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Measurement of the Inclusive Leptonic Asymmetry in Top-Quark Pairs that Decay to Two Charged Leptons at CDFMeasurement of B ( t → W b ) / B ( t → W q ) in Top-Quark-Pair Decays Using Dilepton Events and the Full CDF Run II Data SetCombination of Tevatron searches for the standard model Higgs boson in the W+W- decay modeObservation of the Ξ(b)(0) baryonObservation of the Ω b − baryon and measurement of the properties of the Ξ b − and Ω b − baryonsEvidence for a narrow near-threshold structure in the J/psivarphi mass spectrum in B;{+} --> J/psivarphiK;{+} decaysObservation and mass measurement of the baryon Xib-Observation of Bs(0)-Bs(0) oscillationsMeasurement of the mass difference between top and antitop quarksSearch for Z' --> e+ e- using dielectron mass and angular distributionSearch for electroweak single-top-quark production in p p ¯ collisions at s = 1.96 TeVObservation of the Heavy Baryons Σ b and Σ b *Observation of Electroweak Single Top-Quark ProductionMeasurement of the Mass Difference between t and t ¯ QuarksInvariant Mass Distribution of Jet Pairs Produced in Association with a W Boson in p p ¯ Collisions at s = 1.96 TeVSearch for neutral supersymmetric Higgs bosons in pp collisions at sqrt[s] = 1.8TeV.Production of chi(c1) and chi(c2) in pp collisions at sqrt[S] = 1.8 TeV.Inclusive double-pomeron exchange at the fermilab tevatron p p collider.Search for heavy long-lived particles that decay to photons at CDF II.Search for technicolor particles produced in association with a W Boson at CDF.Measurement of the tt production cross section in pp collisions at square root of s = 1.96 TeV.Measurement of the tt production cross section in pp collisions at square root s = 1.96 TeV using missing E(T) + jets events with secondary vertex b tagging.Measurement of the inclusive jet cross section using the kT algorithm in pp collisions at (square root s)=1.96 TeV.Inclusive search for anomalous production of high-pT like-sign lepton pairs in pp collisions at square root s = 1.8 TeV.Evidence for a particle produced in association with weak bosons and decaying to a bottom-antibottom quark pair in higgs boson searches at the tevatron.Search for new physics with a dijet plus missing E(T) signature in pp collisions at √s=1.96 TeV.Search for the production of scalar bottom quarks in pp collisions at square root(s) = 1.96 TeV.Measurement of W-boson polarization in Top-Quark Decay in pp collisions at sqrt[s]=1.96 TeV.Measurement of the ratio σ{tt}/σ{Z/γ{*}→ll} and precise extraction of the tt cross section.Search for pair production of supersymmetric top quarks in dilepton events from pp collisions at sqrt[s]=1.96 TeV.Search for the Higgs boson using neural networks in events with missing energy and b-quark jets in pp collisions at square root(s) = 1.96 TeV.First measurement of the b-jet cross section in events with a W boson in pp collisions at square root(s) = 1.96 TeV.Search for new bottomlike quark pair decays QQ-->(tW(+)(-))(tW(+)(-)in same-charge dilepton events.Inclusive search for standard model Higgs boson production in the WW decay channel using the CDF II detector.Measurement of the Lambdab0 lifetime in Lambdab0 --> Lambdac+pi- decays in pp collisions at square root of s = 1.96 TeV.Measurement of the WW + WZ production cross section using the lepton + jets final state at CDF II.Search for supersymmetry with gauge-mediated breaking in diphoton events with missing transverse energy at CDF II.Search for the associated production of the standard-model Higgs Boson in the all-hadronic channel.Search for Higgs bosons predicted in two-Higgs-doublet models via decays to tau lepton pairs in 1.96 TeV pp collisions.First observation of B(s)(0) --> D(s)(+/-)K(-/+) and measurement of the ratio of branching fractions B(B(s)(0) --> D(s)(+/-)K(-/+)/B(B(s)(0) --> D(s)(+)pi(-)).
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Q21706455-E891D213-14D9-472B-ADE0-7256047EFE22Q21706460-AC91A707-7F31-4E3B-A55A-917630933591Q27335465-F281B027-B8A9-460E-9A0C-BF940BEB8C87Q27335527-7C533C3A-A65E-457E-84A1-BBCC19BFEC4BQ27342528-A241F696-2C64-4587-BBB2-C3A3C8CDC329Q27345023-105C9921-A819-492E-B240-A86D991466E4Q27345269-FA4BC7E7-CF38-4A36-99C9-86B56B3DCFDBQ27346516-33A8D15B-F94B-4AC0-984D-9218F7C3ECD6Q27346539-0728B01D-E6C2-4879-AC5B-C74A43650B13Q27348469-B5404D14-39A2-4BDE-8525-6CD7446553A1Q27349493-95A6CCA7-A614-472E-9954-C89AF814C8D4Q27350056-5D1E609F-23A1-4F72-8A86-338C89452B83Q27446505-F25F54FC-99C7-464C-AE5A-D5441476394AQ27448063-BC0D97A4-0FB3-4FBA-8F15-4AE6C201D86FQ27448103-A66252E5-D6B4-41A7-B1EE-5F0560546D49Q50232522-DEB77ADE-A968-45B9-8370-10656E0CC1BEQ50232527-70CEF932-40A2-4514-9C43-7BEF5C38E996Q50787533-61516170-B04E-4DFF-BCAC-8093CBBF859DQ50891660-68E86848-1164-43C6-8AB4-50B90A25990BQ51707577-806F283D-7789-4D1D-9957-77D4376C82A5Q51931620-D4883DCC-2959-4B5A-AA41-FA31AD35C8B8Q51938898-D5AAE617-1E3F-4479-8417-41BA5BEA8027Q51944029-8F16EA11-3C27-4A17-986C-A97EFF12743CQ52966415-9FECB01B-7C09-4023-A3FA-4CAF1DDBC19BQ53359586-FD4556B7-388E-464A-92E2-49547E3FB51BQ53442978-1E03BE79-BF08-40B1-B2AB-1FB79D0FA4F6Q53457037-C09921DB-310B-4070-ACE3-E218D5AA1D6AQ53457108-ECF7EA4B-C85C-42E2-822C-333B676DD47CQ53457222-6010FB66-96A1-4226-8F36-F28811D4305FQ53457249-5294F45B-CF39-4C06-ABFE-59E319B70BA3Q53470405-A274625B-5861-4B6A-BE89-E1B4CC321557Q53470438-41A88084-1860-4189-A315-F779D548FB19Q53474756-6FADB4B5-8C4E-47AD-BB76-83B7A4E33635Q53474794-437CC94A-DECD-4805-8D4A-05AB23FE9D43Q53474875-A4680876-20A1-43E4-9B71-4E275CFBD3ABQ53474883-BA396F5F-2784-4295-8582-B8B0C7464A75Q53474907-C025406E-5107-43DD-9C08-2374C2BBA077Q53474973-1E280011-E767-40D3-BA5F-FE5F6FF93D3EQ53475024-BF762827-771C-421E-B9AF-2A7E25E39692Q53475050-386AAAE5-883C-4409-B3BD-43B81BA1C3C3
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description
hulumtues
@sq
researcher
@en
wetenschapper
@nl
հետազոտող
@hy
name
M Lancaster
@nl
M Lancaster
@sl
Mark Lancaster
@en
Mark Lancaster
@es
type
label
M Lancaster
@nl
M Lancaster
@sl
Mark Lancaster
@en
Mark Lancaster
@es
altLabel
M Lancaster
@en
prefLabel
M Lancaster
@nl
M Lancaster
@sl
Mark Lancaster
@en
Mark Lancaster
@es
P108
P1053
F-5254-2018
P106
P1153
35227504300
P21
P31
P3829
P496
0000-0002-8872-7292