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20052014
most citedHiggs production in gluon fusion at next-to-next-to-leading order QCD for finite top mass

239 citations · 1.4k across the 20 of their papers we have counts for

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hep-ph2014★ 4 cited

Universality in W+Multijet Production

Z. Bern, L. J. Dixon, F. Febres Cordero +5

We study -boson production accompanied by multiple jets at 7 TeV at the LHC. We study the jet-production ratio, of total cross sections for +- to +()-jet productio…

hep-ph2014

High multiplicity processes with BlackHat and Sherpa

Jeppe R. Andersen, Stephanie Bartle, Zvi Bern +7

In this contribution, we present an intermediate storage format for next-to-leading order (NLO) events and explain the advantages of presenting a NLO calculation in this format. We…

hep-ph2013

High multiplicity W+jets predictions at NLO

Z. Bern, L. J. Dixon, F. Febres Cordero +5

In these proceedings we present results from a recent calculation for the production of a W boson in conjunction with five jets at next-to-leading order in perturbative QCD. We als…

hep-ph2013★ 130 cited

Next-to-Leading Order W + 5-Jet Production at the LHC

Z. Bern, L. J. Dixon, F. Febres Cordero +5

We present next-to-leading order QCD predictions for the total cross section and for a comprehensive set of transverse-momentum distributions in W + 5-jet production at the Large H…

hep-ph2012

High multiplicity processes at NLO with BlackHat and Sherpa

Zvi Bern, Kemal Ozeren, Lance J. Dixon +5

In this contribution we review recent progress with fixed-order QCD predictions for the production of a vector boson in association with jets at hadron colliders, using the program…

hep-ph2012★ 26 cited

Missing Energy and Jets for Supersymmetry Searches

Z. Bern, G. Diana, L. J. Dixon +6

We extend our investigation of backgrounds to new physics signals, following CMS's data-driven search for supersymmetry at the LHC. The aim is to use different sets of cuts in gamm…

hep-ph2012★ 125 cited

Top-mass effects in differential Higgs production through gluon fusion at order α_s^4

Robert V. Harlander, Tobias Neumann, Kemal J. Ozeren +1

Effects from a finite top quark mass on differential distributions in the Higgs+jet production cross section through gluon fusion are studied at next-to-leading order in the strong…

hep-ph2012

NLO vector boson production with light jets

Z. Bern, G. Diana, L. J. Dixon +8

In this contribution we present recent progress in the computation of next-to-leading order (NLO) QCD corrections for the production of an electroweak vector boson in association w…

hep-ph2011★ 131 cited

Four-Jet Production at the Large Hadron Collider at Next-to-Leading Order in QCD

Z. Bern, G. Diana, L. J. Dixon +6

We present the cross sections for production of up to four jets at the Large Hadron Collider, at next-to-leading order in the QCD coupling. We use the BlackHat library in conjuncti…

hep-ph2011★ 34 cited

Colour Decompositions of Multi-quark One-loop QCD Amplitudes

Harald Ita, Kemal Ozeren

We describe the decomposition of one-loop QCD amplitudes in terms of colour-ordered building blocks. We give new expressions for the coefficients of QCD colour structures in terms…

hep-ph2011★ 52 cited

Driving Missing Data at Next-to-Leading Order

Z. Bern, G. Diana, L. J. Dixon +6

The prediction of backgrounds to new physics signals in topologies with large missing transverse energy and jets is important to new physics searches at the LHC. Following a CMS st…

hep-ph2011★ 82 cited

Left-Handed W Bosons at the LHC

Z. Bern, G. Diana, L. J. Dixon +8

The production of W bosons in association with jets is an important background to new physics at the LHC. Events in which the W carries large transverse momentum and decays leptoni…

hep-ph2010★ 17 cited

Analytic Results for Higgs Production in Bottom Fusion

Kemal J. Ozeren

We evaluate analytically the cross section for Higgs production plus one jet through bottom quark fusion. By considering the small pT limit we derive expressions for the resummatio…

hep-ph2010★ 57 cited

Higgs plus jet production in bottom quark annihilation at next-to-leading order

Robert V. Harlander, Kemal J. Ozeren, Marius Wiesemann

The cross section for Higgs+jet production in bottom quark annihilation is calculated through NLO QCD. The five-flavour scheme is used to derive this contribution to the Higgs+jet…

hep-ph2010

Higgs production in gluon fusion at NNLO for finite top quark mass

Robert Harlander, Hendrik Mantler, Simone Marzani +1

The evaluation of the top quark mass suppressed terms to the Higgs production cross section in gluon fusion at next-to-next-to-leading order is reported on. In the region below thr…

hep-ph2009★ 239 cited

Higgs production in gluon fusion at next-to-next-to-leading order QCD for finite top mass

Robert V. Harlander, Hendrik Mantler, Simone Marzani +1

The inclusive Higgs production cross section from gluon fusion is calculated through NNLO QCD, including its top quark mass dependence. This is achieved through a matching of the 1…

hep-ph2009

Top Mass Effects in Higgs Production at Hadron Colliders

Kemal J. Ozeren

We derive the first four terms of an expansion in mH^2/mtop^2 of the total Higgs cross-section through gluon fusion. At NLO we demonstrate the excellent convergence of this series…

hep-ph2009★ 205 cited

Finite top mass effects for hadronic Higgs production at next-to-next-to-leading order

Robert V. Harlander, Kemal J. Ozeren

The first four terms of an expansion in mH^2/mt^2 of the total inclusive cross section for Higgs production in gluon fusion are evaluated through next-to-next-to-leading order QCD.…

hep-ph2009★ 188 cited

Top mass effects in Higgs production at next-to-next-to-leading order QCD: virtual corrections

Robert V. Harlander, Kemal J. Ozeren

Top quark mass suppressed terms are calculated for the virtual amplitude for Higgs production in gluon fusion at three-loop level, i.e. O(α_s^3). The method of asymptotic expansion…

hep-ph2006★ 35 cited

Scattering amplitudes with massive fermions using BCFW recursion

K. J. Ozeren, W. J. Stirling

We study the QCD scattering amplitudes for \bar{q}q \to gg and \bar{q}q \to ggg where q is a massive fermion. Using a particular choice of massive fermion spinor we are able to der…