mirror of
https://github.com/QuantumPackage/qp2.git
synced 2024-12-23 04:43:45 +01:00
| .. | ||
| deb_aos.irp.f | ||
| deb_deriv_mu.irp.f | ||
| deb_j_bump.irp.f | ||
| deb_j_gauss.irp.f | ||
| deb_j_mu_of_r.irp.f | ||
| deb_j_psi.irp.f | ||
| deb_mos.irp.f | ||
| debug_fit.irp.f | ||
| debug_integ_jmu_modif.irp.f | ||
| grad_squared_manu.irp.f | ||
| grad_squared.irp.f | ||
| grad_tc_int.irp.f | ||
| j12_nucl_utils.irp.f | ||
| j_bump.irp.f | ||
| jast_1e_utils.irp.f | ||
| jast_1e.irp.f | ||
| jast_2e_utils.irp.f | ||
| jast_deriv_mu_of_r.irp.f | ||
| jast_deriv_utils_vect.irp.f | ||
| jast_deriv_utils.irp.f | ||
| jast_deriv.irp.f | ||
| jastrow_psi.irp.f | ||
| mu_of_r_mean_field.irp.f | ||
| mu_of_r.irp.f | ||
| NEED | ||
| new_grad_tc_manu.irp.f | ||
| numerical_integ.irp.f | ||
| plot_j_gauss.irp.f | ||
| plot_mo.irp.f | ||
| plot_mu_of_r.irp.f | ||
| pot_j_gauss.irp.f | ||
| print_j1ecoef_info.irp.f | ||
| print_jastrow_psi.irp.f | ||
| qmckl.irp.f | ||
| README.rst | ||
| tc_integ_num.irp.f | ||
| tc_integ.irp.f | ||
| test_mu_of_r_tc.irp.f | ||
| test_non_h_ints.irp.f | ||
| total_tc_int.irp.f | ||
============= non_h_ints_mu ============= Computes the non hermitian potential of the mu-TC Hamiltonian on the AO and BI-ORTHO MO basis. The operator is defined in Eq. 33 of JCP 154, 084119 (2021) The two providers are : +) ao_non_hermit_term_chemist which returns the non hermitian part of the two-electron TC Hamiltonian on the MO basis. +) mo_non_hermit_term_chemist which returns the non hermitian part of the two-electron TC Hamiltonian on the BI-ORTHO MO basis.