Crack propagation is considered as a random walk process of consecutive atomic bond breaking and healing steps. The total number of steps is propo~ion~ to tfre propa~t~n time, and the difference of the number of breaking and healing steps is propo~ional to the location of the crack tip at that time.
On the theory of propagation in random systems
โ Scribed by V.F. Los'
- Publisher
- Elsevier Science
- Year
- 1991
- Tongue
- English
- Weight
- 222 KB
- Volume
- 175
- Category
- Article
- ISSN
- 0921-4526
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โฆ Synopsis
With the help of a projection operator technique a new representation of the Kubo-Greenwood formula for the conductivity in a disordered system, which contains a vertex function in explicit analytical form, is obtained. The summing up of conventional diagrams in the tight-binding approximation gives an expression for the conductivity tensor which describes the Anderson localization of electrons in a strongly disordered alloy. This expression does not coincide with previous results.
In our opinion, a direct theory of conductivity in strongly disordered systems is absent at this moment. There are some ambiguities in papers dealing with electron localization in such systems (see, e.g., refs. [1,2]).
To re-examine this problem we propose a new and direct approach to the investigation of the conductivity of disordered systems based on a projection operator technique. Let us consider noninteracting electrons scattering on a static potential. The conductivity of such a system is given by the Kubo-Greenwood formula
๐ SIMILAR VOLUMES
Some existence theorems for the Hehnholtz equation in three dimensions and in all space are proven, when the index of refraction is characterized by a random function. These results are used to apply the Born approximation for the scattering of a wave incident in a thin indefinite layer.