NAG Library Function Document
nag_real_sparse_eigensystem_monit (f12aec)
Note: this function uses optional parameters to define choices in the problem specification. If you wish to use default
settings for all of the optional parameters, then the option setting function nag_real_sparse_eigensystem_option (f12adc) need not be called.
If, however, you wish to reset some or all of the settings please refer to Section 11 in nag_real_sparse_eigensystem_option (f12adc) for a detailed description of the specification of the optional parameters.
1
Purpose
nag_real_sparse_eigensystem_monit (f12aec) can be used to return additional monitoring information during computation. It is in a suite of functions consisting of
nag_real_sparse_eigensystem_init (f12aac),
nag_real_sparse_eigensystem_iter (f12abc),
nag_real_sparse_eigensystem_sol (f12acc),
nag_real_sparse_eigensystem_option (f12adc) and
nag_real_sparse_eigensystem_monit (f12aec).
2
Specification
#include <nag.h> |
#include <nagf12.h> |
|
3
Description
The suite of functions is designed to calculate some of the eigenvalues, , (and optionally the corresponding eigenvectors, ) of a standard eigenvalue problem , or of a generalized eigenvalue problem of order , where is large and the coefficient matrices and are sparse, real and nonsymmetric. The suite can also be used to find selected eigenvalues/eigenvectors of smaller scale dense, real and nonsymmetric problems.
On an intermediate exit from
nag_real_sparse_eigensystem_iter (f12abc) with
,
nag_real_sparse_eigensystem_monit (f12aec) may be called to return monitoring information on the progress of the Arnoldi iterative process. The information returned by
nag_real_sparse_eigensystem_monit (f12aec) is:
– |
the number of the current Arnoldi iteration; |
– |
the number of converged eigenvalues at this point; |
– |
the real and imaginary parts of the converged eigenvalues; |
– |
the error bounds on the converged eigenvalues. |
nag_real_sparse_eigensystem_monit (f12aec) does not have an equivalent function from the ARPACK package which prints various levels of detail of monitoring information through an output channel controlled via an argument value (see
Lehoucq et al. (1998) for details of ARPACK routines).
nag_real_sparse_eigensystem_monit (f12aec) should not be called at any time other than immediately following an
return from
nag_real_sparse_eigensystem_iter (f12abc).
4
References
Lehoucq R B (2001) Implicitly restarted Arnoldi methods and subspace iteration SIAM Journal on Matrix Analysis and Applications 23 551–562
Lehoucq R B and Scott J A (1996) An evaluation of software for computing eigenvalues of sparse nonsymmetric matrices Preprint MCS-P547-1195 Argonne National Laboratory
Lehoucq R B and Sorensen D C (1996) Deflation techniques for an implicitly restarted Arnoldi iteration SIAM Journal on Matrix Analysis and Applications 17 789–821
Lehoucq R B, Sorensen D C and Yang C (1998) ARPACK Users' Guide: Solution of Large-scale Eigenvalue Problems with Implicitly Restarted Arnoldi Methods SIAM, Philidelphia
5
Arguments
- 1:
– Integer *Output
-
On exit: the number of the current Arnoldi iteration.
- 2:
– Integer *Output
-
On exit: the number of converged eigenvalues so far.
- 3:
– doubleOutput
-
Note: the dimension,
dim, of the array
ritzr
must be at least
(see
nag_real_sparse_eigensystem_init (f12aac)).
On exit: the first
nconv locations of the array
ritzr contain the real parts of the converged approximate eigenvalues.
- 4:
– doubleOutput
-
Note: the dimension,
dim, of the array
ritzi
must be at least
(see
nag_real_sparse_eigensystem_init (f12aac)).
On exit: the first
nconv locations of the array
ritzi contain the imaginary parts of the converged approximate eigenvalues.
- 5:
– doubleOutput
-
Note: the dimension,
dim, of the array
rzest
must be at least
(see
nag_real_sparse_eigensystem_init (f12aac)).
On exit: the first
nconv locations of the array
rzest contain the Ritz estimates (error bounds) on the converged approximate eigenvalues.
- 6:
– const IntegerCommunication Array
-
Note: the dimension,
dim, of the array
icomm
must be at least
, where
licomm
is passed to the setup function
(see
nag_real_sparse_eigensystem_init (f12aac)).
On entry: the array
icomm output by the preceding call to
nag_real_sparse_eigensystem_iter (f12abc).
- 7:
– const doubleCommunication Array
-
Note: the dimension,
dim, of the array
comm
must be at least
, where
lcomm
is passed to the setup function
(see
nag_real_sparse_eigensystem_init (f12aac)).
On entry: the array
comm output by the preceding call to
nag_real_sparse_eigensystem_iter (f12abc).
6
Error Indicators and Warnings
None.
7
Accuracy
A Ritz value,
, is deemed to have converged if its Ritz estimate
. The default
used is the
machine precision given by
nag_machine_precision (X02AJC).
8
Parallelism and Performance
nag_real_sparse_eigensystem_monit (f12aec) is not threaded in any implementation.
None.
10
Example
This example solves in shifted-real mode, where is the tridiagonal matrix with on the diagonal, on the subdiagonal and on the superdiagonal. The matrix is the tridiagonal matrix with on the diagonal and on the off-diagonals. The shift sigma, , is a complex number, and the operator used in the shifted-real iterative process is .
10.1
Program Text
Program Text (f12aece.c)
10.2
Program Data
Program Data (f12aece.d)
10.3
Program Results
Program Results (f12aece.r)