\\mathcal{C}_{10}$, $\\mathcal{C}^{'}_9$ and $\\mathcal{C}^{'}_{10}$ are all in better agreement than $\\mathcal{C}_9$ with the Standard Model and the global significance is at the level of $1.5\\sigma$. The model used also accounts for nonlocal contributions from $B^{0}\\to K^{*0}\\left[\\tau^+\\tau^-\\to \\mu^+\\mu^-\\right]$ rescattering, resulting in the first direct measurement of the $b s\\tau\\tau$ vector effective-coupling $\\mathcal{C}_{9\\tau}$.","data_keywords":{"cmenergies":[],"phrases":["Weak Effective Theory","LHCb","Form factors","Amplitudes","Nonlocal","Wilson Coefficients"],"reactions":["$B^0 \\to K^{*0} \\mu^+ \\mu^-$","$b \\to s \\ell^+ \\ell^-$"]},"date":"27 May 2024","doc_type":"publication","doi":"10.1007/JHEP09(2024)026","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"hepdata_doi":"10.17182/hepdata.161096","id":161096,"inspire_id":"2795535","journal_info":"JHEP 09 (2024) 026","keywords":[{"source":"author","value":"B Physics"},{"source":"author","value":"Flavour Changing Neutral Currents"},{"source":"author","value":"Flavour Physics"},{"source":"author","value":"Hadron-Hadron Scattering"},{"schema":"INSPIRE","value":"p p: scattering"},{"schema":"INSPIRE","value":"p p: colliding beams"},{"schema":"INSPIRE","value":"B0: semileptonic decay"},{"schema":"INSPIRE","value":"K*(892): hadronic decay"},{"schema":"INSPIRE","value":"muon: pair production"},{"schema":"INSPIRE","value":"dimuon: mass spectrum"},{"schema":"INSPIRE","value":"mass spectrum: (muon+ muon-)"},{"schema":"INSPIRE","value":"form factor: nonlocal"},{"schema":"INSPIRE","value":"interference"},{"schema":"INSPIRE","value":"charmonium"},{"schema":"INSPIRE","value":"narrow resonance"},{"schema":"INSPIRE","value":"Wilson"},{"schema":"INSPIRE","value":"LHC-B"},{"schema":"INSPIRE","value":"CERN LHC Coll"},{"schema":"INSPIRE","value":"two-particle"},{"schema":"INSPIRE","value":"one-particle"},{"schema":"INSPIRE","value":"phase space"},{"schema":"INSPIRE","value":"data analysis method"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"B0 --> K*(892) muon+ muon-"},{"schema":"INSPIRE","value":"K*(892) --> K+ pi-"},{"schema":"INSPIRE","value":"7000 GeV-cms"},{"schema":"INSPIRE","value":"8000 GeV-cms"},{"schema":"INSPIRE","value":"13000 GeV-cms"}],"last_updated":"2025-08-20T16:39:18","parent_child_join":{"name":"parent_publication"},"publication_date":"2024-08-20T00:00:00","recid":161096,"resources":[{"description":"Created with hepdata_lib 0.17.0","type":"zenodo","url":"https://doi.org/10.5281/zenodo.1217998"},{"description":"All figures and tables, along with any supplementary material and additional information, are available at this https URL (LHCb public pages)","type":"html","url":"https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2024-011.html"},{"description":"Additional information including table relating textual parameter names to the corresponding published parameter symbols.","type":"pdf","url":"https://www.hepdata.net/record/resource/3947668?landing_page=true"},{"description":"arXiv","type":"html","url":"https://arxiv.org/abs/2405.17347"},{"description":"CDS","type":"html","url":"https://cds.cern.ch/search?ln=en&p=LHCB-PAPER-2024-011&c=LHCb+Papers"}],"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},{"affiliation":"Warwick U.","full_name":"Abdelmotteleb, Ahmed Sameh Wagih"},{"affiliation":"Zurich U.","full_name":"Abellan Beteta, Carlos"},{"affiliation":"Warwick U.","full_name":"Abudin\u00e9n, Fernando Jesus"},{"affiliation":"Liverpool U.","full_name":"Ackernley, Thomas"},{"affiliation":"Syracuse U.","full_name":"Adefisoye, A.A."},{"affiliation":"U. Santiago de Compostela (main)","full_name":"Adeva, Bernardo"},{"affiliation":"Bristol U.","full_name":"Adinolfi, Marco"},{"affiliation":"Uppsala U.","full_name":"Adlarson, Patrik Harri"},{"affiliation":"IJCLab, Orsay","full_name":"Agapopoulou, Christina"}],"title":"Comprehensive analysis of local and nonlocal amplitudes in the $B^0\\rightarrow K^{*0}\\mu^+\\mu^-$ decay","total_tables":3,"type":["article"],"uuid":"89db3027-4892-4a25-8abb-434879581689","version":1,"year":"2024"},{"abstract":"The first measurement of the $Z$ boson production cross-section at centre-of-mass energy $\\sqrt{s} = 5.02\\,$TeV in the forward region is reported, using $pp$ collision data collected by the LHCb experiment in year 2017, corresponding to an integrated luminosity of $100 \\pm 2\\,\\rm{pb^{-1}}$. The production cross-section is measured for final-state muons in the pseudorapidity range $2.0<\\eta<4.5$ with transverse momentum $p_{\\rm{T}}> 20\\,\\rm{GeV/}\\it{c}$. The integrated cross-section is determined to be \n\\[ \\sigma_{Z \\rightarrow \\mu^{+}\\mu^{-}} = 39.6 \\pm 0.7\\,(\\rm{stat}) \\pm 0.6\\,(\\rm{syst}) \\pm 0.8\\,(\\rm{lumi}) \\ \\rm{pb} \\]\n for the di-muon invariant mass in the range $60<M_{\\mu\\mu}<120\\,\\rm{GeV/}\\it{c^{2}}$. This result and the differential cross-section results are in good agreement with theoretical predictions at next-to-next-to-leading order in the strong coupling. Based on a previous LHCb measurement of the $Z$ boson production cross-section in $p$Pb collisions at $\\sqrt{s_{NN}}=5.02$ TeV, the nuclear modification factor $R_{p\\rm{Pb}}$ is measured for the first time at this energy. The measured values are $1.2^{+0.5}_{-0.3}\\,(\\rm{stat}) \\pm 0.1\\,(\\rm{syst})$ in the forward region ($1.53<y^*_{\\mu}<4.03$) and $3.6^{+1.6}_{-0.9}\\,(\\rm{stat}) \\pm 0.2\\,(\\rm{syst})$ in the backward region ($-4.97<y^*_{\\mu}<-2.47$), where $y^*_{\\mu}$ represents the muon rapidity in the centre-of-mass frame.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2690798/2/csv","json":"https://www.hepdata.net/download/submission/ins2690798/2/json","root":"https://www.hepdata.net/download/submission/ins2690798/2/root","yaml":"https://www.hepdata.net/download/submission/ins2690798/2/yaml","yoda":"https://www.hepdata.net/download/submission/ins2690798/2/yoda"}},"analyses":[],"arxiv_id":"arXiv:2308.12940","authors":["Aaij, Roel","Abdelmotteleb, Ahmed Sameh Wagih","Abellan Beteta, Carlos","Abudin\u00e9n, Fernando Jesus","Ackernley, Thomas","Adeva, Bernardo","Adinolfi, Marco","Adlarson, Patrik Harri","Afsharnia, Hossein","Agapopoulou, 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percentage.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2690798/Table8/csv","json":"https://www.hepdata.net/download/table/ins2690798/Table8/json","root":"https://www.hepdata.net/download/table/ins2690798/Table8/root","yaml":"https://www.hepdata.net/download/table/ins2690798/Table8/yaml","yoda":"https://www.hepdata.net/download/table/ins2690798/Table8/yoda"}},"authors":null,"collaborations":["LHCb"],"control_number":"154900","creation_date":"2023-08-24","data_keywords":{"cmenergies":[],"observables":["Closure","Background","FSR","Calibration","Migration","Efficiency"]},"date":"24 Aug 2023","doc_type":"datatable","doi":"10.17182/hepdata.147274.v2/t2","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":154900,"inspire_id":"2690798","journal_info":"JHEP 02 (2024) 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The first uncertainty is statistical, the second systematic, and the third is from the uncertainty on the integrated luminosity.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2690798/Table10/csv","json":"https://www.hepdata.net/download/table/ins2690798/Table10/json","root":"https://www.hepdata.net/download/table/ins2690798/Table10/root","yaml":"https://www.hepdata.net/download/table/ins2690798/Table10/yaml","yoda":"https://www.hepdata.net/download/table/ins2690798/Table10/yoda"}},"authors":null,"collaborations":["LHCb"],"control_number":"154902","creation_date":"2023-08-24","data_keywords":{"cmenergies":[],"observables":["differential cross-section"],"reactions":["P P --> Z0/gamma* --> mu+ mu-"]},"date":"24 Aug 2023","doc_type":"datatable","doi":"10.17182/hepdata.147274.v2/t4","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":154902,"inspire_id":"2690798","journal_info":"JHEP 02 (2024) 070","keywords":[{"name":"observables","synonyms":"","value":"differential cross-section"},{"name":"reactions","synonyms":"","value":"P P --> Z0/gamma* --> mu+ mu-"}],"last_updated":"2024-10-17T12:44:56","parent_child_join":{"name":"child_datatable","parent":"147274"},"recid":154902,"related_publication":147274,"resources":[],"title":"Table10","uuid":"135b9647-774e-4ba8-8faa-63b9373d7370"},{"abstract":"Measured single differential cross-sections in bins of $p_{T}^{Z}$. The first uncertainty is statistical, the second systematic, and the third is due to the luminosity.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2690798/Table11/csv","json":"https://www.hepdata.net/download/table/ins2690798/Table11/json","root":"https://www.hepdata.net/download/table/ins2690798/Table11/root","yaml":"https://www.hepdata.net/download/table/ins2690798/Table11/yaml","yoda":"https://www.hepdata.net/download/table/ins2690798/Table11/yoda"}},"authors":null,"collaborations":["LHCb"],"control_number":"154903","creation_date":"2023-08-24","data_keywords":{"cmenergies":[],"observables":["differential cross-section"],"reactions":["P P --> Z0/gamma* --> mu+ mu-"]},"date":"24 Aug 2023","doc_type":"datatable","doi":"10.17182/hepdata.147274.v2/t5","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":154903,"inspire_id":"2690798","journal_info":"JHEP 02 (2024) 070","keywords":[{"name":"observables","synonyms":"","value":"differential cross-section"},{"name":"reactions","synonyms":"","value":"P P --> Z0/gamma* --> mu+ mu-"}],"last_updated":"2024-10-17T12:44:56","parent_child_join":{"name":"child_datatable","parent":"147274"},"recid":154903,"related_publication":147274,"resources":[],"title":"Table11","uuid":"a4f9909b-a9bb-40c5-a6b0-353cbff11ab9"},{"abstract":"Measured single differential cross-sections in bins of $\\phi_{\\eta}^{*}$. The first uncertainty is statistical, the second systematic, and the third is due to the luminosity.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2690798/Table12/csv","json":"https://www.hepdata.net/download/table/ins2690798/Table12/json","root":"https://www.hepdata.net/download/table/ins2690798/Table12/root","yaml":"https://www.hepdata.net/download/table/ins2690798/Table12/yaml","yoda":"https://www.hepdata.net/download/table/ins2690798/Table12/yoda"}},"authors":null,"collaborations":["LHCb"],"control_number":"154904","creation_date":"2023-08-24","data_keywords":{"cmenergies":[],"observables":["differential cross-section"],"reactions":["P P --> Z0/gamma* --> mu+ mu-"]},"date":"24 Aug 2023","doc_type":"datatable","doi":"10.17182/hepdata.147274.v2/t6","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":154904,"inspire_id":"2690798","journal_info":"JHEP 02 (2024) 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measurement.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2690798/Table13/csv","json":"https://www.hepdata.net/download/table/ins2690798/Table13/json","root":"https://www.hepdata.net/download/table/ins2690798/Table13/root","yaml":"https://www.hepdata.net/download/table/ins2690798/Table13/yaml","yoda":"https://www.hepdata.net/download/table/ins2690798/Table13/yoda"}},"authors":null,"collaborations":["LHCb"],"control_number":"154905","creation_date":"2023-08-24","data_keywords":{"cmenergies":[]},"date":"24 Aug 2023","doc_type":"datatable","doi":"10.17182/hepdata.147274.v2/t7","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":154905,"inspire_id":"2690798","journal_info":"JHEP 02 (2024) 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measurement.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2690798/Table16/csv","json":"https://www.hepdata.net/download/table/ins2690798/Table16/json","root":"https://www.hepdata.net/download/table/ins2690798/Table16/root","yaml":"https://www.hepdata.net/download/table/ins2690798/Table16/yaml","yoda":"https://www.hepdata.net/download/table/ins2690798/Table16/yoda"}},"authors":null,"collaborations":["LHCb"],"control_number":"154908","creation_date":"2023-08-24","data_keywords":{"cmenergies":[]},"date":"24 Aug 2023","doc_type":"datatable","doi":"10.17182/hepdata.147274.v2/t10","first_author":{"affiliation":"Nikhef, Amsterdam","full_name":"Aaij, Roel"},"id":154908,"inspire_id":"2690798","journal_info":"JHEP 02 (2024) 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Using collisions of protons with an energy of 6.5 TeV incident on helium nuclei at rest in the proximity of the interaction region of the LHCb experiment, the ratio of antiprotons originating from antihyperon decays to prompt production is measured for antiproton momenta between 12 and 110 GeV/c. The dominant antihyperon contribution, namely $\\bar{\\Lambda} \\to \\bar{p} \\pi^+$ decays from promptly produced $\\bar{\\Lambda}$ particles, is also exclusively measured. The results complement the measurement of prompt antiproton production obtained from the same data sample. At the energy scale of this measurement, the antihyperon contributions to antiproton production are observed to be significantly larger than predictions of commonly used hadronic production models.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2084295/1/csv","json":"https://www.hepdata.net/download/submission/ins2084295/1/json","root":"https://www.hepdata.net/download/submission/ins2084295/1/root","yaml":"https://www.hepdata.net/download/submission/ins2084295/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins2084295/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:2205.09009","authors":["Aaij, R.","Abdelmotteleb, A.S. 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The average momentum and transverse momentum, as predicted by the EPOS-LHC generator for prompt antiprotons, are also listed for each interval. The uncertainty is split into an uncorrelated component, denoted with delta_uncorr, and a component that is fully correlated among the kinematic intervals, denoted delta_corr.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins2084295/Table 2/csv","json":"https://www.hepdata.net/download/table/ins2084295/Table 2/json","root":"https://www.hepdata.net/download/table/ins2084295/Table 2/root","yaml":"https://www.hepdata.net/download/table/ins2084295/Table 2/yaml","yoda":"https://www.hepdata.net/download/table/ins2084295/Table 2/yoda"}},"authors":null,"collaborations":["LHCb"],"control_number":"132123","creation_date":"2022-05-18","data_keywords":{"cmenergies":[{"gte":110.5,"lte":110.5}],"observables":["D2SIG(P HE --> LBAR X --> PBAR X)/D2SIG(P HE --> PBAR X)"],"phrases":["Double Differential Cross Section","Antiproton Production","Proton-Helium Scattering"],"reactions":["P HE --> PBAR X","P HE --> LBAR X --> PBAR X"]},"date":"18 May 2022","doc_type":"datatable","doi":"10.17182/hepdata.130780.v1/t2","first_author":{},"id":132123,"inspire_id":"2084295","journal_info":"Eur.Phys.J.C 83 (2023) 543","keywords":[{"name":"reactions","synonyms":"","value":"P HE --> PBAR X"},{"name":"reactions","synonyms":"","value":"P HE --> LBAR X --> PBAR X"},{"name":"observables","synonyms":"","value":"D2SIG(P HE --> LBAR X --> PBAR X)/D2SIG(P HE --> PBAR X)"},{"name":"cmenergies","synonyms":"","value":"110.5"},{"name":"phrases","synonyms":"","value":"Double Differential Cross Section"},{"name":"phrases","synonyms":"","value":"Proton-Helium Scattering"},{"name":"phrases","synonyms":"","value":"Antiproton Production"}],"last_updated":"2022-07-13T17:29:18","parent_child_join":{"name":"child_datatable","parent":"130780"},"recid":132123,"related_publication":130780,"resources":[{"description":"web page with related paper and auxiliary material","type":"html","url":"https://lhcbproject.web.cern.ch/lhcbproject/Publications/LHCbProjectPublic/LHCb-PAPER-2022-006.html"}],"title":"Table 2","uuid":"e279ccc9-228c-4252-91b3-4106c782bdd7"}],"data_abstract":null,"data_keywords":{"cmenergies":[{"gte":110.5,"lte":110.5}],"observables":["D2SIG(P HE --> LBAR X --> PBAR X)/D2SIG(P HE --> PBAR X)","D2SIG(P HE --> HBAR X --> PBAR X)/D2SIG(P HE --> PBAR X)"],"phrases":["Double Differential Cross Section","Proton-Helium Scattering","Antiproton Production"],"reactions":["P HE --> PBAR X","P HE --> HBAR X --> PBAR X","P HE --> LBAR X --> PBAR X"]},"date":"18 May 2022","doc_type":"publication","doi":"10.1140/epjc/s10052-023-11673-x","first_author":{"affiliation":"NIKHEF, Amsterdam","full_name":"Aaij, R."},"hepdata_doi":"10.17182/hepdata.130780","id":130780,"inspire_id":"2084295","journal_info":"Eur.Phys.J.C 83 (2023) 543","keywords":[{"schema":"INSPIRE","value":"p nucleus: interaction"},{"schema":"INSPIRE","value":"anti-p: production"},{"schema":"INSPIRE","value":"antihyperon: decay"},{"schema":"INSPIRE","value":"Antilambda: hadronic decay"},{"schema":"INSPIRE","value":"anti-p: cosmic radiation"},{"schema":"INSPIRE","value":"cosmic radiation: primary"},{"schema":"INSPIRE","value":"vertex: primary"},{"schema":"INSPIRE","value":"model: production"},{"schema":"INSPIRE","value":"anti-p: flux"},{"schema":"INSPIRE","value":"anti-p: momentum"},{"schema":"INSPIRE","value":"helium: nucleus"},{"schema":"INSPIRE","value":"anti-p: yield"},{"schema":"INSPIRE","value":"yield: ratio: measured"},{"schema":"INSPIRE","value":"LHC-B"},{"schema":"INSPIRE","value":"CERN LHC Coll"},{"schema":"INSPIRE","value":"at rest"},{"schema":"INSPIRE","value":"direct production"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"Antilambda --> anti-p pi+"},{"schema":"INSPIRE","value":"110 GeV-cms/nucleon"}],"last_updated":"2022-07-13T17:29:18","parent_child_join":{"name":"parent_publication"},"publication_date":"2023-05-07T00:00:00","recid":130780,"resources":[{"description":"web page with related paper and auxiliary material","type":"html","url":"https://lhcbproject.web.cern.ch/lhcbproject/Publications/LHCbProjectPublic/LHCb-PAPER-2022-006.html"}],"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"NIKHEF, Amsterdam","full_name":"Aaij, R."},{"affiliation":"Warwick U.","full_name":"Abdelmotteleb, A.S. 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The nuclear modification factor of prompt $D^0$ mesons is determined as a function of the transverse momentum $p_\\mathrm{T}$, and rapidity in the nucleon-nucleon center-of-mass frame $y^*$. In the forward rapidity region, significantly suppressed production with respect to $pp$ collisions is measured, which provides significant constraints of nuclear parton distributions and hadron production down to the very low Bjorken-$x$ region of $\\sim 10^{-5}$. In the backward rapidity region, a suppression with a significance of 2.0 - 3.8 standard deviations compared to nPDF expectations is found in the kinematic region of $p_\\mathrm{T}>6~\\mathrm{GeV}/c$ and $-3.25<y^*<-2.5$, corresponding to $x\\sim 0.01$.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins2694685/2/csv","json":"https://www.hepdata.net/download/submission/ins2694685/2/json","root":"https://www.hepdata.net/download/submission/ins2694685/2/root","yaml":"https://www.hepdata.net/download/submission/ins2694685/2/yaml","yoda":"https://www.hepdata.net/download/submission/ins2694685/2/yoda"}},"analyses":[{"analysis":"http://rivet.hepforge.org/analyses/LHCB_2022_I2694685","type":"rivet"}],"arxiv_id":"arXiv:2205.03936","authors":["Aaij, R.","Charpentier, Philippe","Abdelmotteleb, A.S.W.","Fischer, Kamil Leszek","Abellan Beteta, C.","Abudin\u00e9n, F.","Ackernley, T.","Adinolfi, M.","Afsharnia, H.","Charpentier, 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