Mazur, Adam

[["dc.bibliographiccitation.firstpage","165"],["dc.bibliographiccitation.issue","3"],["dc.bibliographiccitation.journal","Physics Letters B"],["dc.bibliographiccitation.lastpage","171"],["dc.bibliographiccitation.volume","713"],["dc.contributor.author","Abazov, V. M."],["dc.contributor.author","Abbott, B."],["dc.contributor.author","Acharya, B. S."],["dc.contributor.author","Adams, M."],["dc.contributor.author","Adams, T."],["dc.contributor.author","Alexeev, G. D."],["dc.contributor.author","Alkhazov, G."],["dc.contributor.author","Alton, A."],["dc.contributor.author","Alverson, G."],["dc.contributor.author","Aoki, M."],["dc.contributor.authorgroup","D0 Collaboration"],["dc.date.accessioned","2015-01-27T08:42:02Z"],["dc.date.accessioned","2021-10-11T11:34:06Z"],["dc.date.available","2015-01-27T08:42:02Z"],["dc.date.available","2021-10-11T11:34:06Z"],["dc.date.issued","2012"],["dc.description.abstract","We present measurements of the tWb coupling form factors using information from electroweak single top quark production and from the helicity of W bosons from top quark decays in t¯t events. We set upper limits on anomalous tWb coupling form factors using data collected with the D0 detector at the Tevatron p¯p collider corresponding to an integrated luminosity of 5.4 fb−1."],["dc.identifier.doi","10.1016/j.physletb.2012.05.048"],["dc.identifier.purl","https://resolver.sub.uni-goettingen.de/purl?gs-1/11530"],["dc.identifier.uri","https://resolver.sub.uni-goettingen.de/purl?gro-2/90647"],["dc.language.iso","en"],["dc.notes.intern","Migrated from goescholar"],["dc.relation.issn","0370-2693"],["dc.relation.issn","0370-2693"],["dc.relation.orgunit","Fakultät für Physik"],["dc.rights","CC BY 3.0"],["dc.rights.access","openAccess"],["dc.rights.uri","https://creativecommons.org/licenses/by/3.0/"],["dc.subject","anomalous top quark couplings; p¯p collisions"],["dc.title","Combination of searches for anomalous top quark couplings with 5.4 fb−1 of pp collisions"],["dc.type","journal_article"],["dc.type.internalPublication","yes"],["dc.type.peerReviewed","yes"],["dc.type.version","submitted_version"],["dspace.entity.type","Publication"]]

[["dc.bibliographiccitation.firstpage","224"],["dc.bibliographiccitation.issue","3"],["dc.bibliographiccitation.journal","Physics Letters B"],["dc.bibliographiccitation.lastpage","232"],["dc.bibliographiccitation.volume","681"],["dc.contributor.author","Abazov, V. M."],["dc.contributor.author","Abbott, B."],["dc.contributor.author","Abolins, M."],["dc.contributor.author","Acharya, B. S."],["dc.contributor.author","Adams, M."],["dc.contributor.author","Adams, T."],["dc.contributor.author","Aguilo, E."],["dc.contributor.author","Ahsan, M."],["dc.contributor.author","Alexeev, G. D."],["dc.contributor.author","Alkhazov, G."],["dc.contributor.author","Zverev, E. G."],["dc.date.accessioned","2014-12-12T09:00:14Z"],["dc.date.accessioned","2021-10-11T11:23:57Z"],["dc.date.available","2014-12-12T09:00:14Z"],["dc.date.available","2021-10-11T11:23:57Z"],["dc.date.issued","2009"],["dc.description.abstract","A search for pair production of first-generation leptoquarks (LQ ) is performed with data collected by the DØ experiment in View the MathML sourcepp¯ collisions at View the MathML sources=1.96 TeV at the Fermilab Tevatron Collider. In a sample of data corresponding to ∼1 fb−1∼1 fb−1 the search has been performed on the final states with two electrons and two jets or one electron, two jets and missing transverse energy. We find our data consistent with standard model expectations. The results are combined with those found in a previous analysis of events with two jets and missing transverse energy to obtain scalar LQ mass limits. We set 95% C.L. lower limits on a scalar LQ mass of 299 GeV, 284 GeV and 216 GeV for β=1β=1, β=0.5β=0.5 and β=0.02β=0.02 respectively, where β is the LQ branching ratio in the eq channel. This improves the results obtained with a lower luminosity sample from Run II of the Tevatron. Lower limits on vector LQ masses with different couplings from 357 GeV to 464 GeV for β=0.5β=0.5 are also set using this analysis."],["dc.identifier.doi","10.1016/j.physletb.2009.10.016"],["dc.identifier.purl","https://resolver.sub.uni-goettingen.de/purl?gs-1/11294"],["dc.identifier.uri","https://resolver.sub.uni-goettingen.de/purl?gro-2/90463"],["dc.language.iso","en"],["dc.notes.intern","Migrated from goescholar"],["dc.relation.issn","0370-2693"],["dc.relation.issn","0370-2693"],["dc.relation.orgunit","Fakultät für Physik"],["dc.rights","CC BY 3.0"],["dc.rights.access","openAccess"],["dc.rights.uri","https://creativecommons.org/licenses/by/3.0/"],["dc.subject","pair production; leptoquarks"],["dc.title","Measurement of direct photon pair production cross sections in p¯p collisions at √s = 1.96 TeV"],["dc.type","journal_article"],["dc.type.internalPublication","yes"],["dc.type.peerReviewed","yes"],["dc.type.version","published_version"],["dspace.entity.type","Publication"]]

[["dc.bibliographiccitation.firstpage","56"],["dc.bibliographiccitation.issue","1"],["dc.bibliographiccitation.journal","Physics Letters B"],["dc.bibliographiccitation.lastpage","63"],["dc.bibliographiccitation.volume","718"],["dc.contributor.author","Abazov, V. M."],["dc.contributor.author","Abbott, B."],["dc.contributor.author","Acharya, B. S."],["dc.contributor.author","Adams, M."],["dc.contributor.author","Adams, T."],["dc.contributor.author","Alexeev, G. D."],["dc.contributor.author","Alkhazov, G."],["dc.contributor.author","Alton, A."],["dc.contributor.author","Alverson, G."],["dc.contributor.author","Askew, A."],["dc.contributor.authorgroup","D0 Collaboration"],["dc.date.accessioned","2015-01-23T16:56:47Z"],["dc.date.accessioned","2021-10-11T11:34:29Z"],["dc.date.available","2015-01-23T16:56:47Z"],["dc.date.available","2021-10-11T11:34:29Z"],["dc.date.issued","2012"],["dc.description.abstract","We present a measurement of the average value of a new observable at hadron colliders that is sensitive to QCD dynamics and to the strong coupling constant, while being only weakly sensitive to parton distribution functions. The observable measures the angular correlations of jets and is defined as the number of neighboring jets above a given transverse momentum threshold which accompany a given jet within a given distance R in the plane of rapidity and azimuthal angle. The ensemble average over all jets in an inclusive jet sample is measured and the results are presented as a function of transverse momentum of the inclusive jets, in different regions of R and for different transverse momentum requirements for the neighboring jets. The measurement is based on a data set corresponding to an integrated luminosity of 0.7 fb−1 collected with the D0 detector at the Fermilab Tevatron Collider in p¯p collisions at √ s = 1.96 TeV. The results are well described by a perturbative QCD calculation in next-toleading order in the strong coupling constant, corrected for non-perturbative effects. From these results, we extract the strong coupling and test the QCD predictions for its running over a range of momentum transfers of 50–400 GeV."],["dc.identifier.doi","10.1016/j.physletb.2012.10.003"],["dc.identifier.purl","https://resolver.sub.uni-goettingen.de/purl?gs-1/11514"],["dc.identifier.uri","https://resolver.sub.uni-goettingen.de/purl?gro-2/90676"],["dc.language.iso","en"],["dc.notes.intern","Migrated from goescholar"],["dc.relation.issn","0370-2693"],["dc.relation.issn","0370-2693"],["dc.relation.orgunit","Fakultät für Physik"],["dc.rights","CC BY 3.0"],["dc.rights.access","openAccess"],["dc.rights.uri","https://creativecommons.org/licenses/by/3.0/"],["dc.subject","angular correlations of jets; strong coupling; high momentum transfers"],["dc.title","Measurement of angular correlations of jets at √ s = 1.96 TeV and determination of the strong coupling at high momentum transfers"],["dc.type","journal_article"],["dc.type.internalPublication","yes"],["dc.type.peerReviewed","yes"],["dc.type.version","published_version"],["dspace.entity.type","Publication"]]

[["dc.bibliographiccitation.firstpage","515"],["dc.bibliographiccitation.issue","5"],["dc.bibliographiccitation.journal","Physics Letters B"],["dc.bibliographiccitation.lastpage","521"],["dc.bibliographiccitation.volume","693"],["dc.contributor.author","Abazov, V. M."],["dc.contributor.author","Abbott, B."],["dc.contributor.author","Abolins, M."],["dc.contributor.author","Acharya, B. S."],["dc.contributor.author","Adams, M."],["dc.contributor.author","Adams, T."],["dc.contributor.author","Aguilo, E."],["dc.contributor.author","Alexeev, G. D."],["dc.contributor.author","Alkhazov, G."],["dc.contributor.author","Alton, A."],["dc.contributor.author","Zverev, E. G."],["dc.date.accessioned","2014-12-12T08:32:58Z"],["dc.date.accessioned","2021-10-11T11:19:31Z"],["dc.date.available","2014-12-12T08:32:58Z"],["dc.date.available","2021-10-11T11:19:31Z"],["dc.date.issued","2010"],["dc.description.abstract","We present a measurement of the differential cross section for View the MathML sourcett¯ events produced in View the MathML sourcepp¯ collisions at View the MathML sources=1.96 TeV as a function of the transverse momentum (pTpT) of the top quark. The selected events contain a high-pTpT lepton (ℓ ), a large imbalance in pTpT, four or more jets with at least one candidate for a b jet, and correspond to 1 fb−1 of integrated luminosity recorded with the D0 detector. Objects in the event are associated through a constrained kinematic fit to the View the MathML sourcett¯→WbWb¯→ℓνbqq¯′b¯ process. Results from next and next-to-next-to-leading-order perturbative QCD calculations agree with the measured differential cross section. Comparisons are also provided to predictions from Monte Carlo event generators using QCD calculations at different levels of precision."],["dc.identifier.doi","10.1016/j.physletb.2010.09.011"],["dc.identifier.purl","https://resolver.sub.uni-goettingen.de/purl?gs-1/11287"],["dc.identifier.uri","https://resolver.sub.uni-goettingen.de/purl?gro-2/90459"],["dc.language.iso","en"],["dc.notes.intern","Migrated from goescholar"],["dc.relation.issn","0370-2693"],["dc.relation.orgunit","Fakultät für Physik"],["dc.rights","CC BY 3.0"],["dc.rights.access","openAccess"],["dc.rights.uri","https://creativecommons.org/licenses/by/3.0/"],["dc.subject","Top quark; Differential cross sections; Perturbative QCD"],["dc.title","Dependence of the t¯t production cross section on the transverse momentum of the top quark"],["dc.type","journal_article"],["dc.type.internalPublication","yes"],["dc.type.peerReviewed","yes"],["dc.type.version","published_version"],["dspace.entity.type","Publication"]]

[["dc.bibliographiccitation.firstpage","451"],["dc.bibliographiccitation.issue","2"],["dc.bibliographiccitation.journal","Physics Letters B"],["dc.bibliographiccitation.lastpage","459"],["dc.bibliographiccitation.volume","718"],["dc.contributor.author","Abazov, V. M."],["dc.contributor.author","Abbott, B."],["dc.contributor.author","Acharya, B. S."],["dc.contributor.author","Adams, M."],["dc.contributor.author","Adams, T."],["dc.contributor.author","Alexeev, G. D."],["dc.contributor.author","Alkhazov, G."],["dc.contributor.author","Alton, A."],["dc.contributor.author","Askew, A."],["dc.contributor.author","Atkins, S."],["dc.contributor.authorgroup","D0 Collaboration"],["dc.date.accessioned","2015-01-27T09:00:46Z"],["dc.date.accessioned","2021-10-11T11:35:16Z"],["dc.date.available","2015-01-27T09:00:46Z"],["dc.date.available","2021-10-11T11:35:16Z"],["dc.date.issued","2012"],["dc.description.abstract","We present searches for the anomalous γWW and ZWW trilinear gauge boson couplings from WW and W Z production using lepton plus dijet final states and a combination with results from Wγ , WW, and W Z production with leptonic final states. The analyzed data correspond to up to 8.6 fb−1 of integrated luminosity collected by the D0 detector in p¯p collisions at √ s = 1.96 TeV. We set the most stringent limits at a hadron collider to date assuming two different relations between the anomalous coupling parameters κγ , λ, and g Z 1 for a cutoff energy scale Λ = 2 TeV. The combined 68% C.L. limits are −0.057< κγ < 0.154, −0.015 < λ < 0.028, and −0.008< g Z 1 < 0.054 for the LEP parameterization, and −0.007< κ < 0.081 and −0.017 < λ < 0.028 for the equal couplings parameterization. We also present the most stringent limits of the W boson magnetic dipole and electric quadrupole moments."],["dc.identifier.doi","10.1016/j.physletb.2012.10.062"],["dc.identifier.purl","https://resolver.sub.uni-goettingen.de/purl?gs-1/11532"],["dc.identifier.uri","https://resolver.sub.uni-goettingen.de/purl?gro-2/90742"],["dc.language.iso","en"],["dc.notes.intern","Migrated from goescholar"],["dc.relation.issn","0370-2693"],["dc.relation.issn","0370-2693"],["dc.relation.orgunit","Fakultät für Physik"],["dc.rights","CC BY 3.0"],["dc.rights.access","openAccess"],["dc.rights.uri","https://creativecommons.org/licenses/by/3.0/"],["dc.subject","anomalous trilinear gauge boson couplings; pp collisions"],["dc.title","Limits on anomalous trilinear gauge boson couplings from WW, WZ and Wγ production in pp collisions at √ s = 1.96 TeV"],["dc.type","journal_article"],["dc.type.internalPublication","yes"],["dc.type.peerReviewed","yes"],["dc.type.version","published_version"],["dspace.entity.type","Publication"]]

[["dc.bibliographiccitation.firstpage","422"],["dc.bibliographiccitation.issue","4"],["dc.bibliographiccitation.journal","Physics Letters B"],["dc.bibliographiccitation.lastpage","427"],["dc.bibliographiccitation.volume","703"],["dc.contributor.author","Abazov, V. M."],["dc.contributor.author","Abbott, B."],["dc.contributor.author","Acharya, B. S."],["dc.contributor.author","Adams, M."],["dc.contributor.author","Adams, T."],["dc.contributor.author","Alexeev, G. D."],["dc.contributor.author","Alkhazov, G."],["dc.contributor.author","Alton, A."],["dc.contributor.author","Alverson, G."],["dc.contributor.author","Alves, G. A."],["dc.contributor.authorgroup","D0 Collaboration"],["dc.date.accessioned","2015-01-26T16:01:49Z"],["dc.date.accessioned","2021-10-11T11:34:53Z"],["dc.date.available","2015-01-26T16:01:49Z"],["dc.date.available","2021-10-11T11:34:53Z"],["dc.date.issued","2011"],["dc.description.abstract","We use higher-order quantum chromodynamics calculations to extract the mass of the top quark from the t¯t cross section measured in the lepton + jets channel in p¯p collisions at √ s = 1.96 TeV using 5.3 fb−1 of integrated luminosity collected by the D0 experiment at the Fermilab Tevatron Collider. The extracted top quark pole mass and MS mass are compared to the current Tevatron average top quark mass obtained from direct measurements."],["dc.identifier.doi","10.1016/j.physletb.2011.08.015"],["dc.identifier.purl","https://resolver.sub.uni-goettingen.de/purl?gs-1/11523"],["dc.identifier.uri","https://resolver.sub.uni-goettingen.de/purl?gro-2/90711"],["dc.language.iso","en"],["dc.notes.intern","Migrated from goescholar"],["dc.relation.issn","0370-2693"],["dc.relation.issn","0370-2693"],["dc.relation.orgunit","Fakultät für Physik"],["dc.rights","CC BY 3.0"],["dc.rights.access","openAccess"],["dc.rights.uri","https://creativecommons.org/licenses/by/3.0/"],["dc.subject","top quark;"],["dc.title","Determination of the pole and MS¯ masses of the top quark from the tt¯ cross section"],["dc.type","journal_article"],["dc.type.internalPublication","yes"],["dc.type.peerReviewed","yes"],["dc.type.version","published_version"],["dspace.entity.type","Publication"]]

[["dc.bibliographiccitation.firstpage","539"],["dc.bibliographiccitation.issue","5"],["dc.bibliographiccitation.journal","Physics Letters B"],["dc.bibliographiccitation.lastpage","544"],["dc.bibliographiccitation.volume","693"],["dc.contributor.author","Abazov, V. M."],["dc.contributor.author","Abbott, B."],["dc.contributor.author","Abolins, M."],["dc.contributor.author","Acharya, B. S."],["dc.contributor.author","Adams, M."],["dc.contributor.author","Adams, T."],["dc.contributor.author","Alexeev, G. D."],["dc.contributor.author","Alkhazov, G."],["dc.contributor.author","Alton, A."],["dc.contributor.author","Alverson, G."],["dc.contributor.author","Zivkovic, L."],["dc.date.accessioned","2014-12-12T08:20:40Z"],["dc.date.accessioned","2021-10-11T11:19:28Z"],["dc.date.available","2014-12-12T08:20:40Z"],["dc.date.available","2021-10-11T11:19:28Z"],["dc.date.issued","2010"],["dc.description.abstract","We present the results of a search for the flavor changing neutral current decay View the MathML sourceBs0→μ+μ− using 6.1 fb−16.1 fb−1 of View the MathML sourcepp¯ collisions at View the MathML sources=1.96 TeV collected by the D0 experiment at the Fermilab Tevatron Collider. The observed number of View the MathML sourceBs0 candidates is consistent with background expectations. The resulting upper limit on the branching fraction is View the MathML sourceB(Bs0→μ+μ−)<5.1×10−8 at the 95% C.L. This limit is a factor of 2.4 better than that of the previous D0 analysis and the best limit to date."],["dc.identifier.doi","10.1016/j.physletb.2010.09.024"],["dc.identifier.purl","https://resolver.sub.uni-goettingen.de/purl?gs-1/11284"],["dc.identifier.uri","https://resolver.sub.uni-goettingen.de/purl?gro-2/90456"],["dc.language.iso","en"],["dc.notes.intern","Migrated from goescholar"],["dc.relation.issn","0370-2693"],["dc.relation.orgunit","Fakultät für Physik"],["dc.rights","CC BY 3.0"],["dc.rights.access","openAccess"],["dc.rights.uri","https://creativecommons.org/licenses/by/3.0/"],["dc.subject","b-quarks; Rare decays"],["dc.title","Search for the rare decay B0s →μ+μ−"],["dc.type","journal_article"],["dc.type.internalPublication","yes"],["dc.type.peerReviewed","yes"],["dc.type.version","published_version"],["dspace.entity.type","Publication"]]

[["dc.bibliographiccitation.firstpage","285"],["dc.bibliographiccitation.issue","2"],["dc.bibliographiccitation.journal","Physics Letters B"],["dc.bibliographiccitation.lastpage","293"],["dc.bibliographiccitation.volume","716"],["dc.contributor.author","Abazov, V. M."],["dc.contributor.author","Abbott, B."],["dc.contributor.author","Acharya, B. S."],["dc.contributor.author","Adams, M."],["dc.contributor.author","Adams, T."],["dc.contributor.author","Alexeev, G. D."],["dc.contributor.author","Alkhazov, G."],["dc.contributor.author","Alton, A."],["dc.contributor.author","Alverson, G."],["dc.contributor.author","Askew, A."],["dc.contributor.authorgroup","D0 Collaboration"],["dc.date.accessioned","2015-01-27T09:04:04Z"],["dc.date.accessioned","2021-10-11T11:35:18Z"],["dc.date.available","2015-01-27T09:04:04Z"],["dc.date.available","2021-10-11T11:35:18Z"],["dc.date.issued","2012"],["dc.description.abstract","We present a search for the standard model Higgs boson in 9.5 fb−1 of p¯p collisions at √ s = 1.96 TeV collected with the D0 detector at the Fermilab Tevatron Collider. The final state considered contains a pair of b jets and is characterized by an imbalance in transverse energy, as expected from p¯p → ZH → ν¯ν b¯b production. The search is also sensitive to the WH → νb¯b channel when the charged lepton is not identified. The data are found to be in good agreement with the expected background. For a Higgs boson mass of 125 GeV, we set a limit at the 95% C.L. on the cross section σ(p¯p →[Z/W]H), assuming standard model branching fractions, that is a factor of 4.3 times larger than the theoretical standard model value, while the expected factor is 3.9. The search is also used to measure a combined W Z and Z Z production cross section that is a factor of 0.94 ± 0.31 (stat) ± 0.34 (syst) times the standard model prediction of 4.4 pb, with an observed significance of 2.0 standard deviations."],["dc.identifier.doi","10.1016/j.physletb.2012.08.034"],["dc.identifier.purl","https://resolver.sub.uni-goettingen.de/purl?gs-1/11533"],["dc.identifier.uri","https://resolver.sub.uni-goettingen.de/purl?gro-2/90746"],["dc.language.iso","en"],["dc.notes.intern","Migrated from goescholar"],["dc.relation.issn","0370-2693"],["dc.relation.issn","0370-2693"],["dc.relation.orgunit","Fakultät für Physik"],["dc.rights","CC BY 3.0"],["dc.rights.access","openAccess"],["dc.rights.uri","https://creativecommons.org/licenses/by/3.0/"],["dc.subject","Higgs boson; pp collisions"],["dc.title","Search for the standard model Higgs boson in the ZH →ν¯νb¯b channel in 9.5 fb−1 of p¯p collisions at √ s = 1.96 TeV"],["dc.type","journal_article"],["dc.type.internalPublication","yes"],["dc.type.peerReviewed","yes"],["dc.type.version","published_version"],["dspace.entity.type","Publication"]]

[["dc.bibliographiccitation.firstpage","1314"],["dc.bibliographiccitation.issue","4-5"],["dc.bibliographiccitation.journal","Physics Letters B"],["dc.bibliographiccitation.lastpage","1320"],["dc.bibliographiccitation.volume","718"],["dc.contributor.author","Abazov, V. M."],["dc.contributor.author","Abbott, B."],["dc.contributor.author","Acharya, B. S."],["dc.contributor.author","Adams, M."],["dc.contributor.author","Adams, T."],["dc.contributor.author","Alexeev, G. D."],["dc.contributor.author","Alkhazov, G."],["dc.contributor.author","Alton, A."],["dc.contributor.author","Askew, A."],["dc.contributor.author","Atkins, S."],["dc.contributor.authorgroup","D0 Collaboration"],["dc.date.accessioned","2015-01-27T09:21:48Z"],["dc.date.accessioned","2021-10-11T11:36:07Z"],["dc.date.available","2015-01-27T09:21:48Z"],["dc.date.available","2021-10-11T11:36:07Z"],["dc.date.issued","2013"],["dc.description.abstract","We present a measurement of the cross section for W boson production in association with at least one b-quark jet in proton–antiproton collisions. The measurement is made using data corresponding to an integrated luminosity of 6.1 fb−1 recorded with the D0 detector at the Fermilab Tevatron p¯p √ Collider at s = 1.96 TeV. We measure an inclusive cross section of σ(W(→μν) + b + X) = 1.04 ± 0.05 (stat.) ± 0.12 (syst.) pb and σ(W(→eν)+b+ X) = 1.00±0.04 (stat.)±0.12 (syst.) pb in the phase space defined by pνT > 25 GeV, pb-jet T > 20 GeV, "],["dc.identifier.doi","10.1016/j.physletb.2012.12.044"],["dc.identifier.purl","https://resolver.sub.uni-goettingen.de/purl?gs-1/11535"],["dc.identifier.uri","https://resolver.sub.uni-goettingen.de/purl?gro-2/90758"],["dc.language.iso","en"],["dc.notes.intern","Migrated from goescholar"],["dc.relation.issn","0370-2693"],["dc.relation.issn","0370-2693"],["dc.relation.orgunit","Fakultät für Physik"],["dc.rights","CC BY 3.0"],["dc.rights.access","openAccess"],["dc.rights.uri","https://creativecommons.org/licenses/by/3.0/"],["dc.subject","production; cross section;"],["dc.title","Measurement of the pp →W +b + X production cross section at √ s = 1.96 TeV"],["dc.type","journal_article"],["dc.type.internalPublication","yes"],["dc.type.peerReviewed","yes"],["dc.type.version","published_version"],["dspace.entity.type","Publication"]]

[["dc.bibliographiccitation.firstpage","6"],["dc.bibliographiccitation.issue","1"],["dc.bibliographiccitation.journal","Physics Letters B"],["dc.bibliographiccitation.lastpage","13"],["dc.bibliographiccitation.volume","698"],["dc.contributor.author","Abazov, V. M."],["dc.contributor.author","Abbott, B."],["dc.contributor.author","Acharya, B. S."],["dc.contributor.author","Adams, M."],["dc.contributor.author","Adams, T."],["dc.contributor.author","Alexeev, G. D."],["dc.contributor.author","Alkhazov, G."],["dc.contributor.author","Alton, A."],["dc.contributor.author","Alverson, G."],["dc.contributor.author","Alves, G. A."],["dc.contributor.author","Zivkovic, L."],["dc.date.accessioned","2015-01-26T16:24:43Z"],["dc.date.accessioned","2021-10-11T11:34:55Z"],["dc.date.available","2015-01-26T16:24:43Z"],["dc.date.available","2021-10-11T11:34:55Z"],["dc.date.issued","2011"],["dc.description.abstract","We present a search for associated production of Higgs and W bosons in p¯p collisions at a center of mass energy of √ s = 1.96 TeV in 5.3 fb−1 of integrated luminosity recorded by the D0 experiment. Multivariate analysis techniques are applied to events containing one lepton, an imbalance in transverse energy, and one or two b-tagged jets to discriminate a potential WH signal from Standard Model backgrounds. We observe good agreement between data and expected backgrounds, and set an upper limit of 4.5 (at 95% confidence level and for mH = 115 GeV) on the ratio of the WH cross section multiplied by the branching fraction of H →b¯b to its Standard Model prediction, which is consistent with an expected limit of 4.8."],["dc.identifier.doi","10.1016/j.physletb.2011.02.036"],["dc.identifier.purl","https://resolver.sub.uni-goettingen.de/purl?gs-1/11526"],["dc.identifier.uri","https://resolver.sub.uni-goettingen.de/purl?gro-2/90714"],["dc.language.iso","en"],["dc.notes.intern","Migrated from goescholar"],["dc.relation.issn","0370-2693"],["dc.relation.orgunit","Fakultät für Physik"],["dc.rights","CC BY 3.0"],["dc.rights.access","openAccess"],["dc.rights.uri","https://creativecommons.org/licenses/by/3.0/"],["dc.subject","Tevatron; Standard Model; Higgs boson; Electroweak symmetry breaking"],["dc.title","Search for WH associated production in 5.3 fb−1 of pp¯ collisions at the Fermilab Tevatron"],["dc.type","journal_article"],["dc.type.internalPublication","yes"],["dc.type.peerReviewed","yes"],["dc.type.version","published_version"],["dspace.entity.type","Publication"]]