Searched refs:gamma_N (Results 1 – 5 of 5) sorted by relevance
/dports/science/py-phono3py/phono3py-1.22.3/phono3py/phonon3/ |
H A D | conductivity_RTA.py | 220 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 …]
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/dports/math/xlife++/xlifepp-sources-v2.0.1-2018-05-09/doc/tex/ |
H A D | Maxwell_BEM.tex | 75 $$[\gamma_t]_\Gamma=\gamma_t^+-\gamma_t^-,\ [\gamma_N]_\Gamma=\gamma_N^+-\gamma_N^-,\ 76 \{\gamma_t\}_\Gamma=\half(\gamma_t^++\gamma_t^-),\ \{\gamma_N\}_\Gamma=\half(\gamma_N^++\gamma_N^-… 175 …$$\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 …]
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/dports/science/py-phono3py/phono3py-1.22.3/phono3py/ |
H A D | file_IO.py | 778 gamma_N=None, argument 840 if gamma_N is not None: 841 w.create_dataset('gamma_N', data=gamma_N,
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/dports/science/py-phono3py/phono3py-1.22.3/c/ |
H A D | _phono3py.c | 736 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()
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/dports/science/py-phono3py/phono3py-1.22.3/doc/ |
H A D | command-options.rst | 701 accessed by ``gamma_N`` and ``gamma_U`` keys. The shape of the arrays 719 'gamma_N', 735 In [5]: f['gamma_N'].shape
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