An active line of research into functionals that go beyond the GGA
at the moment is the meta-GGA (MGGA) form [65,66].
MGGAs include additional semi-local information beyond the first-order
density gradient contained in the GGA, such as higher order density
gradients, or more popular is the inclusion of the kinetic energy
density
which involves derivatives of the occupied
Kohn-Sham orbitals,
![]() |
(2.46) |
![]() |
(2.47) |
There are several MGGA forms now in existence
[67,68,69,70,71,72,73,74,75,76] and
some improvement has been obtained over the GGA in a limited number of
tests [77]. However a few cautionary words should be said
about the MGGA. At present, MGGA calculations for solids are performed
inconsistently because they resort to using GGA orbitals and densities
to evaluate
,
since the orbital dependence does not permit an easy evaluation of a
multiplicative exchange-correlation potential
. Therefore properties are only calculated at experimental
structures. To achieve self-consistency using a multiplicative potential,
computationally expensive methods such as the optimised effective
potential (OEP) [78,79] must be invoked, however this
has yet to be implemented - indeed it may eventually prove too costly
for practical computations. Another point to highlight is that all MGGA
forms are constructed using experimental molecular data to define the
form. This will have the effect of introducing an element of bias into
the character of the functional. This issue is investigated in
Chapter
with regard to GGA functionals.