Self-consistent Hartree-Fock approach to Phase Transitions: Difference between revisions

Revision as of 17:20, 30 November 2012

$\nu ={\frac {1}{2}}\sum _{\sigma \sigma ^{\prime }}\int d^{3}rd^{3}r^{\prime }v({\vec {r}}-{\vec {r^{\prime }}})\psi _{\sigma }$

Revision as of 17:20, 30 November 2012 (view source) TimKeiper (talk \| contribs) (→‎Hartree-Fock in second quantized form) ← Older edit		Revision as of 17:20, 30 November 2012 (view source) TimKeiper (talk \| contribs) (→‎Hartree-Fock in second quantized form) Newer edit →
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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} v(\~~vector~~{r}-\~~vector~~{r^{\prime}}) \psi_{\sigma} </math>		<math> \nu = \frac{1}{2} \sum_{\sigma \sigma^{\prime}} \int d^{3}r d^{3}r^{\prime} v(\vec{r}-\vec{r^{\prime}}) \psi_{\sigma} </math>