Home
last modified time | relevance | path

Searched refs:gamma_N (Results 1 – 5 of 5) sorted by relevance

/dports/science/py-phono3py/phono3py-1.22.3/phono3py/phonon3/
H A Dconductivity_RTA.py220 gamma_N, gamma_U = br.get_gamma_N_U()
234 if gamma_N is None:
274 if gamma_N is None:
291 gamma_N=gamma_N_at_sigma,
340 gamma_N, gamma_U = br.get_gamma_N_U()
359 if gamma_N is None:
362 gamma_N_at_sigma = gamma_N[i]
405 gamma_N = np.zeros_like(gamma)
430 gamma_N[j] = data['gamma_N']
486 br.set_gamma_N_U(gamma_N, gamma_U)
[all …]
/dports/math/xlife++/xlifepp-sources-v2.0.1-2018-05-09/doc/tex/
H A DMaxwell_BEM.tex75 $$[\gamma_t]_\Gamma=\gamma_t^+-\gamma_t^-,\ [\gamma_N]_\Gamma=\gamma_N^+-\gamma_N^-,\
76 \{\gamma_t\}_\Gamma=\half(\gamma_t^++\gamma_t^-),\ \{\gamma_N\}_\Gamma=\half(\gamma_N^++\gamma_N^-…
175 …$$\gamma_N^\pm\vpsi_{SL}=\gamma_t^\pm\vpsi_{DL},\ \ \gamma_N^\pm\vpsi_{DL}=\gamma_t^\pm\vpsi_{SL}.…
210 \gamma_N^-\vE=S(\gamma_t^-\vE)+\half\gamma_N^-\vE+C(\gamma_N^-\vE), &
211 \gamma_N^+\vE=-S(\gamma_t^+\vE)+\half\gamma_N^+\vE-C(\gamma_N^+\vE).
372 \{\gamma_N\}_\Gamma E=-S([\gamma_t]_\Gamma E)-C([\gamma_N]_\Gamma E) \label{trace_N}
380 $$S(\gamma_N^+ E)=(\half\Id+C)(\gamma_t^+E_i).$$
382 $$\half\gamma_N^+E=-S(\gamma_t^+E)-C(\half\gamma_N^+E)$$
386 $$\gamma_t^+E=-S([\gamma_N]_\Gamma E)$$
388 $$S([\gamma_N]_\Gamma E)=\gamma_t^+E_i.$$
[all …]
/dports/science/py-phono3py/phono3py-1.22.3/phono3py/
H A Dfile_IO.py778 gamma_N=None, argument
840 if gamma_N is not None:
841 w.create_dataset('gamma_N', data=gamma_N,
/dports/science/py-phono3py/phono3py-1.22.3/c/
H A D_phono3py.c736 double *gamma_N; in py_get_detailed_imag_self_energy_with_g() local
763 gamma_N = (double*)PyArray_DATA(py_gamma_N); in py_get_detailed_imag_self_energy_with_g()
773 gamma_N, in py_get_detailed_imag_self_energy_with_g()
/dports/science/py-phono3py/phono3py-1.22.3/doc/
H A Dcommand-options.rst701 accessed by ``gamma_N`` and ``gamma_U`` keys. The shape of the arrays
719 'gamma_N',
735 In [5]: f['gamma_N'].shape