Condensed Matter
Group members
Permanent staff
Thomas Ayral
Silke Biermann (Coordinator)
Maria Chatzieleftheriou
Olesia Dmytruk
Michel Ferrero
Antoine Georges
Karyn Le Hur
Han Ma
Leonid Poyurovskiy
Marc-Olivier Renou
Laurent Sanchez-Palencia
Evgeny Stepanov
Alaska Subedi
Filippo Vicentini
PhD Students
Gusein Bedirkhanov
Francesco Buonemani
Yeqin Cheng
Owen Colire
Matteo Costa
Tom de Coninck
Tristan Diotte
Félix Fossati
Alexandre Georgin
Jakob Huhn
Adrien Kahn
Magali Korolev
Dachi Khutsidze
István Markó
Antoine Misery
Nathan Moumique
Danilo Nascimento Guimaraes
Martin Plazanet
Louis Sharma
Ahmedeo Shokry
Jie Xiong
Shengjie Yu
Akli Zemirli
Xiaoxu Zhou
Post-Docs
Niccolo Baldelli
Francesco Cassol
Nicolas Lopez Corral
Eduard Naichuk
Denis Rochette
Fabio Salvati
Isadora Veeren
Research activities
The research activities of the condensed matter group are devoted to the theory of correlated quantum systems, covering the whole spectrum from crystalline materials, mesoscopic or nanoscopic systems to ultracold atom gases and systems coupling matter and radiation. We aim at
1. Identifying and describing emergent collective behaviour arising from the interactions in fermionic or bosonic systems;
2. Characterizing novel quantum phases of matter (including their topological properties) and the associated quantum phase transitions;
3. Understanding structural, spectral, magnetic and transport properties of correlated systems.
An important aspect of our work is the development of theoretical approaches to tackle such systems. We make use of a wide panel of techniques, including analytical approaches (e.g. mean field theory, Bethe ansatz, Yang-Yang theory, bosonization, renormalization group analysis, slave-rotor techniques...) and large-scale numerical simulations for many-body systems (e.g. dynamical mean field theory (DMFT), exact diagonalization, quantum Monte Carlo, density matrix renormalization group (DMRG) and matrix-product states,...) and within an ab initio framework (density functional theory (DFT) and density functional perturbation theory, ab initio many-body perturbation theory (“GW approximation”), constrained random phase approximation techniques...).