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subroutine, public | em_resp_calc_oct_m::lr_calc_current (st, space, gr, lr, lr_m) |
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character(len=12) function, public | em_resp_calc_oct_m::freq2str (freq) |
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character(len=100) function, public | em_resp_calc_oct_m::em_rho_tag (freq, dir, dir2, ipert) |
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character(len=100) function, public | em_resp_calc_oct_m::em_wfs_tag (idir, ifactor, idir2, ipert) |
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integer pure function, public | em_resp_calc_oct_m::magn_dir (dir, ind) |
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character(len=2) pure function | em_resp_calc_oct_m::index2pert (ipert) |
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subroutine, public | em_resp_calc_oct_m::dlr_calc_elf (st, space, gr, kpoints, lr, lr_m) |
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subroutine, public | em_resp_calc_oct_m::dcalc_polarizability_periodic (space, mesh, symm, st, em_lr, kdotp_lr, nsigma, zpol, ndir, zpol_k) |
| alpha_ij(w) = -e sum(m occ, k) [(<u_mk(0)|-id/dk_i)|u_mkj(1)(w)> + <u_mkj(1)(-w)|(-id/dk_i|u_mk(0)>)] More...
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subroutine, public | em_resp_calc_oct_m::dcalc_polarizability_finite (namespace, space, gr, st, hm, lr, nsigma, pert, zpol, doalldirs, ndir) |
| alpha_ij(w) = - sum(m occ) [<psi_m(0)|r_i|psi_mj(1)(w)> + <psi_mj(1)(-w)|r_i|psi_m(0)>] minus sign is from electronic charge -e More...
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subroutine, public | em_resp_calc_oct_m::dlr_calc_susceptibility (namespace, space, gr, st, hm, lr, nsigma, pert, chi_para, chi_dia) |
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subroutine, public | em_resp_calc_oct_m::dlr_calc_beta (sh, namespace, space, gr, st, hm, xc, em_lr, dipole, beta, kdotp_lr, kdotp_em_lr, occ_response, dl_eig) |
| See (16) in X Andrade et al., J. Chem. Phys. 126, 184106 (2006) for finite systems and (10) in A Dal Corso et al., Phys. Rev. B 15, 15638 (1996) for periodic systems Supply only em_lr for finite systems, and both kdotp_lr and kdotp_em_lr for periodic em_lr(dir, sigma, omega) = electric perturbation of ground-state wavefunctions kdotp_lr(dir) = kdotp perturbation of ground-state wavefunctions kdotp_em_lr(dir1, dir2, sigma, omega) = kdotp perturbation of electric-perturbed wfns. More...
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subroutine | get_permutation (ii, pp) |
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subroutine | get_matrix_elements () |
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subroutine, public | em_resp_calc_oct_m::dpost_orthogonalize (space, mesh, st, nfactor, nsigma, freq_factor, omega, eta, em_lr, kdotp_em_lr) |
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subroutine, public | em_resp_calc_oct_m::dem_resp_calc_eigenvalues (space, mesh, latt, st, dl_eig) |
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subroutine, public | em_resp_calc_oct_m::dlr_calc_magneto_optics_finite (sh, sh_mo, namespace, space, gr, st, hm, ions, nsigma, nfactor, lr_e, lr_b, chi) |
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subroutine | em_resp_calc_oct_m::dcalc_kvar_energy (sh_mo, mesh, st, lr1, lr2, lr3, hpol_density) |
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subroutine, public | em_resp_calc_oct_m::dlr_calc_magneto_optics_periodic (sh, sh2, namespace, space, gr, st, hm, ions, nsigma, nfactor, nfactor_ke, freq_factor, lr_e, lr_b, lr_k, lr_ke, lr_kb, frequency, zpol, zpol_kout) |
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subroutine | apply_v (add_hartree, add_fxc, nsigma_h, nsigma_in, dir, ist0, ik0, frequency0, hvar_in, lr_in, psi_out) |
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subroutine, public | em_resp_calc_oct_m::dlr_calc_magnetization_periodic (namespace, space, mesh, st, hm, lr_k, magn) |
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subroutine, public | em_resp_calc_oct_m::dlr_calc_susceptibility_periodic (namespace, space, symm, mesh, st, hm, lr_k, lr_b, lr_kk, lr_kb, magn) |
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subroutine | em_resp_calc_oct_m::dinhomog_per_component (namespace, space, gr, st, hm, ions, idir, ik, psi_k2, psi_out, factor_tot, factor_k, factor_second) |
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subroutine | em_resp_calc_oct_m::dinhomog_per_component_2nd_order (namespace, space, gr, st, hm, ions, idir, ik, psi_k2, psi_e, psi_out, factor_tot, factor_k, factor_e) |
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subroutine, public | em_resp_calc_oct_m::dinhomog_b (sh, namespace, space, gr, st, hm, ions, idir1, idir2, lr_k1, lr_k2, psi_out) |
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subroutine | em_resp_calc_oct_m::dinhomog_eb (mesh, st, ik, add_hartree, add_fxc, hvar, psi_b, psi_kb, factor_b, psi_out, psi_k1, psi_k2) |
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subroutine | calc_hvar_lr2 (tlr_k1, tlr_k2, hvar_e, factor_tot) |
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subroutine | em_resp_calc_oct_m::dinhomog_be (namespace, space, gr, st, hm, ions, idir1, idir2, ik, add_hartree, add_fxc, hvar, psi_e1, psi_e2, psi_ek1, psi_ek2, psi_k1, psi_k2, factor_e1, factor_e2, psi_out) |
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subroutine | em_resp_calc_oct_m::dinhomog_ke (namespace, space, gr, st, hm, ions, idir, ik, psi_e, psi_out) |
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subroutine | em_resp_calc_oct_m::dinhomog_k2 (namespace, space, gr, st, hm, ions, idir1, idir2, ik, psi_k2, psi_out) |
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subroutine | em_resp_calc_oct_m::dinhomog_kb (namespace, gr, space, st, hm, ions, idir, idir1, idir2, ik, psi_b, psi_k1, psi_k2, psi_out) |
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subroutine, public | em_resp_calc_oct_m::dinhomog_kb_tot (sh, namespace, space, gr, st, hm, ions, idir, idir1, idir2, lr_k, lr_b, lr_k1, lr_k2, lr_kk1, lr_kk2, psi_out) |
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subroutine, public | em_resp_calc_oct_m::dinhomog_ke_tot (sh, namespace, space, gr, st, hm, ions, idir, nsigma, lr_k, lr_e, lr_kk, psi_out) |
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subroutine, public | em_resp_calc_oct_m::dinhomog_k2_tot (namespace, space, gr, st, hm, ions, idir1, idir2, lr_k1, lr_k2, psi_out) |
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subroutine | em_resp_calc_oct_m::dcalc_rho (mesh, st, factor, factor_sum, factor_e, factor_k, lr_e, lr_k, lr0) |
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subroutine | em_resp_calc_oct_m::dcalc_hvar_psi (mesh, st, ik, hvar, psi_out) |
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subroutine | em_resp_calc_oct_m::dcalc_hvar_lr (mesh, st, ik, hvar, psi_in, factor1, factor2, psi_out) |
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subroutine | em_resp_calc_oct_m::dmf_dotp_matrix (mesh, nst, dim, psi1, psi2, res, factor) |
| Multiplication of two blocks of states. More...
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subroutine, public | em_resp_calc_oct_m::zlr_calc_elf (st, space, gr, kpoints, lr, lr_m) |
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subroutine, public | em_resp_calc_oct_m::zcalc_polarizability_periodic (space, mesh, symm, st, em_lr, kdotp_lr, nsigma, zpol, ndir, zpol_k) |
| alpha_ij(w) = -e sum(m occ, k) [(<u_mk(0)|-id/dk_i)|u_mkj(1)(w)> + <u_mkj(1)(-w)|(-id/dk_i|u_mk(0)>)] More...
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subroutine, public | em_resp_calc_oct_m::zcalc_polarizability_finite (namespace, space, gr, st, hm, lr, nsigma, pert, zpol, doalldirs, ndir) |
| alpha_ij(w) = - sum(m occ) [<psi_m(0)|r_i|psi_mj(1)(w)> + <psi_mj(1)(-w)|r_i|psi_m(0)>] minus sign is from electronic charge -e More...
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subroutine, public | em_resp_calc_oct_m::zlr_calc_susceptibility (namespace, space, gr, st, hm, lr, nsigma, pert, chi_para, chi_dia) |
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subroutine, public | em_resp_calc_oct_m::zlr_calc_beta (sh, namespace, space, gr, st, hm, xc, em_lr, dipole, beta, kdotp_lr, kdotp_em_lr, occ_response, dl_eig) |
| See (16) in X Andrade et al., J. Chem. Phys. 126, 184106 (2006) for finite systems and (10) in A Dal Corso et al., Phys. Rev. B 15, 15638 (1996) for periodic systems Supply only em_lr for finite systems, and both kdotp_lr and kdotp_em_lr for periodic em_lr(dir, sigma, omega) = electric perturbation of ground-state wavefunctions kdotp_lr(dir) = kdotp perturbation of ground-state wavefunctions kdotp_em_lr(dir1, dir2, sigma, omega) = kdotp perturbation of electric-perturbed wfns. More...
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subroutine, public | em_resp_calc_oct_m::zpost_orthogonalize (space, mesh, st, nfactor, nsigma, freq_factor, omega, eta, em_lr, kdotp_em_lr) |
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subroutine, public | em_resp_calc_oct_m::zem_resp_calc_eigenvalues (space, mesh, latt, st, dl_eig) |
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subroutine, public | em_resp_calc_oct_m::zlr_calc_magneto_optics_finite (sh, sh_mo, namespace, space, gr, st, hm, ions, nsigma, nfactor, lr_e, lr_b, chi) |
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subroutine | em_resp_calc_oct_m::zcalc_kvar_energy (sh_mo, mesh, st, lr1, lr2, lr3, hpol_density) |
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subroutine, public | em_resp_calc_oct_m::zlr_calc_magneto_optics_periodic (sh, sh2, namespace, space, gr, st, hm, ions, nsigma, nfactor, nfactor_ke, freq_factor, lr_e, lr_b, lr_k, lr_ke, lr_kb, frequency, zpol, zpol_kout) |
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subroutine | apply_v (add_hartree, add_fxc, nsigma_h, nsigma_in, dir, ist0, ik0, frequency0, hvar_in, lr_in, psi_out) |
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subroutine, public | em_resp_calc_oct_m::zlr_calc_magnetization_periodic (namespace, space, mesh, st, hm, lr_k, magn) |
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subroutine, public | em_resp_calc_oct_m::zlr_calc_susceptibility_periodic (namespace, space, symm, mesh, st, hm, lr_k, lr_b, lr_kk, lr_kb, magn) |
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subroutine | em_resp_calc_oct_m::zinhomog_per_component (namespace, space, gr, st, hm, ions, idir, ik, psi_k2, psi_out, factor_tot, factor_k, factor_second) |
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subroutine | em_resp_calc_oct_m::zinhomog_per_component_2nd_order (namespace, space, gr, st, hm, ions, idir, ik, psi_k2, psi_e, psi_out, factor_tot, factor_k, factor_e) |
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subroutine, public | em_resp_calc_oct_m::zinhomog_b (sh, namespace, space, gr, st, hm, ions, idir1, idir2, lr_k1, lr_k2, psi_out) |
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subroutine | em_resp_calc_oct_m::zinhomog_eb (mesh, st, ik, add_hartree, add_fxc, hvar, psi_b, psi_kb, factor_b, psi_out, psi_k1, psi_k2) |
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subroutine | calc_hvar_lr2 (tlr_k1, tlr_k2, hvar_e, factor_tot) |
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subroutine | em_resp_calc_oct_m::zinhomog_be (namespace, space, gr, st, hm, ions, idir1, idir2, ik, add_hartree, add_fxc, hvar, psi_e1, psi_e2, psi_ek1, psi_ek2, psi_k1, psi_k2, factor_e1, factor_e2, psi_out) |
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subroutine | em_resp_calc_oct_m::zinhomog_ke (namespace, space, gr, st, hm, ions, idir, ik, psi_e, psi_out) |
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subroutine | em_resp_calc_oct_m::zinhomog_k2 (namespace, space, gr, st, hm, ions, idir1, idir2, ik, psi_k2, psi_out) |
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subroutine | em_resp_calc_oct_m::zinhomog_kb (namespace, gr, space, st, hm, ions, idir, idir1, idir2, ik, psi_b, psi_k1, psi_k2, psi_out) |
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subroutine, public | em_resp_calc_oct_m::zinhomog_kb_tot (sh, namespace, space, gr, st, hm, ions, idir, idir1, idir2, lr_k, lr_b, lr_k1, lr_k2, lr_kk1, lr_kk2, psi_out) |
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subroutine, public | em_resp_calc_oct_m::zinhomog_ke_tot (sh, namespace, space, gr, st, hm, ions, idir, nsigma, lr_k, lr_e, lr_kk, psi_out) |
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subroutine, public | em_resp_calc_oct_m::zinhomog_k2_tot (namespace, space, gr, st, hm, ions, idir1, idir2, lr_k1, lr_k2, psi_out) |
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subroutine | em_resp_calc_oct_m::zcalc_rho (mesh, st, factor, factor_sum, factor_e, factor_k, lr_e, lr_k, lr0) |
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subroutine | em_resp_calc_oct_m::zcalc_hvar_psi (mesh, st, ik, hvar, psi_out) |
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subroutine | em_resp_calc_oct_m::zcalc_hvar_lr (mesh, st, ik, hvar, psi_in, factor1, factor2, psi_out) |
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subroutine | em_resp_calc_oct_m::zmf_dotp_matrix (mesh, nst, dim, psi1, psi2, res, factor) |
| Multiplication of two blocks of states. More...
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