Infrared-finite algorithms in QED: the groundstate of an atom interacting with the quantized radiation field

From MaRDI portal
Publication:852406

DOI10.1007/s00220-005-1478-3zbMath1118.81083OpenAlexW2020049265MaRDI QIDQ852406

Alessandro Pizzo, Volker Bach, Jürg Fröhlich

Publication date: 29 November 2006

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

Full work available at URL: https://doi.org/10.1007/s00220-005-1478-3




Related Items (42)

Kramers degeneracy theorem in nonrelativistic QEDOn the theory of resonances in non-relativistic quantum electrodynamics and related modelsHyperfine splitting in non-relativistic QED: uniqueness of the dressed hydrogen atom ground stateOn the absence of excited eigenstates of atoms in QEDOn the ultraviolet limit of the Pauli-Fierz Hamiltonian in the Lieb-Loss modelAn infrared-finite algorithm for Rayleigh scattering amplitudes, and Bohr's frequency conditionSpectral Properties for Hamiltonians of Weak InteractionsConstruction of the ground state in nonrelativistic QED by continuous flowsEffective dynamics of an electron coupled to an external potential in non-relativistic QEDON SPECTRAL RENORMALIZATION GROUPA new approach to continuous multi-scale analysis in nonrelativistic QED: ground states and photon number bounds for the spin-boson model with critical infrared singularitySpectral theory for a mathematical model of the weak interaction. I: The decay of the intermediate vector bosons \(W^{\pm}\)On dilation analyticity and spatial exponential decay of atomic ground states in non-relativistic QEDLocal decay for weak interactions with massless particlesAbsence of submultiplicative norms for Wick-ordered operator productsInfraparticle scattering states in non-relativistic QED. I: The Bloch-Nordsieck paradigmFunctional integral representations of the Pauli-Fierz model with spin 1/2Quantitative estimates on the binding energy for hydrogen in non-relativistic QEDOn asymptotic expansions in spin-boson modelsThe ground state energy of the massless spin-boson modelConvergent expansions in non-relativistic QED: analyticity of the ground stateSmoothness and analyticity of perturbation expansions in QEDThe mass shell in the semi-relativistic Pauli-Fierz modelSpectral theory for a mathematical model of the weak interaction: The decay of the intermediate vector bosons \(W^{\pm }\). IILocal decay in non-relativistic QEDResolvent smoothness and local decay at low energies for the standard model of non-relativistic QEDSPECTRAL RENORMALIZATION GROUP AND LOCAL DECAY IN THE STANDARD MODEL OF NON-RELATIVISTIC QUANTUM ELECTRODYNAMICSEXISTENCE OF GROUND STATES OF HYDROGEN-LIKE ATOMS IN RELATIVISTIC QED I: THE SEMI-RELATIVISTIC PAULI–FIERZ OPERATORRayleigh scattering at atoms with dynamical nucleiRenormalization analysis for degenerate ground statesA new asymptotic perturbation theory with applications to models of massless quantum fieldsSpectral theory for the standard model of non-relativistic QEDGround states in the spin Boson modelThe lower part of the spectrum of the Hamiltonian of the spinless Pauli–Fierz model (A two-component Bose field interacting with a charged particle)Exponential localization of hydrogen-like atoms in relativistic quantum electrodynamicsOn the ground state energy of the translation invariant Pauli-Fierz modelInfrared-finite algorithms in QED. II. The expansion of the groundstate of an atom interacting with the quantized radiation fieldGround state and resonances in the standard model of the non-relativistic QEDInfraparticle scattering states in nonrelativistic quantum electrodynamics. II. Mass shell propertiesMathematical analysis of quantum fields—Historical survey and a new asymptotic perturbation theoryExistence of ground states of hydrogen-like atoms in relativistic quantum electrodynamics. II. The no-pair operatorExistence and construction of resonances for atoms coupled to the quantized radiation field



Cites Work


This page was built for publication: Infrared-finite algorithms in QED: the groundstate of an atom interacting with the quantized radiation field