1.

Analytic results for colorsinglet production at NNLO QCD with the nested softcollinear subtraction scheme
/ Caola, Fabrizio ; Melnikov, Kirill ; Röntsch, Raoul
We present analytic formulas that describe the fullydifferential production of colorsinglet final states in qq¯ and gg annihilation, including all the relevant partonic channels, through NNLO QCD. [...]
Published in EPJC 79 (2019) 386
10.1140/epjc/s1005201968807
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2.

Bottomquark effects in Higgs production at intermediate transverse momentum
/ Caola, Fabrizio ; Lindert, Jonas ; Melnikov, Kirill ; Monni, Pier ; et al
We provide a precise description of the Higgs boson transverse momentum distribution including top and bottom quark contributions, that is valid for transverse momenta in the range m b ≲ p ⊥ ≲ m t , where m b and m t are the bottom and top quark masses. [...]
Published in JHEP 1809 (2018) 035
10.1007/JHEP09(2018)035
arXiv:1804.07632
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3.

The doublesoft integral for an arbitrary angle between hard radiators
/ Caola, Fabrizio ; Delto, Maximilian ; Frellesvig, Hjalte ; Melnikov, Kirill
We consider the doublesoft limit of a generic QCD process involving massless partons and integrate analytically the doublesoft eikonal functions over the phasespace of soft partons (gluons or quarks) allowing for an arbitrary relative angle between the threemomenta of two hard massless radiators. [...]
Published in EPJC 78 (2018) 687
10.1140/epjc/s1005201861807
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4.

NNLO QCD corrections to associated $WH$ production and $H\to b\overline{b}$ decay
/ Caola, Fabrizio ; Luisoni, Gionata ; Melnikov, Kirill ; Röntsch, Raoul
We present a computation of the nexttonexttoleadingorder (NNLO) QCD corrections to the production of a Higgs boson in association with a $W$ boson at the LHC and the subsequent decay of the Higgs boson into a $b\overline{b}$ pair, treating the $b$ quarks as massless. [...]
Published in Physical Review D 97 (2018)
10.1103/PhysRevD.97.074022
arXiv:1712.06954
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5.

Nested softcollinear subtractions in NNLO QCD computations
/ Caola, Fabrizio ; Melnikov, Kirill ; Röntsch, Raoul
We discuss a modification of the nexttonexttoleading order (NNLO) subtraction scheme based on the residueimproved sector decomposition that reduces the number of doublereal emission sectors from five to four. [...]
Published in EPJC 77 (2017) 248
10.1140/epjc/s1005201747740
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6.

The Higgs transverse momentum spectrum with finite quark masses beyond leading order
/ Caola, Fabrizio ; Forte, Stefano ; Marzani, Simone ; Muselli, Claudio ; et al
We apply the leadinglog highenergy resummation technique recently derived by some of us to the transverse momentum distribution for production of a Higgs boson in gluon fusion. [...]
Published in JHEP 1608 (2016) 150
10.1007/JHEP08(2016)150
arXiv:1606.04100
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7.

QCD corrections to vector boson pair production in gluon fusion including interference effects with offshell Higgs at the LHC
/ Caola, Fabrizio ; Dowling, Matthew ; Melnikov, Kirill ; Röntsch, Raoul ; et al
We compute nexttoleading order (NLO) QCD corrections to the production of two massive electroweak bosons in gluon fusion. [...]
Published in JHEP 1607 (2016) 087
10.1007/JHEP07(2016)087
arXiv:1605.04610
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8.

Jetvetoed Higgs cross section in gluon fusion at N 3 LO+NNLL with smallR resummation
/ Banfi, Andrea ; Caola, Fabrizio ; Dreyer, Frédéric ; Monni, Pier ; et al
We present new results for the jetveto efficiency and zerojet cross section in Higgs production through gluon fusion. [...]
Published in JHEP 1604 (2016) 049
10.1007/JHEP04(2016)049
arXiv:1511.02886
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9.

QCD corrections to W + W − production through gluon fusion
/ Caola, Fabrizio ; Melnikov, Kirill ; Röntsch, Raoul ; Tancredi, Lorenzo
We compute the nexttoleading order (NLO) QCD corrections to the gg→W+W−→l1+ν1l2−ν¯2 process, mediated by a massless quark loop, at the LHC. [...]
Published in Physics letters B (2016)
10.1016/j.physletb.2016.01.046
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10.

Twoloop helicity amplitudes for the production of two offshell electroweak bosons in gluon fusion
/ Caola, Fabrizio ; Henn, Johannes ; Melnikov, Kirill ; Smirnov, Alexander ; et al
We compute the part of the twoloop virtual amplitude for the process gg → V 1 V 2 → l 1 l ¯ 2 ′ l 2 l ¯ 2 ′ $$ gg\to {V}_1{V}_2\to \left({l}_1{\overline{l}}_2^{\prime}\right)\left({l}_2{\overline{l}}_2^{\prime}\right) $$ , where V 1,2 are arbitrary electroweak gauge bosons, that receives contributions from loops of massless quarks. [...]
Published in JHEP 1506 (2015) 129
10.1007/JHEP06(2015)129
arXiv:1503.08759
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