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In the case when the density-kernel
is expanded in terms of an
auxiliary matrix
e.g. in order to construct a positive semi-definite
density-matrix, it is necessary to be able to calculate the auxiliary
matrix
which corresponds to a given density-kernel
by
 |
(8.14) |
This can be achieved by minimising the function
given by
![\begin{displaymath}
{\cal I}(T) = {\rm Tr} \left[ (K - T T^{\dag })^2 \right]
\end{displaymath}](img1148.gif) |
(8.15) |
whose derivative with respect to
is
![\begin{displaymath}
\frac{\partial {\cal I}(T)}{\partial T^{\alpha \beta}} =
-4 \left[ T^{\dag } (K - T T^{\dag }) \right]_{\beta \alpha} .
\end{displaymath}](img1149.gif) |
(8.16) |
This derivative vanishes at the minimum, and so we find that the matrix
which minimises
is the desired auxiliary matrix (the
solution
corresponds to a local maximum). We therefore choose to
minimise
by the conjugate gradients method to obtain the
auxiliary matrix.
Next: Optimising the support functions
Up: Density-matrices from Kohn-Sham orbitals
Previous: Projecting plane-wave eigenstates onto
  Contents
Peter D. Haynes
1999-09-21