Universal bounds for large determinants from non-commutative Hölder inequalities in fermionic constructive quantum field theory

Efficiently bounding large determinants is an essential step in non-relativistic fermionic constructive quantum field theory to prove the absolute convergence of the perturbation expansion of correlation functions in terms of powers of the strength $u\in \mathbb{R}$ of the interparticle interaction....

Descripción completa

Detalles Bibliográficos
Autores: Bru, J.-B., de Siqueira Pedra, W.
Tipo de recurso: artículo
Estado:Versión aceptada para publicación
Fecha de publicación:2017
País:España
Institución:Basque Center for Applied Mathematics (BCAM)
Repositorio:BIRD. BCAM's Institutional Repository Data
OAI Identifier:oai:bird.bcamath.org:20.500.11824/719
Acceso en línea:http://hdl.handle.net/20.500.11824/719
Access Level:acceso embargado
Palabra clave:Determinant bounds
Hölder inequalities for non-commutative Lp -spaces
interacting fermions
constructive quantum field theory
Descripción
Sumario:Efficiently bounding large determinants is an essential step in non-relativistic fermionic constructive quantum field theory to prove the absolute convergence of the perturbation expansion of correlation functions in terms of powers of the strength $u\in \mathbb{R}$ of the interparticle interaction. We provide, for large determinants of fermionic convariances, sharp bounds which hold for all (bounded and unbounded, the latter not being limited to semibounded) one-particle Hamiltonians. We find the smallest universal determinant bound to be exactly 1. In particular, the convergence of perturbation series at $u=0$ of any fermionic quantum field theory is ensured if the matrix entries, with respect to some fixed orthonormal basis, of the covariance and the interparticle interaction decay sufficiently fast. Our proofs use H\"{o}lder inequalities for general non-commutative Lp-spaces derived by Araki and Masuda.