about
Charged-particle multiplicities in pp interactions at root s=900 GeV measured with the ATLAS detector at the LHC ATLAS CollaborationObservation of Associated Near-Side and Away-Side Long-Range Correlations in s N N = 5.02 TeV Proton-Lead Collisions with the ATLAS DetectorThe ATLAS Experiment at the CERN Large Hadron ColliderCombination of Tevatron searches for the standard model Higgs boson in the W+W- decay modeBounds on an anomalous dijet resonance in W+jets production in pp collisions at √s = 1.96 TeVSearch for Supersymmetry Using Final States with One Lepton, Jets, and Missing Transverse Momentum with the ATLAS Detector in s = 7 TeV p p CollisionsDirect observation of the strange b baryon Xib-Measurement of the Bs(0) lifetime using semileptonic decaysObservation and properties of the X(3872) decaying to J/psipi(+)pi(-) in pp collisions at sqrt[s]=1.96 TeVSimultaneous measurement of the ratio R=B(t --> Wb)/B(t --> Wq) and the top-quark pair production cross section with the D0 detector at sqrt(s) = 1.96 TeVSearch for next-to-minimal supersymmetric Higgs bosons in the h --> aa --> micromicromicromicro, micromicrotautau channels using pp[over] collisions at sqrt[s] = 1.96 TeVExperimental Discrimination between Charge 2 e / 3 Top Quark and Charge 4 e / 3 Exotic Quark Production ScenariosObservation of Single Top-Quark ProductionDirect Limits on the B s 0 Oscillation FrequencyDirect measurement of the mass difference between top and antitop quarksMeasurement of the anomalous like-sign dimuon charge asymmetry with 9 fb − 1 of p p ¯ collisionsObservation of the Doubly Strange b Baryon Ω b −Direct Measurement of the Mass Difference between Top and Antitop QuarksEvidence for Production of Single Top Quarks and First Direct Measurement of | V t b |A precision measurement of the mass of the top quark.Search for resonant pair production of neutral long-lived particles decaying to bb in pp collisions at square root(S)=1.96 TeV.Measurement of dijet azimuthal decorrelations at central rapidities in pp collisions at sqrt s =1.96 TeV.Measurement of the B0s lifetime in the exclusive decay channel B0s-->J/psiphi.Search for supersymmetry with gauge-mediated breaking in diphoton events at D0.Search for doubly charged higgs boson pair production in the decay to mu(+)mu(+)mu(-)mu(-) in pp collisions at sqrt[s]=1.96 TeV.Search for narrow tt resonances in pp collisions at square root of (s)=1.8 TeV.Measurement of the forward-backward charge asymmetry in top-quark pair production.Search for anomalous heavy-flavor quark production in association with W bosons.Measurement of the semileptonic charge asymmetry using B(s)(0) → D(s)μX decays.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 the standard model Higgs boson in associated WH production in 9.7 fb(-1) of pp collisions with the D0 detector.Measurements of WW and WZ production in W + jets final states in pp collisions.Search for universal extra dimensions in pp collisions.Evidence for spin correlation in t ̅t production.Wγ production and limits on anomalous WWγ couplings in pp collisions at sqrt[s] = 1.96 TeV.Search for a fermiophobic and standard model Higgs boson in diphoton final states.Precision measurement of the ratio B(t→Wb)/B(t→Wq) and extraction of V(tb).Search for neutral minimal supersymmetric standard model Higgs bosons decaying to tau pairs produced in association with b quarks in pp collisions at √s = 1.96 TeV.Precise measurement of the top quark mass in the dilepton channel at D0.Search for a fourth generation t' Quark in p ̄p collisions at √s = 1.96 TeV.
P50
Q21521425-FB31FA64-A242-4413-ABEA-7453851FFF5BQ21559757-8ADE1BC0-02A0-4E0D-8B82-082A7359BE70Q21994528-97D0CEB6-F51D-4001-BD62-955F092A73E1Q27335465-4BB5BC34-82BF-4300-B5CE-DD7757DC9BC0Q27335913-586B9680-72BC-4C11-A34A-19BC9A5A0F1EQ27336831-EA9CC231-9DB0-46F9-B67D-8A3B2CB7C806Q27339572-02D26E6B-8CA3-4B9C-AEEB-80CD08E56B63Q27340392-8AB7AA34-DD73-4D02-B408-B95E5A7A4B2AQ27345508-23AE22B2-E767-4DA0-A2DE-BA245AB4CA0FQ27348257-17FC8B81-4719-41CB-A20D-15DD34E930E7Q27348927-1EEDD590-D01A-44FD-90E1-119090A3B479Q27349997-A75F2FC0-5A85-4B36-A1C8-8251B57C9544Q27350445-0DB4F77D-AA00-44A7-85FE-A246BF95BC86Q27350737-10C0A6EB-90D9-4CF0-AB5E-5C97E2CAD348Q27444296-EB4A4E91-8718-4846-9BE2-CC70E43A6A80Q27444420-1AE52587-FD16-4D9B-A504-6E2CAC971651Q27445657-3913F598-E99B-444B-AAD4-672DE0512C73Q27447182-34E7C933-B995-4AF0-960E-F65C8AF6D796Q27454610-B63E530A-97E0-4266-8F13-80D9FCB3CC29Q39128523-77AB8664-ABF4-40E9-AE24-42BED948EFC6Q48834547-90BF2B99-6FE1-40CC-8ADE-E43A94ECB02DQ50759063-13A90C01-9389-4FA7-A11D-EF9B9CD13423Q50774179-75BFF143-8970-46BE-BFB9-19EA59F9545AQ50774210-BD6B1701-E4BA-4C5B-837C-03F61FD5592FQ50787522-7A42421C-2F1E-4BA2-9204-8897DF3DD5D6Q50799590-73D0DBAD-6808-4AA2-BA7A-EC6C4205AECDQ51877035-A9D9B9D0-B0A6-4DD3-80A4-451D5D44AE46Q51973336-EB34B450-F3EE-4FA0-AFDD-2D024DE98E94Q53342476-A339F6B3-DBD4-4BCA-A4F9-C3A26D513494Q53359586-ACD63A48-6F89-4E5E-8DDE-BF84DB336199Q53359695-45951284-24F4-46E5-8911-35197EF6A8ADQ53372659-CC27A871-D713-4A0D-807D-B4969847EFEFQ53378576-2F90D1B0-5446-46D5-8A09-68587BBD0EA2Q53384885-0E1B72BC-1BFC-402B-859C-04D0CC71836AQ53391513-D986A102-FA42-4A35-91FB-FBE9C481C565Q53397356-325902D7-16D6-44EF-9AE6-C24C10B23B7CQ53400961-5DC4E083-9223-471C-BC1B-657355B8B8FBQ53400969-864E4C1E-79D8-442C-9586-E5EEBD7C1AE7Q53405891-9F0F6D3D-A962-42B8-ACB3-893E3C8014EFQ53405905-0E0C1F9C-0E0E-46A0-8195-0FF37FF7AB9C
P50
description
hulumtues
@sq
researcher
@en
wetenschapper
@nl
հետազոտող
@hy
name
H Evans
@nl
H Evans
@sl
Harold Evans
@en
Harold Evans
@es
type
label
H Evans
@nl
H Evans
@sl
Harold Evans
@en
Harold Evans
@es
altLabel
H Evans
@en
prefLabel
H Evans
@nl
H Evans
@sl
Harold Evans
@en
Harold Evans
@es
P106
P21
P31
P496
0000-0003-2183-3127