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Deviations from the expectations based on currently available parton distribution functions are observed, showing the need for including W boson data in nuclear parton distribution global fits.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins1353541/1/csv","json":"https://www.hepdata.net/download/submission/ins1353541/1/json","root":"https://www.hepdata.net/download/submission/ins1353541/1/root","yaml":"https://www.hepdata.net/download/submission/ins1353541/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins1353541/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:1503.05825","authors":["Khachatryan, Vardan","Sirunyan, Albert M","Tumasyan, Armen","Adam, Wolfgang","Bergauer, Thomas","Dragicevic, Marko","Er\u00f6, Janos","Friedl, Markus","Fruehwirth, Rudolf","Ghete, Vasile Mihai"],"collaborations":["CMS"],"control_number":"69232","creation_date":"2015-03-19","data":[{"abstract":"Lepton charge asymmetry, $(N_{\\ell}^+ - N_{\\ell}^-)/(N_{\\ell}^+ + N_{\\ell}^-)$ as a function of the lepton pseudorapidity.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1353541/Table 1/csv","json":"https://www.hepdata.net/download/table/ins1353541/Table 1/json","root":"https://www.hepdata.net/download/table/ins1353541/Table 1/root","yaml":"https://www.hepdata.net/download/table/ins1353541/Table 1/yaml","yoda":"https://www.hepdata.net/download/table/ins1353541/Table 1/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"69234","creation_date":"2015-03-19","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["ASYM"],"phrases":["Inclusive"],"reactions":["P PB --> W X"]},"date":"19 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.69232.v1/t1","first_author":{"affiliation":"Yerevan Phys. 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The global normalization uncertainty of 3.5\\% is not included in the listed uncertainties.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1353541/Table 2/csv","json":"https://www.hepdata.net/download/table/ins1353541/Table 2/json","root":"https://www.hepdata.net/download/table/ins1353541/Table 2/root","yaml":"https://www.hepdata.net/download/table/ins1353541/Table 2/yaml","yoda":"https://www.hepdata.net/download/table/ins1353541/Table 2/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"69235","creation_date":"2015-03-19","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["DSIG/DETA"],"phrases":["Inclusive","Single Differential Cross Section","W Production"],"reactions":["P PB --> W+ X"]},"date":"19 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.69232.v1/t2","first_author":{"affiliation":"Yerevan Phys. 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Values are given first for muons and electrons separately, then combined. The global normalization uncertainty of 3.5\\% is not included in the listed uncertainties.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1353541/Table 3/csv","json":"https://www.hepdata.net/download/table/ins1353541/Table 3/json","root":"https://www.hepdata.net/download/table/ins1353541/Table 3/root","yaml":"https://www.hepdata.net/download/table/ins1353541/Table 3/yaml","yoda":"https://www.hepdata.net/download/table/ins1353541/Table 3/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"69236","creation_date":"2015-03-19","data_keywords":{"cmenergies":[{"gte":5020.0,"lte":5020.0}],"observables":["DSIG/DETA"],"phrases":["Inclusive","Single Differential Cross Section","W Production"],"reactions":["P PB --> W- X"]},"date":"19 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.69232.v1/t3","first_author":{"affiliation":"Yerevan Phys. 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Inst.","full_name":"Khachatryan, Vardan"},{"affiliation":"Yerevan Phys. Inst.","full_name":"Sirunyan, Albert M"},{"affiliation":"Yerevan Phys. Inst.","full_name":"Tumasyan, Armen"},{"affiliation":"Vienna, OAW","full_name":"Adam, Wolfgang"},{"affiliation":"Vienna, OAW","full_name":"Bergauer, Thomas"},{"affiliation":"Vienna, OAW","full_name":"Dragicevic, Marko"},{"affiliation":"Vienna, OAW","full_name":"Er\u00f6, Janos"},{"affiliation":"Vienna, OAW","full_name":"Friedl, Markus"},{"affiliation":"Vienna, OAW","full_name":"Fruehwirth, Rudolf"},{"affiliation":"Vienna, OAW","full_name":"Ghete, Vasile Mihai"}],"title":"Study of W boson production in pPb collisions at sqrt(s[NN]) = 5.02 TeV","total_tables":6,"type":["article"],"uuid":"170469e5-0fb6-4c77-8964-51a855d513b6","version":1,"year":"2015"},{"abstract":"Measurements of the ZZ production cross sections in proton-proton collisions at center-of-mass energies of 7 and 8 TeV are presented. Candidate events for the leptonic decay mode ZZ to 2 l 2 nu, where l denotes an electron or a muon, are reconstructed and selected from data corresponding to an integrated luminosity of 5.1 (19.6) inverse femtobarns at 7 (8) TeV collected with the CMS experiment. The measured cross sections, sigma(pp to ZZ) = 5.1 -1.4 +1.5 (stat) -1.1 +1.4 (syst) +/- 0.1 (lumi) pb at 7 TeV, and 7.2 -0.8 +0.8 (stat.) -1.5 +1.9 (syst) +/- 0.2 (lumi) pb at 8 TeV, are in good agreement with the standard model predictions with next-to-leading-order accuracy. The selected data are analyzed to search for anomalous triple gauge couplings involving the ZZ final state. In the absence of any deviation from the standard model predictions, limits are set on the relevant parameters. These limits are then combined with the previously published CMS results for ZZ in 4 l final states, yielding the most stringent constraints on the anomalous couplings.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins1353393/1/csv","json":"https://www.hepdata.net/download/submission/ins1353393/1/json","root":"https://www.hepdata.net/download/submission/ins1353393/1/root","yaml":"https://www.hepdata.net/download/submission/ins1353393/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins1353393/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:1503.05467","authors":["Khachatryan, Vardan","Sirunyan, Albert M","Tumasyan, Armen","Adam, Wolfgang","Bergauer, Thomas","Dragicevic, Marko","Er\u00f6, Janos","Friedl, Markus","Fruehwirth, Rudolf","Ghete, Vasile Mihai"],"collaborations":["CMS"],"control_number":"69984","creation_date":"2015-03-18","data":[{"abstract":"pp->ZZ->2l2nu reduced-MET distribution in the 7 TeV dataset. Uncertainties are statistical. Last bin includes overflow events.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1353393/Table 1/csv","json":"https://www.hepdata.net/download/table/ins1353393/Table 1/json","root":"https://www.hepdata.net/download/table/ins1353393/Table 1/root","yaml":"https://www.hepdata.net/download/table/ins1353393/Table 1/yaml","yoda":"https://www.hepdata.net/download/table/ins1353393/Table 1/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"69986","creation_date":"2015-03-18","data_keywords":{"cmenergies":[],"observables":["SIG"],"phrases":["Inclusive","Proton-Proton Scattering","Z pair Production","Cross Section","Integrated Cross Section","Z Production"],"reactions":["P P --> Z0 Z0 X"]},"date":"18 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.69984.v1/t1","first_author":{"affiliation":"Yerevan Phys. 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Last bin includes overflow events.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1353393/Table 2/csv","json":"https://www.hepdata.net/download/table/ins1353393/Table 2/json","root":"https://www.hepdata.net/download/table/ins1353393/Table 2/root","yaml":"https://www.hepdata.net/download/table/ins1353393/Table 2/yaml","yoda":"https://www.hepdata.net/download/table/ins1353393/Table 2/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"69987","creation_date":"2015-03-18","data_keywords":{"cmenergies":[],"observables":["SIG"],"phrases":["Inclusive","Proton-Proton Scattering","Z pair Production","Cross Section","Integrated Cross Section","Z Production"],"reactions":["P P --> Z0 Z0 X"]},"date":"18 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.69984.v1/t2","first_author":{"affiliation":"Yerevan Phys. 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Last bin includes overflow events.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1353393/Table 3/csv","json":"https://www.hepdata.net/download/table/ins1353393/Table 3/json","root":"https://www.hepdata.net/download/table/ins1353393/Table 3/root","yaml":"https://www.hepdata.net/download/table/ins1353393/Table 3/yaml","yoda":"https://www.hepdata.net/download/table/ins1353393/Table 3/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"69988","creation_date":"2015-03-18","data_keywords":{"cmenergies":[],"observables":["SIG"],"phrases":["Inclusive","Proton-Proton Scattering","Z pair Production","Cross Section","Integrated Cross Section","Z Production"],"reactions":["P P --> Z0 Z0 X"]},"date":"18 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.69984.v1/t3","first_author":{"affiliation":"Yerevan Phys. 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Last bin includes overflow events.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1353393/Table 4/csv","json":"https://www.hepdata.net/download/table/ins1353393/Table 4/json","root":"https://www.hepdata.net/download/table/ins1353393/Table 4/root","yaml":"https://www.hepdata.net/download/table/ins1353393/Table 4/yaml","yoda":"https://www.hepdata.net/download/table/ins1353393/Table 4/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"69989","creation_date":"2015-03-18","data_keywords":{"cmenergies":[],"observables":["SIG"],"phrases":["Inclusive","Proton-Proton Scattering","Z pair Production","Cross Section","Integrated Cross Section","Z Production"],"reactions":["P P --> Z0 Z0 X"]},"date":"18 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.69984.v1/t4","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":69989,"inspire_id":1353393,"journal_info":"Eur.Phys.J.C 75 (2015) 511","keywords":[{"name":"reactions","synonyms":"","value":"P P --> Z0 Z0 X"},{"name":"observables","synonyms":"","value":"SIG"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"phrases","synonyms":"","value":"Integrated Cross Section"},{"name":"phrases","synonyms":"","value":"Cross Section"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Z Production"},{"name":"phrases","synonyms":"","value":"Z pair Production"}],"last_updated":"2016-10-14T18:39:33","parent_child_join":{"name":"child_datatable","parent":"69984"},"recid":69989,"related_publication":69984,"title":"Table 4","uuid":"c52561c0-19d7-4245-bc0c-16ae2a16cd9a"},{"abstract":"Using a maximum-likelihood fit to the reduced-MET data distributions, with all the systematic uncertainties incorporated as nuisance parameters, we obtain the following cross sections for the pp->ZZ process (with both Z bosons in the mass range 60-120 GeV).\nThe first systematic uncertainty is the combined systematic uncertainty excluding luminosity, the second is the luminosity.\nThe theory calculations are 6.2+0.3-0.2 pb at 7 TeV and 7.6+0.4-0.3 pb at 8 TeV, including NLO QCD and NLO EW corrections.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1353393/Table 5/csv","json":"https://www.hepdata.net/download/table/ins1353393/Table 5/json","root":"https://www.hepdata.net/download/table/ins1353393/Table 5/root","yaml":"https://www.hepdata.net/download/table/ins1353393/Table 5/yaml","yoda":"https://www.hepdata.net/download/table/ins1353393/Table 5/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"69990","creation_date":"2015-03-18","data_keywords":{"cmenergies":[],"observables":["SIG"],"phrases":["Inclusive","Proton-Proton Scattering","Z pair Production","Cross Section","Integrated Cross Section","Z Production"],"reactions":["P P --> Z0 Z0 X"]},"date":"18 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.69984.v1/t5","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":69990,"inspire_id":1353393,"journal_info":"Eur.Phys.J.C 75 (2015) 511","keywords":[{"name":"reactions","synonyms":"","value":"P P --> Z0 Z0 X"},{"name":"observables","synonyms":"","value":"SIG"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"phrases","synonyms":"","value":"Integrated Cross Section"},{"name":"phrases","synonyms":"","value":"Cross Section"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Z Production"},{"name":"phrases","synonyms":"","value":"Z pair Production"}],"last_updated":"2016-10-14T18:39:33","parent_child_join":{"name":"child_datatable","parent":"69984"},"recid":69990,"related_publication":69984,"title":"Table 5","uuid":"c8f965f0-bcd6-4b78-824e-5bf20753aba7"}],"data_keywords":{"cmenergies":[],"observables":["SIG"],"phrases":["Z pair Production","Inclusive","Proton-Proton Scattering","Cross Section","Integrated Cross Section","Z Production"],"reactions":["P P --> Z0 Z0 X"]},"date":"18 Mar 2015","doc_type":"publication","doi":"10.1140/epjc/s10052-015-3706-0","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"hepdata_doi":"10.17182/hepdata.69984","id":69984,"inspire_id":1353393,"journal_info":"Eur.Phys.J.C 75 (2015) 511","keywords":[{"schema":"INSPIRE","value":"p p: colliding beams"},{"schema":"INSPIRE","value":"Z0: pair production"},{"schema":"INSPIRE","value":"Z0: leptonic decay"},{"schema":"INSPIRE","value":"coupling: (3gauge boson)"},{"schema":"INSPIRE","value":"p p: scattering"},{"schema":"INSPIRE","value":"channel cross section: measured"},{"schema":"INSPIRE","value":"higher-order: 1"},{"schema":"INSPIRE","value":"coupling: anomaly"},{"schema":"INSPIRE","value":"CMS"},{"schema":"INSPIRE","value":"CERN LHC Coll"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"p p --> 2Z0 anything"},{"schema":"INSPIRE","value":"Z0 --> lepton+ lepton-"},{"schema":"INSPIRE","value":"Z0 --> neutrino antineutrino"},{"schema":"INSPIRE","value":"7000 GeV-cms"},{"schema":"INSPIRE","value":"8000 GeV-cms"},{"schema":"PDG","value":"S044ZZZ"}],"last_updated":"2016-05-04T15:48:18","parent_child_join":{"name":"parent_publication"},"publication_date":"2015-12-11T00:00:00","recid":69984,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},{"affiliation":"Yerevan Phys. Inst.","full_name":"Sirunyan, Albert M"},{"affiliation":"Yerevan Phys. Inst.","full_name":"Tumasyan, Armen"},{"affiliation":"Vienna, OAW","full_name":"Adam, Wolfgang"},{"affiliation":"Vienna, OAW","full_name":"Bergauer, Thomas"},{"affiliation":"Vienna, OAW","full_name":"Dragicevic, Marko"},{"affiliation":"Vienna, OAW","full_name":"Er\u00f6, Janos"},{"affiliation":"Vienna, OAW","full_name":"Friedl, Markus"},{"affiliation":"Vienna, OAW","full_name":"Fruehwirth, Rudolf"},{"affiliation":"Vienna, OAW","full_name":"Ghete, Vasile Mihai"}],"title":"Measurements of the ZZ production cross sections in the 2 l 2 nu channel in proton-proton collisions at sqrt(s) = 7 and 8 TeV and combined constraints on triple gauge couplings","total_tables":5,"type":["article"],"uuid":"0b799853-7a54-495e-a4ff-e03e2904cc59","version":1,"year":"2015"},{"abstract":"A systematic study of the factorization of long-range azimuthal two-particle correlations into a product of single-particle anisotropies is presented as a function of pt and eta of both particles, and as a function of the particle multiplicity in PbPb and pPb collisions. The data were taken with the CMS detector for PbPb collisions at sqrt(s[NN]) = 2.76 TeV and pPb collisions at sqrt(s[NN]) = 5.02 TeV, covering a very wide range of multiplicity. Factorization is observed to be broken as a function of both particle pt and eta. When measured with particles of different pt, the magnitude of the factorization breakdown for the second Fourier harmonic reaches 20% for very central PbPb collisions but decreases rapidly as the multiplicity decreases. The data are consistent with viscous hydrodynamic predictions, which suggest that the effect of factorization breaking is mainly sensitive to the initial-state conditions rather than to the transport properties (e.g., shear viscosity) of the medium. The factorization breakdown is also computed with particles of different eta. The effect is found to be weakest for mid-central PbPb events but becomes larger for more central or peripheral PbPb collisions, and also for very high-multiplicity pPb collisions. The eta-dependent factorization data provide new insights to the longitudinal evolution of the medium formed in heavy ion collisions.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins1347386/1/csv","json":"https://www.hepdata.net/download/submission/ins1347386/1/json","root":"https://www.hepdata.net/download/submission/ins1347386/1/root","yaml":"https://www.hepdata.net/download/submission/ins1347386/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins1347386/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:1503.01692","authors":["Khachatryan, Vardan","Sirunyan, Albert M","Tumasyan, Armen","Adam, Wolfgang","A\u015f\u0131lar, Ece","Bergauer, Thomas","Brandstetter, Johannes","Dragicevic, Marko","Er\u00f6, Janos","Flechl, Martin"],"collaborations":["CMS"],"control_number":"67151","creation_date":"2015-03-05","data":[{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ for $1.0
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CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t2","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67160,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"2760.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67160,"related_publication":67151,"title":"Table 2","uuid":"09f55619-9fbd-4e96-996b-f88c31041b49"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ for $2.0
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t3","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67162,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"2760.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67162,"related_publication":67151,"title":"Table 3","uuid":"39e26f21-f4f7-46c4-9106-c36eb7e4b11e"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ for $2.5
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t4","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67163,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"2760.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67163,"related_publication":67151,"title":"Table 4","uuid":"200ed751-ce30-47dc-9407-8535434f31c7"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ for $1.0
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t5","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67164,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"2760.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67164,"related_publication":67151,"title":"Table 5","uuid":"7a3c82b5-788b-4a6a-bb16-36bb03d74f5b"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ for $1.5
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t6","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67165,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"2760.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67165,"related_publication":67151,"title":"Table 6","uuid":"380c49a1-ee81-4075-b99d-6f5ca2d4313f"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ for $2.0
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t7","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67166,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"2760.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67166,"related_publication":67151,"title":"Table 7","uuid":"55180ef4-aff5-4d08-a612-62971197bf23"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ for $2.5
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t8","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67167,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"2760.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67167,"related_publication":67151,"title":"Table 8","uuid":"86c88977-d689-47af-9ca5-3b04f2e05fe8"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ for $1.0
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t9","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67168,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"2760.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67168,"related_publication":67151,"title":"Table 9","uuid":"416b781e-54e6-4424-a88b-75cd6b8bfbd1"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ for $1.5
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t10","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67169,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"2760.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67169,"related_publication":67151,"title":"Table 10","uuid":"0927abfa-d747-4b74-a4f5-a50edbf6061e"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ for $2.0
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t11","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67170,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"2760.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67170,"related_publication":67151,"title":"Table 11","uuid":"8795f3eb-fea9-42a5-9a43-7973f57bd2e9"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ for $2.5
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t12","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67171,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"2760.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67171,"related_publication":67151,"title":"Table 12","uuid":"98195d7f-a5a5-4155-8d12-76479f839e3a"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ for $1.0
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t13","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67172,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"2760.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67172,"related_publication":67151,"title":"Table 13","uuid":"106bd3e1-db90-4167-a0e4-7d52ba0f0211"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ for $1.5
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t14","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67173,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"2760.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67173,"related_publication":67151,"title":"Table 14","uuid":"f9dda73f-d8b7-4b67-a199-c6af3f5434bd"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ for $2.0
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t15","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67174,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"2760.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67174,"related_publication":67151,"title":"Table 15","uuid":"83d017ff-3e87-41d9-91a2-1111711f4732"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ for $2.5
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CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t99","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67256,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"2760.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67256,"related_publication":67151,"title":"Table 99","uuid":"fa6b9085-da60-4ff9-8ffc-c522ed10f0c5"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ with $2.5
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t100","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67257,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"PB PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"2760.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67257,"related_publication":67151,"title":"Table 100","uuid":"3589bf0f-6623-4e68-a5d4-a8e6217be28c"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ with $1.0
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t101","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67258,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"P PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67258,"related_publication":67151,"title":"Table 101","uuid":"db49a6d4-f1cc-487e-9593-78bcffc61b8e"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ with $1.5
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t102","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67259,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"P PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67259,"related_publication":67151,"title":"Table 102","uuid":"3206cc39-c5c1-4acc-b90d-97d06e1333cf"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ with $2.0
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t103","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67260,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"P PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67260,"related_publication":67151,"title":"Table 103","uuid":"80812d69-f896-41e8-af83-792f8c840deb"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ with $2.5
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t104","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67261,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"P PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67261,"related_publication":67151,"title":"Table 104","uuid":"1999d1fc-2fa6-4900-b2e5-6b8aaa3f18af"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ with $1.0
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t105","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67262,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"P PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67262,"related_publication":67151,"title":"Table 105","uuid":"3ebbd2c9-ed44-4723-a82e-3d93872a7e04"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ with $1.5
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t106","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67263,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"P PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67263,"related_publication":67151,"title":"Table 106","uuid":"84e31588-e42c-4439-9b9b-d7f3915c2cb5"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ with $2.0
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t107","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67264,"inspire_id":1347386,"journal_info":"Phys.Rev.C 92 (2015) 034911","keywords":[{"name":"reactions","synonyms":"","value":"P PB --> CHARGED X"},{"name":"observables","synonyms":"","value":"CORR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"cmenergies","synonyms":"","value":"5020.0"}],"last_updated":"2016-10-14T18:08:15","parent_child_join":{"name":"child_datatable","parent":"67151"},"recid":67264,"related_publication":67151,"title":"Table 107","uuid":"2ad6082a-8ada-4206-a062-27f192315df4"},{"abstract":"The $p_{T}$-dependent factorization ratio, $r_{2}$, as a function of $p^{a}_{T} - p^{b}_{T}$ with $2.5
CHARGED X"]},"date":"05 Mar 2015","doc_type":"datatable","doi":"10.17182/hepdata.67151.v1/t108","first_author":{"affiliation":"Yerevan Phys. 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Inst.","full_name":"Khachatryan, Vardan"},{"affiliation":"Yerevan Phys. Inst.","full_name":"Sirunyan, Albert M"},{"affiliation":"Yerevan Phys. Inst.","full_name":"Tumasyan, Armen"},{"affiliation":"Vienna, OAW","full_name":"Adam, Wolfgang"},{"affiliation":"Vienna, OAW","full_name":"A\u015f\u0131lar, Ece"},{"affiliation":"Vienna, OAW","full_name":"Bergauer, Thomas"},{"affiliation":"Vienna, OAW","full_name":"Brandstetter, Johannes"},{"affiliation":"Vienna, OAW","full_name":"Dragicevic, Marko"},{"affiliation":"Vienna, OAW","full_name":"Er\u00f6, Janos"},{"affiliation":"Vienna, OAW","full_name":"Flechl, Martin"}],"title":"Evidence for transverse momentum and pseudorapidity dependent event plane fluctuations in PbPb and pPb collisions","total_tables":162,"type":["article"],"uuid":"6f9e61f9-b990-48db-a9a6-668610e03877","version":1,"year":"2015"},{"abstract":"The differential cross sections for the production of photons in Z to mu+ mu- gamma decays are presented as a function of the transverse energy of the photon and its separation from the nearest muon. The data for these measurements were collected with the CMS detector and correspond to an integrated luminosity of 4.7 inverse femtobarns of pp collisions at sqrt(s) = 7 TeV delivered by the CERN LHC. The cross sections are compared to simulations with POWHEG and PYTHIA, where PYTHIA is used to simulate parton showers and final-state photons. These simulations match the data to better than 5%.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins1346843/1/csv","json":"https://www.hepdata.net/download/submission/ins1346843/1/json","root":"https://www.hepdata.net/download/submission/ins1346843/1/root","yaml":"https://www.hepdata.net/download/submission/ins1346843/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins1346843/1/yoda"}},"analyses":[{"analysis":"http://rivet.hepforge.org/analyses/CMS_2015_I1346843","type":"rivet"}],"arxiv_id":"arXiv:1502.07940","authors":["Khachatryan, Vardan","Sirunyan, Albert M.","Tumasyan, Armen","Adam, Wolfgang","Bergauer, Thomas","Dragicevic, Marko","Er\u00f6, Janos","Friedl, Markus","Fruehwirth, Rudolf","Ghete, Vasile Mihai"],"collaborations":["CMS"],"control_number":"67634","creation_date":"2015-02-27","data":[{"abstract":"Measured differential cross section dsigma/dET in pb/GeV. For the data values, the first\nuncertainty is statistical and the second is systematic. For the theory values, the uncertainty\ncombines statistical, PDF, and renormalization/factorization scale components.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1346843/Table 1/csv","json":"https://www.hepdata.net/download/table/ins1346843/Table 1/json","root":"https://www.hepdata.net/download/table/ins1346843/Table 1/root","yaml":"https://www.hepdata.net/download/table/ins1346843/Table 1/yaml","yoda":"https://www.hepdata.net/download/table/ins1346843/Table 1/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"67636","creation_date":"2015-02-27","data_keywords":{"cmenergies":[{"gte":7000.0,"lte":7000.0}],"observables":["DSIG/DET"],"phrases":["Muon production","Proton-Proton Scattering","Di-Muon Production","Single Differential Cross Section","Z Production","Inclusive","Drell Yan"],"reactions":["P P --> MU+ MU- GAMMA X","P P --> Z0 X","P P --> GAMMA* X"]},"date":"27 Feb 2015","doc_type":"datatable","doi":"10.17182/hepdata.67634.v1/t1","first_author":{"affiliation":"Yerevan Phys. 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For the data values, the first\nuncertainty is statistical and the second is systematic. For the theory values, the uncertainty\ncombines statistical, PDF, and renormalization/factorization scale components.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1346843/Table 2/csv","json":"https://www.hepdata.net/download/table/ins1346843/Table 2/json","root":"https://www.hepdata.net/download/table/ins1346843/Table 2/root","yaml":"https://www.hepdata.net/download/table/ins1346843/Table 2/yaml","yoda":"https://www.hepdata.net/download/table/ins1346843/Table 2/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"67637","creation_date":"2015-02-27","data_keywords":{"cmenergies":[{"gte":7000.0,"lte":7000.0}],"observables":["DSIG/DET"],"phrases":["Muon production","Proton-Proton Scattering","Di-Muon Production","Single Differential Cross Section","Z Production","Inclusive","Drell Yan"],"reactions":["P P --> MU+ MU- GAMMA X","P P --> Z0 X","P P --> GAMMA* X"]},"date":"27 Feb 2015","doc_type":"datatable","doi":"10.17182/hepdata.67634.v1/t2","first_author":{"affiliation":"Yerevan Phys. 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For the data values, the first\nuncertainty is statistical and the second is systematic. For the theory values, the uncertainty\ncombines statistical, PDF, and renormalization/factorization scale components.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1346843/Table 3/csv","json":"https://www.hepdata.net/download/table/ins1346843/Table 3/json","root":"https://www.hepdata.net/download/table/ins1346843/Table 3/root","yaml":"https://www.hepdata.net/download/table/ins1346843/Table 3/yaml","yoda":"https://www.hepdata.net/download/table/ins1346843/Table 3/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"67638","creation_date":"2015-02-27","data_keywords":{"cmenergies":[{"gte":7000.0,"lte":7000.0}],"observables":["DSIG/DET"],"phrases":["Muon production","Proton-Proton Scattering","Di-Muon Production","Single Differential Cross Section","Z Production","Inclusive","Drell Yan"],"reactions":["P P --> MU+ MU- GAMMA X","P P --> Z0 X","P P --> GAMMA* X"]},"date":"27 Feb 2015","doc_type":"datatable","doi":"10.17182/hepdata.67634.v1/t3","first_author":{"affiliation":"Yerevan Phys. 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For the data values, the first\nuncertainty is statistical and the second is systematic. For the theory values, the uncertainty\ncombines statistical, PDF, and renormalization/factorization scale components.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1346843/Table 4/csv","json":"https://www.hepdata.net/download/table/ins1346843/Table 4/json","root":"https://www.hepdata.net/download/table/ins1346843/Table 4/root","yaml":"https://www.hepdata.net/download/table/ins1346843/Table 4/yaml","yoda":"https://www.hepdata.net/download/table/ins1346843/Table 4/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"67639","creation_date":"2015-02-27","data_keywords":{"cmenergies":[{"gte":7000.0,"lte":7000.0}],"observables":["DSIG/DET"],"phrases":["Muon production","Proton-Proton Scattering","Di-Muon Production","Single Differential Cross Section","Z Production","Inclusive","Drell Yan"],"reactions":["P P --> MU+ MU- GAMMA X","P P --> Z0 X","P P --> GAMMA* X"]},"date":"27 Feb 2015","doc_type":"datatable","doi":"10.17182/hepdata.67634.v1/t4","first_author":{"affiliation":"Yerevan Phys. 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For the data values, the first\nuncertainty is statistical and the second is systematic. For the theory values, the uncertainty\ncombines statistical, PDF, and renormalization/factorization scale components.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1346843/Table 5/csv","json":"https://www.hepdata.net/download/table/ins1346843/Table 5/json","root":"https://www.hepdata.net/download/table/ins1346843/Table 5/root","yaml":"https://www.hepdata.net/download/table/ins1346843/Table 5/yaml","yoda":"https://www.hepdata.net/download/table/ins1346843/Table 5/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"67640","creation_date":"2015-02-27","data_keywords":{"cmenergies":[{"gte":7000.0,"lte":7000.0}],"observables":["DSIG/DET"],"phrases":["Muon production","Proton-Proton Scattering","Di-Muon Production","Single Differential Cross Section","Z Production","Inclusive","Drell Yan"],"reactions":["P P --> MU+ MU- GAMMA X","P P --> Z0 X","P P --> GAMMA* X"]},"date":"27 Feb 2015","doc_type":"datatable","doi":"10.17182/hepdata.67634.v1/t5","first_author":{"affiliation":"Yerevan Phys. 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For the data values, the first\nuncertainty is statistical and the second is systematic. For the theory values, the uncertainty\ncombines statistical, PDF, and renormalization/factorization scale components.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1346843/Table 6/csv","json":"https://www.hepdata.net/download/table/ins1346843/Table 6/json","root":"https://www.hepdata.net/download/table/ins1346843/Table 6/root","yaml":"https://www.hepdata.net/download/table/ins1346843/Table 6/yaml","yoda":"https://www.hepdata.net/download/table/ins1346843/Table 6/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"67641","creation_date":"2015-02-27","data_keywords":{"cmenergies":[{"gte":7000.0,"lte":7000.0}],"observables":["DSIG/DDR"],"phrases":["Muon production","Proton-Proton Scattering","Di-Muon Production","Single Differential Cross Section","Z Production","Inclusive","Drell Yan"],"reactions":["P P --> MU+ MU- GAMMA X","P P --> Z0 X","P P --> GAMMA* X"]},"date":"27 Feb 2015","doc_type":"datatable","doi":"10.17182/hepdata.67634.v1/t6","first_author":{"affiliation":"Yerevan Phys. 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For the data values, the first\nuncertainty is statistical and the second is systematic. For the theory values, the uncertainty\ncombines statistical, PDF, and renormalization/factorization scale components.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1346843/Table 7/csv","json":"https://www.hepdata.net/download/table/ins1346843/Table 7/json","root":"https://www.hepdata.net/download/table/ins1346843/Table 7/root","yaml":"https://www.hepdata.net/download/table/ins1346843/Table 7/yaml","yoda":"https://www.hepdata.net/download/table/ins1346843/Table 7/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"67642","creation_date":"2015-02-27","data_keywords":{"cmenergies":[{"gte":7000.0,"lte":7000.0}],"observables":["DSIG/DDR"],"phrases":["Muon production","Proton-Proton Scattering","Di-Muon Production","Single Differential Cross Section","Z Production","Inclusive","Drell Yan"],"reactions":["P P --> MU+ MU- GAMMA X","P P --> Z0 X","P P --> GAMMA* X"]},"date":"27 Feb 2015","doc_type":"datatable","doi":"10.17182/hepdata.67634.v1/t7","first_author":{"affiliation":"Yerevan Phys. 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For the data values, the first\nuncertainty is statistical and the second is systematic. For the theory values, the uncertainty\ncombines statistical, PDF, and renormalization/factorization scale components.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1346843/Table 8/csv","json":"https://www.hepdata.net/download/table/ins1346843/Table 8/json","root":"https://www.hepdata.net/download/table/ins1346843/Table 8/root","yaml":"https://www.hepdata.net/download/table/ins1346843/Table 8/yaml","yoda":"https://www.hepdata.net/download/table/ins1346843/Table 8/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"67643","creation_date":"2015-02-27","data_keywords":{"cmenergies":[{"gte":7000.0,"lte":7000.0}],"observables":["DSIG/DDR"],"phrases":["Muon production","Proton-Proton Scattering","Di-Muon Production","Single Differential Cross Section","Z Production","Inclusive","Drell Yan"],"reactions":["P P --> MU+ MU- GAMMA X","P P --> Z0 X","P P --> GAMMA* X"]},"date":"27 Feb 2015","doc_type":"datatable","doi":"10.17182/hepdata.67634.v1/t8","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":67643,"inspire_id":1346843,"journal_info":"Phys.Rev.D 91 (2015) 092012","keywords":[{"name":"reactions","synonyms":"","value":"P P --> GAMMA* X"},{"name":"reactions","synonyms":"","value":"P P --> Z0 X"},{"name":"reactions","synonyms":"","value":"P P --> MU+ MU- GAMMA X"},{"name":"observables","synonyms":"","value":"DSIG/DDR"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"phrases","synonyms":"","value":"Single Differential Cross Section"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Drell Yan"},{"name":"phrases","synonyms":"","value":"Di-Muon Production"},{"name":"phrases","synonyms":"","value":"Z Production"},{"name":"phrases","synonyms":"","value":"Muon production"},{"name":"cmenergies","synonyms":"","value":"7000.0"}],"last_updated":"2016-10-14T18:11:17","parent_child_join":{"name":"child_datatable","parent":"67634"},"recid":67643,"related_publication":67634,"title":"Table 8","uuid":"b7d512c4-dd64-4aa4-bd4b-04fc61d6a476"}],"data_keywords":{"cmenergies":[{"gte":7000.0,"lte":7000.0}],"observables":["DSIG/DET","DSIG/DDR"],"phrases":["Muon production","Proton-Proton Scattering","Di-Muon Production","Single Differential Cross Section","Z Production","Inclusive","Drell Yan"],"reactions":["P P --> MU+ MU- GAMMA X","P P --> Z0 X","P P --> GAMMA* X"]},"date":"27 Feb 2015","doc_type":"publication","doi":"10.1103/PhysRevD.91.092012","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"hepdata_doi":"10.17182/hepdata.67634","id":67634,"inspire_id":1346843,"journal_info":"Phys.Rev.D 91 (2015) 092012","keywords":[{"schema":"PACS","value":"14.70.Hp"},{"schema":"PACS","value":"12.38.-t"},{"schema":"PACS","value":"13.40.Ks"},{"schema":"INSPIRE","value":"p p: scattering"},{"schema":"INSPIRE","value":"p p: colliding beams"},{"schema":"INSPIRE","value":"photon: transverse energy"},{"schema":"INSPIRE","value":"parton: showers"},{"schema":"INSPIRE","value":"Z0: leptonic decay"},{"schema":"INSPIRE","value":"radiation: final-state interaction"},{"schema":"INSPIRE","value":"numerical calculations: Monte Carlo"},{"schema":"INSPIRE","value":"PYTHIA"},{"schema":"INSPIRE","value":"differential cross section: measured"},{"schema":"INSPIRE","value":"CERN LHC Coll"},{"schema":"INSPIRE","value":"CERN Lab"},{"schema":"INSPIRE","value":"dimuon: mass spectrum"},{"schema":"INSPIRE","value":"CMS"},{"schema":"INSPIRE","value":"experimental results"},{"schema":"INSPIRE","value":"p p --> Z0 photon anything"},{"schema":"INSPIRE","value":"Z0 --> muon+ muon-"},{"schema":"INSPIRE","value":"7000 GeV-cms"}],"last_updated":"2015-05-03T09:48:12","parent_child_join":{"name":"parent_publication"},"publication_date":"2015-12-11T00:00:00","recid":67634,"subject_area":["hep-ex"],"summary_authors":[{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},{"affiliation":"Yerevan Phys. Inst.","full_name":"Sirunyan, Albert M."},{"affiliation":"Yerevan Phys. Inst.","full_name":"Tumasyan, Armen"},{"affiliation":"Vienna, OAW","full_name":"Adam, Wolfgang"},{"affiliation":"Vienna, OAW","full_name":"Bergauer, Thomas"},{"affiliation":"Vienna, OAW","full_name":"Dragicevic, Marko"},{"affiliation":"Vienna, OAW","full_name":"Er\u00f6, Janos"},{"affiliation":"Vienna, OAW","full_name":"Friedl, Markus"},{"affiliation":"Vienna, OAW","full_name":"Fruehwirth, Rudolf"},{"affiliation":"Vienna, OAW","full_name":"Ghete, Vasile Mihai"}],"title":"A study of final-state radiation in decays of Z bosons produced in pp collisions at 7 TeV","total_tables":8,"type":["article"],"uuid":"087f4cf4-a241-4024-8227-9b569f82fd3a","version":1,"year":"2015"},{"abstract":"The cross section for the production of Z gamma in proton-proton collisions at 8 TeV is measured based on data collected by the CMS experiment at the LHC corresponding to an integrated luminosity of 19.5 inverse femtobarns. Events with an oppositely-charged pair of muons or electrons together with an isolated photon are selected. The differential cross section as a function of the photon transverse momentum is measured inclusively and exclusively, where the exclusive selection applies a veto on central jets. The observed cross sections are compatible with the expectations of next-to-next-to-leading-order quantum chromodynamics. Limits on anomalous triple gauge couplings of Z Z gamma and Z gamma gamma are set that improve on previous experimental results obtained with the charged lepton decay modes of the Z boson.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins1345354/1/csv","json":"https://www.hepdata.net/download/submission/ins1345354/1/json","root":"https://www.hepdata.net/download/submission/ins1345354/1/root","yaml":"https://www.hepdata.net/download/submission/ins1345354/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins1345354/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:1502.05664","authors":["Khachatryan, Vardan","Sirunyan, Albert M","Tumasyan, Armen","Adam, Wolfgang","Bergauer, Thomas","Dragicevic, Marko","Er\u00f6, Janos","Friedl, Markus","Fruehwirth, Rudolf","Ghete, Vasile Mihai"],"collaborations":["CMS"],"control_number":"66985","creation_date":"2015-02-19","data":[{"abstract":"Inclusive fiducial cross sections in bins of pT(gamma) with statistical, systematic, and luminosity uncertainties, respectivley. Results are not divided by bin-widths. The last bin is the cross section for pT(gamma) > 120 GeV. Combined result of electron and muon channels.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1345354/Table 1/csv","json":"https://www.hepdata.net/download/table/ins1345354/Table 1/json","root":"https://www.hepdata.net/download/table/ins1345354/Table 1/root","yaml":"https://www.hepdata.net/download/table/ins1345354/Table 1/yaml","yoda":"https://www.hepdata.net/download/table/ins1345354/Table 1/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"66987","creation_date":"2015-02-19","data_keywords":{"cmenergies":[{"gte":8000.0,"lte":8000.0}],"observables":["DSIG/DPT"],"phrases":["Inclusive","Proton-Proton Scattering","Transverse Momentum Dependence","Single Differential Cross Section","Electron production","Z Production","Muon production"],"reactions":["P P --> Z0 GAMMA X"]},"date":"19 Feb 2015","doc_type":"datatable","doi":"10.17182/hepdata.66985.v1/t1","first_author":{"affiliation":"Yerevan Phys. Inst.","full_name":"Khachatryan, Vardan"},"id":66987,"inspire_id":1345354,"journal_info":"JHEP 04 (2015) 164","keywords":[{"name":"reactions","synonyms":"","value":"P P --> Z0 GAMMA X"},{"name":"observables","synonyms":"","value":"DSIG/DPT"},{"name":"phrases","synonyms":"","value":"Inclusive"},{"name":"phrases","synonyms":"","value":"Single Differential Cross Section"},{"name":"phrases","synonyms":"","value":"Transverse Momentum Dependence"},{"name":"phrases","synonyms":"","value":"Proton-Proton Scattering"},{"name":"phrases","synonyms":"","value":"Z Production"},{"name":"phrases","synonyms":"","value":"Muon production"},{"name":"phrases","synonyms":"","value":"Electron production"},{"name":"cmenergies","synonyms":"","value":"8000.0"}],"last_updated":"2016-10-14T18:04:45","parent_child_join":{"name":"child_datatable","parent":"66985"},"recid":66987,"related_publication":66985,"title":"Table 1","uuid":"2bd04aa5-5b2b-4df2-bda1-7ae5208e8df1"},{"abstract":"Fiducial cross sections with jet-veto in bins of pT(gamma) with statistical, systematic, and luminosity uncertainties, respectivley. Results are not divided by bin-widths. The last bin is the cross section for pT(gamma) > 120 GeV. Combined result of electron and muon channels.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1345354/Table 2/csv","json":"https://www.hepdata.net/download/table/ins1345354/Table 2/json","root":"https://www.hepdata.net/download/table/ins1345354/Table 2/root","yaml":"https://www.hepdata.net/download/table/ins1345354/Table 2/yaml","yoda":"https://www.hepdata.net/download/table/ins1345354/Table 2/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"66988","creation_date":"2015-02-19","data_keywords":{"cmenergies":[{"gte":8000.0,"lte":8000.0}],"observables":["DSIG/DPT"],"phrases":["Inclusive","Proton-Proton Scattering","Transverse Momentum Dependence","Single Differential Cross Section","Electron production","Z Production","Muon production"],"reactions":["P P --> Z0 GAMMA X"]},"date":"19 Feb 2015","doc_type":"datatable","doi":"10.17182/hepdata.66985.v1/t2","first_author":{"affiliation":"Yerevan Phys. 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The last bin is the cross section for pT(gamma) > 120 GeV. Combined result of electron and muon channels.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1345354/Table 3/csv","json":"https://www.hepdata.net/download/table/ins1345354/Table 3/json","root":"https://www.hepdata.net/download/table/ins1345354/Table 3/root","yaml":"https://www.hepdata.net/download/table/ins1345354/Table 3/yaml","yoda":"https://www.hepdata.net/download/table/ins1345354/Table 3/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"66989","creation_date":"2015-02-19","data_keywords":{"cmenergies":[{"gte":8.0,"lte":8.0}],"observables":["SIG/SIG"],"phrases":["Inclusive","Proton-Proton Scattering","Cross Section","Integrated Cross Section","Electron production","Z Production","Muon production"],"reactions":["P P --> Z0 GAMMA X"]},"date":"19 Feb 2015","doc_type":"datatable","doi":"10.17182/hepdata.66985.v1/t3","first_author":{"affiliation":"Yerevan Phys. 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Combined result of electron and muon channels.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1345354/Table 4/csv","json":"https://www.hepdata.net/download/table/ins1345354/Table 4/json","root":"https://www.hepdata.net/download/table/ins1345354/Table 4/root","yaml":"https://www.hepdata.net/download/table/ins1345354/Table 4/yaml","yoda":"https://www.hepdata.net/download/table/ins1345354/Table 4/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"66990","creation_date":"2015-02-19","data_keywords":{"cmenergies":[{"gte":8000.0,"lte":8000.0}],"observables":["SIG"],"phrases":["Inclusive","Proton-Proton Scattering","Cross Section","Integrated Cross Section","Electron production","Z Production","Muon production"],"reactions":["P P --> Z0 GAMMA X"]},"date":"19 Feb 2015","doc_type":"datatable","doi":"10.17182/hepdata.66985.v1/t4","first_author":{"affiliation":"Yerevan Phys. 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Inst.","full_name":"Khachatryan, Vardan"},{"affiliation":"Yerevan Phys. Inst.","full_name":"Sirunyan, Albert M"},{"affiliation":"Yerevan Phys. Inst.","full_name":"Tumasyan, Armen"},{"affiliation":"Vienna, OAW","full_name":"Adam, Wolfgang"},{"affiliation":"Vienna, OAW","full_name":"Bergauer, Thomas"},{"affiliation":"Vienna, OAW","full_name":"Dragicevic, Marko"},{"affiliation":"Vienna, OAW","full_name":"Er\u00f6, Janos"},{"affiliation":"Vienna, OAW","full_name":"Friedl, Markus"},{"affiliation":"Vienna, OAW","full_name":"Fruehwirth, Rudolf"},{"affiliation":"Vienna, OAW","full_name":"Ghete, Vasile Mihai"}],"title":"Measurement of the Z gamma production cross section in pp collisions at 8 TeV and search for anomalous triple gauge boson couplings","total_tables":4,"type":["article"],"uuid":"79147bd8-0752-4602-b672-13f48a5866fd","version":1,"year":"2015"},{"abstract":"The second-order azimuthal anisotropy Fourier harmonics, v2, are obtained in pPb and PbPb collisions over a wide pseudorapidity (eta) range based on correlations among six or more charged particles. The pPb data, corresponding to an integrated luminosity of 35 inverse nanobarns, were collected during the 2013 LHC pPb run at a nucleon-nucleon center-of-mass energy of 5.02 TeV by the CMS experiment. A sample of semi-peripheral PbPb collision data at sqrt(s[NN])= 2.76 TeV, corresponding to an integrated luminosity of 2.5 inverse microbarns and covering a similar range of particle multiplicities as the pPb data, is also analyzed for comparison. The six- and eight-particle cumulant and the Lee-Yang zeros methods are used to extract the v2 coefficients, extending previous studies of two- and four-particle correlations. For both the pPb and PbPb systems, the v2 values obtained with correlations among more than four particles are consistent with previously published four-particle results. These data support the interpretation of a collective origin for the previously observed long-range (large Delta[eta]) correlations in both systems. The ratios of v2 values corresponding to correlations including different numbers of particles are compared to theoretical predictions that assume a hydrodynamic behavior of a pPb system dominated by fluctuations in the positions of participant nucleons. These results provide new insights into the multi-particle dynamics of collision systems with a very small overlapping region.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins1345262/1/csv","json":"https://www.hepdata.net/download/submission/ins1345262/1/json","root":"https://www.hepdata.net/download/submission/ins1345262/1/root","yaml":"https://www.hepdata.net/download/submission/ins1345262/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins1345262/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:1502.05382","authors":["Khachatryan, Vardan","Sirunyan, Albert M","Tumasyan, Armen","Adam, Wolfgang","Bergauer, Thomas","Dragicevic, Marko","Er\u00f6, Janos","Friedl, Markus","Fruehwirth, Rudolf","Ghete, Vasile Mihai"],"collaborations":["CMS"],"control_number":"67530","creation_date":"2015-02-18","data":[{"abstract":"The cumulant $c_2\\{6\\}$ extracted for all charged particles with $0.3 < p_T < 3.0$ GeV/c as a function of $N_{trk}^{offline}$ in PbPb collisions.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1345262/Table 1/csv","json":"https://www.hepdata.net/download/table/ins1345262/Table 1/json","root":"https://www.hepdata.net/download/table/ins1345262/Table 1/root","yaml":"https://www.hepdata.net/download/table/ins1345262/Table 1/yaml","yoda":"https://www.hepdata.net/download/table/ins1345262/Table 1/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"67532","creation_date":"2015-02-18","data_keywords":{"cmenergies":[{"gte":2.76,"lte":2.76}],"observables":["CORR"],"phrases":["Inclusive"],"reactions":["PB PB --> CHARGED X"]},"date":"18 Feb 2015","doc_type":"datatable","doi":"10.17182/hepdata.67530.v1/t1","first_author":{"affiliation":"Yerevan Phys. 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The analysis uses J/psi and psi(2S) dimuon samples collected by CMS, corresponding to integrated luminosities of 4.55 and 4.90 inverse femtobarns, respectively. The results are based on a two-dimensional analysis of the dimuon invariant mass and decay length, and extend to pt = 120 and 100 GeV for the J/psi and psi(2S), respectively, when integrated over the interval abs(y) < 1.2. The ratio of the psi(2S) to J/psi cross sections is also reported for abs(y) < 1.2, over the range 10 < pt < 100 GeV. These are the highest pt values for which the cross sections and ratio have been measured.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins1345023/1/csv","json":"https://www.hepdata.net/download/submission/ins1345023/1/json","root":"https://www.hepdata.net/download/submission/ins1345023/1/root","yaml":"https://www.hepdata.net/download/submission/ins1345023/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins1345023/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:1502.04155","authors":["Khachatryan, Vardan","Sirunyan, Albert M","Tumasyan, Armen","Adam, Wolfgang","Bergauer, Thomas","Dragicevic, Marko","Er\u00f6, Janos","Friedl, Markus","Fruehwirth, Rudolf","Ghete, Vasile Mihai"],"collaborations":["CMS"],"control_number":"66886","creation_date":"2015-02-13","data":[{"abstract":"J/psi double-differential cross section times branching fraction assuming unpolarized production as a function of pT and y for 0.0 < |y| < 0.3, 0.3 < |y| < 0.6, 0.6 < |y| < 0.9 and 0.9 < |y| < 1.2.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1345023/Table 1/csv","json":"https://www.hepdata.net/download/table/ins1345023/Table 1/json","root":"https://www.hepdata.net/download/table/ins1345023/Table 1/root","yaml":"https://www.hepdata.net/download/table/ins1345023/Table 1/yaml","yoda":"https://www.hepdata.net/download/table/ins1345023/Table 1/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"66888","creation_date":"2015-02-13","data_keywords":{"cmenergies":[{"gte":7000.0,"lte":7000.0}],"observables":["D2SIG/DPT/DYRAP"],"phrases":["J/Psi","Prompt","Transverse Momentum Dependence","Double Differential Cross Section","Rapidity Dependence","Muon production","Psi","Proton-Proton Scattering","Inclusive"],"reactions":["P P --> J/PSI X"]},"date":"13 Feb 2015","doc_type":"datatable","doi":"10.17182/hepdata.66886.v1/t1","first_author":{"affiliation":"Yerevan Phys. 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Events with hadronic jets and one or two oppositely charged leptons are selected from a data sample corresponding to an integrated luminosity of 19.5 inverse femtobarns collected by the CMS experiment at the LHC in pp collisions at a centre-of-mass energy of 8 TeV. In order to separate the signal from the larger t t-bar + jets background, this analysis uses a matrix element method that assigns a probability density value to each reconstructed event under signal or background hypotheses. The ratio between the two values is used in a maximum likelihood fit to extract the signal yield. The results are presented in terms of the measured signal strength modifier, mu, relative to the standard model prediction for a Higgs boson mass of 125 GeV. The observed (expected) exclusion limit at a 95% confidence level is mu < 4.2 (3.3), corresponding to a best fit value mu-hat = 1.2 +1.6 -1.5.","access_urls":{"links":{"csv":"https://www.hepdata.net/download/submission/ins1343506/1/csv","json":"https://www.hepdata.net/download/submission/ins1343506/1/json","root":"https://www.hepdata.net/download/submission/ins1343506/1/root","yaml":"https://www.hepdata.net/download/submission/ins1343506/1/yaml","yoda":"https://www.hepdata.net/download/submission/ins1343506/1/yoda"}},"analyses":[],"arxiv_id":"arXiv:1502.02485","authors":["Khachatryan, Vardan","Sirunyan, Albert M","Tumasyan, Armen","Adam, Wolfgang","Bergauer, Thomas","Dragicevic, Marko","Er\u00f6, Janos","Friedl, Markus","Fruehwirth, Rudolf","Ghete, Vasile Mihai"],"collaborations":["CMS"],"control_number":"68402","creation_date":"2015-02-09","data":[{"abstract":"The best-fit values of the signal strength modifier obtained from the single lepton (SL) and dilepton (DL) channels alone,and from their combination (COMBINED). The observed 95% CL upper limit (UL) on mu are given in the third column, and are compared to the median expected limits for both the signal-plus-background and for the background-only hypotheses. For the latter, the 1sigma and 2sigma CL intervals are also given.\n","access_urls":{"links":{"csv":"https://www.hepdata.net/download/table/ins1343506/Table 1/csv","json":"https://www.hepdata.net/download/table/ins1343506/Table 1/json","root":"https://www.hepdata.net/download/table/ins1343506/Table 1/root","yaml":"https://www.hepdata.net/download/table/ins1343506/Table 1/yaml","yoda":"https://www.hepdata.net/download/table/ins1343506/Table 1/yoda"}},"authors":null,"collaborations":["CMS"],"control_number":"68403","creation_date":"2015-02-09","data_keywords":{"cmenergies":[{"gte":8000.0,"lte":8000.0}],"observables":["SIG"],"phrases":["Top","Proton-Proton Scattering","Bottom","Integrated Cross Section","Cross Section","Beauty","Higgs","Inclusive"],"reactions":["P P --> TOP TOPBAR HIGGS X"]},"date":"09 Feb 2015","doc_type":"datatable","doi":"10.17182/hepdata.68402.v1/t1","first_author":{"affiliation":"Yerevan Phys. 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