Dynamical Mean Field Theory (DMFT) Solvers
Dynamical mean field theory (DMFT) maps the lattice Hubbard model onto a self-consistently determined quantum impurity problem, capturing strongly correlated phenomena — such as the Mott metal-insulator transition — that static mean-field theories miss entirely. These tutorials work through the ALPS DMFT self-consistency loop and its quantum impurity solvers, then apply them to a series of physically motivated examples on the Bethe lattice and beyond.
Introduction
- DMFT-01 An introduction to DMFT — motivates the DMFT approximation and its mapping onto a quantum impurity problem, and gives a roadmap of the tutorials that follow.
Impurity Solvers
ALPS provides three solvers for the DMFT impurity problem, all applied here to the same metal–antiferromagnetic-insulator transition so their results can be directly compared: the continuous-time hybridization-expansion algorithm (CT-HYB), the continuous-time interaction-expansion algorithm (CT-INT), and the older discrete-time Hirsch-Fye algorithm, whose systematic errors motivated the development of the continuous-time methods.
- DMFT-02 CT-HYB: the CT-HYB QMC solver — introduces the hybridization-expansion solver and uses it to trace out the metal–antiferromagnetic-insulator transition of the Hubbard model on the Bethe lattice as a function of temperature.
- DMFT-03 CT-INT: the CT-INT QMC solver — repeats the same exercise with the interaction-expansion solver.
- DMFT-07 The Hirsch-Fye solver — repeats the exercise once more with the discrete-time Hirsch-Fye solver, and discusses why continuous-time algorithms have largely superseded it.
Physics Applications
- DMFT-04 Mott Transition — studies the paramagnetic Mott transition, the metal-insulator transition realized in materials such as , by suppressing antiferromagnetic order and scanning the interaction strength at fixed temperature.
- DMFT-05 Orbitally Selective Mott Transition — extends the method to a two-band model in which one orbital can become Mott insulating while the other remains metallic, a phenomenon first identified in ruthenates such as CaSrRuO.
- DMFT-06 Paramagnetic metal and extrapolation errors — compares CT-HYB and CT-INT self-energies for a paramagnetic metal against Hirsch-Fye and exact-diagonalization benchmarks, illustrating how discretization and statistical errors show up in practice.
Beyond the Bethe Lattice
- DMFT-08 Setting a particular lattice — shows how to move beyond the default semicircular Bethe-lattice density of states to a general lattice, including square, cubic, and hexagonal geometries and two-dimensional dispersions evaluated by Hilbert-transformed k-space integration.
Putting It Together
- DMFT-09 Néel transition in single site DMFT — a combined example that reproduces the antiferromagnetic Néel transition with all three impurity solvers side by side, so their results can be compared directly.