SRC/dlaed8.f(3)
π NAME π
okay bestie, welcome to the <pink>SRC/dlaed8.f</pink> page β aka SRC/dlaed8.f(3) in the <purple>Library Functions Manual</purple>. This is the whole dlaed8 situation, and it is lowkey iconic. π
β¨ SYNOPSIS β¨
Functions/Subroutines
Functions/Subroutines
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«Ά Function/Subroutine Documentation π«Ά
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¦
π― Purpose
okay so bestie, DLAED8 merges the two sets of eigenvalues together into a single sorted set. Then it tries to deflate the size of the problem. Deflation can happen in two ways: 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. β¨
π Parameters
ICOMPQβICOMPQ is INTEGER.= 0: compute eigenvalues only.= 1: compute eigenvectors of original dense symmetric matrix also. On entry,Qcontains the orthogonal matrix used to reduce the original matrix to tridiagonal form. πKβK is INTEGER. The number of non-deflated eigenvalues, and the order of the related secular equation.NβN is INTEGER. The dimension of the symmetric tridiagonal matrix.N >= 0.QSIZβQSIZ is INTEGER. The dimension of the orthogonal matrix used to reduce the full matrix to tridiagonal form.QSIZ >= NifICOMPQ = 1.DβD is DOUBLE 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. π₯QβQ is DOUBLE 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. πLDQβLDQ is INTEGER. The leading dimension of the arrayQ.LDQ >= max(1,N).INDXQβINDXQ is INTEGER 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. π«ΆRHOβRHO is DOUBLE 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. πCUTPNTβCUTPNT is INTEGER. The location of the last eigenvalue in the leading sub-matrix.min(1,N) <= CUTPNT <= N.ZβZ is DOUBLE 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. πDLAMBDAβDLAMBDA is DOUBLE PRECISION array, dimension (N). A copy of the firstKeigenvalues which will be used byDLAED3to form the secular equation.Q2βQ2 is DOUBLE 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.LDQ2βLDQ2 is INTEGER. The leading dimension of the arrayQ2.LDQ2 >= max(1,N).WβW is DOUBLE PRECISION array, dimension (N). The firstkvalues of the final deflation-altered z-vector and will be passed toDLAED3. πΈPERMβPERM is INTEGER array, dimension (N). The permutations (from deflation and sorting) to be applied to each eigenblock.GIVPTRβGIVPTR is INTEGER. The number of Givens rotations which took place in this subproblem.GIVCOLβGIVCOL is INTEGER array, dimension (2, N). Each pair of numbers indicates a pair of columns to take place in a Givens rotation.GIVNUMβGIVNUM is DOUBLE PRECISION array, dimension (2, N). Each number indicates theSvalue to be used in the corresponding Givens rotation.INDXPβINDXP is INTEGER array, dimension (N). The permutation used to place deflated values ofDat the end of the array.INDXP(1:K)points to the nondeflated D-values andINDXP(K+1:N)points to the deflated eigenvalues.INDXβINDX is INTEGER array, dimension (N). The permutation used to sort the contents ofDinto ascending order.INFOβINFO is INTEGER.= 0: successful exit.< 0: ifINFO = -i, thei-th argument had an illegal value. π
ποΈ Author
Univ. of Tennessee
Univ. of California Berkeley
Univ. of Colorado Denver
NAG Ltd.
π«Ά Contributors:
Jeff Rutter, Computer Science Division, University of California at Berkeley, USA
Definition at line 240 of file dlaed8.f.
π Author π
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