This process can be calculated at LO, NLO, and NNLO. These processes represent the production of a W boson which subsequently decays leptonically, in association with a Standard Model Higgs boson that decays into a tau pair (nproc=91, 96), decays into a b-quark pair (nproc=92, 97), a pair of photons (nproc=93, 98), or a pair of W-bosons (nproc=94, 99), a pair of Z bosons (nproc=95, 100). Note that in the cases of Higgs decay to W,(Z) pairs, below the W,(Z) pair threshold one of the W,(Z) bosons is virtual and therefore one must set zerowidth=.false.. The calculation may be performed at NNLO for these processes.
Radiation from the bottom quarks in the decay, an NLO effect, is included in (nproc=920, 970). nproc=900 may be used to compute the sum over both W charges in one run (with the decay products 3 and 4 representing lepton and antilepton respectively). This sum is performed by adjustng the CKM matrix to allow both charges of the W boson.
When removebr is .true., neither the W boson nor the Higgs decays.
For more information on this process see refs. [1, 2, 3]. NLO calculations can be performed by subtraction, zero-jettiness slicing and qT-slicing. NNLO calculations can be performed by zero-jettiness slicing and qT-slicing. Input files for these 6 possibilities are given in the link below.
nplotter_auto.f is the default plotting routine.
[1] J.M. Campbell, R.K. Ellis and C. Williams, Associated production of a Higgs boson at NNLO, JHEP 06 (2016) 179 [1601.00658].
[2] R. Boughezal, J.M. Campbell, R.K. Ellis, C. Focke, W. Giele, X. Liu et al., Color singlet production at NNLO in MCFM, Eur. Phys. J. C 77 (2017) 7 [1605.08011].
[3] J.M. Campbell, R.K. Ellis and S. Seth, Non-local slicing approaches for NNLO QCD in MCFM, 2202.07738.