Differences
This shows you the differences between two versions of the page.
| Both sides previous revision Previous revision | Next revision Both sides next revision | ||
|
classical_microcanonical_phase_volume [2013/11/02 03:28] nikolaj |
classical_microcanonical_phase_volume [2013/11/02 03:28] nikolaj |
||
|---|---|---|---|
| Line 10: | Line 10: | ||
| === Alternative definitions === | === Alternative definitions === | ||
| - | $\Gamma(E):=\frac{1}{h^{3N}N!}\int_{\Gamma_{\mathcal M}}\ \hat\rho(E;{\bf q},{\bf p}) \ \mathrm d\Gamma $ | + | $\Gamma(E):=\frac{1}{h^{3N}N!}\int_{\Gamma_{\mathcal M}} \hat\rho(E;{\bf q},{\bf p}) \ \mathrm d\Gamma $ |
| And here we see that this is the analog of [[Classical canonical partition function]] for the [[Classical canonical ensemble]]. | And here we see that this is the analog of [[Classical canonical partition function]] for the [[Classical canonical ensemble]]. | ||
