Category:Constrained-random-phase approximation: Difference between revisions
Line 2: | Line 2: | ||
== Theoretical Background == | == Theoretical Background == | ||
The constrained random phase approximation (CRPA) is a method that allows to calculate the effective interaction | The constrained random phase approximation (CRPA) is a method that allows to calculate the effective interaction parameter U, J and J' for model Hamiltonians. | ||
The main idea is to neglect screening effects of states in the screened Coulomb interaction. | The main idea is to neglect screening effects of specific '''target states''' in the screened Coulomb interaction W of the [[The GW approximation of Hedin's equations|GW method]]. | ||
The resulting partially screened Coulomb interaction is usually evaluated in a localized basis that spans the target space and is described by the model Hamiltonian. | |||
The target space is typically low-dimensional and therefore allows for the application of a higher level theory, such as dynamical mean field theory. | |||
== How to == | == How to == |
Revision as of 12:26, 6 April 2022
All tags and articles that deal with CRPA calculations are members of this category.
Theoretical Background
The constrained random phase approximation (CRPA) is a method that allows to calculate the effective interaction parameter U, J and J' for model Hamiltonians. The main idea is to neglect screening effects of specific target states in the screened Coulomb interaction W of the GW method. The resulting partially screened Coulomb interaction is usually evaluated in a localized basis that spans the target space and is described by the model Hamiltonian. The target space is typically low-dimensional and therefore allows for the application of a higher level theory, such as dynamical mean field theory.
How to
Pages in category "Constrained-random-phase approximation"
The following 7 pages are in this category, out of 7 total.