F12AUF (PDF version)
F12 Chapter Contents
F12 Chapter Introduction
NAG Library Manual

NAG Library Routine Document

F12AUF

Note:  before using this routine, please read the Users' Note for your implementation to check the interpretation of bold italicised terms and other implementation-dependent details.
Note: this routine 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 routine F12ARF need not be called. If, however, you wish to reset some or all of the settings please refer to Section 11 in F12ARF for a detailed description of the specification of the optional parameters.

 Contents

    1  Purpose
    7  Accuracy

1  Purpose

F12AUF is the main solver routine in a suite of routines consisting of F12ARF, F12ATF and F12AUF. It must be called following an initial call to F12ATF and following any calls to F12ARF.
F12AUF returns approximations to selected eigenvalues, and (optionally) the corresponding eigenvectors, of a standard or generalized eigenvalue problem defined by complex banded non-Hermitian matrices. The banded matrix must be stored using the LAPACK storage format for complex banded non-Hermitian matrices.

2  Specification

SUBROUTINE F12AUF ( KL, KU, AB, LDAB, MB, LDMB, SIGMA, NCONV, D, Z, LDZ, RESID, V, LDV, COMM, ICOMM, IFAIL)
INTEGER  KL, KU, LDAB, LDMB, NCONV, LDZ, LDV, ICOMM(140), IFAIL
COMPLEX (KIND=nag_wp)  AB(LDAB,*), MB(LDMB,*), SIGMA, D(NEV), Z(LDZ,*), RESID(N), V(LDV,*), COMM(60)

3  Description

The suite of routines is designed to calculate some of the eigenvalues, λ , (and optionally the corresponding eigenvectors, x ) of a standard eigenvalue problem Ax = λx , or of a generalized eigenvalue problem Ax = λBx  of order n , where n  is large and the coefficient matrices A  and B  are banded, complex and non-Hermitian.
Following a call to the initialization routine F12ATF, F12AUF returns the converged approximations to eigenvalues and (optionally) the corresponding approximate eigenvectors and/or a unitary basis for the associated approximate invariant subspace. The eigenvalues (and eigenvectors) are selected from those of a standard or generalized eigenvalue problem defined by complex banded non-Hermitian matrices. There is negligible additional computational cost to obtain eigenvectors; a unitary basis is always computed, but there is an additional storage cost if both are requested.
The banded matrices A  and B must be stored using the LAPACK column ordered storage format for banded non-Hermitian matrices; please refer to Section 3.3.4 in the F07 Chapter Introduction for details on this storage format.
F12AUF is based on the banded driver routines znbdr1 to znbdr4 from the ARPACK package, which uses 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 non-Hermitian matrices is provided in Lehoucq and Scott (1996). This suite of routines offers the same functionality as the ARPACK banded driver software for complex non-Hermitian problems, but the interface design is quite different in order to make the option setting clearer and to combine the different drivers into a general purpose routine.
F12AUF, is a general purpose routine that must be called following initialization by F12ATF. F12AUF uses options, set either by default or explicitly by calling F12ARF, to return the converged approximations to selected eigenvalues and (optionally):
the corresponding approximate eigenvectors;
a unitary basis for the associated approximate invariant subspace;
both.

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  Parameters

Note: in the following description N, NEV and NCV appears. In every case they should be interpretted as the value associated with the identically named parameter in a prior call to F12ATF.
1:     KL – INTEGERInput
On entry: the number of subdiagonals of the matrices A  and B.
Constraint: KL0.
2:     KU – INTEGERInput
On entry: the number of superdiagonals of the matrices A  and B.
Constraint: KU0.
3:     ABLDAB* – COMPLEX (KIND=nag_wp) arrayInput
Note: the second dimension of the array AB must be at least max1,N (see F12ATF).
On entry: must contain the matrix A in LAPACK banded storage format for non-Hermitian matrices (see Section 3.3.4 in the F07 Chapter Introduction).
4:     LDAB – INTEGERInput
On entry: the first dimension of the array AB as declared in the (sub)program from which F12AUF is called.
Constraint: LDAB 2×KL+KU+1.
5:     MBLDMB* – COMPLEX (KIND=nag_wp) arrayInput
Note: the second dimension of the array MB must be at least max1,N (see F12ATF).
On entry: must contain the matrix B in LAPACK banded storage format for non-Hermitian matrices (see Section 3.3.4 in the F07 Chapter Introduction).
6:     LDMB – INTEGERInput
On entry: the first dimension of the array MB as declared in the (sub)program from which F12AUF is called.
Constraint: LDMB2×KL+KU+1.
7:     SIGMA – COMPLEX (KIND=nag_wp)Input
On entry: if the Shifted Inverse mode (see F12ARF) has been selected then SIGMA must contain the shift used; otherwise SIGMA is not referenced. Section 4.2 in the F12 Chapter Introduction describes the use of shift and invert transformations.
8:     NCONV – INTEGEROutput
On exit: the number of converged eigenvalues.
9:     DNEV – COMPLEX (KIND=nag_wp) arrayOutput
On exit: the first NCONV locations of the array D contain the converged approximate eigenvalues.
10:   ZLDZ* – COMPLEX (KIND=nag_wp) arrayOutput
Note: the second dimension of the array Z must be at least NEV if the default option Vectors=Ritz has been selected and at least 1 if the option Vectors=None or Schur has been selected (see F12ARF and F12ATF).
On exit: if the default option Vectors=RITZ (see F12ARF) has been selected then Z contains the final set of eigenvectors corresponding to the eigenvalues held in D, otherwise Z is not referenced. The complex eigenvector associated with an eigenvalue Dj is stored in the corresponding array section of Z, namely Zij, for i=1,2,,N and j=1,2,,NCONV.
11:   LDZ – INTEGERInput
On entry: the first dimension of the array Z as declared in the (sub)program from which F12AUF is called.
Constraints:
  • if the default option Vectors=Ritz has been selected, LDZN;
  • if the option Vectors=None or Schur has been selected, LDZ1.
12:   RESIDN – COMPLEX (KIND=nag_wp) arrayInput/Output
On entry: need not be set unless the option Initial Residual has been set in a prior call to F12ARF in which case RESID must contain an initial residual vector.
On exit: contains the final residual vector. This can be used as the starting residual to improve convergence on the solution of a closely related eigenproblem. This has no relation to the error residual Ax-λx or Ax-λBx.
13:   VLDV* – COMPLEX (KIND=nag_wp) arrayOutput
Note: the second dimension of the array V must be at least max1,NCV (see F12ATF).
On exit: if the option Vectors=SCHUR or RITZ (see F12ARF) has been set and a separate array Z has been passed (i.e., Z does not equal V), then the first NCONV columns of V will contain approximate Schur vectors that span the desired invariant subspace.
The jth Schur vector is stored in the ith column of V.
14:   LDV – INTEGERInput
On entry: the first dimension of the array V as declared in the (sub)program from which F12AUF is called.
Constraint: LDVN.
15:   COMM60 – COMPLEX (KIND=nag_wp) arrayCommunication Array
On entry: must remain unchanged from the prior call to F12ARF and F12ATF.
16:   ICOMM140 – INTEGER arrayCommunication Array
On entry: must remain unchanged from the prior call to F12ARF and F12ATF.
17:   IFAIL – INTEGERInput/Output
On entry: IFAIL must be set to 0, -1​ or ​1. If you are unfamiliar with this parameter you should refer to Section 3.3 in the Essential Introduction for details.
For environments where it might be inappropriate to halt program execution when an error is detected, the value -1​ or ​1 is recommended. If the output of error messages is undesirable, then the value 1 is recommended. Otherwise, if you are not familiar with this parameter, the recommended value is 0. When the value -1​ or ​1 is used it is essential to test the value of IFAIL on exit.
On exit: IFAIL=0 unless the routine detects an error or a warning has been flagged (see Section 6).

6  Error Indicators and Warnings

If on entry IFAIL=0 or -1, explanatory error messages are output on the current error message unit (as defined by X04AAF).
Errors or warnings detected by the routine:
IFAIL=1
On entry, KL=value.
Constraint: KL 0.
IFAIL=2
On entry, KU=value.
Constraint: KU 0.
IFAIL=3
On entry, LDAB=value, 2×KL+KU+1=value.
Constraint: LDAB2×KL+KU+1.
IFAIL=5
The maximum number of iterations 0, the option Iteration Limit has been set to value.
IFAIL=6
The options Generalized and Regular are incompatible.
IFAIL=7
The option Initial Residual was selected but the starting vector held in RESID is zero.
IFAIL=8
Either the initialization routine has not been called prior to the first call of this routine or a communication array has become corrupted.
IFAIL=9
On entry, LDZ=value, N=value in F12AFF.
Constraint: LDZN.
IFAIL=10
On entry, Vectors = Select , but this is not yet implemented.
IFAIL=11
The number of eigenvalues found to sufficient accuracy is zero.
IFAIL=12
Could not build an Arnoldi factorization. The size of the current Arnoldi factorization = value.
IFAIL=13
Error in internal call to compute eigenvalues and corresponding error bounds of the current upper Hessenberg matrix. Please contact NAG.
IFAIL=14
During calculation of a Schur form, there was a failure to compute a number of eigenvalues Please contact NAG.
IFAIL=15
The computed Schur form could not be reordered by an internal call. Please contact NAG.
IFAIL=16
Error in internal call to compute eigenvectors. Please contact NAG.
IFAIL=17
Failure during internal factorization of real banded matrix. Please contact NAG.
IFAIL=18
Failure during internal solution of real banded matrix. Please contact NAG.
IFAIL=19
Failure during internal factorization of complex banded matrix. Please contact NAG.
IFAIL=20
Failure during internal solution of complex banded matrix. Please contact NAG.
IFAIL=21
The maximum number of iterations has been reached. The maximum number of iterations=value. The number of converged eigenvalues =value.
IFAIL=22
No shifts could be applied during a cycle of the implicitly restarted Arnoldi iteration.
IFAIL=23
Overflow occurred during transformation of Ritz values to those of the original problem.
IFAIL=-99
An unexpected error has been triggered by this routine. Please contact NAG.
See Section 3.8 in the Essential Introduction for further information.
IFAIL=-399
Your licence key may have expired or may not have been installed correctly.
See Section 3.7 in the Essential Introduction for further information.
IFAIL=-999
Dynamic memory allocation failed.
See Section 3.6 in the Essential Introduction for further information.

7  Accuracy

The relative accuracy of a Ritz value, λ , is considered acceptable if its Ritz estimate Tolerance × λ . The default Tolerance used is the machine precision given by X02AJF.

8  Parallelism and Performance

F12AUF is threaded by NAG for parallel execution in multithreaded implementations of the NAG Library.
F12AUF 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 routine. Please also consult the Users' Note for your implementation for any additional implementation-specific information.

9  Further Comments

None.

10  Example

This example constructs the matrices A  and B  using LAPACK band storage format and solves Ax=λBx  in shifted inverse mode using the complex shift σ .

10.1  Program Text

Program Text (f12aufe.f90)

10.2  Program Data

Program Data (f12aufe.d)

10.3  Program Results

Program Results (f12aufe.r)


F12AUF (PDF version)
F12 Chapter Contents
F12 Chapter Introduction
NAG Library Manual

© The Numerical Algorithms Group Ltd, Oxford, UK. 2015