DLAED8(3)
π DLAED8(3) β Library Functions Manual π
okay so welcome to DLAED8(3), bestie β this is a page from the Library Functions Manual, and it's all about one very specific LAPACK routine. Buckle up, because this is giving linear algebra main character energy. π
π NAME π
/home/abuild/rpmbuild/BUILD/lapack-static-3.12.0-build/lapack-3.12.0/SRC/dlaed8.f β that's the exact source file path this page is named after, no cap.
β¨ SYNOPSIS β¨
πΈ Functions/Subroutines πΈ
subroutine DLAED8 (icompq, k, n, qsiz, d, q, ldq, indxq, rho, cutpnt, z,
dlambda, q2, ldq2, w, perm, givptr, givcol, givnum, indxp, indx,
info)
DLAED8 used by DSTEDC. Merges eigenvalues and deflates secular
equation. Used when the original matrix is dense.
π Function/Subroutine Documentation π
subroutine DLAED8 (integer icompq, integer k, integer n, integer qsiz,
double precision, dimension( * ) d, double precision, dimension( ldq, *
) q, integer ldq, integer, dimension( * ) indxq, double precision rho,
integer cutpnt, double precision, dimension( * ) z, double precision,
dimension( * ) dlambda, double precision, dimension( ldq2, * ) q2,
integer ldq2, double precision, dimension( * ) w, integer, dimension( *
) perm, integer givptr, integer, dimension( 2, * ) givcol, double
precision, dimension( 2, * ) givnum, integer, dimension( * ) indxp,
integer, dimension( * ) indx, integer info)
DLAED8 used by DSTEDC. Merges eigenvalues and deflates secular equation. Used when the original matrix is dense.
π― Purpose π―
Okay so here's the tea: DLAED8 merges the two sets of eigenvalues together into a single sorted set. Then it tries to deflate the size of the problem. There are two ways in which deflation can occur: when two or more eigenvalues are close together, or if there is a tiny element in the Z vector. For each such occurrence, the order of the related secular equation problem is reduced by one. Periodt. π
π§Ύ Parameters π§Ύ
ICOMPQβINTEGER.= 0: compute eigenvalues only.= 1: compute eigenvectors of the original dense symmetric matrix also. On entry,Qcontains the orthogonal matrix used to reduce the original matrix to tridiagonal form. πKβINTEGER. The number of non-deflated eigenvalues, and the order of the related secular equation.NβINTEGER. The dimension of the symmetric tridiagonal matrix.N >= 0.QSIZβINTEGER. The dimension of the orthogonal matrix used to reduce the full matrix to tridiagonal form.QSIZ >= NifICOMPQ = 1.DβDOUBLE PRECISION array, dimension (N). On entry, the eigenvalues of the two submatrices to be combined. On exit, the trailing(N-K)updated eigenvalues (those which were deflated) sorted into increasing order.QβDOUBLE PRECISION array, dimension (LDQ,N). IfICOMPQ = 0,Qis not referenced. Otherwise, on entry,Qcontains the eigenvectors of the partially solved system which has been previously updated in matrix multiplies with other partially solved eigensystems. On exit,Qcontains the trailing(N-K)updated eigenvectors (those which were deflated) in its lastN-Kcolumns.LDQβINTEGER. The leading dimension of the arrayQ.LDQ >= max(1,N).INDXQβINTEGER array, dimension (N). The permutation which separately sorts the two sub-problems inDinto ascending order. Note that elements in the second half of this permutation must first haveCUTPNTadded to their values in order to be accurate.RHOβDOUBLE PRECISION. On entry, the off-diagonal element associated with the rank-1 cut which originally split the two submatrices which are now being recombined. On exit,RHOhas been modified to the value required byDLAED3.CUTPNTβINTEGER. The location of the last eigenvalue in the leading sub-matrix.min(1,N) <= CUTPNT <= N.ZβDOUBLE PRECISION array, dimension (N). On entry,Zcontains the updating vector (the last row of the first sub-eigenvector matrix and the first row of the second sub-eigenvector matrix). On exit, the contents ofZare destroyed by the updating process.
Heads up, bestie: on exit, the contents of Z are destroyed by the updating process. π
DLAMBDAβDOUBLE PRECISION array, dimension (N). A copy of the firstKeigenvalues which will be used byDLAED3to form the secular equation.Q2βDOUBLE PRECISION array, dimension (LDQ2,N). IfICOMPQ = 0,Q2is not referenced. Otherwise, a copy of the firstKeigenvectors which will be used byDLAED7in a matrix multiply (DGEMM) to update the new eigenvectors.LDQ2βINTEGER. The leading dimension of the arrayQ2.LDQ2 >= max(1,N).WβDOUBLE PRECISION array, dimension (N). The firstkvalues of the final deflation-altered z-vector and will be passed toDLAED3.PERMβINTEGER array, dimension (N). The permutations (from deflation and sorting) to be applied to each eigenblock.GIVPTRβINTEGER. The number of Givens rotations which took place in this subproblem.GIVCOLβINTEGER array, dimension (2, N). Each pair of numbers indicates a pair of columns to take place in a Givens rotation.GIVNUMβDOUBLE PRECISION array, dimension (2, N). Each number indicates theSvalue to be used in the corresponding Givens rotation.INDXPβINTEGER array, dimension (N). The permutation used to place deflated values ofDat the end of the array.INDXP(1:K)points to the nondeflatedD-values andINDXP(K+1:N)points to the deflated eigenvalues.INDXβINTEGER array, dimension (N). The permutation used to sort the contents ofDinto ascending order.INFOβINTEGER.= 0: successful exit.< 0: ifINFO = -i, thei-th argument had an illegal value.
Vibe check onINFO:< 0means an argument was illegal, andINFO = -itells you it was thei-th one. π
π Author π
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
π«Ά Contributors π«Ά
- Jeff Rutter, Computer Science Division, University of California at Berkeley, USA
π Definition π
Definition at line 240 of file dlaed8.f.
π¦ Author π¦
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