PDF version (NAG web site
, 64-bit version, 64-bit version)
NAG Toolbox: nag_lapack_zhbgvx (f08up)
Purpose
nag_lapack_zhbgvx (f08up) computes selected the eigenvalues and, optionally, the eigenvectors of a complex generalized Hermitian-definite banded eigenproblem, of the form
where
and
are Hermitian and banded, and
is also positive definite. Eigenvalues and eigenvectors can be selected by specifying either all eigenvalues, a range of values or a range of indices for the desired eigenvalues.
Syntax
[
ab,
bb,
q,
m,
w,
z,
jfail,
info] = f08up(
jobz,
range,
uplo,
ka,
kb,
ab,
bb,
vl,
vu,
il,
iu,
abstol, 'n',
n)
[
ab,
bb,
q,
m,
w,
z,
jfail,
info] = nag_lapack_zhbgvx(
jobz,
range,
uplo,
ka,
kb,
ab,
bb,
vl,
vu,
il,
iu,
abstol, 'n',
n)
Description
The generalized Hermitian-definite band problem
is first reduced to a standard band Hermitian problem
where
is a Hermitian band matrix, using Wilkinson's modification to Crawford's algorithm (see
Crawford (1973) and
Wilkinson (1977)). The Hermitian eigenvalue problem is then solved for the required eigenvalues and eigenvectors, and the eigenvectors are then backtransformed to the eigenvectors of the original problem.
The eigenvectors are normalized so that
References
Anderson E, Bai Z, Bischof C, Blackford S, Demmel J, Dongarra J J, Du Croz J J, Greenbaum A, Hammarling S, McKenney A and Sorensen D (1999)
LAPACK Users' Guide (3rd Edition) SIAM, Philadelphia
http://www.netlib.org/lapack/lug
Crawford C R (1973) Reduction of a band-symmetric generalized eigenvalue problem Comm. ACM 16 41–44
Demmel J W and Kahan W (1990) Accurate singular values of bidiagonal matrices SIAM J. Sci. Statist. Comput. 11 873–912
Golub G H and Van Loan C F (1996) Matrix Computations (3rd Edition) Johns Hopkins University Press, Baltimore
Wilkinson J H (1977) Some recent advances in numerical linear algebra The State of the Art in Numerical Analysis (ed D A H Jacobs) Academic Press
Parameters
Compulsory Input Parameters
- 1:
– string (length ≥ 1)
-
Indicates whether eigenvectors are computed.
- Only eigenvalues are computed.
- Eigenvalues and eigenvectors are computed.
Constraint:
or .
- 2:
– string (length ≥ 1)
-
If
, all eigenvalues will be found.
If , all eigenvalues in the half-open interval will be found.
If
, the
ilth to
iuth eigenvalues will be found.
Constraint:
, or .
- 3:
– string (length ≥ 1)
-
If
, the upper triangles of
and
are stored.
If , the lower triangles of and are stored.
Constraint:
or .
- 4:
– int64int32nag_int scalar
-
If
, the number of superdiagonals,
, of the matrix
.
If , the number of subdiagonals, , of the matrix .
Constraint:
.
- 5:
– int64int32nag_int scalar
-
If
, the number of superdiagonals,
, of the matrix
.
If , the number of subdiagonals, , of the matrix .
Constraint:
.
- 6:
– complex array
-
The first dimension of the array
ab must be at least
.
The second dimension of the array
ab must be at least
.
The upper or lower triangle of the
by
Hermitian band matrix
.
The matrix is stored in rows
to
, more precisely,
- if , the elements of the upper triangle of within the band must be stored with element in ;
- if , the elements of the lower triangle of within the band must be stored with element in
- 7:
– complex array
-
The first dimension of the array
bb must be at least
.
The second dimension of the array
bb must be at least
.
The upper or lower triangle of the
by
Hermitian positive definite band matrix
.
The matrix is stored in rows
to
, more precisely,
- if , the elements of the upper triangle of within the band must be stored with element in ;
- if , the elements of the lower triangle of within the band must be stored with element in
- 8:
– double scalar
- 9:
– double scalar
-
If
, the lower and upper bounds of the interval to be searched for eigenvalues.
If
or
,
vl and
vu are not referenced.
Constraint:
if , .
- 10:
– int64int32nag_int scalar
- 11:
– int64int32nag_int scalar
-
If
, the indices (in ascending order) of the smallest and largest eigenvalues to be returned.
If
or
,
il and
iu are not referenced.
Constraints:
- if and , and ;
- if and , .
- 12:
– double scalar
-
The absolute error tolerance for the eigenvalues. An approximate eigenvalue is accepted as converged when it is determined to lie in an interval
of width less than or equal to
where
is the
machine precision. If
abstol is less than or equal to zero, then
will be used in its place, where
is the tridiagonal matrix obtained by reducing
to tridiagonal form. Eigenvalues will be computed most accurately when
abstol is set to twice the underflow threshold
, not zero. If this function returns with
, indicating that some eigenvectors did not converge, try setting
abstol to
. See
Demmel and Kahan (1990).
Optional Input Parameters
- 1:
– int64int32nag_int scalar
-
Default:
the second dimension of the arrays
ab,
bb.
, the order of the matrices and .
Constraint:
.
Output Parameters
- 1:
– complex array
-
The first dimension of the array
ab will be
.
The second dimension of the array
ab will be
.
The contents of
ab are overwritten.
- 2:
– complex array
-
The first dimension of the array
bb will be
.
The second dimension of the array
bb will be
.
The factor
from the split Cholesky factorization
, as returned by
nag_lapack_zpbstf (f08ut).
- 3:
– complex array
-
The first dimension,
, of the array
q will be
- if , ;
- otherwise .
The second dimension of the array
q will be
if
and
otherwise.
If
, the
by
matrix,
used in the reduction of the standard form, i.e.,
, from symmetric banded to tridiagonal form.
If
,
q is not referenced.
- 4:
– int64int32nag_int scalar
-
The total number of eigenvalues found.
.
If , .
If , .
- 5:
– double array
-
The eigenvalues in ascending order.
- 6:
– complex array
-
The first dimension,
, of the array
z will be
- if , ;
- otherwise .
The second dimension of the array
z will be
if
and
otherwise.
If
,
z contains the matrix
of eigenvectors, with the
th column of
holding the eigenvector associated with
. The eigenvectors are normalized so that
.
If
,
z is not referenced.
- 7:
– int64int32nag_int array
-
The dimension of the array
jfail will be
If
, then
- if , the first m elements of jfail are zero;
- if , jfail contains the indices of the eigenvectors that failed to converge.
If
,
jfail is not referenced.
- 8:
– int64int32nag_int scalar
unless the function detects an error (see
Error Indicators and Warnings).
Error Indicators and Warnings
Cases prefixed with W are classified as warnings and
do not generate an error of type NAG:error_n. See nag_issue_warnings.
-
If , parameter had an illegal value on entry. The parameters are numbered as follows:
1:
jobz, 2:
range, 3:
uplo, 4:
n, 5:
ka, 6:
kb, 7:
ab, 8:
ldab, 9:
bb, 10:
ldbb, 11:
q, 12:
ldq, 13:
vl, 14:
vu, 15:
il, 16:
iu, 17:
abstol, 18:
m, 19:
w, 20:
z, 21:
ldz, 22:
work, 23:
rwork, 24:
iwork, 25:
jfail, 26:
info.
It is possible that
info refers to a parameter that is omitted from the MATLAB interface. This usually indicates that an error in one of the other input parameters has caused an incorrect value to be inferred.
- W
-
If
, then
eigenvectors failed to converge. Their indices are stored in array
jfail. Please see
abstol.
-
-
nag_lapack_dpbstf (f08uf) returned an error code; i.e., if
, for
, then the leading minor of order
of
is not positive definite. The factorization of
could not be completed and no eigenvalues or eigenvectors were computed.
Accuracy
If
is ill-conditioned with respect to inversion, then the error bounds for the computed eigenvalues and vectors may be large, although when the diagonal elements of
differ widely in magnitude the eigenvalues and eigenvectors may be less sensitive than the condition of
would suggest. See Section 4.10 of
Anderson et al. (1999) for details of the error bounds.
Further Comments
The total number of floating-point operations is proportional to if and , and assuming that , is approximately proportional to if . Otherwise the number of floating-point operations depends upon the number of eigenvectors computed.
The real analogue of this function is
nag_lapack_dsbgvx (f08ub).
Example
This example finds the eigenvalues in the half-open interval
, and corresponding eigenvectors, of the generalized band Hermitian eigenproblem
, where
and
Open in the MATLAB editor:
f08up_example
function f08up_example
fprintf('f08up example results\n\n');
uplo = 'U';
ka = int64(2);
ab = [ 0, 0 + 0i, -1.40 + 0.25i, -0.67 + 0.34i;
0 + 0i, 1.94 - 2.10i, -0.82 - 0.89i, -1.10 - 0.16i;
-1.13 + 0i, -1.91 + 0i, -1.87 + 0i, 0.50 + 0i];
kb = int64(1);
bb = [ 0, 1.08 - 1.73i, -0.04 + 0.29i, -0.33 + 2.24i;
9.89 + 0i, 1.69 + 0i, 2.65 + 0i, 2.17 + 0i];
jobz = 'Vectors';
range = 'Values in range';
vl = 0; vu = 2;
il = int64(0); iu = il;
abstol = 0;
[~, ~, ~, m, w, z, jfail, info] = ...
f08up( ...
jobz, range, uplo, ka, kb, ab, bb, vl, vu, il, iu, abstol);
disp('Selected eigenvalues');
disp(w(1:m)');
for i = 1:m
[~,k] = max(abs(real(z(:,i)))+abs(imag(z(:,i))));
z(:,i) = z(:,i)*conj(z(k,i))/abs(z(k,i));
end
disp('Corresponding eigenvectors');
disp(z(:,1:m));
f08up example results
Selected eigenvalues
0.1603 1.7712
Corresponding eigenvectors
-0.1026 - 0.1614i 0.0068 + 0.0492i
-0.0028 - 0.1738i -0.4307 + 0.2705i
-0.0466 + 0.0890i -0.1123 - 0.9664i
0.3586 + 0.0000i 1.3241 + 0.0000i
PDF version (NAG web site
, 64-bit version, 64-bit version)
© The Numerical Algorithms Group Ltd, Oxford, UK. 2009–2015