Self-consistent Hartree-Fock approach to Phase Transitions: Difference between revisions
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==== Hartree-Fock in second quantized form ==== | ==== Hartree-Fock in second quantized form ==== | ||
<math> \nu = \frac{1}{2} \sum_{\sigma \sigma\prime} \int d^{3}r d^{3}r\prime </math> | <math> \nu = \frac{1}{2} \sum_{\sigma \sigma^{\prime}} \int d^{3}r d^{3}r^{\prime} v(\vector{r}-\vector{r^{\prime}}) \psi_{\sigma}^{\dagger} </math> | ||
Revision as of 17:19, 30 November 2012
Hartree-Fock approach to Phase Transitions
Hartree-Fock in second quantized form
Failed to parse (unknown function "\vector"): {\displaystyle \nu = \frac{1}{2} \sum_{\sigma \sigma^{\prime}} \int d^{3}r d^{3}r^{\prime} v(\vector{r}-\vector{r^{\prime}}) \psi_{\sigma}^{\dagger} }