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Perturbative Unitarity and the 4-Point Vertices in the Constructive Standard Model
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abstract
We find a complete set of 4-point vertices in the Constructive Standard Model (CSM). This set is smaller than in Feynman diagrams as the CSM does not need or allow any additional 4-point vertices (or "contact" terms) beyond what is present in Feynman diagrams and, furthermore, it does $\textit{not}$ need or allow a 4-point vertex for $Z Z \bar{W} W$, $W W \bar{W} \bar{W}$, $\gamma Z W \bar{W}$ or $\gamma \gamma W \bar{W}$, in addition to the already known absence of the 4-gluon vertex. We show that with this set of 4-point vertices, perturbative unitarity is satisfied in the CSM. Additionally, we show that many constructive diagrams are not Feynman diagrams rewritten in spinor form. In fact, we show that there is a significant rearrangement of contributions from the diagrams in constructive calculations relative to Feynman diagrams, for some processes. In addition to the already known or expected rearrangement in diagrams involving external photons, we also find that diagrams involving 4 vector bosons are also significantly different than their Feynman counterparts.
Forward citations
Cited by 2 Pith papers
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Massive Gauge Theories from Consistency Conditions of Amplitudes
Massive vector-boson and scalar amplitudes through four points are uniquely fixed by two on-shell consistency conditions, forcing spontaneously-broken gauge theories — or Stueckelberg theory when scalar masses are equ...
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On-shell recursion relations for higher-spin Compton amplitudes
The all-line transverse shift makes four-point electromagnetic and gravitational Compton amplitudes on-shell constructible for massive spin s≤3/2 and s≤5/2, respectively, starting from minimal three-point amplitudes.
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