function get_one_body_diag_kvec(nI, spin, k_shift, t_sign) result(hel)
integer, intent(in) :: nI(nel)
integer, intent(in) :: spin, k_shift(3)
logical, intent(in), optional :: t_sign
HElement_t(dp) :: hel
integer :: i, sgn
#ifdef DEBUG_
character(*), parameter :: this_routine = "get_one_body_diag_kvec"
#endif
! change this routine to also use just the symmetry symbols
integer :: sym_shift
type(symmetry) :: sym
logical :: t_sign_
def_default(t_sign_, t_sign, .false.)
! the spin input: -1 is beta, +1 is alpha, 0 is both!
! if spin is not present, default is both!
hel = h_cast(0.0_dp)
! k_shift is actually always present..
! work on the newest, hopefully correct way to do this..
! i need -s k vector for the triples contribution to the doubles..
if (t_sign_) then
sgn = -1
else
sgn = 1
end if
sym_shift = lat%k_to_sym(k_shift(1), k_shift(2), k_shift(3))
if (sgn == 1) then
ASSERT(spin == -1 .or. spin == 1)
if (spin == -1) then
do i = 1, nel
if (is_beta(nI(i))) then
sym = SymTable(G1(nI(i))%sym%s, sym_shift)
hel = hel + epsilon_kvec(sym)
end if
end do
else if (spin == 1) then
do i = 1, nel
if (is_alpha(nI(i))) then
sym = SymTable(G1(nI(i))%sym%s, sym_shift)
hel = hel + epsilon_kvec(sym)
end if
end do
end if
else if (sgn == -1) then
ASSERT(spin == -1 .or. spin == 1)
if (spin == -1) then
do i = 1, nel
if (is_beta(nI(i))) then
sym = SymTable(sym_shift, SymConjTab(G1(nI(i))%sym%s))
hel = hel + epsilon_kvec(sym)
end if
end do
else if (spin == 1) then
do i = 1, nel
if (is_alpha(nI(i))) then
sym = SymTable(sym_shift, SymConjTab(G1(nI(i))%sym%s))
hel = hel + epsilon_kvec(sym)
end if
end do
end if
end if
end function get_one_body_diag_kvec