273 f(-p₁)+f(-p₂) → H(→ W⁺(ν(p₃),e⁺(p₄))W^-(e^-(p₅),ν(p₆)))+f(p₇)+f(p₈), (in heavy top limit)

273.1 H + 2 jet production, (m_t = ∞), processes 270–274

These processes represent the production of a Standard Model Higgs boson in association with two jets. The Higgs boson subsequently decays to either a pair of photons (nproc=270), a bottom quark pair (nproc=271), a pair of tau’s (nproc=272), a pair of leptonically decaying W’s (nproc=273) or a pair of leptonically decaying Z’s (nproc=274).

The matrix elements are included in the infinite top mass limit using the effective Lagrangian approach.

When removebr is true, the Higgs boson does not decay.

273.2 Plotter

nplotter_auto.f is the default plotting routine.

273.3 Example input and output file(s)

input273.ini process273.out

273 f(-p1)+f(-p2) → H(→ W+(ν(p3),e+(p4))W-(e-(p5),ν(p6)))+f(p7)+f(p8), (in heavy top limit)

273.1 H + 2 jet production, (mt = ∞), processes 270–274

273.2 Plotter

273.3 Example input and output file(s)

References

273 f(-p₁)+f(-p₂) → H(→ W⁺(ν(p₃),e⁺(p₄))W^-(e^-(p₅),ν(p₆)))+f(p₇)+f(p₈), (in heavy top limit)

273.1 H + 2 jet production, (m_t = ∞), processes 270–274