SRC/zhbgvx.f(3)
π NAME π
SRC/zhbgvx.f β okay bestie, this is the zhbgvx.f(3) page from the Library Functions Manual, and itβs all about the ZHBGVX subroutine. π
β¨ SYNOPSIS β¨
Functions/Subroutines
subroutine zhbgvx (jobz, range, uplo, n, ka, kb, ab, ldab, bb, ldbb, q,
ldq, vl, vu, il, iu, abstol, m, w, z, ldz, work, rwork, iwork,
ifail, info)
ZHBGVX β the icon herself. π
π» Function/Subroutine Documentation π»
subroutine zhbgvx (character jobz, character range, character uplo, integer
n, integer ka, integer kb, complex*16, dimension( ldab, * ) ab, integer
ldab, complex*16, dimension( ldbb, * ) bb, integer ldbb, complex*16,
dimension( ldq, * ) q, integer ldq, double precision vl, double
precision vu, integer il, integer iu, double precision abstol, integer
m, double precision, dimension( * ) w, complex*16, dimension( ldz, * )
z, integer ldz, complex*16, dimension( * ) work, double precision,
dimension( * ) rwork, integer, dimension( * ) iwork, integer, dimension(
* ) ifail, integer info)
ZHBGVX π
π Purpose π
ZHBGVX computes all the eigenvalues, and optionally the eigenvectors, of a complex generalized Hermitian-definite banded eigenproblem, of the form A*x=(lambda)*B*x. Here A and B are assumed to be Hermitian and banded, and B 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. β¨
π§Έ Parameters π§Έ
JOBZ
JOBZ is CHARACTER*1.
= 'N': Compute eigenvalues only;= 'V': Compute eigenvalues and eigenvectors.
RANGE
RANGE is CHARACTER*1.
= 'A': all eigenvalues will be found;= 'V': all eigenvalues in the half-open interval(VL,VU]will be found;= 'I': theIL-th throughIU-th eigenvalues will be found.
UPLO
UPLO is CHARACTER*1.
= 'U': Upper triangles ofAandBare stored;= 'L': Lower triangles ofAandBare stored.
N
N is INTEGER. The order of the matrices A and B. N >= 0. π«Ά
KA
KA is INTEGER. The number of superdiagonals of the matrix A if UPLO = 'U', or the number of subdiagonals if UPLO = 'L'. KA >= 0.
KB
KB is INTEGER. The number of superdiagonals of the matrix B if UPLO = 'U', or the number of subdiagonals if UPLO = 'L'. KB >= 0.
AB
AB is COMPLEX*16 array, dimension (LDAB, N).
On entry, the upper or lower triangle of the Hermitian band matrix A, stored in the first ka+1 rows of the array. The j-th column of A is stored in the j-th column of the array AB as follows:
if UPLO = 'U', AB(ka+1+i-j,j) = A(i,j) for max(1,j-ka)<=i<=j;
if UPLO = 'L', AB(1+i-j,j) = A(i,j) for j<=i<=min(n,j+ka).
On exit, the contents of AB are destroyed. π
LDAB
LDAB is INTEGER. The leading dimension of the array AB. LDAB >= KA+1.
BB
BB is COMPLEX*16 array, dimension (LDBB, N).
On entry, the upper or lower triangle of the Hermitian band matrix B, stored in the first kb+1 rows of the array. The j-th column of B is stored in the j-th column of the array BB as follows:
if UPLO = 'U', BB(kb+1+i-j,j) = B(i,j) for max(1,j-kb)<=i<=j;
if UPLO = 'L', BB(1+i-j,j) = B(i,j) for j<=i<=min(n,j+kb).
On exit, the factor S from the split Cholesky factorization B = S**H*S, as returned by ZPBSTF.
LDBB
LDBB is INTEGER. The leading dimension of the array BB. LDBB >= KB+1.
Q
Q is COMPLEX*16 array, dimension (LDQ, N).
If JOBZ = 'V', the n-by-n matrix used in the reduction of A*x = (lambda)*B*x to standard form, i.e. C*x = (lambda)*x, and consequently C to tridiagonal form.
If JOBZ = 'N', the array Q is not referenced. π
LDQ
LDQ is INTEGER. The leading dimension of the array Q. If JOBZ = 'N', LDQ >= 1. If JOBZ = 'V', LDQ >= max(1,N).
VL
VL is DOUBLE PRECISION.
If RANGE='V', the lower bound of the interval to be searched for eigenvalues. VL < VU. Not referenced if RANGE = 'A' or 'I'.
VU
VU is DOUBLE PRECISION.
If RANGE='V', the upper bound of the interval to be searched for eigenvalues. VL < VU. Not referenced if RANGE = 'A' or 'I'.
IL
IL is INTEGER.
If RANGE='I', the index of the smallest eigenvalue to be returned. 1 <= IL <= IU <= N, if N > 0; IL = 1 and IU = 0 if N = 0. Not referenced if RANGE = 'A' or 'V'.
IU
IU is INTEGER.
If RANGE='I', the index of the largest eigenvalue to be returned. 1 <= IL <= IU <= N, if N > 0; IL = 1 and IU = 0 if N = 0. Not referenced if RANGE = 'A' or 'V'.
ABSTOL
ABSTOL is DOUBLE PRECISION. The absolute error tolerance for the eigenvalues. An approximate eigenvalue is accepted as converged when it is determined to lie in an interval [a,b] of width less than or equal to
ABSTOL + EPS * max( |a|,|b| ) ,
where EPS is the machine precision. If ABSTOL is less than or equal to zero, then EPS*|T| will be used in its place, where |T| is the 1-norm of the tridiagonal matrix obtained by reducing AP to tridiagonal form.
Eigenvalues will be computed most accurately when ABSTOL is set to twice the underflow threshold 2*DLAMCH('S'), not zero. If this routine returns with INFO>0, indicating that some eigenvectors did not converge, try setting ABSTOL to 2*DLAMCH('S'). π₯
M
M is INTEGER. The total number of eigenvalues found. 0 <= M <= N. If RANGE = 'A', M = N, and if RANGE = 'I', M = IU-IL+1.
W
W is DOUBLE PRECISION array, dimension (N). If INFO = 0, the eigenvalues in ascending order. πΈ
Z
Z is COMPLEX*16 array, dimension (LDZ, N).
If JOBZ = 'V', then if INFO = 0, Z contains the matrix Z of eigenvectors, with the i-th column of Z holding the eigenvector associated with W(i). The eigenvectors are normalized so that Z**H*B*Z = I.
If JOBZ = 'N', then Z is not referenced.
LDZ
LDZ is INTEGER. The leading dimension of the array Z. LDZ >= 1, and if JOBZ = 'V', LDZ >= N.
WORK
WORK is COMPLEX*16 array, dimension (N).
RWORK
RWORK is DOUBLE PRECISION array, dimension (7*N).
IWORK
IWORK is INTEGER array, dimension (5*N).
IFAIL
IFAIL is INTEGER array, dimension (N).
If JOBZ = 'V', then if INFO = 0, the first M elements of IFAIL are zero. If INFO > 0, then IFAIL contains the indices of the eigenvectors that failed to converge. If JOBZ = 'N', then IFAIL is not referenced.
INFO
INFO is INTEGER.
= 0: successful exit< 0: ifINFO = -i, the i-th argument had an illegal value> 0: ifINFO = i, and i is:<= N: then i eigenvectors failed to converge. Their indices are stored in arrayIFAIL.> N: ifINFO = N + i, for1 <= i <= N, thenZPBSTFreturnedINFO = i:Bis not positive definite. The factorization ofBcould not be completed and no eigenvalues or eigenvectors were computed. π
π Author π
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
πΈ Contributors πΈ
Mark Fahey, Department of Mathematics, Univ. of Kentucky, USA.
π Definition π
Definition at line 297 of file zhbgvx.f.
π€ Author π€
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