Model definition: {{{ model = SM }}} Neutrino and quark containers: {{{ alias n = n1:n2:n3 alias N = N1:N2:N3 alias q = u:d:s:c alias Q = U:D:S:C }}} The Higgsstrahlung process {{{ process zh = e1, E1 => Z, h }}} The missing-energy channel {{{ process nnbb = e1, E1 => n, N, b, B }}} Other channels (for the 4-jet channels we combine EW and QCD contributions) {{{ process qqbb = e1, E1 => q, Q, b, B process bbbb = e1, E1 => b, B, b, B process eebb = e1, E1 => e1, E1, b, B process qqtt = e1, E1 => q, Q, e3, E3 process bbtt = e1, E1 => b, B, e3, E3 }}} Compilation (optional) {{{ compile }}} The final LEP energy: {{{ sqrts = 209 GeV }}} Set the input parameters {{{ mH = 115 GeV wH = 3.228 MeV # Running b mass mb = 2.9 GeV me = 0 ms = 0 mc = 0 }}} Soft-collinear cuts for the jets {{{ cuts = all M >= 10 GeV [q,Q] }}} Integrate the processes: {{{ integrate (zh) { iterations = 5:5000} integrate(nnbb,qqbb,bbbb,eebb, qqtt,bbtt) { iterations = 12:20000 } }}} Define title etc. as global variables, that will be used by PLOT {{{ $description = "A WHIZARD 2.0 Example. Using weighted events to speed things up." $ylabel = "$N_{\textrm{events}}$" }}} Allocate plots {{{ $title = "Invisible mass distribution in $e^+e^- \to \nu\bar\nu b \bar b$" $xlabel = "$M_{\nu\nu}$/GeV" histogram m_invisible (70 GeV, 130 GeV, 0.5 GeV) $title = "$bb$ invariant mass distribution in $e^+e^- \to \nu\bar\nu b \bar b$" $xlabel = "$M_{b\bar b}$/GeV" histogram m_bb (70 GeV, 130 GeV, 0.5 GeV) }}} Define the analysis set-up: {{{ analysis = record m_invisible (eval M [n,N]); record m_bb (eval M [b,B]) }}} Luminosity and simulation: {{{ luminosity = 10 simulate (nnbb) }}} Some more plots and simulations: {{{ $title = "Dijet invariant mass distribution in $e^+e^- \to q \bar q b \bar b$" $xlabel = "$M_{q\bar q}$/GeV" histogram m_jj (70 GeV, 130 GeV, 0.5 GeV) simulate (qqbb) { analysis = record m_jj (eval M / 1 GeV [combine [q,Q]]) } }}} Perform the analysis: {{{ compile_analysis { $out_file = "lep_higgs.dat" } }}}