f12ab: FL CL CPP AD PY MB

NAG CL Interface
f12abc (real_iter)

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 f12adc need not be called. If, however, you wish to reset some or all of the settings please refer to Section 11 in f12adc for a detailed description of the specification of the optional parameters.

Keyword Search:

NAG Library Manual, Mark 30.1

Interfaces: FL CL CPP AD PY MB

NAG CL Interface Introduction

F12 (Sparseig) Chapter Contents

F12 (Sparseig) Chapter Introduction

f12ab: FL CL CPP AD PY MB

▸▿ Contents

1 Purpose

2 Specification

3 Description

4 References

5 Arguments

6 Error Indicators and Warnings

7 Accuracy

8 Parallelism and Performance

9 Further Comments

▸▿ 10 Example

10.1 Program Text

10.2 Program Data

10.3 Program Results

Settings help

CL Name Style:
Short (a00aac)
Long (impl_details)
Full (nag_info_impl_details)

1 Purpose

f12abc is an iterative solver in a suite of functions consisting of f12aac, f12abc, f12acc, f12adc and f12aec. It is used to find some of the eigenvalues (and optionally the corresponding eigenvectors) of a standard or generalized eigenvalue problem defined by real nonsymmetric matrices.

2 Specification

#include <nag.h>

void	f12abc (Integer irevcm, double resid[], double v[], double x, double y, double mx, Integer nshift, double comm[], Integer icomm[], NagError *fail)

The function may be called by the names: f12abc, nag_sparseig_real_iter or nag_real_sparse_eigensystem_iter.

3 Description

The suite of functions is designed to calculate some of the eigenvalues,

λ

, (and optionally the corresponding eigenvectors,

x

) of a standard eigenvalue problem

A x = λ x

, or of a generalized eigenvalue problem

A x = λ B x

of order

n

, where

n

is large and the coefficient matrices

A

and

B

are sparse, real and nonsymmetric. The suite can also be used to find selected eigenvalues/eigenvectors of smaller scale dense, real and nonsymmetric problems.

f12abc is a reverse communication function, based on the ARPACK routine dnaupd, using the Implicitly Restarted Arnoldi iteration method. The method is described in Lehoucq and Sorensen (1996) and Lehoucq (2001) while its use within the ARPACK software is described in great detail in Lehoucq et al. (1998). An evaluation of software for computing eigenvalues of sparse nonsymmetric matrices is provided in Lehoucq and Scott (1996). This suite of functions offers the same functionality as the ARPACK software for real nonsymmetric problems, but the interface design is quite different in order to make the option setting clearer and to simplify the interface of f12abc.

The setup function f12aac must be called before f12abc, the reverse communication iterative solver. Options may be set for f12abc by prior calls to the option setting function f12adc and a post-processing function f12acc must be called following a successful final exit from f12abc. f12aec, may be called following certain flagged, intermediate exits from f12abc to provide additional monitoring information about the computation.

f12abc uses reverse communication, i.e., it returns repeatedly to the calling program with the argument irevcm (see Section 5) set to specified values which require the calling program to carry out one of the following tasks:

–compute the matrix-vector product $y = op (x)$ , where $op$ is defined by the computational mode;
–compute the matrix-vector product $y = B x$ ;
–notify the completion of the computation;
–allow the calling program to monitor the solution.

The problem type to be solved (standard or generalized), the spectrum of eigenvalues of interest, the mode used (regular, regular inverse, shifted inverse, shifted real or shifted imaginary) and other options can all be set using the option setting function f12adc (see Section 11.1 in f12adc for details on setting options and of the default settings).

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, Philadelphia

5 Arguments

Note: this function uses reverse communication. Its use involves an initial entry, intermediate exits and re-entries, and a final exit, as indicated by the argument irevcm. Between intermediate exits and re-entries, all arguments other than x and y must remain unchanged.

1: $irevcm$ – Integer * Input/Output

On initial entry:

irevcm = 0

, otherwise an error condition will be raised.

On intermediate re-entry: must be unchanged from its previous exit value. Changing irevcm to any other value between calls will result in an error.

On intermediate exit: has the following meanings.

$irevcm = −1$: The calling program must compute the matrix-vector product $y = op (x)$ , where $x$ is stored in x and the result $y$ is placed in y. If $B$ is not symmetric semidefinite then the precomputed values in mx should not be used (see the explanation under $irevcm = 2$ ).
$irevcm = 1$: The calling program must compute the matrix-vector product $y = op (x)$ . This is similar to the case $irevcm = −1$ except that the result of the matrix-vector product $B x$ (as required in some computational modes) has already been computed and is available in mx.
$irevcm = 2$: The calling program must compute the matrix-vector product $y = B x$ , where $x$ is stored as described in the case $irevcm = −1$ and $y$ is placed in y. This computation is requested when solving the $Generalized$ problem using either $Shifted Inverse Imaginary$ or $Shifted Inverse Real$ ; in these cases $B$ is used as an inner-product space and requires that $B$ be symmetric semidefinite. If neither $A$ nor $B$ is symmetric semidefinite then the problem should be reformulated in a $Standard$ form.
$irevcm = 3$: Compute the nshift real and imaginary parts of the shifts where the real parts are to be placed in the first nshift locations of the array y and the imaginary parts are to be placed in the first nshift locations of the array mx. Only complex conjugate pairs of shifts may be applied and the pairs must be placed in consecutive locations. This value of irevcm will only arise if the optional parameter $Supplied Shifts$ is set in a prior call to f12adc which is intended for experienced users only; the default and recommended option is to use exact shifts (see Lehoucq et al. (1998) for details).
$irevcm = 4$: Monitoring step: a call to f12aec can now be made to return the number of Arnoldi iterations, the number of converged Ritz values, their real and imaginary parts, and the corresponding Ritz estimates.

On final exit:

irevcm = 5

: f12abc has completed its tasks. The value of fail determines whether the iteration has been successfully completed, or whether errors have been detected. On successful completion f12acc must be called to return the requested eigenvalues and eigenvectors (and/or Schur vectors).

Constraint: on initial entry,

irevcm = 0

; on re-entry irevcm must remain unchanged.

Note: any values you return to f12abc as part of the reverse communication procedure should not include floating-point NaN (Not a Number) or infinity values, since these are not handled by f12abc. If your code inadvertently does return any NaNs or infinities, f12abc is likely to produce unexpected results.

2: $resid [\dim]$ – double Input/Output

Note: the dimension, dim, of the array resid must be at least

n

(see f12aac).

On initial entry: need not be set unless the option

Initial Residual

has been set in a prior call to f12adc in which case resid should contain an initial residual vector, possibly from a previous run.

On intermediate re-entry: must be unchanged from its previous exit. Changing resid to any other value between calls may result in an error exit.

On intermediate exit: contains the current residual vector.

On final exit: contains the final residual vector.

3: $v [n \times ncv]$ – double Input/Output

The

i

th element of the

j

th basis vector is stored in location

v [n \times (i - 1) + j - 1]

, for

i = 1, 2, \dots, n

and

j = 1, 2, \dots, ncv

On initial entry: need not be set.

On intermediate re-entry: must be unchanged from its previous exit.

On intermediate exit: contains the current set of Arnoldi basis vectors.

On final exit: contains the final set of Arnoldi basis vectors.

4: $x$ – double ** Input/Output

On initial entry: need not be set, it is used as a convenient mechanism for accessing elements of comm.

On intermediate re-entry: is not normally changed.

On intermediate exit: contains the vector

x

when irevcm returns the value

- 1

+ 1

2

On final exit: does not contain useful data.

5: $y$ – double ** Input/Output

On initial entry: need not be set, it is used as a convenient mechanism for accessing elements of comm.

On intermediate re-entry: must contain the result of

y = op (x)

when irevcm returns the value

- 1

+ 1

. It must contain the real parts of the computed shifts when irevcm returns the value

3

On intermediate exit: does not contain useful data.

On final exit: does not contain useful data.

6: $mx$ – double ** Input/Output

On initial entry: need not be set, it is used as a convenient mechanism for accessing elements of comm.

On intermediate re-entry: must contain the result of

y = B x

when irevcm returns the value

2

. It must contain the imaginary parts of the computed shifts when irevcm returns the value

3

On intermediate exit: contains the vector

B x

when irevcm returns the value

+ 1

On final exit: does not contain any useful data.

7: $nshift$ – Integer * Output

On intermediate exit: if the option

Supplied Shifts

is set and irevcm returns a value of

3

, nshift returns the number of complex shifts required.

8: $comm [\dim]$ – double Communication Array

Note: the actual argument supplied must be the array comm supplied to the initialization routine f12aac.

On initial entry: must remain unchanged following a call to the setup function f12aac.

On exit: contains data defining the current state of the iterative process.

9: $icomm [\dim]$ – Integer Communication Array

Note: the actual argument supplied must be the array icomm supplied to the initialization routine f12aac.

On initial entry: must remain unchanged following a call to the setup function f12aac.

On exit: contains data defining the current state of the iterative process.

10: $fail$ – NagError * Input/Output

The NAG error argument (see Section 7 in the Introduction to the NAG Library CL Interface).

6 Error Indicators and Warnings

NE_ALLOC_FAIL: Dynamic memory allocation failed.
See Section 3.1.2 in the Introduction to the NAG Library CL Interface for further information.
NE_BAD_PARAM: On entry, argument $⟨ value ⟩$ had an illegal value.
NE_INITIALIZATION: Either the initialization function has not been called prior to the first call of this function or a communication array has become corrupted.
NE_INT: The maximum number of iterations $\leq 0$ , the option $Iteration Limit$ has been set to $⟨ value ⟩$ .
NE_INTERNAL_EIGVAL_FAIL: Error in internal call to compute eigenvalues and corresponding error bounds of the current upper Hessenberg matrix. Please contact NAG.
NE_INTERNAL_ERROR: An internal error has occurred in this function. Check the function call and any array sizes. If the call is correct then please contact NAG for assistance.
See Section 7.5 in the Introduction to the NAG Library CL Interface for further information.
NE_MAX_ITER: The maximum number of iterations has been reached. The maximum number of $iterations = ⟨ value ⟩$ . The number of converged eigenvalues $= ⟨ value ⟩$ . The post-processing function f12acc may be called to recover the converged eigenvalues at this point. Alternatively, the maximum number of iterations may be increased by a call to the option setting function f12adc and the reverse communication loop restarted. A large number of iterations may indicate a poor choice for the values of nev and ncv; it is advisable to experiment with these values to reduce the number of iterations (see f12aac).
NE_NO_ARNOLDI_FAC: Could not build an Arnoldi factorization. The size of the current Arnoldi factorization $= ⟨ value ⟩$ .
NE_NO_LICENCE: Your licence key may have expired or may not have been installed correctly.
See Section 8 in the Introduction to the NAG Library CL Interface for further information.
NE_NO_SHIFTS_APPLIED: No shifts could be applied during a cycle of the implicitly restarted Arnoldi iteration.
NE_OPT_INCOMPAT: The options $Generalized$ and $Regular$ are incompatible.
NE_ZERO_INIT_RESID: The option $Initial Residual$ was selected but the starting vector held in resid is zero.

7 Accuracy

The relative accuracy of a Ritz value,

λ

, is considered acceptable if its Ritz estimate

\leq Tolerance \times | λ |

. The default

Tolerance

used is the machine precision given by X02AJC.

8 Parallelism and Performance

Background information to multithreading can be found in the Multithreading documentation.

f12abc is threaded by NAG for parallel execution in multithreaded implementations of the NAG Library.

f12abc makes calls to BLAS and/or LAPACK routines, which may be threaded within the vendor library used by this implementation. Consult the documentation for the vendor library for further information.

Please consult the X06 Chapter Introduction for information on how to control and interrogate the OpenMP environment used within this function. Please also consult the Users' Note for your implementation for any additional implementation-specific information.

9 Further Comments

None.

10 Example

This example solves

A x = λ x

in shift-invert mode, where

A

is obtained from the standard central difference discretization of the convection-diffusion operator

\frac{\partial^{2} u}{\partial x^{2}} + \frac{\partial^{2} u}{\partial y^{2}} + ρ \frac{\partial u}{\partial x}

on the unit square, with zero Dirichlet boundary conditions. The shift used is a real number.

f12ab: FL CL CPP AD PY MB

NAG CL Interfacef12abc (real_​iter)

▸▿ Contents

1 Purpose

2 Specification

3 Description

4 References

5 Arguments

6 Error Indicators and Warnings

7 Accuracy

8 Parallelism and Performance

9 Further Comments

10 Example

10.1 Program Text

10.2 Program Data

10.3 Program Results

NAG CL Interface
f12abc (real_iter)