2015-11-19 17:16:24 +01:00
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subroutine pt2_h_core(det_pert,c_pert,e_2_pert,H_pert_diag,Nint,ndet,N_st,minilist,idx_minilist,N_minilist)
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2015-03-19 21:14:52 +01:00
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use bitmasks
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implicit none
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integer, intent(in) :: Nint,ndet,N_st
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integer(bit_kind), intent(in) :: det_pert(Nint,2)
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double precision , intent(out) :: c_pert(N_st),e_2_pert(N_st),H_pert_diag(N_st)
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double precision :: i_H_psi_array(N_st)
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2015-11-19 17:16:24 +01:00
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integer, intent(in) :: N_minilist
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integer, intent(in) :: idx_minilist(0:N_det_selectors)
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integer(bit_kind), intent(in) :: minilist(Nint,2,N_det_selectors)
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2015-03-19 21:14:52 +01:00
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BEGIN_DOC
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! compute the standard Epstein-Nesbet perturbative first order coefficient and second order energetic contribution
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!
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! for the various N_st states.
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!
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! c_pert(i) = <psi(i)|H|det_pert>/( E(i) - <det_pert|H|det_pert> )
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!
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! e_2_pert(i) = <psi(i)|H|det_pert>^2/( E(i) - <det_pert|H|det_pert> )
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!
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END_DOC
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integer :: i,j
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double precision :: diag_H_mat_elem, h
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ASSERT (Nint == N_int)
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ASSERT (Nint > 0)
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integer :: exc(0:2,2,2)
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integer :: degree
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double precision :: phase
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call get_excitation(ref_bitmask,det_pert,exc,degree,phase,N_int)
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h = diag_H_mat_elem(det_pert,N_int)
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print*,'delta E = ',h-ref_bitmask_energy
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if(h<ref_bitmask_energy)then
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c_pert = 0.d0
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e_2_pert = 0.d0
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H_pert_diag = 0.d0
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return
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endif
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if(degree>1)then
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c_pert = 0.d0
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e_2_pert = 0.d0
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H_pert_diag = 0.d0
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return
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endif
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integer :: h1,p1,h2,p2,s1,s2
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call decode_exc(exc,degree,h1,p1,h2,p2,s1,s2)
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c_pert = phase * mo_mono_elec_integral(h1,p1)
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e_2_pert = -dabs(mo_mono_elec_integral(h1,p1)+1.d0)
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end
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