SUMMARY
This discussion focuses on the definitions and distinctions between local and nonlocal operators in Quantum Field Theory (QFT). A local operator, denoted as ##\mathcal{O}(\vec{x})##, satisfies the transformation property ##\mathcal{O}(\vec{x})=e^{-i\vec{P}\cdot \vec{x}}\mathcal{O}e^{i\vec{P}\cdot \vec{x}}##, where ##\langle \Omega,\mathcal{O}\Omega\rangle=0## with ##\Omega## being the vacuum vector. Nonlocal operators, such as the product ##O(x)O(y)## or integrals involving local operators, do not adhere to the same transformation properties and cannot be expressed as a single space-time argument. The axioms governing local operators are referenced, particularly those outlined by Osterwalder and Schrader.
PREREQUISITES
- Understanding of Quantum Field Theory (QFT) principles
- Familiarity with operator-valued distributions
- Knowledge of the Poincaré group and its representations
- Basic concepts of functional analysis, particularly in Hilbert spaces
NEXT STEPS
- Study the axioms for Euclidean Green’s functions as described by K. Osterwalder and R. Schrader
- Explore the Epstein-Glaser approach to causal perturbation theory in QFT
- Learn about operator-valued distributions and their applications in quantum mechanics
- Investigate the implications of nonlocal operators in quantum field theories
USEFUL FOR
Researchers, physicists, and students in theoretical physics, particularly those specializing in Quantum Field Theory and operator algebra.