Next-to-next-to-leading-order subtraction formalism in hadron collisions and its application to Higgs-boson production at the large hadron collider.
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Measurements of differential and double-differential Drell-Yan cross sections in proton-proton collisions at [Formula: see text][Formula: see text]Hadronic Higgs production through NLO [Formula: see text] PS in the SM, the 2HDM and the MSSM.The Standard Model from LHC to future colliders.QCD corrections to [Formula: see text] in FDR.Nested soft-collinear subtractions in NNLO QCD computations.Associated Higgs-W-boson production at hadron colliders: a fully exclusive QCD calculation at NNLO.Vector boson production at hadron colliders: a fully exclusive QCD calculation at next-to-next-to-leading order.Next-to-Next-to Leading Order QCD Predictions for Single Jet Inclusive Production at the LHC.Higgs production at the lHCSearch for new phenomena in events containing a same-flavour opposite-sign dilepton pair, jets, and large missing transverse momentum in [Formula: see text] [Formula: see text][Formula: see text] collisions with the ATLAS detectorPerformance of algorithms that reconstruct missing transverse momentum in [Formula: see text]= 8 TeV proton-proton collisions in the ATLAS detectorSearch for an additional, heavy Higgs boson in the [Formula: see text] decay channel at [Formula: see text] in [Formula: see text] collision data with the ATLAS detectorTest of CP invariance in vector-boson fusion production of the Higgs boson using the method in the ditau decay channel with the ATLAS detectorMeasurements of the Total and Differential Higgs Boson Production Cross Sections Combining the H→γγ and H→ZZ^{*}→4ℓ Decay Channels at sqrt[s]=8 TeV with the ATLAS DetectorSearch for supersymmetry in events containing a same-flavour opposite-sign dilepton pair, jets, and large missing transverse momentum in [Formula: see text] TeV collisions with the ATLAS detectorSearch for new phenomena in final states with an energetic jet and large missing transverse momentum in collisions at [Formula: see text]TeV with the ATLAS detectorMeasurement of the muon charge asymmetry in inclusivepp→W+Xproduction ats=7 TeVand an improved determination of light parton distribution functionsMeasurement of the differential and double-differential Drell-Yan cross sections in proton-proton collisions at $ \sqrt{s} $ = 7 TeVMeasurement of the Drell-Yan cross section in pp collisions at $ \sqrt {s} = 7 $ TeVMeasurements of properties of the Higgs boson decaying into the four-lepton final state in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeVSearch for new phenomena using the invariant mass distribution of same-flavour opposite-sign dilepton pairs in events with missing transverse momentum in collisions with the ATLAS detectorMeasurement of inclusive and differential cross sections in the H → ZZ * → 4ℓ decay channel in pp collisions at s = 13 $$ \sqrt{s}=13 $$ TeV with the ATLAS detectorMeasurement of the k t splitting scales in Z → ℓℓ events in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detectorPrecision measurement and interpretation of inclusive , and production cross sections with the ATLAS detectorMeasurements of top-quark pair to Z-boson cross-section ratios at s = 13 $$ \sqrt{s}=13 $$ , 8, 7 TeV with the ATLAS detectorMeasurement of total and differential W + W − production cross sections in proton-proton collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detector and limits on anomalous triple-gauge-boson couplingsSearch for new phenomena in final states with an energetic jet and large missing transverse momentum inppcollisions ats=13 TeVusing the ATLAS detectorMeasurement of fiducial differential cross sections of gluon-fusion production of Higgs bosons decaying to WW ∗→eνμν with the ATLAS detector at s = 8 $$ \sqrt{s}=8 $$ TeVMeasurement of the double-differential high-mass Drell-Yan cross section in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detectorSearch for the standard model Higgs boson produced in association with a vector boson and decaying into a tau pair inppcollisions ats=8 TeVwith the ATLAS detectorSearch for a high-mass Higgs boson decaying to a W boson pair in pp collisions at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detectorStudy of (W/Z)H production and Higgs boson couplings using H→ W W ∗ decays with the ATLAS detectorObservation and measurement of Higgs boson decays toWW*with the ATLAS detectorEvidence for the Higgs-boson Yukawa coupling to tau leptons with the ATLAS detectorSearch for squarks and gluinos in events with isolated leptons, jets and missing transverse momentum at s = 8 $$ \sqrt{s}=8 $$ TeV with the ATLAS detectorMeasurement of the Z/γ * boson transverse momentum distribution in pp collisions at s = 7 $$ \sqrt{s}=7 $$ TeV with the ATLAS detectorSearch for pair-produced third-generation squarks decaying via charm quarks or in compressed supersymmetric scenarios inppcollisions ats=8 TeVwith the ATLAS detectorMeasurement of the low-mass Drell-Yan differential cross section at s $$ \sqrt{s} $$ = 7 TeV using the ATLAS detectorMeasurement of the inclusiveW±andZ/γ*cross sections in theeandμdecay channels inppcollisions ats=7 TeVwith the ATLAS detectorMeasurement of the transverse momentum distribution ofWbosons inppcollisions ats=7 TeVwith the ATLAS detector
P2860
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P2860
Next-to-next-to-leading-order subtraction formalism in hadron collisions and its application to Higgs-boson production at the large hadron collider.
description
2007 nî lūn-bûn
@nan
2007年の論文
@ja
2007年学术文章
@wuu
2007年学术文章
@zh-cn
2007年学术文章
@zh-hans
2007年学术文章
@zh-my
2007年学术文章
@zh-sg
2007年學術文章
@yue
2007年學術文章
@zh
2007年學術文章
@zh-hant
name
Next-to-next-to-leading-order ...... at the large hadron collider.
@en
Next-to-next-to-leading-order ...... at the large hadron collider.
@nl
type
label
Next-to-next-to-leading-order ...... at the large hadron collider.
@en
Next-to-next-to-leading-order ...... at the large hadron collider.
@nl
prefLabel
Next-to-next-to-leading-order ...... at the large hadron collider.
@en
Next-to-next-to-leading-order ...... at the large hadron collider.
@nl
P2860
P1476
Next-to-next-to-leading-order ...... n at the large hadron collider
@en
P2093
Stefano Catani
P2860
P304
P356
10.1103/PHYSREVLETT.98.222002
P407
P577
2007-05-30T00:00:00Z
P698
P818
hep-ph/0703012