T-7: Difference between revisions
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We introduce the <ins>Green functions</ins> <math> G_{ab}(z) </math>: these are functions of a complex variable belonging to the upper half of the complex plane, and are defined by | We introduce the <ins>Green functions</ins> <math> G_{ab}(z) </math>: these are functions of a complex variable belonging to the upper half of the complex plane, and are defined by [NOTA SU STILTJIES] | ||
<center> <math> | <center> <math> | ||
G_{ab}(z)= \langle a| \frac{1}{z-H}| b \rangle | G_{ab}(z)= \langle a| \frac{1}{z-H}| b \rangle | ||
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</math> | </math> | ||
</center> | </center> | ||
It is clear that when the kinetic term <math>V </math> in the Hamiltonian vanishes, the local self-energies vanish; these quantities encode how much the energy levels <math> \epsilon_a </math> are shifted by the presence of the kinetic term <math>V </math>. | It is clear that when the kinetic term <math>V </math> in the Hamiltonian vanishes, the local self-energies vanish; these quantities encode how much the energy levels <math> \epsilon_a </math> are shifted by the presence of the kinetic term <math>V </math>. </li> | ||
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<ins> Y </ins>. | <ins> Y </ins>. | ||
- model on the be the lattice | - model on the be the lattice |
Revision as of 17:19, 13 January 2024
Goal: the goal of this set of problems is to derive an estimate for the transition point for the Anderson model on the Bethe lattice.
Techniques: cavity method, stability analysis.
A criterion for localization
- Green functions and self-energies. Given a lattice with sites , we call the wave function completely localised in site . The Anderson model has Hamiltonian
We introduce the Green functions : these are functions of a complex variable belonging to the upper half of the complex plane, and are defined by [NOTA SU STILTJIES]
The local self-energies are functions defined by the equality
- Bouchaud. Weak ergodicity breaking and aging in disordered systems [1]
Y . - model on the be the lattice - self energy -criterion for localization - links to ergo breaking
Problem 7.1:
the cavity equation and the linearisation