Lorentz covariance of the \(\lambda (\varphi^ 4)_ 2\) quantum field theory

DOI10.1007/BF01646027zbMath0194.29003MaRDI QIDQ2538840

Arthur Jaffe, John T. Cannon

Publication date: 1970

Published in: Communications in Mathematical Physics (Search for Journal in Brave)

zbMATH Keywords

quantum theory

Related Items (10)

Probing quantum gravity through exactly soluble midi-superspaces I ⋮ Self-adjointness of the Yukawa\(_{2}\) Hamiltonian ⋮ Ground state for point particles interacting through a massless scalar Bose field ⋮ Unnamed Item ⋮ Quadratic Expressions in a Free Boson Field ⋮ Quantum field theoretic properties of a model of Nelson: domain and eigenvector stability for perturbed linear operators ⋮ Almost positive perturbations of positive selfadjoint operators ⋮ Hypercontra ctive semigroups and two dimensional self-coupled Bose fields ⋮ Some essentially self-adjoint Dirac operators with spherically symmetric potentials ⋮ \({\mathcal P}(\phi)_ 2\) models with variable coefficients

Cites Work

• Unnamed Item
• Yukawa coupling of quantum fields in two dimensions. I
• Boson fields with nonlinear selfinteraction in two dimensions
• The \(\lambda (\varphi^ 4)_ 2\) quantum field theory without cutoffs. II: The field operators and the approximate vacuum
• NOTES TOWARD THE CONSTRUCTION OF NONLINEAR RELATIVISTIC QUANTUM FIELDS, I. THE HAMILTONIAN IN TWO SPACE-TIME DIMENSIONS AS THE GENERATOR OF A C ^* -AUTOMORPHISM GROUP
• Singular perturbations of selfadjoint operators
• A<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>λ</mml:mi><mml:mrow><mml:msup><mml:mrow><mml:mi>ϕ</mml:mi></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>Quantum Field Theory without Cutoffs. I
• Infinite Renormalization of the Hamiltonian Is Necessary

This page was built for publication: Lorentz covariance of the \(\lambda (\varphi^ 4)_ 2\) quantum field theory