SRC/zhegvx.f(3)
π¦ SRC/zhegvx.f β ZHEGVX π¦
okay bestie, welcome to the Library Functions Manual page for SRC/zhegvx.f. Itβs giving LAPACK linear-algebra main character energy, and the subroutine on deck is ZHEGVX. No cap. π
β¨
π NAME
SRC/zhegvx.f β yes bestie, thatβs the file. The star of the show is the subroutine ZHEGVX, and this page is literally its docs. π
β¨ SYNOPSIS
Functions/Subroutines
subroutine zhegvx (itype, jobz, range, uplo, n, a, lda, b, ldb, vl, vu,
il, iu, abstol, m, w, z, ldz, work, lwork, rwork, iwork, ifail,
info)
ZHEGVX
π§ Function/Subroutine Documentation
subroutine zhegvx (integer itype, character jobz, character range, character
uplo, integer n, complex*16, dimension( lda, * ) a, integer lda,
complex*16, dimension( ldb, * ) b, integer ldb, 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, integer lwork,
double precision, dimension( * ) rwork, integer, dimension( * ) iwork,
integer, dimension( * ) ifail, integer info)
ZHEGVX
Purpose π‘
ZHEGVX computes selected eigenvalues, and optionally eigenvectors, of a complex generalized Hermitian-definite eigenproblem. The forms are A*x=(lambda)*B*x, A*Bx=(lambda)*x, or B*A*x=(lambda)*x. Here A and B are assumed to be Hermitian, and B is also positive definite. Eigenvalues and eigenvectors can be selected by specifying either a range of values or a range of indices for the desired eigenvalues. π¦
Parameters ποΈ
ITYPEβITYPE is INTEGER. It specifies the problem type to be solved:= 1: A*x = (lambda)*B*x,= 2: A*B*x = (lambda)*x,= 3: B*A*x = (lambda)*x. πJOBZβJOBZ is CHARACTER*1.= 'N': Compute eigenvalues only;= 'V': Compute eigenvalues and eigenvectors.β¨RANGEβRANGE is CHARACTER*1.= 'A': all eigenvalues will be found.= 'V': all eigenvalues in the half-open interval (VL,VU] will be found.= 'I': the IL-th through IU-th eigenvalues will be found.πUPLOβUPLO is CHARACTER*1.= 'U': Upper triangles of A and B are stored;= 'L': Lower triangles of A and B are stored.πNβN is INTEGER. The order of the matrices A and B.N >= 0. πAβA is COMPLEX*16 array, dimension (LDA, N). On entry, the Hermitian matrix A. IfUPLO = 'U', the leading N-by-N upper triangular part of A contains the upper triangular part of the matrix A. IfUPLO = 'L', the leading N-by-N lower triangular part of A contains the lower triangular part of the matrix A.
On exit, the lower triangle (if UPLO='L') or the upper triangle (if UPLO='U') of A, including the diagonal, is destroyed. π
LDAβLDA is INTEGER. The leading dimension of the array A.LDA >= max(1,N). πBβB is COMPLEX*16 array, dimension (LDB, N). On entry, the Hermitian matrix B. IfUPLO = 'U', the leading N-by-N upper triangular part of B contains the upper triangular part of the matrix B. IfUPLO = 'L', the leading N-by-N lower triangular part of B contains the lower triangular part of the matrix B.
On exit, if INFO <= N, the part of B containing the matrix is overwritten by the triangular factor U or L from the Cholesky factorization B = U**H*U or B = L*L**H. π«Ά
LDBβLDB is INTEGER. The leading dimension of the array B.LDB >= max(1,N). πΈVLβVL is DOUBLE PRECISION. IfRANGE='V', the lower bound of the interval to be searched for eigenvalues.VL < VU. Not referenced ifRANGE = 'A'or'I'. πVUβVU is DOUBLE PRECISION. IfRANGE='V', the upper bound of the interval to be searched for eigenvalues.VL < VU. Not referenced ifRANGE = 'A'or'I'. πILβIL is INTEGER. IfRANGE='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 ifRANGE = 'A'or'V'. π₯IUβIU is INTEGER. IfRANGE='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 ifRANGE = 'A'or'V'. π₯ABSTOLβABSTOL 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 C to tridiagonal form, where C is the symmetric matrix of the standard symmetric problem to which the generalized problem is transformed.
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
MβM is INTEGER. The total number of eigenvalues found.0 <= M <= N. IfRANGE = 'A',M = N, and ifRANGE = 'I',M = IU-IL+1. πWβW is DOUBLE PRECISION array, dimension (N). The first M elements contain the selected eigenvalues in ascending order. πZβZ is COMPLEX*16 array, dimension (LDZ, max(1,M)). IfJOBZ = 'N', then Z is not referenced. IfJOBZ = 'V', then ifINFO = 0, the first M columns of Z contain the orthonormal eigenvectors of the matrix A corresponding to the selected eigenvalues, with the i-th column of Z holding the eigenvector associated withW(i).
The eigenvectors are normalized as follows: if ITYPE = 1 or 2, Z**T*B*Z = I; if ITYPE = 3, Z**T*inv(B)*Z = I.
If an eigenvector fails to converge, then that column of Z contains the latest approximation to the eigenvector, and the index of the eigenvector is returned in IFAIL. Note: the user must ensure that at least max(1,M) columns are supplied in the array Z; if RANGE = 'V', the exact value of M is not known in advance and an upper bound must be used. π¦
LDZβLDZ is INTEGER. The leading dimension of the array Z.LDZ >= 1, and ifJOBZ = 'V',LDZ >= max(1,N). πWORKβWORK is COMPLEX*16 array, dimension (MAX(1,LWORK)). On exit, ifINFO = 0,WORK(1)returns the optimalLWORK. β¨LWORKβLWORK is INTEGER. The length of the array WORK.LWORK >= max(1,2*N). For optimal efficiency,LWORK >= (NB+1)*N, where NB is the blocksize forZHETRDreturned byILAENV.
If LWORK = -1, then a workspace query is assumed; the routine only calculates the optimal size of the WORK array, returns this value as the first entry of the WORK array, and no error message related to LWORK is issued by XERBLA. π§
RWORKβRWORK is DOUBLE PRECISION array, dimension (7*N). πΈIWORKβIWORK is INTEGER array, dimension (5*N). πΈIFAILβIFAIL is INTEGER array, dimension (N). IfJOBZ = 'V', then ifINFO = 0, the first M elements ofIFAILare zero. IfINFO > 0, thenIFAILcontains the indices of the eigenvectors that failed to converge. IfJOBZ = 'N', thenIFAILis not referenced. πINFOβINFO is INTEGER.= 0: successful exit.< 0: if INFO = -i, the i-th argument had an illegal value.> 0: ZPOTRF or ZHEEVX returned an error code:<= N: if INFO = i, ZHEEVX failed to converge; i eigenvectors failed to converge. Their indices are stored in array IFAIL.> N: if INFO = N + i, for 1 <= i <= N, then the leading principal minor of order i of B is not positive. The factorization of B could not be completed and no eigenvalues or eigenvectors were computed.π
π Author
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
π Contributors
- Mark Fahey, Department of Mathematics, Univ. of Kentucky, USA
π Definition
Definition at line 304 of file zhegvx.f.
π«Ά Author
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