2012
DOI: 10.1007/jhep02(2012)141
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Real-virtual corrections for gluon scattering at NNLO

Abstract: We use the antenna subtraction method to isolate the mixed real-virtual infrared singularities present in gluonic scattering amplitudes at next-to-next-to-leading order. In a previous paper, we derived the subtraction term that rendered the double real radiation tree-level process finite in the single and double unresolved regions of phase space. Here, we show how to construct the real-virtual subtraction term using antenna functions with both initial-and final-state partons which removes the explicit infrared… Show more

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Cited by 30 publications
(5 citation statements)
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“…The calculation of the full NNLO QCD corrections to this process is still in progress (see Refs. [205,206] and references therein). This precludes a consistent use of the Tevatron jet data in our NNLO PDF fit.…”
Section: Hadronic Jet Productionmentioning
confidence: 99%
“…The calculation of the full NNLO QCD corrections to this process is still in progress (see Refs. [205,206] and references therein). This precludes a consistent use of the Tevatron jet data in our NNLO PDF fit.…”
Section: Hadronic Jet Productionmentioning
confidence: 99%
“…A study of joint jet radius and threshold resummation has been presented in [23]. Progress in next-to-next-to-leading-order (NNLO) QCD calculations has been made over the past several years [24][25][26][27]. After the completion of the first calculations of the gluons-only subprocess [28,29], the complete leading-colour and leading-N F NNLO QCD corrections to the single jet inclusive production [30] and to di-jet production [31] were obtained recently.…”
Section: Introductionmentioning
confidence: 99%
“…This method has been derived in [108] and successfully applied to the calculation of the NNLO corrections to 3-jet production and related event shape observables in electron-positron annihilation in [183]. The extension of the scheme to the treatment of initial state radiation relevant for calculations of jet observables in hadronic collisions at LHC has been established at NLO in [109] and at NNLO in [133,[184][185][186][187][188][189][190]. In a first subsection we review the NLO version of the scheme followed by the generalisation to NNLO.…”
Section: Antenna Subtraction Schemementioning
confidence: 99%