F11JBF solves a system of linear equations involving the incomplete Cholesky preconditioning matrix generated by
F11JAF.
F11JBF solves a system of linear equations
involving the preconditioning matrix
, corresponding to an incomplete Cholesky decomposition of a sparse symmetric matrix stored in symmetric coordinate storage (SCS) format (see
Section 2.1.2 in the F11 Chapter Introduction), as generated by
F11JAF.
In the above decomposition
is a lower triangular sparse matrix with unit diagonal,
is a diagonal matrix and
is a permutation matrix.
and
are supplied to F11JBF through the matrix
which is a lower triangular
N by
N sparse matrix, stored in SCS format, as returned by
F11JAF. The permutation matrix
is returned from
F11JAF via the array
IPIV.
It is envisaged that a common use of F11JBF will be to carry out the preconditioning step required in the application of
F11GEF to sparse symmetric linear systems. F11JBF is used for this purpose by the Black Box routine
F11JCF.
F11JBF may also be used in combination with
F11JAF to solve a sparse symmetric positive definite system of linear equations directly (see
Section 9.4 in F11JAF). This use of F11JBF is demonstrated in
Section 10.
None.
If on entry
or
, explanatory error messages are output on the current error message unit (as defined by
X04AAF).
The computed solution
is the exact solution of a perturbed system of equations
, where
is a modest linear function of
, and
is the
machine precision.
Not applicable.
The time taken for a call to F11JBF is proportional to the value of
NNZC returned from
F11JAF.
It is expected that a common use of F11JBF will be to carry out the preconditioning step required in the application of
F11GEF to sparse symmetric linear systems. In this situation F11JBF is likely to be called many times with the same matrix
. In the interests of both reliability and efficiency, you are recommended to set
for the first of such calls, and to set
for all subsequent calls.
This example reads in a symmetric positive definite sparse matrix
and a vector
. It then calls
F11JAF, with
and
, to compute the
complete Cholesky decomposition of
:
Then it calls F11JBF to solve the system
It then repeats the exercise for the same matrix permuted with the bandwidth-reducing Reverse Cuthill–McKee permutation, calculated with
F11YEF.