/* -- translated by f2c (version 20100827).
You must link the resulting object file with libf2c:
on Microsoft Windows system, link with libf2c.lib;
on Linux or Unix systems, link with .../path/to/libf2c.a -lm
or, if you install libf2c.a in a standard place, with -lf2c -lm
-- in that order, at the end of the command line, as in
cc *.o -lf2c -lm
Source for libf2c is in /netlib/f2c/libf2c.zip, e.g.,
http://www.netlib.org/f2c/libf2c.zip
*/
#include "f2c.h"
/* Table of constant values */
static integer c__0 = 0;
static integer c__1 = 1;
static doublereal c_b31 = 1.;
/* -----------------------------------------------------------------------
\BeginDoc
\Name: dstqrb
\Description:
Computes all eigenvalues and the last component of the eigenvectors
of a symmetric tridiagonal matrix using the implicit QL or QR method.
This is mostly a modification of the LAPACK routine dsteqr.
See Remarks.
\Usage:
call dstqrb
( N, D, E, Z, WORK, INFO )
\Arguments
N Integer. (INPUT)
The number of rows and columns in the matrix. N >= 0.
D Double precision array, dimension (N). (INPUT/OUTPUT)
On entry, D contains the diagonal elements of the
tridiagonal matrix.
On exit, D contains the eigenvalues, in ascending order.
If an error exit is made, the eigenvalues are correct
for indices 1,2,...,INFO-1, but they are unordered and
may not be the smallest eigenvalues of the matrix.
E Double precision array, dimension (N-1). (INPUT/OUTPUT)
On entry, E contains the subdiagonal elements of the
tridiagonal matrix in positions 1 through N-1.
On exit, E has been destroyed.
Z Double precision array, dimension (N). (OUTPUT)
On exit, Z contains the last row of the orthonormal
eigenvector matrix of the symmetric tridiagonal matrix.
If an error exit is made, Z contains the last row of the
eigenvector matrix associated with the stored eigenvalues.
WORK Double precision array, dimension (max(1,2*N-2)). (WORKSPACE)
Workspace used in accumulating the transformation for
computing the last components of the eigenvectors.
INFO Integer. (OUTPUT)
= 0: normal return.
< 0: if INFO = -i, the i-th argument had an illegal value.
> 0: if INFO = +i, the i-th eigenvalue has not converged
after a total of 30*N iterations.
\Remarks
1. None.
-----------------------------------------------------------------------
\BeginLib
\Local variables:
xxxxxx real
\Routines called:
daxpy Level 1 BLAS that computes a vector triad.
dcopy Level 1 BLAS that copies one vector to another.
dswap Level 1 BLAS that swaps the contents of two vectors.
lsame LAPACK character comparison routine.
dlae2 LAPACK routine that computes the eigenvalues of a 2-by-2
symmetric matrix.
dlaev2 LAPACK routine that eigendecomposition of a 2-by-2 symmetric
matrix.
dlamch LAPACK routine that determines machine constants.
dlanst LAPACK routine that computes the norm of a matrix.
dlapy2 LAPACK routine to compute sqrt(x**2+y**2) carefully.
dlartg LAPACK Givens rotation construction routine.
dlascl LAPACK routine for careful scaling of a matrix.
dlaset LAPACK matrix initialization routine.
dlasr LAPACK routine that applies an orthogonal transformation to
a matrix.
dlasrt LAPACK sorting routine.
dsteqr LAPACK routine that computes eigenvalues and eigenvectors
of a symmetric tridiagonal matrix.
xerbla LAPACK error handler routine.
\Authors
Danny Sorensen Phuong Vu
Richard Lehoucq CRPC / Rice University
Dept. of Computational & Houston, Texas
Applied Mathematics
Rice University
Houston, Texas
\SCCS Information: @(#)
FILE: stqrb.F SID: 2.5 DATE OF SID: 8/27/96 RELEASE: 2
\Remarks
1. Starting with version 2.5, this routine is a modified version
of LAPACK version 2.0 subroutine SSTEQR. No lines are deleted,
only commeted out and new lines inserted.
All lines commented out have "c$$$" at the beginning.
Note that the LAPACK version 1.0 subroutine SSTEQR contained
bugs.
\EndLib
-----------------------------------------------------------------------
Subroutine */ int igraphdstqrb_(integer *n, doublereal *d__, doublereal *e,
doublereal *z__, doublereal *work, integer *info)
{
/* System generated locals */
integer i__1, i__2;
doublereal d__1, d__2;
/* Builtin functions */
double sqrt(doublereal), d_sign(doublereal *, doublereal *);
/* Local variables */
doublereal b, c__, f, g;
integer i__, j, k, l, m;
doublereal p, r__, s;
integer l1, ii, mm, lm1, mm1, nm1;
doublereal rt1, rt2, eps;
integer lsv;
doublereal tst, eps2;
integer lend, jtot;
extern /* Subroutine */ int igraphdlae2_(doublereal *, doublereal *, doublereal
*, doublereal *, doublereal *), igraphdlasr_(char *, char *, char *,
integer *, integer *, doublereal *, doublereal *, doublereal *,
integer *);
doublereal anorm;
extern /* Subroutine */ int igraphdlaev2_(doublereal *, doublereal *,
doublereal *, doublereal *, doublereal *, doublereal *,
doublereal *);
integer lendm1, lendp1;
extern doublereal igraphdlapy2_(doublereal *, doublereal *), igraphdlamch_(char *);
integer iscale;
extern /* Subroutine */ int igraphdlascl_(char *, integer *, integer *,
doublereal *, doublereal *, integer *, integer *, doublereal *,
integer *, integer *);
doublereal safmin;
extern /* Subroutine */ int igraphdlartg_(doublereal *, doublereal *,
doublereal *, doublereal *, doublereal *);
doublereal safmax;
extern doublereal igraphdlanst_(char *, integer *, doublereal *, doublereal *);
extern /* Subroutine */ int igraphdlasrt_(char *, integer *, doublereal *,
integer *);
integer lendsv, nmaxit, icompz;
doublereal ssfmax, ssfmin;
/* %------------------%
| Scalar Arguments |
%------------------%
%-----------------%
| Array Arguments |
%-----------------%
test the input parameters.
Parameter adjustments */
--work;
--z__;
--e;
--d__;
/* Function Body */
*info = 0;
/* $$$ IF( LSAME( COMPZ, 'N' ) ) THEN
$$$ ICOMPZ = 0
$$$ ELSE IF( LSAME( COMPZ, 'V' ) ) THEN
$$$ ICOMPZ = 1
$$$ ELSE IF( LSAME( COMPZ, 'I' ) ) THEN
$$$ ICOMPZ = 2
$$$ ELSE
$$$ ICOMPZ = -1
$$$ END IF
$$$ IF( ICOMPZ.LT.0 ) THEN
$$$ INFO = -1
$$$ ELSE IF( N.LT.0 ) THEN
$$$ INFO = -2
$$$ ELSE IF( ( LDZ.LT.1 ) .OR. ( ICOMPZ.GT.0 .AND. LDZ.LT.MAX( 1,
$$$ $ N ) ) ) THEN
$$$ INFO = -6
$$$ END IF
$$$ IF( INFO.NE.0 ) THEN
$$$ CALL XERBLA( 'SSTEQR', -INFO )
$$$ RETURN
$$$ END IF
*** New starting with version 2.5 *** */
icompz = 2;
/* *************************************
quick return if possible */
if (*n == 0) {
return 0;
}
if (*n == 1) {
if (icompz == 2) {
z__[1] = 1.;
}
return 0;
}
/* determine the unit roundoff and over/underflow thresholds. */
eps = igraphdlamch_("e");
/* Computing 2nd power */
d__1 = eps;
eps2 = d__1 * d__1;
safmin = igraphdlamch_("s");
safmax = 1. / safmin;
ssfmax = sqrt(safmax) / 3.;
ssfmin = sqrt(safmin) / eps2;
/* compute the eigenvalues and eigenvectors of the tridiagonal
matrix.
$$ if( icompz.eq.2 )
$$$ $ call dlaset( 'full', n, n, zero, one, z, ldz )
*** New starting with version 2.5 *** */
if (icompz == 2) {
i__1 = *n - 1;
for (j = 1; j <= i__1; ++j) {
z__[j] = 0.;
/* L5: */
}
z__[*n] = 1.;
}
/* ************************************* */
nmaxit = *n * 30;
jtot = 0;
/* determine where the matrix splits and choose ql or qr iteration
for each block, according to whether top or bottom diagonal
element is smaller. */
l1 = 1;
nm1 = *n - 1;
L10:
if (l1 > *n) {
goto L160;
}
if (l1 > 1) {
e[l1 - 1] = 0.;
}
if (l1 <= nm1) {
i__1 = nm1;
for (m = l1; m <= i__1; ++m) {
tst = (d__1 = e[m], abs(d__1));
if (tst == 0.) {
goto L30;
}
if (tst <= sqrt((d__1 = d__[m], abs(d__1))) * sqrt((d__2 = d__[m
+ 1], abs(d__2))) * eps) {
e[m] = 0.;
goto L30;
}
/* L20: */
}
}
m = *n;
L30:
l = l1;
lsv = l;
lend = m;
lendsv = lend;
l1 = m + 1;
if (lend == l) {
goto L10;
}
/* scale submatrix in rows and columns l to lend */
i__1 = lend - l + 1;
anorm = igraphdlanst_("i", &i__1, &d__[l], &e[l]);
iscale = 0;
if (anorm == 0.) {
goto L10;
}
if (anorm > ssfmax) {
iscale = 1;
i__1 = lend - l + 1;
igraphdlascl_("g", &c__0, &c__0, &anorm, &ssfmax, &i__1, &c__1, &d__[l], n,
info);
i__1 = lend - l;
igraphdlascl_("g", &c__0, &c__0, &anorm, &ssfmax, &i__1, &c__1, &e[l], n,
info);
} else if (anorm < ssfmin) {
iscale = 2;
i__1 = lend - l + 1;
igraphdlascl_("g", &c__0, &c__0, &anorm, &ssfmin, &i__1, &c__1, &d__[l], n,
info);
i__1 = lend - l;
igraphdlascl_("g", &c__0, &c__0, &anorm, &ssfmin, &i__1, &c__1, &e[l], n,
info);
}
/* choose between ql and qr iteration */
if ((d__1 = d__[lend], abs(d__1)) < (d__2 = d__[l], abs(d__2))) {
lend = lsv;
l = lendsv;
}
if (lend > l) {
/* ql iteration
look for small subdiagonal element. */
L40:
if (l != lend) {
lendm1 = lend - 1;
i__1 = lendm1;
for (m = l; m <= i__1; ++m) {
/* Computing 2nd power */
d__2 = (d__1 = e[m], abs(d__1));
tst = d__2 * d__2;
if (tst <= eps2 * (d__1 = d__[m], abs(d__1)) * (d__2 = d__[m
+ 1], abs(d__2)) + safmin) {
goto L60;
}
/* L50: */
}
}
m = lend;
L60:
if (m < lend) {
e[m] = 0.;
}
p = d__[l];
if (m == l) {
goto L80;
}
/* if remaining matrix is 2-by-2, use dlae2 or dlaev2
to compute its eigensystem. */
if (m == l + 1) {
if (icompz > 0) {
igraphdlaev2_(&d__[l], &e[l], &d__[l + 1], &rt1, &rt2, &c__, &s);
work[l] = c__;
work[*n - 1 + l] = s;
/* $$$ call dlasr( 'r', 'v', 'b', n, 2, work( l ),
$$$ $ work( n-1+l ), z( 1, l ), ldz )
*** New starting with version 2.5 *** */
tst = z__[l + 1];
z__[l + 1] = c__ * tst - s * z__[l];
z__[l] = s * tst + c__ * z__[l];
/* ************************************* */
} else {
igraphdlae2_(&d__[l], &e[l], &d__[l + 1], &rt1, &rt2);
}
d__[l] = rt1;
d__[l + 1] = rt2;
e[l] = 0.;
l += 2;
if (l <= lend) {
goto L40;
}
goto L140;
}
if (jtot == nmaxit) {
goto L140;
}
++jtot;
/* form shift. */
g = (d__[l + 1] - p) / (e[l] * 2.);
r__ = igraphdlapy2_(&g, &c_b31);
g = d__[m] - p + e[l] / (g + d_sign(&r__, &g));
s = 1.;
c__ = 1.;
p = 0.;
/* inner loop */
mm1 = m - 1;
i__1 = l;
for (i__ = mm1; i__ >= i__1; --i__) {
f = s * e[i__];
b = c__ * e[i__];
igraphdlartg_(&g, &f, &c__, &s, &r__);
if (i__ != m - 1) {
e[i__ + 1] = r__;
}
g = d__[i__ + 1] - p;
r__ = (d__[i__] - g) * s + c__ * 2. * b;
p = s * r__;
d__[i__ + 1] = g + p;
g = c__ * r__ - b;
/* if eigenvectors are desired, then save rotations. */
if (icompz > 0) {
work[i__] = c__;
work[*n - 1 + i__] = -s;
}
/* L70: */
}
/* if eigenvectors are desired, then apply saved rotations. */
if (icompz > 0) {
mm = m - l + 1;
/* $$$ call dlasr( 'r', 'v', 'b', n, mm, work( l ), work( n-1+l ),
$$$ $ z( 1, l ), ldz )
*** New starting with version 2.5 *** */
igraphdlasr_("r", "v", "b", &c__1, &mm, &work[l], &work[*n - 1 + l], &
z__[l], &c__1);
/* ************************************* */
}
d__[l] -= p;
e[l] = g;
goto L40;
/* eigenvalue found. */
L80:
d__[l] = p;
++l;
if (l <= lend) {
goto L40;
}
goto L140;
} else {
/* qr iteration
look for small superdiagonal element. */
L90:
if (l != lend) {
lendp1 = lend + 1;
i__1 = lendp1;
for (m = l; m >= i__1; --m) {
/* Computing 2nd power */
d__2 = (d__1 = e[m - 1], abs(d__1));
tst = d__2 * d__2;
if (tst <= eps2 * (d__1 = d__[m], abs(d__1)) * (d__2 = d__[m
- 1], abs(d__2)) + safmin) {
goto L110;
}
/* L100: */
}
}
m = lend;
L110:
if (m > lend) {
e[m - 1] = 0.;
}
p = d__[l];
if (m == l) {
goto L130;
}
/* if remaining matrix is 2-by-2, use dlae2 or dlaev2
to compute its eigensystem. */
if (m == l - 1) {
if (icompz > 0) {
igraphdlaev2_(&d__[l - 1], &e[l - 1], &d__[l], &rt1, &rt2, &c__, &s)
;
/* $$$ work( m ) = c
$$$ work( n-1+m ) = s
$$$ call dlasr( 'r', 'v', 'f', n, 2, work( m ),
$$$ $ work( n-1+m ), z( 1, l-1 ), ldz )
*** New starting with version 2.5 *** */
tst = z__[l];
z__[l] = c__ * tst - s * z__[l - 1];
z__[l - 1] = s * tst + c__ * z__[l - 1];
/* ************************************* */
} else {
igraphdlae2_(&d__[l - 1], &e[l - 1], &d__[l], &rt1, &rt2);
}
d__[l - 1] = rt1;
d__[l] = rt2;
e[l - 1] = 0.;
l += -2;
if (l >= lend) {
goto L90;
}
goto L140;
}
if (jtot == nmaxit) {
goto L140;
}
++jtot;
/* form shift. */
g = (d__[l - 1] - p) / (e[l - 1] * 2.);
r__ = igraphdlapy2_(&g, &c_b31);
g = d__[m] - p + e[l - 1] / (g + d_sign(&r__, &g));
s = 1.;
c__ = 1.;
p = 0.;
/* inner loop */
lm1 = l - 1;
i__1 = lm1;
for (i__ = m; i__ <= i__1; ++i__) {
f = s * e[i__];
b = c__ * e[i__];
igraphdlartg_(&g, &f, &c__, &s, &r__);
if (i__ != m) {
e[i__ - 1] = r__;
}
g = d__[i__] - p;
r__ = (d__[i__ + 1] - g) * s + c__ * 2. * b;
p = s * r__;
d__[i__] = g + p;
g = c__ * r__ - b;
/* if eigenvectors are desired, then save rotations. */
if (icompz > 0) {
work[i__] = c__;
work[*n - 1 + i__] = s;
}
/* L120: */
}
/* if eigenvectors are desired, then apply saved rotations. */
if (icompz > 0) {
mm = l - m + 1;
/* $$$ call dlasr( 'r', 'v', 'f', n, mm, work( m ), work( n-1+m ),
$$$ $ z( 1, m ), ldz )
*** New starting with version 2.5 *** */
igraphdlasr_("r", "v", "f", &c__1, &mm, &work[m], &work[*n - 1 + m], &
z__[m], &c__1);
/* ************************************* */
}
d__[l] -= p;
e[lm1] = g;
goto L90;
/* eigenvalue found. */
L130:
d__[l] = p;
--l;
if (l >= lend) {
goto L90;
}
goto L140;
}
/* undo scaling if necessary */
L140:
if (iscale == 1) {
i__1 = lendsv - lsv + 1;
igraphdlascl_("g", &c__0, &c__0, &ssfmax, &anorm, &i__1, &c__1, &d__[lsv],
n, info);
i__1 = lendsv - lsv;
igraphdlascl_("g", &c__0, &c__0, &ssfmax, &anorm, &i__1, &c__1, &e[lsv], n,
info);
} else if (iscale == 2) {
i__1 = lendsv - lsv + 1;
igraphdlascl_("g", &c__0, &c__0, &ssfmin, &anorm, &i__1, &c__1, &d__[lsv],
n, info);
i__1 = lendsv - lsv;
igraphdlascl_("g", &c__0, &c__0, &ssfmin, &anorm, &i__1, &c__1, &e[lsv], n,
info);
}
/* check for no convergence to an eigenvalue after a total
of n*maxit iterations. */
if (jtot < nmaxit) {
goto L10;
}
i__1 = *n - 1;
for (i__ = 1; i__ <= i__1; ++i__) {
if (e[i__] != 0.) {
++(*info);
}
/* L150: */
}
goto L190;
/* order eigenvalues and eigenvectors. */
L160:
if (icompz == 0) {
/* use quick sort */
igraphdlasrt_("i", n, &d__[1], info);
} else {
/* use selection sort to minimize swaps of eigenvectors */
i__1 = *n;
for (ii = 2; ii <= i__1; ++ii) {
i__ = ii - 1;
k = i__;
p = d__[i__];
i__2 = *n;
for (j = ii; j <= i__2; ++j) {
if (d__[j] < p) {
k = j;
p = d__[j];
}
/* L170: */
}
if (k != i__) {
d__[k] = d__[i__];
d__[i__] = p;
/* $$$ call dswap( n, z( 1, i ), 1, z( 1, k ), 1 )
*** New starting with version 2.5 *** */
p = z__[k];
z__[k] = z__[i__];
z__[i__] = p;
/* ************************************* */
}
/* L180: */
}
}
L190:
return 0;
/* %---------------%
| End of dstqrb |
%---------------% */
} /* igraphdstqrb_ */