BEGIN_PROVIDER [ integer, nnuc ] implicit none BEGIN_DOC ! Number of nuclei END_DOC nnuc = 2 END_PROVIDER BEGIN_PROVIDER [ integer, typenuc ] &BEGIN_PROVIDER [integer, typenuc_arr, (nnuc)] implicit none BEGIN_DOC ! Type of the nuclei END_DOC typenuc = 1 typenuc_arr = (/1, 1/) END_PROVIDER BEGIN_PROVIDER [ double precision, nuc_coord, (nnuc, 3) ] implicit none BEGIN_DOC ! Nuclei coordinates END_DOC character(len=*), parameter :: FILE_NAME = "geometry.txt" integer :: fu, rc, i open(action='read', file=FILE_NAME, iostat=rc, newunit=fu) do i = 1, nnuc read(fu, *) nuc_coord(i, :) end do close(fu) END_PROVIDER BEGIN_PROVIDER [ double precision, elnuc_dist, (nelec, nnuc) ] implicit none BEGIN_DOC ! e-n distance END_DOC integer :: i, j double precision :: x, y, z do j = 1, nnuc do i = 1, nelec x = elec_coord(i, 1) - nuc_coord(j, 1) y = elec_coord(i, 2) - nuc_coord(j, 2) z = elec_coord(i, 3) - nuc_coord(j, 3) elnuc_dist(i, j) = dsqrt( x*x + y*y + z*z ) enddo enddo END_PROVIDER BEGIN_PROVIDER [double precision, factor_en] implicit none BEGIN_DOC ! Electron-nuclei contribution to Jastrow factor END_DOC integer :: i, a, p, q double precision :: pow_ser, x factor_en = 0.0d0 do a = 1 , nnuc do i = 1, nelec x = rescale_en(i, a) pow_ser = 0.0d0 do p = 2, naord x = x * rescale_en(i, a) pow_ser = pow_ser + aord_vect(p + 1, typenuc_arr(a)) * x end do factor_en = factor_en + aord_vect(1, typenuc_arr(a)) * rescale_en(i, a) & / (1.0d0 + aord_vect(2, typenuc_arr(a)) * rescale_en(i, a)) + pow_ser end do end do END_PROVIDER BEGIN_PROVIDER [double precision, factor_en_deriv_e, (4, nelec) ] implicit none BEGIN_DOC ! Dimensions 1-3 : dx, dy, dz ! Dimension 4 : d2x + d2y + d2z END_DOC integer :: i, ii, a, p, q double precision :: x, x_inv, y, den, invden, lap1, lap2 double precision, dimension(4) :: dx, pow_ser_g factor_en_deriv_e = 0.0d0 do a = 1 , nnuc do i = 1, nelec pow_ser_g = 0.0d0 den = 1.0d0 + aord_vect(2, typenuc_arr(a)) * rescale_en(i, a) invden = 1.0d0 / den do ii = 1, 4 dx(ii) = rescale_en_deriv_e(ii, i, a) enddo lap1 = 0.0d0 lap2 = 0.0d0 do ii = 1, 3 x = rescale_en(i, a) x_inv = 1.0d0 / x do p = 2, naord pow_ser_g(ii) += p * aord_vect(p + 1, typenuc_arr(a)) * x * dx(ii) pow_ser_g(4) += p * (p - 1) * aord_vect(p + 1, typenuc_arr(a)) * x * x_inv * dx(ii) * dx(ii) lap2 += p * aord_vect(p + 1, typenuc_arr(a)) * x x = x * rescale_en(i, a) end do ! (a1 (-2 a2 r'[i,a]^2+(1+a2 r[i,a]) r''[i,a]))/(1+a2 r[i,a])^3 lap1 += -2.0d0 * aord_vect(2, typenuc_arr(a)) * dx(ii) * dx(ii) ! \frac{\text{a1} r'(i,a)}{(\text{a2} r(i,a)+1)^2} factor_en_deriv_e(ii, i) += aord_vect(1, typenuc_arr(a)) & * dx(ii) * invden * invden + pow_ser_g(ii) enddo ii = 4 lap1 += den * dx(ii) lap1 = lap1 * aord_vect(1, typenuc_arr(a)) * invden * invden * invden pow_ser_g(ii) += lap1 + lap2 * dx(ii) factor_en_deriv_e(ii, i) += pow_ser_g(ii) end do end do END_PROVIDER