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The subject of the thesis focuses on new approximations studied in a formalism based on a perturbation theory allowing to describe the electronic properties of many-body systems in an approximate way. We excite a system with a small disturbance, by sending light on it or by applying a weak electric field to it, for example and the system "responds" to the disturbance, in the framework of linear response, which means that the response of the system is proportional to the disturbance. The goal is to determine what we call the neutral excitations or bound states of the system, and more particularly the single excitations. These correspond to the transitions from the ground state to an excited state. To do this, we describe in a simplified way the interactions of the particles of a many-body system using an effective interaction that we average over the whole system. The objective of such an approach is to be able to study a system without having to use the exact formalism which consists in diagonalizing the N-body Hamiltonian, which is not possible for systems with more than two particles.

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We present the multi-channel Dyson equation that combines two or more many-body Green's functions to describe the electronic structure of materials. In this thesis, we use it to model photoemission spectra by coupling the one-body Green's function with the three-body Green's function and to model neutral excitation by coupling the two-body Green's function with the four-body Green's function . We demonstrate that, unlike methods using only the one-body Green's function, our approach puts the description of quasiparticles and satellites on an equal footing. We propose a multi-channel self-energy that is static and only contains the bare Coulomb interaction, making frequency convolutions and self-consistency unnecessary. Despite its simplicity, we demonstrate with a diagrammatic analysis that the physics it describes is extremely rich. Finally, we present a framework based on an effective Hamiltonian that can be solved for any many-body system using standard numerical tools. We illustrate our approach by applying it to the Hubbard dimer and show that it is exact both at 1/4 and 1/2 filling.

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We present the second release of the real-time time-dependent density functional theory code “Quantum Dissipative Dynamics” (QDD). It augments the first version [1] by a parallelization on a GPU coded with CUDA fortran. The extension focuses on the dynamical part only because this is the most time consuming part when applying the QDD code. The performance of the new GPU implementation as compared to OpenMP parallelization has been tested and checked on a couple of small sodium clusters and small covalent molecules. OpenMP parallelization allows a speed-up by one order of magnitude in average, as compared to a sequential computation. The use of a GPU permits a gain of an additional order of magnitude. The performance gain outweighs even the larger energy consumption of a GPU. The impressive speed-up opens the door for more demanding applications, not affordable before

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We present the multi-channel Dyson equation that combines two or more many-body Green's functions to describe the electronic structure of materials. In this work we use it to model photoemission spectra by coupling the one-body Green's function with the three-body Green's function. We demonstrate that, unlike methods using only the one-body Green's function, our approach puts the description of quasiparticles and satellites on an equal footing. We propose a multi-channel self-energy that is static and only contains the bare Coulomb interaction, making frequency convolutions and self-consistency unnecessary. Despite its simplicity, we demonstrate with a diagrammatic analysis that the physics it describes is extremely rich. Finally, we present a framework based on an effective Hamiltonian that can be solved for any many-body system using standard numerical tools. We illustrate our approach by applying it to the Hubbard dimer and show that it is exact both at 1/4 and 1/2 filling.

Continuer la lecture Partager

Sujets

Angle-resolved photoelectron spectroscopy Lasers intenses Clusters Coulomb explosion Hubbard model Metal clusters High intensity lasers Ionization mechanisms 3115ee Méthode multiréférence Agrégats Density-functional theory Interactions de photons avec des systèmes libres Explosion coulombienne Collision frequency Environment Laser Electric field MBPT Photon interactions with free systems Electron correlation Méchanismes d'ionisation Fonction de Green Matel clusters Ar environment Instability Dynamique moléculaire Deposition dynamics Au-delà du champ moyen Collisional time-dependent Hartree-Fock Embedded metal cluster Corrélations Neutronique Greens function methods Energy spectrum Instabilité Atom laser Matrice densité Agregats Corrélation forte Monte-Carlo Approximation GW Molecular dynamics Green's function Nucléaire Nuclear Corrélations dynamiques Molecules Aggregates Electronic excitation Coulomb presssure Electronic properties of metal clusters and organic molecules Electronic emission Correction d'auto-interaction Photo-electron distributions Metal cluster Numbers 3360+q 3620Kd Density Functional Theory Electron emission Chaos GW approximation TDDFT Molecular irradiation Landau damping Dissipative effects Fission Inverse bremsstrahlung collisions FOS Physical sciences CAO Neutron Induced Activation Champ-moyen Méthodes des fonctions de Green 3640Cg Théorie de la fonctionnelle de la densité Hierarchical method Mean-field Extended time-dependent Hartree-Fock Activation neutronique Deposition Oxyde de nickel Neutronic Time-dependent density-functional theory Optical response Hierarchical model Nanoplasma Relaxation Nickel oxide Irradiation moléculaire Modèle de Hubbard Photo-Electron Spectrum Effets dissipatifs Multirefence methods Dissipation Damping Semiclassic Electronic properties of sodium and carbon clusters Electron-surface collision Diffusion Dynamics

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