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195 lines
7.1 KiB
Fortran
195 lines
7.1 KiB
Fortran
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subroutine ecmd_pbe_ueg_at_r(mu,r,eps_c_md_PBE)
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implicit none
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BEGIN_DOC
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! provides the integrand of Eq. (13) of Phys.Chem.Lett.2019, 10, 2931 2937
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!
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! !!! WARNING !!! This is the total integrand of Eq. (13), which is e_cmd * n
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!
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! such a function is based on the exact behaviour of the Ecmd at large mu
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!
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! but with the exact on-top estimated with that of the UEG
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!
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! You enter with r(3), you get out with eps_c_md_PBE(1:N_states)
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END_DOC
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double precision, intent(in) :: mu , r(3)
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double precision, intent(out) :: eps_c_md_PBE(N_states)
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double precision :: pi, e_PBE, beta
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double precision :: aos_array(ao_num), grad_aos_array(3,ao_num)
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double precision :: rho_a(N_states),rho_b(N_states)
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double precision :: grad_rho_a(3,N_states),grad_rho_b(3,N_states)
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double precision :: grad_rho_a_2(N_states),grad_rho_b_2(N_states),grad_rho_a_b(N_states)
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double precision :: rhoc,rhoo,sigmacc,sigmaco,sigmaoo,vrhoc,vrhoo,vsigmacc,vsigmaco,vsigmaoo
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double precision :: g0_UEG_mu_inf, denom
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integer :: m, istate
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pi = 4.d0 * datan(1.d0)
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eps_c_md_PBE = 0.d0
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call density_and_grad_alpha_beta_and_all_aos_and_grad_aos_at_r(r,rho_a,rho_b, grad_rho_a, grad_rho_b, aos_array, grad_aos_array)
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grad_rho_a_2 = 0.d0
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grad_rho_b_2 = 0.d0
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grad_rho_a_b = 0.d0
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do istate = 1, N_states
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do m = 1, 3
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grad_rho_a_2(istate) += grad_rho_a(m,istate)*grad_rho_a(m,istate)
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grad_rho_b_2(istate) += grad_rho_b(m,istate)*grad_rho_b(m,istate)
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grad_rho_a_b(istate) += grad_rho_a(m,istate)*grad_rho_b(m,istate)
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enddo
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enddo
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do istate = 1, N_states
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! convertion from (alpha,beta) formalism to (closed, open) formalism
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call rho_ab_to_rho_oc(rho_a(istate),rho_b(istate),rhoo,rhoc)
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call grad_rho_ab_to_grad_rho_oc(grad_rho_a_2(istate),grad_rho_b_2(istate),grad_rho_a_b(istate),sigmaoo,sigmacc,sigmaco)
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call ec_pbe_only(0.d0,rhoc,rhoo,sigmacc,sigmaco,sigmaoo,e_PBE)
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if(mu == 0.d0) then
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eps_c_md_PBE(istate)=e_PBE
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else
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! note: the on-top pair density is (1-zeta^2) rhoc^2 g0 = 4 rhoa * rhob * g0
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denom = (-2.d0+sqrt(2d0))*sqrt(2.d0*pi) * 4.d0*rho_a(istate)*rho_b(istate)*g0_UEG_mu_inf(rho_a(istate),rho_b(istate))
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if (dabs(denom) > 1.d-12) then
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beta = (3.d0*e_PBE)/denom
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eps_c_md_PBE(istate)=e_PBE/(1.d0+beta*mu**3)
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else
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eps_c_md_PBE(istate)=0.d0
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endif
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endif
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enddo
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end
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subroutine eps_c_md_PBE_from_density(mu,rho_a,rho_b, grad_rho_a, grad_rho_b,eps_c_md_PBE) ! EG
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implicit none
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BEGIN_DOC
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! provides the integrand of Eq. (13) of Phys.Chem.Lett.2019, 10, 2931 2937
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!
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! !!! WARNING !!! This is the total integrand of Eq. (13), which is e_cmd * n
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!
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! such a function is based on the exact behaviour of the Ecmd at large mu
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!
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! but with the exact on-top estimated with that of the UEG
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!
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! You enter with the alpha/beta density and density gradients
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!
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! You get out with eps_c_md_PBE(1:N_states)
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END_DOC
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double precision, intent(in) :: mu(N_states) , rho_a(N_states),rho_b(N_states), grad_rho_a(3,N_states),grad_rho_b(3,N_states)
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double precision, intent(out) :: eps_c_md_PBE(N_states)
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double precision :: pi, e_PBE, beta
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double precision :: aos_array(ao_num), grad_aos_array(3,ao_num)
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double precision :: grad_rho_a_2(N_states),grad_rho_b_2(N_states),grad_rho_a_b(N_states)
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double precision :: rhoc,rhoo,sigmacc,sigmaco,sigmaoo,vrhoc,vrhoo,vsigmacc,vsigmaco,vsigmaoo
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double precision :: g0_UEG_mu_inf, denom
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integer :: m, istate
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pi = 4.d0 * datan(1.d0)
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eps_c_md_PBE = 0.d0
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grad_rho_a_2 = 0.d0
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grad_rho_b_2 = 0.d0
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grad_rho_a_b = 0.d0
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do istate = 1, N_states
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do m = 1, 3
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grad_rho_a_2(istate) += grad_rho_a(m,istate)*grad_rho_a(m,istate)
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grad_rho_b_2(istate) += grad_rho_b(m,istate)*grad_rho_b(m,istate)
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grad_rho_a_b(istate) += grad_rho_a(m,istate)*grad_rho_b(m,istate)
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enddo
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enddo
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do istate = 1, N_states
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! convertion from (alpha,beta) formalism to (closed, open) formalism
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call rho_ab_to_rho_oc(rho_a(istate),rho_b(istate),rhoo,rhoc)
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call grad_rho_ab_to_grad_rho_oc(grad_rho_a_2(istate),grad_rho_b_2(istate),grad_rho_a_b(istate),sigmaoo,sigmacc,sigmaco)
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call ec_pbe_only(0.d0,rhoc,rhoo,sigmacc,sigmaco,sigmaoo,e_PBE)
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if(mu(istate) == 0.d0) then
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eps_c_md_PBE(istate)=e_PBE
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else
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! note: the on-top pair density is (1-zeta^2) rhoc^2 g0 = 4 rhoa * rhob * g0
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denom = (-2.d0+sqrt(2d0))*sqrt(2.d0*pi) * 4.d0*rho_a(istate)*rho_b(istate)*g0_UEG_mu_inf(rho_a(istate),rho_b(istate))
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if (dabs(denom) > 1.d-12) then
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beta = (3.d0*e_PBE)/denom
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eps_c_md_PBE(istate)=e_PBE/(1.d0+beta*mu(istate)**3)
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else
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eps_c_md_PBE(istate)=0.d0
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endif
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endif
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enddo
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end
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subroutine eps_c_md_PBE_at_grid_pt(mu,i_point,eps_c_md_PBE)
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implicit none
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BEGIN_DOC
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! provides the integrand of Eq. (13) of Phys.Chem.Lett.2019, 10, 2931 2937
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|
|
!
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! !!! WARNING !!! This is the total integrand of Eq. (13), which is e_cmd * n
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|
|
!
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! such a function is based on the exact behaviour of the Ecmd at large mu
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|
|
!
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! but with the exact on-top estimated with that of the UEG
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!
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! You enter with the alpha/beta density and density gradients
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!
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! You get out with eps_c_md_PBE(1:N_states)
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END_DOC
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double precision, intent(in) :: mu
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double precision, intent(out) :: eps_c_md_PBE(N_states)
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integer, intent(in) :: i_point
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double precision :: two_dm, pi, e_pbe,beta,mu_correction_of_on_top
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double precision :: grad_rho_a(3),grad_rho_b(3)
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double precision :: grad_rho_a_2,grad_rho_b_2,grad_rho_a_b
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double precision :: rhoc,rhoo,ec_pbe_88
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double precision :: delta,two_dm_corr,rho_a,rho_b
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double precision :: grad_rho_2,denom,g0_UEG_mu_inf
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double precision :: sigmacc,sigmaco,sigmaoo
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integer :: m, istate
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pi = 4.d0 * datan(1.d0)
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eps_c_md_PBE = 0.d0
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do istate = 1, N_states
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! total and spin density
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rhoc = one_e_dm_and_grad_alpha_in_r(4,i_point,istate) + one_e_dm_and_grad_beta_in_r(4,i_point,istate)
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rhoo = one_e_dm_and_grad_alpha_in_r(4,i_point,istate) - one_e_dm_and_grad_beta_in_r(4,i_point,istate)
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! gradients of the effective spin density
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grad_rho_a_2 = 0.D0
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grad_rho_b_2 = 0.D0
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grad_rho_a_b = 0.D0
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do m = 1, 3
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grad_rho_a_2 += one_e_dm_and_grad_alpha_in_r(m,i_point,istate)**2.d0
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grad_rho_b_2 += one_e_dm_and_grad_beta_in_r(m,i_point,istate) **2.d0
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grad_rho_a_b += one_e_dm_and_grad_alpha_in_r(m,i_point,istate) * one_e_dm_and_grad_beta_in_r(m,i_point,istate)
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enddo
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sigmacc = grad_rho_a_2 + grad_rho_b_2 + 2.d0 * grad_rho_a_b
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sigmaco = 0.d0
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sigmaoo = 0.d0
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rho_a = one_e_dm_and_grad_alpha_in_r(4,i_point,istate)
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rho_b = one_e_dm_and_grad_beta_in_r(4,i_point,istate)
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call ec_pbe_only(0.d0,rhoc,rhoo,sigmacc,sigmaco,sigmaoo,e_PBE)
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if(e_PBE.gt.0.d0)then
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print*,'PBE gt 0 with regular dens'
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endif
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if(mu == 0.d0) then
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eps_c_md_PBE(istate)=e_PBE
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else
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! note: the on-top pair density is (1-zeta^2) rhoc^2 g0 = 4 rhoa * rhob * g0
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denom = (-2.d0+dsqrt(2d0))*sqrt(2.d0*pi) * 4.d0*rho_a*rho_b*g0_UEG_mu_inf(rho_a,rho_b)
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if (dabs(denom) > 1.d-12) then
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beta = (3.d0*e_PBE)/denom
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! Ecmd functional with the UEG ontop pair density when mu -> infty
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! and the usual PBE correlation energy when mu = 0
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eps_c_md_PBE(istate)=e_PBE/(1.d0+beta*mu**3)
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else
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eps_c_md_PBE(istate)=0.d0
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endif
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endif
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enddo
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end
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