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Hadronic production of a Higgs boson in association with two jets at ...

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3.2. The cut-constructible parts 85−++−++−+−−+−+−++−+−+−+−−Figure 3.7: For each three mass triangle there is always <strong>at</strong> least one vertex correspond<strong>in</strong>gto a zero tree-level amplitude. As <strong>in</strong> previous diagrams external neg<strong>at</strong>iveheclicity gluons are represented as green l<strong>in</strong>es and there can be an arbitrary number<strong>of</strong> positive helicity gluons <strong>at</strong> each vertex.j (i − 1)(j − 1)K 2(i + 1)i = K 1Figure 3.8: The k<strong>in</strong>em<strong>at</strong>ic structure <strong>of</strong> a generic <strong>two</strong>-mass triangle which appears<strong>in</strong> our calcul<strong>at</strong>ions. The same k<strong>in</strong>em<strong>at</strong>ics can be used to represent the one-masstriangle <strong>with</strong> (i − 1) = j <strong>with</strong> no loss <strong>of</strong> generality.

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