subroutine pt2_epstein_nesbet(det_pert,c_pert,e_2_pert,H_pert_diag,Nint,ndet,n_st) use bitmasks implicit none integer, intent(in) :: Nint,ndet,n_st integer(bit_kind), intent(in) :: det_pert(Nint,2) double precision , intent(out) :: c_pert(n_st),e_2_pert(n_st),H_pert_diag double precision :: i_H_psi_array(N_st) BEGIN_DOC ! compute the standard Epstein-Nesbet perturbative first order coefficient and second order energetic contribution ! ! for the various n_st states. ! ! c_pert(i) = /( E(i) - ) ! ! e_2_pert(i) = ^2/( E(i) - ) ! END_DOC integer :: i,j double precision :: diag_H_mat_elem double precision, parameter :: eps = tiny(1.d0) ASSERT (Nint == N_int) ASSERT (Nint > 0) call i_H_psi(det_pert,psi_ref,psi_ref_coef,Nint,ndet,psi_ref_size,n_st,i_H_psi_array) H_pert_diag = diag_H_mat_elem(det_pert,Nint) do i =1,n_st c_pert(i) = i_H_psi_array(i) / (reference_energy(i) - H_pert_diag + eps) e_2_pert(i) = c_pert(i) * i_H_psi_array(i) enddo end subroutine pt2_epstein_nesbet_2x2(det_pert,c_pert,e_2_pert,H_pert_diag,Nint,ndet,n_st) use bitmasks implicit none integer, intent(in) :: Nint,ndet,n_st integer(bit_kind), intent(in) :: det_pert(Nint,2) double precision , intent(out) :: c_pert(n_st),e_2_pert(n_st),H_pert_diag double precision :: i_H_psi_array(N_st) BEGIN_DOC ! compute the Epstein-Nesbet 2x2 diagonalization coefficient and energetic contribution ! ! for the various n_st states. ! ! e_2_pert(i) = 0.5 * (( - E(i) ) - sqrt( ( - E(i)) ^2 + 4 ^2 ) ! ! c_pert(i) = e_2_pert(i)/ ! END_DOC integer :: i,j double precision :: diag_H_mat_elem,delta_e double precision, parameter :: eps = tiny(1.d0) ASSERT (Nint == N_int) ASSERT (Nint > 0) call i_H_psi(det_pert,psi_ref,psi_ref_coef,Nint,N_det_ref,psi_ref_size,n_st,i_H_psi_array) H_pert_diag = diag_H_mat_elem(det_pert,Nint) do i =1,n_st delta_e = H_pert_diag - reference_energy(i) e_2_pert(i) = 0.5d0 * (delta_e - dsqrt(delta_e * delta_e + 4.d0 * i_H_psi_array(i) * i_H_psi_array(i))) c_pert(i) = e_2_pert(i)/(i_H_psi_array(i)+eps) enddo end