L-7: Difference between revisions
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(Created page with "<Strong> Goal </Strong>: This is the first lecture about the localization. Localization is a <Strong> wave phenomenon induced by disorder.</Strong> == The Gaussian packet of free particles: the ballistic behaviour == == The conductance and the diffusive behaviour == Ohm's laws characterize electric transport of (good or bad) conductors: * First law: <center><math> \frac{V}{I}= R, \quad \text{or} \quad \frac{I}{V}= G </math></center> Here <math>R </math> is the res...") |
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== The Gaussian packet of free particles: the ballistic behaviour == | == The Gaussian packet of free particles: the ballistic behaviour == | ||
[[File:Localization1DB.png|thumb|left|x140px|BCE and 1D localization]] | |||
[[File:Localization1DA.png|thumb|left|x140px|BCE and 1D localization]] | |||
== The conductance and the diffusive behaviour == | == The conductance and the diffusive behaviour == |
Revision as of 18:42, 7 March 2024
Goal : This is the first lecture about the localization. Localization is a wave phenomenon induced by disorder.
The Gaussian packet of free particles: the ballistic behaviour
File:Localization1DA.png
BCE and 1D localization
The conductance and the diffusive behaviour
Ohm's laws characterize electric transport of (good or bad) conductors:
- First law:
Here is the resistence of the sample and is its conductance.\
- Second law
Here are the resistivity and the conductivity. These are material properties, independent of the geometry of the sample These phenomenological laws are a macroscpic manifestation of the diffusive motion of the electrons. From the Drude model we know that disorder is the crucial ingredient to justify the presence of diffusion. ]