home
***
CD-ROM
|
disk
|
FTP
|
other
***
search
/
IRIX 6.2 Development Libraries
/
SGI IRIX 6.2 Development Libraries.iso
/
dist
/
complib.idb
/
usr
/
share
/
catman
/
p_man
/
cat3
/
complib
/
dlaed1.z
/
dlaed1
Wrap
Text File
|
1996-03-14
|
4KB
|
133 lines
DDDDLLLLAAAAEEEEDDDD1111((((3333FFFF)))) DDDDLLLLAAAAEEEEDDDD1111((((3333FFFF))))
NNNNAAAAMMMMEEEE
DLAED1 - compute the updated eigensystem of a diagonal matrix after
modification by a rank-one symmetric matrix
SSSSYYYYNNNNOOOOPPPPSSSSIIIISSSS
SUBROUTINE DLAED1( N, D, Q, LDQ, INDXQ, RHO, CUTPNT, WORK, IWORK, INFO )
INTEGER CUTPNT, INFO, LDQ, N
DOUBLE PRECISION RHO
INTEGER INDXQ( * ), IWORK( * )
DOUBLE PRECISION D( * ), Q( LDQ, * ), WORK( * )
PPPPUUUURRRRPPPPOOOOSSSSEEEE
DLAED1 computes the updated eigensystem of a diagonal matrix after
modification by a rank-one symmetric matrix. This routine is used only
for the eigenproblem which requires all eigenvalues and eigenvectors of a
tridiagonal matrix. DLAED7 handles the case in which eigenvalues only or
eigenvalues and eigenvectors of a full symmetric matrix (which was
reduced to tridiagonal form) are desired.
T = Q(in) ( D(in) + RHO * Z*Z' ) Q'(in) = Q(out) * D(out) * Q'(out)
where Z = Q'u, u is a vector of length N with ones in the
CUTPNT and CUTPNT + 1 th elements and zeros elsewhere.
The eigenvectors of the original matrix are stored in Q, and the
eigenvalues are in D. The algorithm consists of three stages:
The first stage consists of deflating the size of the problem
when there are multiple eigenvalues or if there is a zero in
the Z vector. For each such occurence the dimension of the
secular equation problem is reduced by one. This stage is
performed by the routine DLAED2.
The second stage consists of calculating the updated
eigenvalues. This is done by finding the roots of the secular
equation via the routine DLAED4 (as called by SLAED3).
This routine also calculates the eigenvectors of the current
problem.
The final stage consists of computing the updated eigenvectors
directly using the updated eigenvalues. The eigenvectors for
the current problem are multiplied with the eigenvectors from
the overall problem.
PPPPaaaaggggeeee 1111
DDDDLLLLAAAAEEEEDDDD1111((((3333FFFF)))) DDDDLLLLAAAAEEEEDDDD1111((((3333FFFF))))
ARGUMENTS
N (input) INTEGER
The dimension of the symmetric tridiagonal matrix. N >= 0.
D (input/output) DOUBLE PRECISION array, dimension (N)
On entry, the eigenvalues of the rank-1-perturbed matrix. On
exit, the eigenvalues of the repaired matrix.
Q (input/output) DOUBLE PRECISION array, dimension (LDQ,N)
On entry, the eigenvectors of the rank-1-perturbed matrix. On
exit, the eigenvectors of the repaired tridiagonal matrix.
LDQ (input) INTEGER
The leading dimension of the array Q. LDQ >= max(1,N).
INDXQ (input/output) INTEGER array, dimension (N)
On entry, the permutation which separately sorts the two
subproblems in D into ascending order. On exit, the permutation
which will reintegrate the subproblems back into sorted order,
i.e. D( INDXQ( I = 1, N ) ) will be in ascending order.
RHO (input) DOUBLE PRECISION
The subdiagonal entry used to create the rank-1 modification.
CUTPNT (input) INTEGER The location of the last eigenvalue in the
leading sub-matrix. min(1,N) <= CUTPNT <= N.
WORK (workspace) DOUBLE PRECISION array, dimension (3*N+2*N**2)
IWORK (workspace) INTEGER array, dimension (4*N)
INFO (output) INTEGER
= 0: successful exit.
< 0: if INFO = -i, the i-th argument had an illegal value.
> 0: if INFO = 1, an eigenvalue did not converge
PPPPaaaaggggeeee 2222