T-7: Difference between revisions
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</math> | </math> | ||
</center> | </center> | ||
We introduce the | 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 | ||
<center> <math> | <center> <math> | ||
G_{ab}= \langle a| \frac{1}{z-H}| b \rangle | G_{ab}(z)= \langle a| \frac{1}{z-H}| b \rangle | ||
</math> | </math> | ||
</center> | </center> | ||
The <ins>local self-energies</ins> <math> \sigma_a(z)</math> are functions defined by the equality | |||
<center> <math> | |||
G_{aa}(z)= \langle a| \frac{1}{z-H}| a\rangle = \frac{1}{z- \epsilon_a-\sigma_a(z)}. | |||
</math> | |||
</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>. | |||
<ins> Y </ins>. | <ins> Y </ins>. |
Revision as of 17:18, 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
The local self-energies are functions defined by the equality
It is clear that when the kinetic term in the Hamiltonian vanishes, the local self-energies vanish; these quantities encode how much the energy levels are shifted by the presence of the kinetic term .
Y .
- Bouchaud. Weak ergodicity breaking and aging in disordered systems [1]
- model on the be the lattice - self energy -criterion for localization - links to ergo breaking
Problem 7.1:
the cavity equation and the linearisation