SRC/zhpgvx.f(3)
π NAME π
SRC/zhpgvx.f β bestie, this is the LAPACK routine zhpgvx, and it's literally out here computing selected eigenvalues and (optionally!) eigenvectors of a complex generalized Hermitian-definite eigenproblem. Sound like a lot? It is. But we're gonna get through it together π«Ά
β¨ SYNOPSIS β¨
Functions/Subroutines
subroutine zhpgvx (itype, jobz, range, uplo, n, ap, bp, vl, vu, il, iu,
abstol, m, w, z, ldz, work, rwork, iwork, ifail, info)
ZHPGVX β that's her name, that's her whole brand π
π¦ Function/Subroutine Documentation π¦
subroutine zhpgvx β the full signature, no cap
subroutine zhpgvx (integer itype, character jobz, character range, character
uplo, integer n, complex*16, dimension( * ) ap, complex*16, dimension( *
) bp, 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)
ZHPGVX
π Purpose π
!> !> ZHPGVX computes selected eigenvalues and, optionally, eigenvectors !> of a complex generalized Hermitian-definite eigenproblem, of the form !> A*x=(lambda)*B*x, A*Bx=(lambda)*x, or B*A*x=(lambda)*x. Here A and !> B are assumed to be Hermitian, stored in packed format, 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. !>
So like β A and B are Hermitian, they're living their packed-format life, B is also positive definite (she's gotta be, it's the rules), and you get to pick which eigenvalues you want. Main character selection energy, honestly.
πΈ Parameters πΈ
ITYPEβITYPE is INTEGER. It's the problem type, and she comes in three flavors:
!> 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 !>
JOBZβJOBZ is CHARACTER*1, aka the "do you want the eigenvectors or nah" switch:
!> = 'N': Compute eigenvalues only; !> = 'V': Compute eigenvalues and eigenvectors. !>
RANGEβRANGE is CHARACTER*1, the picker:
!> = '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. !>
UPLOβUPLO is CHARACTER*1, which triangle of A and B is stored:
!> = 'U': Upper triangles of A and B are stored; !> = 'L': Lower triangles of A and B are stored. !>
NβN is INTEGER. The order of the matrices A and B.N >= 0. That's it, that's the whole vibe check.APβAP is COMPLEX*16 array, dimension (N*(N+1)/2)
!> On entry, the upper or lower triangle of the Hermitian matrix !> A, packed columnwise in a linear array. The j-th column of A !> is stored in the array AP as follows: !> if UPLO = 'U', AP(i + (j-1)j/2) = A(i,j) for 1<=i<=j; !> if UPLO = 'L', AP(i + (j-1)(2*n-j)/2) = A(i,j) for j<=i<=n. !> !> On exit, the contents of AP are destroyed. !>
β οΈ Yes bestie, destroyed. On exit AP is gone-gone. Do not come looking for her.
BPβBP is COMPLEX*16 array, dimension (N*(N+1)/2)
!> On entry, the upper or lower triangle of the Hermitian matrix !> B, packed columnwise in a linear array. The j-th column of B !> is stored in the array BP as follows: !> if UPLO = 'U', BP(i + (j-1)j/2) = B(i,j) for 1<=i<=j; !> if UPLO = 'L', BP(i + (j-1)(2*n-j)/2) = B(i,j) for j<=i<=n. !> !> On exit, the triangular factor U or L from the Cholesky !> factorization B = UH*U or B = L*LH, in the same storage !> format as B. !>
So BP gets a glow-up on exit: she comes back as the triangular factor U or L from the Cholesky factorization B = U**H*U or B = L*L**H, same storage format as before. Iconic transformation arc π«
VLβVL 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'. !>
VUβVU 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'. !>
Note the duo: VL < VU, strictly. No equality shenanigans.
ILβIL 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'. !>
IUβIU 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'. !>
ABSTOLβABSTOL is DOUBLE PRECISION. The absolute error tolerance for the eigenvalues. She's the "close enough is close enough" queen:
!> 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― Real talk: set it to 2*DLAMCH('S') for max accuracy, not zero. And if it comes back with INFO>0 (some eigenvectors didn't converge), your move is setting ABSTOL to 2*DLAMCH('S'). That's the tip, take it.
MβM is INTEGER. The total number of eigenvalues found.0 <= M <= N. IfRANGE = 'A',M = N, and ifRANGE = 'I',M = IU-IL+1.WβW is DOUBLE PRECISION array, dimension (N)
!> On normal exit, the first M elements contain the selected !> eigenvalues in ascending order. !>
Ascending order, as she should π
ZβZ is COMPLEX*16 array, dimension (LDZ, N)
!> If JOBZ = 'N', then Z is not referenced. !> If JOBZ = 'V', then if INFO = 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 with W(i). !> The eigenvectors are normalized as follows: !> if ITYPE = 1 or 2, ZH*B*Z = I; !> if ITYPE = 3, ZH*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¨ Pay attention to that note, bestie: you have to make sure at least max(1,M) columns are supplied in Z. And if RANGE = 'V', the exact value of M isn't known in advance so you gotta use an upper bound. Don't get caught lacking.
LDZβLDZ is INTEGER. The leading dimension of the array Z.LDZ >= 1, and ifJOBZ = 'V',LDZ >= max(1,N).WORKβWORK is COMPLEX*16 array, dimension (2*N)RWORKβRWORK is DOUBLE PRECISION array, dimension (7*N)IWORKβIWORK is INTEGER array, dimension (5*N)
The workspace trio π they don't do much talking, they just hold space. Respect.
IFAILβIFAIL 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. !>
The receipts array. If something flopped, the indices are in here π
INFOβINFO is INTEGER, the final verdict:
!> = 0: successful exit !> < 0: if INFO = -i, the i-th argument had an illegal value !> > 0: ZPPTRF or ZHPEVX returned an error code: !> <= N: if INFO = i, ZHPEVX 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. !>
β οΈ Read the > N case carefully: if INFO = N + i for 1 <= i <= n, the leading principal minor of order i of B is not positive β the factorization of B could not be completed and no eigenvalues or eigenvectors were computed. Nothing. Zero. Zilch. π
π Author π
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
π§ Contributors: π§
Mark Fahey, Department of Mathematics, Univ. of Kentucky, USA
β Definition β
Definition at line 274 of file zhpgvx.f.
π Author π
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