The Equivalence Theorem for the Heavy-Higgs Standard Model and the Gauged Nonlinear Sigma-Model
arXiv:hep-ph/9405412 · doi:10.1007/BF01571287
Abstract
The equivalence theorem states that the leading part of the amplitude for a process with external longitudinally polarized vector bosons is given by the amplitude in which the longitudinal vector bosons are replaced by the corresponding pseudo-Goldstone bosons. The validity of this theorem within the standard model with a heavy Higgs boson and within the gauged nonlinear sigma-model (in which the Higgs boson is absent) is shown. Furthermore it is examined to what extent also internal lines other than scalar lines can be neglected. A simple power-counting method is developed which determines the leading diagrams for a given process at an arbitrary loop order. This method is also applied to effective Lagrangians with additional nonstandard interaction terms of higher dimension (chiral Lagragians).
17 pages LaTeX, 6 figures as uuencoded eps-files
References in corpus (5)
- The Electroweak Chiral Lagrangian for the Standard Model with a Heavy Higgs
- Proof of the Equivalence Theorem in the Chiral Lagrangian Formalism
- The Equivalence Theorem for Chiral Lagrangians
- The Equivalence Theorem and Effective Lagrangians
- High-Energy Vector-Boson Scattering with Non-Standard Interactions and the Role of a Scalar Sector
Cited by in corpus (7)
- Radiative Corrections to ZZ->ZZ in the Electroweak Standard Model
- Dyson summation without violating Ward identities and the Goldstone-boson equivalence theorem
- RENORMALIZATION and the EQUIVALENCE THEOREM: ON-SHELL SCHEME
- The Higgs Boson in the Standard Model - From LEP to LHC: Expectations, Searches, and Discovery of a Candidate
- Electroweak interactions and high-energy limit
- The Equivalence Theorem and infrared divergences
- Global anomalies and the gauge-boson equivalence theorem