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NAG Toolbox: nag_lapack_zstedc (f08jv)
Purpose
nag_lapack_zstedc (f08jv) computes all the eigenvalues and, optionally, all the eigenvectors of a real by symmetric tridiagonal matrix, or of a complex full or banded Hermitian matrix which has been reduced to tridiagonal form.
Syntax
Description
nag_lapack_zstedc (f08jv) computes all the eigenvalues and, optionally, the eigenvectors of a real symmetric tridiagonal matrix
. That is, the function computes the spectral factorization of
given by
where
is a diagonal matrix whose diagonal elements are the eigenvalues,
, of
and
is an orthogonal matrix whose columns are the eigenvectors,
, of
. Thus
The function may also be used to compute all the eigenvalues and eigenvectors of a complex full, or banded, Hermitian matrix
which has been reduced to real tridiagonal form
as
where
is unitary. The spectral factorization of
is then given by
In this case
must be formed explicitly and passed to
nag_lapack_zstedc (f08jv) in the array
z, and the function called with
. Functions which may be called to form
and
are
When only eigenvalues are required then this function calls
nag_lapack_dsterf (f08jf) to compute the eigenvalues of the tridiagonal matrix
, but when eigenvectors of
are also required and the matrix is not too small, then a divide and conquer method is used, which can be much faster than
nag_lapack_zsteqr (f08js), although more storage is required.
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
Golub G H and Van Loan C F (1996) Matrix Computations (3rd Edition) Johns Hopkins University Press, Baltimore
Parameters
Compulsory Input Parameters
- 1:
– string (length ≥ 1)
-
Indicates whether the eigenvectors are to be computed.
- Only the eigenvalues are computed (and the array z is not referenced).
- The eigenvalues and eigenvectors of are computed (and the array z must contain the matrix on entry).
- The eigenvalues and eigenvectors of are computed (and the array z is initialized by the function).
Constraint:
, or .
- 2:
– double array
-
The dimension of the array
d
must be at least
The diagonal elements of the tridiagonal matrix.
- 3:
– double array
-
The dimension of the array
e
must be at least
The subdiagonal elements of the tridiagonal matrix.
- 4:
– complex array
-
The first dimension,
, of the array
z must satisfy
- if or , ;
- otherwise .
The second dimension of the array
z must be at least
if
or
, and at least
otherwise.
If
,
z must contain the unitary matrix
used in the reduction to tridiagonal form.
Optional Input Parameters
- 1:
– int64int32nag_int scalar
-
Default:
the dimension of the array
d.
, the order of the symmetric tridiagonal matrix .
Constraint:
.
Output Parameters
- 1:
– double array
-
The dimension of the array
d will be
If , the eigenvalues in ascending order.
- 2:
– double array
-
The dimension of the array
e will be
- 3:
– complex array
-
The first dimension,
, of the array
z will be
- if or , ;
- otherwise .
The second dimension of the array
z will be
if
or
and
otherwise.
If
,
z contains the orthonormal eigenvectors of the original Hermitian matrix
, and if
,
z contains the orthonormal eigenvectors of the symmetric tridiagonal matrix
.
If
,
z is not referenced.
- 4:
– int64int32nag_int scalar
unless the function detects an error (see
Error Indicators and Warnings).
Error Indicators and Warnings
-
If , parameter had an illegal value on entry. The parameters are numbered as follows:
1:
compz, 2:
n, 3:
d, 4:
e, 5:
z, 6:
ldz, 7:
work, 8:
lwork, 9:
rwork, 10:
lrwork, 11:
iwork, 12:
liwork, 13:
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.
-
-
The algorithm failed to compute an eigenvalue while working on the submatrix lying in rows and columns through .
Accuracy
The computed eigenvalues and eigenvectors are exact for a nearby matrix
, where
and
is the
machine precision.
If
is an exact eigenvalue and
is the corresponding computed value, then
where
is a modestly increasing function of
.
If
is the corresponding exact eigenvector, and
is the corresponding computed eigenvector, then the angle
between them is bounded as follows:
Thus the accuracy of a computed eigenvector depends on the gap between its eigenvalue and all the other eigenvalues.
See Section 4.7 of
Anderson et al. (1999) for further details. See also
nag_lapack_ddisna (f08fl).
Further Comments
If only eigenvalues are required, the total number of floating-point operations is approximately proportional to
. When eigenvectors are required the number of operations is bounded above by approximately the same number of operations as
nag_lapack_zsteqr (f08js), but for large matrices
nag_lapack_zstedc (f08jv) is usually much faster.
The real analogue of this function is
nag_lapack_dstedc (f08jh).
Example
This example finds all the eigenvalues and eigenvectors of the Hermitian band matrix
is first reduced to tridiagonal form by a call to
nag_lapack_zhbtrd (f08hs).
Open in the MATLAB editor:
f08jv_example
function f08jv_example
fprintf('f08jv example results\n\n');
n = 4;
k = int64(2);
a = [ -3.13 + 0.00i, 1.94 - 2.10i, -3.40 + 0.25i, 0 + 0i;
1.94 + 2.10i, -1.91 + 0.00i, -0.82 - 0.89i, -0.67 + 0.34i;
-3.40 - 0.25i, -0.82 + 0.89i, -2.87 + 0.00i, -2.10 - 0.16i;
0 + 0i, -0.67 - 0.34i, -2.10 + 0.16i, 0.50 + 0i ];
kl = int64(k);
[~, abn, ifail] = f01zd( ...
'P', k, k, a, complex(zeros(k+k+1,n)));
ab = abn(1:k+1,1:n);
compz = 'V';
uplo = 'Upper';
[~, Td, Te, ZTZ, info] = f08hs( ...
compz, uplo, k, ab, complex(zeros(n, n)));
[w, ~, z, info] = f08jv( ...
compz, Td, Te, ZTZ);
for i = 1:n
[~,k] = max(abs(real(z(:,i)))+abs(imag(z(:,i))));
z(:,i) = z(:,i)*conj(z(k,i))/abs(z(k,i));
end
disp(' Eigenvalues of A:');
disp(w');
disp(' Corresponding eigenvectors:');
disp(z);
f08jv example results
Eigenvalues of A:
-7.0042 -4.0038 0.5968 3.0012
Corresponding eigenvectors:
0.7293 + 0.0000i -0.2128 + 0.1511i -0.3354 - 0.1604i 0.4732 + 0.1947i
-0.1654 - 0.2046i 0.7316 + 0.0000i -0.2804 - 0.3413i 0.0891 + 0.4387i
0.6081 + 0.0301i 0.3910 - 0.3843i -0.0144 + 0.1532i -0.5172 - 0.1938i
0.1653 - 0.0303i 0.2775 - 0.1378i 0.8019 + 0.0000i 0.4824 + 0.0000i
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