595 lines
16 KiB
FortranFixed
595 lines
16 KiB
FortranFixed
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c-----------------------------------------------------------------------
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c\BeginDoc
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c
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c\Name: dstqrb
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c
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c\Description:
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c Computes all eigenvalues and the last component of the eigenvectors
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c of a symmetric tridiagonal matrix using the implicit QL or QR method.
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c
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c This is mostly a modification of the LAPACK routine dsteqr.
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c See Remarks.
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c
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c\Usage:
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c call dstqrb
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c ( N, D, E, Z, WORK, INFO )
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c
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c\Arguments
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c N Integer. (INPUT)
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c The number of rows and columns in the matrix. N >= 0.
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c
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c D Double precision array, dimension (N). (INPUT/OUTPUT)
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c On entry, D contains the diagonal elements of the
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c tridiagonal matrix.
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c On exit, D contains the eigenvalues, in ascending order.
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c If an error exit is made, the eigenvalues are correct
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c for indices 1,2,...,INFO-1, but they are unordered and
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c may not be the smallest eigenvalues of the matrix.
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c
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c E Double precision array, dimension (N-1). (INPUT/OUTPUT)
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c On entry, E contains the subdiagonal elements of the
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c tridiagonal matrix in positions 1 through N-1.
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c On exit, E has been destroyed.
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c
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c Z Double precision array, dimension (N). (OUTPUT)
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c On exit, Z contains the last row of the orthonormal
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c eigenvector matrix of the symmetric tridiagonal matrix.
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c If an error exit is made, Z contains the last row of the
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c eigenvector matrix associated with the stored eigenvalues.
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c
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c WORK Double precision array, dimension (max(1,2*N-2)). (WORKSPACE)
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c Workspace used in accumulating the transformation for
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c computing the last components of the eigenvectors.
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c
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c INFO Integer. (OUTPUT)
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c = 0: normal return.
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c < 0: if INFO = -i, the i-th argument had an illegal value.
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c > 0: if INFO = +i, the i-th eigenvalue has not converged
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c after a total of 30*N iterations.
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c
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c\Remarks
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c 1. None.
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c
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c-----------------------------------------------------------------------
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c
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c\BeginLib
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c
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c\Local variables:
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c xxxxxx real
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c
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c\Routines called:
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c daxpy Level 1 BLAS that computes a vector triad.
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c dcopy Level 1 BLAS that copies one vector to another.
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c dswap Level 1 BLAS that swaps the contents of two vectors.
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c lsame LAPACK character comparison routine.
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c dlae2 LAPACK routine that computes the eigenvalues of a 2-by-2
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c symmetric matrix.
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c dlaev2 LAPACK routine that eigendecomposition of a 2-by-2 symmetric
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c matrix.
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c dlamch LAPACK routine that determines machine constants.
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c dlanst LAPACK routine that computes the norm of a matrix.
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c dlapy2 LAPACK routine to compute sqrt(x**2+y**2) carefully.
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c dlartg LAPACK Givens rotation construction routine.
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c dlascl LAPACK routine for careful scaling of a matrix.
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c dlaset LAPACK matrix initialization routine.
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c dlasr LAPACK routine that applies an orthogonal transformation to
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c a matrix.
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c dlasrt LAPACK sorting routine.
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c dsteqr LAPACK routine that computes eigenvalues and eigenvectors
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c of a symmetric tridiagonal matrix.
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c xerbla LAPACK error handler routine.
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c
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c\Authors
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c Danny Sorensen Phuong Vu
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c Richard Lehoucq CRPC / Rice University
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c Dept. of Computational & Houston, Texas
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c Applied Mathematics
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c Rice University
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c Houston, Texas
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c
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c\SCCS Information: @(#)
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c FILE: stqrb.F SID: 2.5 DATE OF SID: 8/27/96 RELEASE: 2
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c
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c\Remarks
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c 1. Starting with version 2.5, this routine is a modified version
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c of LAPACK version 2.0 subroutine SSTEQR. No lines are deleted,
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c only commeted out and new lines inserted.
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c All lines commented out have "c$$$" at the beginning.
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c Note that the LAPACK version 1.0 subroutine SSTEQR contained
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c bugs.
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c
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c\EndLib
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c
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c-----------------------------------------------------------------------
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c
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subroutine dstqrb ( n, d, e, z, work, info )
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c
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c %------------------%
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c | Scalar Arguments |
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c %------------------%
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c
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integer info, n
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c
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c %-----------------%
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c | Array Arguments |
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c %-----------------%
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c
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Double precision
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& d( n ), e( n-1 ), z( n ), work( 2*n-2 )
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c
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c .. parameters ..
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Double precision
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& zero, one, two, three
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parameter ( zero = 0.0D+0, one = 1.0D+0,
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& two = 2.0D+0, three = 3.0D+0 )
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integer maxit
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parameter ( maxit = 30 )
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c ..
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c .. local scalars ..
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integer i, icompz, ii, iscale, j, jtot, k, l, l1, lend,
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& lendm1, lendp1, lendsv, lm1, lsv, m, mm, mm1,
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& nm1, nmaxit
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Double precision
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& anorm, b, c, eps, eps2, f, g, p, r, rt1, rt2,
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& s, safmax, safmin, ssfmax, ssfmin, tst
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c ..
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c .. external functions ..
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logical lsame
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Double precision
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& dlamch, dlanst, dlapy2
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external lsame, dlamch, dlanst, dlapy2
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c ..
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c .. external subroutines ..
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external dlae2, dlaev2, dlartg, dlascl, dlaset, dlasr,
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& dlasrt, dswap, xerbla
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c ..
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c .. intrinsic functions ..
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intrinsic abs, max, sign, sqrt
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c ..
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c .. executable statements ..
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c
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c test the input parameters.
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c
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info = 0
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c
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c$$$ IF( LSAME( COMPZ, 'N' ) ) THEN
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c$$$ ICOMPZ = 0
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c$$$ ELSE IF( LSAME( COMPZ, 'V' ) ) THEN
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c$$$ ICOMPZ = 1
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c$$$ ELSE IF( LSAME( COMPZ, 'I' ) ) THEN
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c$$$ ICOMPZ = 2
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c$$$ ELSE
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c$$$ ICOMPZ = -1
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c$$$ END IF
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c$$$ IF( ICOMPZ.LT.0 ) THEN
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c$$$ INFO = -1
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c$$$ ELSE IF( N.LT.0 ) THEN
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c$$$ INFO = -2
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c$$$ ELSE IF( ( LDZ.LT.1 ) .OR. ( ICOMPZ.GT.0 .AND. LDZ.LT.MAX( 1,
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c$$$ $ N ) ) ) THEN
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c$$$ INFO = -6
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c$$$ END IF
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c$$$ IF( INFO.NE.0 ) THEN
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c$$$ CALL XERBLA( 'SSTEQR', -INFO )
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c$$$ RETURN
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c$$$ END IF
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c
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c *** New starting with version 2.5 ***
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c
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icompz = 2
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c *************************************
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c
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c quick return if possible
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c
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if( n.eq.0 )
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$ return
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c
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if( n.eq.1 ) then
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if( icompz.eq.2 ) z( 1 ) = one
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return
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end if
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c
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c determine the unit roundoff and over/underflow thresholds.
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c
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eps = dlamch( 'e' )
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eps2 = eps**2
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safmin = dlamch( 's' )
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safmax = one / safmin
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ssfmax = sqrt( safmax ) / three
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ssfmin = sqrt( safmin ) / eps2
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c
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c compute the eigenvalues and eigenvectors of the tridiagonal
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c matrix.
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c
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c$$ if( icompz.eq.2 )
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c$$$ $ call dlaset( 'full', n, n, zero, one, z, ldz )
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c
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c *** New starting with version 2.5 ***
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c
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if ( icompz .eq. 2 ) then
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do 5 j = 1, n-1
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z(j) = zero
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5 continue
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z( n ) = one
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end if
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c *************************************
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c
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nmaxit = n*maxit
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jtot = 0
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c
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c determine where the matrix splits and choose ql or qr iteration
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c for each block, according to whether top or bottom diagonal
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c element is smaller.
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c
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l1 = 1
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nm1 = n - 1
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c
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10 continue
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if( l1.gt.n )
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$ go to 160
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if( l1.gt.1 )
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$ e( l1-1 ) = zero
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if( l1.le.nm1 ) then
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do 20 m = l1, nm1
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tst = abs( e( m ) )
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if( tst.eq.zero )
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$ go to 30
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if( tst.le.( sqrt( abs( d( m ) ) )*sqrt( abs( d( m+
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$ 1 ) ) ) )*eps ) then
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e( m ) = zero
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go to 30
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end if
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20 continue
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end if
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m = n
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c
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30 continue
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l = l1
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lsv = l
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lend = m
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lendsv = lend
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l1 = m + 1
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if( lend.eq.l )
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$ go to 10
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c
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c scale submatrix in rows and columns l to lend
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c
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anorm = dlanst( 'i', lend-l+1, d( l ), e( l ) )
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iscale = 0
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if( anorm.eq.zero )
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$ go to 10
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if( anorm.gt.ssfmax ) then
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iscale = 1
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call dlascl( 'g', 0, 0, anorm, ssfmax, lend-l+1, 1, d( l ), n,
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$ info )
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call dlascl( 'g', 0, 0, anorm, ssfmax, lend-l, 1, e( l ), n,
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$ info )
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else if( anorm.lt.ssfmin ) then
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iscale = 2
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call dlascl( 'g', 0, 0, anorm, ssfmin, lend-l+1, 1, d( l ), n,
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$ info )
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call dlascl( 'g', 0, 0, anorm, ssfmin, lend-l, 1, e( l ), n,
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$ info )
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end if
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c
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c choose between ql and qr iteration
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c
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if( abs( d( lend ) ).lt.abs( d( l ) ) ) then
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lend = lsv
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l = lendsv
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end if
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c
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if( lend.gt.l ) then
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c
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c ql iteration
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c
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c look for small subdiagonal element.
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c
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40 continue
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if( l.ne.lend ) then
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lendm1 = lend - 1
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do 50 m = l, lendm1
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tst = abs( e( m ) )**2
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if( tst.le.( eps2*abs( d( m ) ) )*abs( d( m+1 ) )+
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$ safmin )go to 60
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50 continue
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end if
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c
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m = lend
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c
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60 continue
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if( m.lt.lend )
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$ e( m ) = zero
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p = d( l )
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if( m.eq.l )
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$ go to 80
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c
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c if remaining matrix is 2-by-2, use dlae2 or dlaev2
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c to compute its eigensystem.
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c
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if( m.eq.l+1 ) then
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if( icompz.gt.0 ) then
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call dlaev2( d( l ), e( l ), d( l+1 ), rt1, rt2, c, s )
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work( l ) = c
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work( n-1+l ) = s
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c$$$ call dlasr( 'r', 'v', 'b', n, 2, work( l ),
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c$$$ $ work( n-1+l ), z( 1, l ), ldz )
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c
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c *** New starting with version 2.5 ***
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c
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tst = z(l+1)
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z(l+1) = c*tst - s*z(l)
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z(l) = s*tst + c*z(l)
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c *************************************
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else
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call dlae2( d( l ), e( l ), d( l+1 ), rt1, rt2 )
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end if
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d( l ) = rt1
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d( l+1 ) = rt2
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e( l ) = zero
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l = l + 2
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if( l.le.lend )
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$ go to 40
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go to 140
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end if
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c
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if( jtot.eq.nmaxit )
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$ go to 140
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jtot = jtot + 1
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c
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c form shift.
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c
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g = ( d( l+1 )-p ) / ( two*e( l ) )
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r = dlapy2( g, one )
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g = d( m ) - p + ( e( l ) / ( g+sign( r, g ) ) )
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c
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s = one
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c = one
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p = zero
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c
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c inner loop
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c
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mm1 = m - 1
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do 70 i = mm1, l, -1
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f = s*e( i )
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b = c*e( i )
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call dlartg( g, f, c, s, r )
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if( i.ne.m-1 )
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$ e( i+1 ) = r
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g = d( i+1 ) - p
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r = ( d( i )-g )*s + two*c*b
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p = s*r
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d( i+1 ) = g + p
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g = c*r - b
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c
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c if eigenvectors are desired, then save rotations.
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c
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if( icompz.gt.0 ) then
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work( i ) = c
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work( n-1+i ) = -s
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end if
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c
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70 continue
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c
|
||
|
|
c if eigenvectors are desired, then apply saved rotations.
|
||
|
|
c
|
||
|
|
if( icompz.gt.0 ) then
|
||
|
|
mm = m - l + 1
|
||
|
|
c$$$ call dlasr( 'r', 'v', 'b', n, mm, work( l ), work( n-1+l ),
|
||
|
|
c$$$ $ z( 1, l ), ldz )
|
||
|
|
c
|
||
|
|
c *** New starting with version 2.5 ***
|
||
|
|
c
|
||
|
|
call dlasr( 'r', 'v', 'b', 1, mm, work( l ),
|
||
|
|
& work( n-1+l ), z( l ), 1 )
|
||
|
|
c *************************************
|
||
|
|
end if
|
||
|
|
c
|
||
|
|
d( l ) = d( l ) - p
|
||
|
|
e( l ) = g
|
||
|
|
go to 40
|
||
|
|
c
|
||
|
|
c eigenvalue found.
|
||
|
|
c
|
||
|
|
80 continue
|
||
|
|
d( l ) = p
|
||
|
|
c
|
||
|
|
l = l + 1
|
||
|
|
if( l.le.lend )
|
||
|
|
$ go to 40
|
||
|
|
go to 140
|
||
|
|
c
|
||
|
|
else
|
||
|
|
c
|
||
|
|
c qr iteration
|
||
|
|
c
|
||
|
|
c look for small superdiagonal element.
|
||
|
|
c
|
||
|
|
90 continue
|
||
|
|
if( l.ne.lend ) then
|
||
|
|
lendp1 = lend + 1
|
||
|
|
do 100 m = l, lendp1, -1
|
||
|
|
tst = abs( e( m-1 ) )**2
|
||
|
|
if( tst.le.( eps2*abs( d( m ) ) )*abs( d( m-1 ) )+
|
||
|
|
$ safmin )go to 110
|
||
|
|
100 continue
|
||
|
|
end if
|
||
|
|
c
|
||
|
|
m = lend
|
||
|
|
c
|
||
|
|
110 continue
|
||
|
|
if( m.gt.lend )
|
||
|
|
$ e( m-1 ) = zero
|
||
|
|
p = d( l )
|
||
|
|
if( m.eq.l )
|
||
|
|
$ go to 130
|
||
|
|
c
|
||
|
|
c if remaining matrix is 2-by-2, use dlae2 or dlaev2
|
||
|
|
c to compute its eigensystem.
|
||
|
|
c
|
||
|
|
if( m.eq.l-1 ) then
|
||
|
|
if( icompz.gt.0 ) then
|
||
|
|
call dlaev2( d( l-1 ), e( l-1 ), d( l ), rt1, rt2, c, s )
|
||
|
|
c$$$ work( m ) = c
|
||
|
|
c$$$ work( n-1+m ) = s
|
||
|
|
c$$$ call dlasr( 'r', 'v', 'f', n, 2, work( m ),
|
||
|
|
c$$$ $ work( n-1+m ), z( 1, l-1 ), ldz )
|
||
|
|
c
|
||
|
|
c *** New starting with version 2.5 ***
|
||
|
|
c
|
||
|
|
tst = z(l)
|
||
|
|
z(l) = c*tst - s*z(l-1)
|
||
|
|
z(l-1) = s*tst + c*z(l-1)
|
||
|
|
c *************************************
|
||
|
|
else
|
||
|
|
call dlae2( d( l-1 ), e( l-1 ), d( l ), rt1, rt2 )
|
||
|
|
end if
|
||
|
|
d( l-1 ) = rt1
|
||
|
|
d( l ) = rt2
|
||
|
|
e( l-1 ) = zero
|
||
|
|
l = l - 2
|
||
|
|
if( l.ge.lend )
|
||
|
|
$ go to 90
|
||
|
|
go to 140
|
||
|
|
end if
|
||
|
|
c
|
||
|
|
if( jtot.eq.nmaxit )
|
||
|
|
$ go to 140
|
||
|
|
jtot = jtot + 1
|
||
|
|
c
|
||
|
|
c form shift.
|
||
|
|
c
|
||
|
|
g = ( d( l-1 )-p ) / ( two*e( l-1 ) )
|
||
|
|
r = dlapy2( g, one )
|
||
|
|
g = d( m ) - p + ( e( l-1 ) / ( g+sign( r, g ) ) )
|
||
|
|
c
|
||
|
|
s = one
|
||
|
|
c = one
|
||
|
|
p = zero
|
||
|
|
c
|
||
|
|
c inner loop
|
||
|
|
c
|
||
|
|
lm1 = l - 1
|
||
|
|
do 120 i = m, lm1
|
||
|
|
f = s*e( i )
|
||
|
|
b = c*e( i )
|
||
|
|
call dlartg( g, f, c, s, r )
|
||
|
|
if( i.ne.m )
|
||
|
|
$ e( i-1 ) = r
|
||
|
|
g = d( i ) - p
|
||
|
|
r = ( d( i+1 )-g )*s + two*c*b
|
||
|
|
p = s*r
|
||
|
|
d( i ) = g + p
|
||
|
|
g = c*r - b
|
||
|
|
c
|
||
|
|
c if eigenvectors are desired, then save rotations.
|
||
|
|
c
|
||
|
|
if( icompz.gt.0 ) then
|
||
|
|
work( i ) = c
|
||
|
|
work( n-1+i ) = s
|
||
|
|
end if
|
||
|
|
c
|
||
|
|
120 continue
|
||
|
|
c
|
||
|
|
c if eigenvectors are desired, then apply saved rotations.
|
||
|
|
c
|
||
|
|
if( icompz.gt.0 ) then
|
||
|
|
mm = l - m + 1
|
||
|
|
c$$$ call dlasr( 'r', 'v', 'f', n, mm, work( m ), work( n-1+m ),
|
||
|
|
c$$$ $ z( 1, m ), ldz )
|
||
|
|
c
|
||
|
|
c *** New starting with version 2.5 ***
|
||
|
|
c
|
||
|
|
call dlasr( 'r', 'v', 'f', 1, mm, work( m ), work( n-1+m ),
|
||
|
|
& z( m ), 1 )
|
||
|
|
c *************************************
|
||
|
|
end if
|
||
|
|
c
|
||
|
|
d( l ) = d( l ) - p
|
||
|
|
e( lm1 ) = g
|
||
|
|
go to 90
|
||
|
|
c
|
||
|
|
c eigenvalue found.
|
||
|
|
c
|
||
|
|
130 continue
|
||
|
|
d( l ) = p
|
||
|
|
c
|
||
|
|
l = l - 1
|
||
|
|
if( l.ge.lend )
|
||
|
|
$ go to 90
|
||
|
|
go to 140
|
||
|
|
c
|
||
|
|
end if
|
||
|
|
c
|
||
|
|
c undo scaling if necessary
|
||
|
|
c
|
||
|
|
140 continue
|
||
|
|
if( iscale.eq.1 ) then
|
||
|
|
call dlascl( 'g', 0, 0, ssfmax, anorm, lendsv-lsv+1, 1,
|
||
|
|
$ d( lsv ), n, info )
|
||
|
|
call dlascl( 'g', 0, 0, ssfmax, anorm, lendsv-lsv, 1, e( lsv ),
|
||
|
|
$ n, info )
|
||
|
|
else if( iscale.eq.2 ) then
|
||
|
|
call dlascl( 'g', 0, 0, ssfmin, anorm, lendsv-lsv+1, 1,
|
||
|
|
$ d( lsv ), n, info )
|
||
|
|
call dlascl( 'g', 0, 0, ssfmin, anorm, lendsv-lsv, 1, e( lsv ),
|
||
|
|
$ n, info )
|
||
|
|
end if
|
||
|
|
c
|
||
|
|
c check for no convergence to an eigenvalue after a total
|
||
|
|
c of n*maxit iterations.
|
||
|
|
c
|
||
|
|
if( jtot.lt.nmaxit )
|
||
|
|
$ go to 10
|
||
|
|
do 150 i = 1, n - 1
|
||
|
|
if( e( i ).ne.zero )
|
||
|
|
$ info = info + 1
|
||
|
|
150 continue
|
||
|
|
go to 190
|
||
|
|
c
|
||
|
|
c order eigenvalues and eigenvectors.
|
||
|
|
c
|
||
|
|
160 continue
|
||
|
|
if( icompz.eq.0 ) then
|
||
|
|
c
|
||
|
|
c use quick sort
|
||
|
|
c
|
||
|
|
call dlasrt( 'i', n, d, info )
|
||
|
|
c
|
||
|
|
else
|
||
|
|
c
|
||
|
|
c use selection sort to minimize swaps of eigenvectors
|
||
|
|
c
|
||
|
|
do 180 ii = 2, n
|
||
|
|
i = ii - 1
|
||
|
|
k = i
|
||
|
|
p = d( i )
|
||
|
|
do 170 j = ii, n
|
||
|
|
if( d( j ).lt.p ) then
|
||
|
|
k = j
|
||
|
|
p = d( j )
|
||
|
|
end if
|
||
|
|
170 continue
|
||
|
|
if( k.ne.i ) then
|
||
|
|
d( k ) = d( i )
|
||
|
|
d( i ) = p
|
||
|
|
c$$$ call dswap( n, z( 1, i ), 1, z( 1, k ), 1 )
|
||
|
|
c *** New starting with version 2.5 ***
|
||
|
|
c
|
||
|
|
p = z(k)
|
||
|
|
z(k) = z(i)
|
||
|
|
z(i) = p
|
||
|
|
c *************************************
|
||
|
|
end if
|
||
|
|
180 continue
|
||
|
|
end if
|
||
|
|
c
|
||
|
|
190 continue
|
||
|
|
return
|
||
|
|
c
|
||
|
|
c %---------------%
|
||
|
|
c | End of dstqrb |
|
||
|
|
c %---------------%
|
||
|
|
c
|
||
|
|
end
|