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opencv/3rdparty/lapack/slasd4.c

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/* slasd4.f -- translated by f2c (version 20061008).
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 "clapack.h"
/* Subroutine */ int slasd4_(integer *n, integer *i__, real *d__, real *z__,
real *delta, real *rho, real *sigma, real *work, integer *info)
{
/* System generated locals */
integer i__1;
real r__1;
/* Builtin functions */
double sqrt(doublereal);
/* Local variables */
real a, b, c__;
integer j;
real w, dd[3];
integer ii;
real dw, zz[3];
integer ip1;
real eta, phi, eps, tau, psi;
integer iim1, iip1;
real dphi, dpsi;
integer iter;
real temp, prew, sg2lb, sg2ub, temp1, temp2, dtiim, delsq, dtiip;
integer niter;
real dtisq;
logical swtch;
real dtnsq;
extern /* Subroutine */ int slaed6_(integer *, logical *, real *, real *,
real *, real *, real *, integer *);
real delsq2;
extern /* Subroutine */ int slasd5_(integer *, real *, real *, real *,
real *, real *, real *);
real dtnsq1;
logical swtch3;
extern doublereal slamch_(char *);
logical orgati;
real erretm, dtipsq, rhoinv;
/* -- LAPACK auxiliary routine (version 3.2) -- */
/* Univ. of Tennessee, Univ. of California Berkeley and NAG Ltd.. */
/* November 2006 */
/* .. Scalar Arguments .. */
/* .. */
/* .. Array Arguments .. */
/* .. */
/* Purpose */
/* ======= */
/* This subroutine computes the square root of the I-th updated */
/* eigenvalue of a positive symmetric rank-one modification to */
/* a positive diagonal matrix whose entries are given as the squares */
/* of the corresponding entries in the array d, and that */
/* 0 <= D(i) < D(j) for i < j */
/* and that RHO > 0. This is arranged by the calling routine, and is */
/* no loss in generality. The rank-one modified system is thus */
/* diag( D ) * diag( D ) + RHO * Z * Z_transpose. */
/* where we assume the Euclidean norm of Z is 1. */
/* The method consists of approximating the rational functions in the */
/* secular equation by simpler interpolating rational functions. */
/* Arguments */
/* ========= */
/* N (input) INTEGER */
/* The length of all arrays. */
/* I (input) INTEGER */
/* The index of the eigenvalue to be computed. 1 <= I <= N. */
/* D (input) REAL array, dimension ( N ) */
/* The original eigenvalues. It is assumed that they are in */
/* order, 0 <= D(I) < D(J) for I < J. */
/* Z (input) REAL array, dimension (N) */
/* The components of the updating vector. */
/* DELTA (output) REAL array, dimension (N) */
/* If N .ne. 1, DELTA contains (D(j) - sigma_I) in its j-th */
/* component. If N = 1, then DELTA(1) = 1. The vector DELTA */
/* contains the information necessary to construct the */
/* (singular) eigenvectors. */
/* RHO (input) REAL */
/* The scalar in the symmetric updating formula. */
/* SIGMA (output) REAL */
/* The computed sigma_I, the I-th updated eigenvalue. */
/* WORK (workspace) REAL array, dimension (N) */
/* If N .ne. 1, WORK contains (D(j) + sigma_I) in its j-th */
/* component. If N = 1, then WORK( 1 ) = 1. */
/* INFO (output) INTEGER */
/* = 0: successful exit */
/* > 0: if INFO = 1, the updating process failed. */
/* Internal Parameters */
/* =================== */
/* Logical variable ORGATI (origin-at-i?) is used for distinguishing */
/* whether D(i) or D(i+1) is treated as the origin. */
/* ORGATI = .true. origin at i */
/* ORGATI = .false. origin at i+1 */
/* Logical variable SWTCH3 (switch-for-3-poles?) is for noting */
/* if we are working with THREE poles! */
/* MAXIT is the maximum number of iterations allowed for each */
/* eigenvalue. */
/* Further Details */
/* =============== */
/* Based on contributions by */
/* Ren-Cang Li, Computer Science Division, University of California */
/* at Berkeley, USA */
/* ===================================================================== */
/* .. Parameters .. */
/* .. */
/* .. Local Scalars .. */
/* .. */
/* .. Local Arrays .. */
/* .. */
/* .. External Subroutines .. */
/* .. */
/* .. External Functions .. */
/* .. */
/* .. Intrinsic Functions .. */
/* .. */
/* .. Executable Statements .. */
/* Since this routine is called in an inner loop, we do no argument */
/* checking. */
/* Quick return for N=1 and 2. */
/* Parameter adjustments */
--work;
--delta;
--z__;
--d__;
/* Function Body */
*info = 0;
if (*n == 1) {
/* Presumably, I=1 upon entry */
*sigma = sqrt(d__[1] * d__[1] + *rho * z__[1] * z__[1]);
delta[1] = 1.f;
work[1] = 1.f;
return 0;
}
if (*n == 2) {
slasd5_(i__, &d__[1], &z__[1], &delta[1], rho, sigma, &work[1]);
return 0;
}
/* Compute machine epsilon */
eps = slamch_("Epsilon");
rhoinv = 1.f / *rho;
/* The case I = N */
if (*i__ == *n) {
/* Initialize some basic variables */
ii = *n - 1;
niter = 1;
/* Calculate initial guess */
temp = *rho / 2.f;
/* If ||Z||_2 is not one, then TEMP should be set to */
/* RHO * ||Z||_2^2 / TWO */
temp1 = temp / (d__[*n] + sqrt(d__[*n] * d__[*n] + temp));
i__1 = *n;
for (j = 1; j <= i__1; ++j) {
work[j] = d__[j] + d__[*n] + temp1;
delta[j] = d__[j] - d__[*n] - temp1;
/* L10: */
}
psi = 0.f;
i__1 = *n - 2;
for (j = 1; j <= i__1; ++j) {
psi += z__[j] * z__[j] / (delta[j] * work[j]);
/* L20: */
}
c__ = rhoinv + psi;
w = c__ + z__[ii] * z__[ii] / (delta[ii] * work[ii]) + z__[*n] * z__[*
n] / (delta[*n] * work[*n]);
if (w <= 0.f) {
temp1 = sqrt(d__[*n] * d__[*n] + *rho);
temp = z__[*n - 1] * z__[*n - 1] / ((d__[*n - 1] + temp1) * (d__[*
n] - d__[*n - 1] + *rho / (d__[*n] + temp1))) + z__[*n] *
z__[*n] / *rho;
/* The following TAU is to approximate */
/* SIGMA_n^2 - D( N )*D( N ) */
if (c__ <= temp) {
tau = *rho;
} else {
delsq = (d__[*n] - d__[*n - 1]) * (d__[*n] + d__[*n - 1]);
a = -c__ * delsq + z__[*n - 1] * z__[*n - 1] + z__[*n] * z__[*
n];
b = z__[*n] * z__[*n] * delsq;
if (a < 0.f) {
tau = b * 2.f / (sqrt(a * a + b * 4.f * c__) - a);
} else {
tau = (a + sqrt(a * a + b * 4.f * c__)) / (c__ * 2.f);
}
}
/* It can be proved that */
/* D(N)^2+RHO/2 <= SIGMA_n^2 < D(N)^2+TAU <= D(N)^2+RHO */
} else {
delsq = (d__[*n] - d__[*n - 1]) * (d__[*n] + d__[*n - 1]);
a = -c__ * delsq + z__[*n - 1] * z__[*n - 1] + z__[*n] * z__[*n];
b = z__[*n] * z__[*n] * delsq;
/* The following TAU is to approximate */
/* SIGMA_n^2 - D( N )*D( N ) */
if (a < 0.f) {
tau = b * 2.f / (sqrt(a * a + b * 4.f * c__) - a);
} else {
tau = (a + sqrt(a * a + b * 4.f * c__)) / (c__ * 2.f);
}
/* It can be proved that */
/* D(N)^2 < D(N)^2+TAU < SIGMA(N)^2 < D(N)^2+RHO/2 */
}
/* The following ETA is to approximate SIGMA_n - D( N ) */
eta = tau / (d__[*n] + sqrt(d__[*n] * d__[*n] + tau));
*sigma = d__[*n] + eta;
i__1 = *n;
for (j = 1; j <= i__1; ++j) {
delta[j] = d__[j] - d__[*i__] - eta;
work[j] = d__[j] + d__[*i__] + eta;
/* L30: */
}
/* Evaluate PSI and the derivative DPSI */
dpsi = 0.f;
psi = 0.f;
erretm = 0.f;
i__1 = ii;
for (j = 1; j <= i__1; ++j) {
temp = z__[j] / (delta[j] * work[j]);
psi += z__[j] * temp;
dpsi += temp * temp;
erretm += psi;
/* L40: */
}
erretm = dabs(erretm);
/* Evaluate PHI and the derivative DPHI */
temp = z__[*n] / (delta[*n] * work[*n]);
phi = z__[*n] * temp;
dphi = temp * temp;
erretm = (-phi - psi) * 8.f + erretm - phi + rhoinv + dabs(tau) * (
dpsi + dphi);
w = rhoinv + phi + psi;
/* Test for convergence */
if (dabs(w) <= eps * erretm) {
goto L240;
}
/* Calculate the new step */
++niter;
dtnsq1 = work[*n - 1] * delta[*n - 1];
dtnsq = work[*n] * delta[*n];
c__ = w - dtnsq1 * dpsi - dtnsq * dphi;
a = (dtnsq + dtnsq1) * w - dtnsq * dtnsq1 * (dpsi + dphi);
b = dtnsq * dtnsq1 * w;
if (c__ < 0.f) {
c__ = dabs(c__);
}
if (c__ == 0.f) {
eta = *rho - *sigma * *sigma;
} else if (a >= 0.f) {
eta = (a + sqrt((r__1 = a * a - b * 4.f * c__, dabs(r__1)))) / (
c__ * 2.f);
} else {
eta = b * 2.f / (a - sqrt((r__1 = a * a - b * 4.f * c__, dabs(
r__1))));
}
/* Note, eta should be positive if w is negative, and */
/* eta should be negative otherwise. However, */
/* if for some reason caused by roundoff, eta*w > 0, */
/* we simply use one Newton step instead. This way */
/* will guarantee eta*w < 0. */
if (w * eta > 0.f) {
eta = -w / (dpsi + dphi);
}
temp = eta - dtnsq;
if (temp > *rho) {
eta = *rho + dtnsq;
}
tau += eta;
eta /= *sigma + sqrt(eta + *sigma * *sigma);
i__1 = *n;
for (j = 1; j <= i__1; ++j) {
delta[j] -= eta;
work[j] += eta;
/* L50: */
}
*sigma += eta;
/* Evaluate PSI and the derivative DPSI */
dpsi = 0.f;
psi = 0.f;
erretm = 0.f;
i__1 = ii;
for (j = 1; j <= i__1; ++j) {
temp = z__[j] / (work[j] * delta[j]);
psi += z__[j] * temp;
dpsi += temp * temp;
erretm += psi;
/* L60: */
}
erretm = dabs(erretm);
/* Evaluate PHI and the derivative DPHI */
temp = z__[*n] / (work[*n] * delta[*n]);
phi = z__[*n] * temp;
dphi = temp * temp;
erretm = (-phi - psi) * 8.f + erretm - phi + rhoinv + dabs(tau) * (
dpsi + dphi);
w = rhoinv + phi + psi;
/* Main loop to update the values of the array DELTA */
iter = niter + 1;
for (niter = iter; niter <= 20; ++niter) {
/* Test for convergence */
if (dabs(w) <= eps * erretm) {
goto L240;
}
/* Calculate the new step */
dtnsq1 = work[*n - 1] * delta[*n - 1];
dtnsq = work[*n] * delta[*n];
c__ = w - dtnsq1 * dpsi - dtnsq * dphi;
a = (dtnsq + dtnsq1) * w - dtnsq1 * dtnsq * (dpsi + dphi);
b = dtnsq1 * dtnsq * w;
if (a >= 0.f) {
eta = (a + sqrt((r__1 = a * a - b * 4.f * c__, dabs(r__1)))) /
(c__ * 2.f);
} else {
eta = b * 2.f / (a - sqrt((r__1 = a * a - b * 4.f * c__, dabs(
r__1))));
}
/* Note, eta should be positive if w is negative, and */
/* eta should be negative otherwise. However, */
/* if for some reason caused by roundoff, eta*w > 0, */
/* we simply use one Newton step instead. This way */
/* will guarantee eta*w < 0. */
if (w * eta > 0.f) {
eta = -w / (dpsi + dphi);
}
temp = eta - dtnsq;
if (temp <= 0.f) {
eta /= 2.f;
}
tau += eta;
eta /= *sigma + sqrt(eta + *sigma * *sigma);
i__1 = *n;
for (j = 1; j <= i__1; ++j) {
delta[j] -= eta;
work[j] += eta;
/* L70: */
}
*sigma += eta;
/* Evaluate PSI and the derivative DPSI */
dpsi = 0.f;
psi = 0.f;
erretm = 0.f;
i__1 = ii;
for (j = 1; j <= i__1; ++j) {
temp = z__[j] / (work[j] * delta[j]);
psi += z__[j] * temp;
dpsi += temp * temp;
erretm += psi;
/* L80: */
}
erretm = dabs(erretm);
/* Evaluate PHI and the derivative DPHI */
temp = z__[*n] / (work[*n] * delta[*n]);
phi = z__[*n] * temp;
dphi = temp * temp;
erretm = (-phi - psi) * 8.f + erretm - phi + rhoinv + dabs(tau) *
(dpsi + dphi);
w = rhoinv + phi + psi;
/* L90: */
}
/* Return with INFO = 1, NITER = MAXIT and not converged */
*info = 1;
goto L240;
/* End for the case I = N */
} else {
/* The case for I < N */
niter = 1;
ip1 = *i__ + 1;
/* Calculate initial guess */
delsq = (d__[ip1] - d__[*i__]) * (d__[ip1] + d__[*i__]);
delsq2 = delsq / 2.f;
temp = delsq2 / (d__[*i__] + sqrt(d__[*i__] * d__[*i__] + delsq2));
i__1 = *n;
for (j = 1; j <= i__1; ++j) {
work[j] = d__[j] + d__[*i__] + temp;
delta[j] = d__[j] - d__[*i__] - temp;
/* L100: */
}
psi = 0.f;
i__1 = *i__ - 1;
for (j = 1; j <= i__1; ++j) {
psi += z__[j] * z__[j] / (work[j] * delta[j]);
/* L110: */
}
phi = 0.f;
i__1 = *i__ + 2;
for (j = *n; j >= i__1; --j) {
phi += z__[j] * z__[j] / (work[j] * delta[j]);
/* L120: */
}
c__ = rhoinv + psi + phi;
w = c__ + z__[*i__] * z__[*i__] / (work[*i__] * delta[*i__]) + z__[
ip1] * z__[ip1] / (work[ip1] * delta[ip1]);
if (w > 0.f) {
/* d(i)^2 < the ith sigma^2 < (d(i)^2+d(i+1)^2)/2 */
/* We choose d(i) as origin. */
orgati = TRUE_;
sg2lb = 0.f;
sg2ub = delsq2;
a = c__ * delsq + z__[*i__] * z__[*i__] + z__[ip1] * z__[ip1];
b = z__[*i__] * z__[*i__] * delsq;
if (a > 0.f) {
tau = b * 2.f / (a + sqrt((r__1 = a * a - b * 4.f * c__, dabs(
r__1))));
} else {
tau = (a - sqrt((r__1 = a * a - b * 4.f * c__, dabs(r__1)))) /
(c__ * 2.f);
}
/* TAU now is an estimation of SIGMA^2 - D( I )^2. The */
/* following, however, is the corresponding estimation of */
/* SIGMA - D( I ). */
eta = tau / (d__[*i__] + sqrt(d__[*i__] * d__[*i__] + tau));
} else {
/* (d(i)^2+d(i+1)^2)/2 <= the ith sigma^2 < d(i+1)^2/2 */
/* We choose d(i+1) as origin. */
orgati = FALSE_;
sg2lb = -delsq2;
sg2ub = 0.f;
a = c__ * delsq - z__[*i__] * z__[*i__] - z__[ip1] * z__[ip1];
b = z__[ip1] * z__[ip1] * delsq;
if (a < 0.f) {
tau = b * 2.f / (a - sqrt((r__1 = a * a + b * 4.f * c__, dabs(
r__1))));
} else {
tau = -(a + sqrt((r__1 = a * a + b * 4.f * c__, dabs(r__1))))
/ (c__ * 2.f);
}
/* TAU now is an estimation of SIGMA^2 - D( IP1 )^2. The */
/* following, however, is the corresponding estimation of */
/* SIGMA - D( IP1 ). */
eta = tau / (d__[ip1] + sqrt((r__1 = d__[ip1] * d__[ip1] + tau,
dabs(r__1))));
}
if (orgati) {
ii = *i__;
*sigma = d__[*i__] + eta;
i__1 = *n;
for (j = 1; j <= i__1; ++j) {
work[j] = d__[j] + d__[*i__] + eta;
delta[j] = d__[j] - d__[*i__] - eta;
/* L130: */
}
} else {
ii = *i__ + 1;
*sigma = d__[ip1] + eta;
i__1 = *n;
for (j = 1; j <= i__1; ++j) {
work[j] = d__[j] + d__[ip1] + eta;
delta[j] = d__[j] - d__[ip1] - eta;
/* L140: */
}
}
iim1 = ii - 1;
iip1 = ii + 1;
/* Evaluate PSI and the derivative DPSI */
dpsi = 0.f;
psi = 0.f;
erretm = 0.f;
i__1 = iim1;
for (j = 1; j <= i__1; ++j) {
temp = z__[j] / (work[j] * delta[j]);
psi += z__[j] * temp;
dpsi += temp * temp;
erretm += psi;
/* L150: */
}
erretm = dabs(erretm);
/* Evaluate PHI and the derivative DPHI */
dphi = 0.f;
phi = 0.f;
i__1 = iip1;
for (j = *n; j >= i__1; --j) {
temp = z__[j] / (work[j] * delta[j]);
phi += z__[j] * temp;
dphi += temp * temp;
erretm += phi;
/* L160: */
}
w = rhoinv + phi + psi;
/* W is the value of the secular function with */
/* its ii-th element removed. */
swtch3 = FALSE_;
if (orgati) {
if (w < 0.f) {
swtch3 = TRUE_;
}
} else {
if (w > 0.f) {
swtch3 = TRUE_;
}
}
if (ii == 1 || ii == *n) {
swtch3 = FALSE_;
}
temp = z__[ii] / (work[ii] * delta[ii]);
dw = dpsi + dphi + temp * temp;
temp = z__[ii] * temp;
w += temp;
erretm = (phi - psi) * 8.f + erretm + rhoinv * 2.f + dabs(temp) * 3.f
+ dabs(tau) * dw;
/* Test for convergence */
if (dabs(w) <= eps * erretm) {
goto L240;
}
if (w <= 0.f) {
sg2lb = dmax(sg2lb,tau);
} else {
sg2ub = dmin(sg2ub,tau);
}
/* Calculate the new step */
++niter;
if (! swtch3) {
dtipsq = work[ip1] * delta[ip1];
dtisq = work[*i__] * delta[*i__];
if (orgati) {
/* Computing 2nd power */
r__1 = z__[*i__] / dtisq;
c__ = w - dtipsq * dw + delsq * (r__1 * r__1);
} else {
/* Computing 2nd power */
r__1 = z__[ip1] / dtipsq;
c__ = w - dtisq * dw - delsq * (r__1 * r__1);
}
a = (dtipsq + dtisq) * w - dtipsq * dtisq * dw;
b = dtipsq * dtisq * w;
if (c__ == 0.f) {
if (a == 0.f) {
if (orgati) {
a = z__[*i__] * z__[*i__] + dtipsq * dtipsq * (dpsi +
dphi);
} else {
a = z__[ip1] * z__[ip1] + dtisq * dtisq * (dpsi +
dphi);
}
}
eta = b / a;
} else if (a <= 0.f) {
eta = (a - sqrt((r__1 = a * a - b * 4.f * c__, dabs(r__1)))) /
(c__ * 2.f);
} else {
eta = b * 2.f / (a + sqrt((r__1 = a * a - b * 4.f * c__, dabs(
r__1))));
}
} else {
/* Interpolation using THREE most relevant poles */
dtiim = work[iim1] * delta[iim1];
dtiip = work[iip1] * delta[iip1];
temp = rhoinv + psi + phi;
if (orgati) {
temp1 = z__[iim1] / dtiim;
temp1 *= temp1;
c__ = temp - dtiip * (dpsi + dphi) - (d__[iim1] - d__[iip1]) *
(d__[iim1] + d__[iip1]) * temp1;
zz[0] = z__[iim1] * z__[iim1];
if (dpsi < temp1) {
zz[2] = dtiip * dtiip * dphi;
} else {
zz[2] = dtiip * dtiip * (dpsi - temp1 + dphi);
}
} else {
temp1 = z__[iip1] / dtiip;
temp1 *= temp1;
c__ = temp - dtiim * (dpsi + dphi) - (d__[iip1] - d__[iim1]) *
(d__[iim1] + d__[iip1]) * temp1;
if (dphi < temp1) {
zz[0] = dtiim * dtiim * dpsi;
} else {
zz[0] = dtiim * dtiim * (dpsi + (dphi - temp1));
}
zz[2] = z__[iip1] * z__[iip1];
}
zz[1] = z__[ii] * z__[ii];
dd[0] = dtiim;
dd[1] = delta[ii] * work[ii];
dd[2] = dtiip;
slaed6_(&niter, &orgati, &c__, dd, zz, &w, &eta, info);
if (*info != 0) {
goto L240;
}
}
/* Note, eta should be positive if w is negative, and */
/* eta should be negative otherwise. However, */
/* if for some reason caused by roundoff, eta*w > 0, */
/* we simply use one Newton step instead. This way */
/* will guarantee eta*w < 0. */
if (w * eta >= 0.f) {
eta = -w / dw;
}
if (orgati) {
temp1 = work[*i__] * delta[*i__];
temp = eta - temp1;
} else {
temp1 = work[ip1] * delta[ip1];
temp = eta - temp1;
}
if (temp > sg2ub || temp < sg2lb) {
if (w < 0.f) {
eta = (sg2ub - tau) / 2.f;
} else {
eta = (sg2lb - tau) / 2.f;
}
}
tau += eta;
eta /= *sigma + sqrt(*sigma * *sigma + eta);
prew = w;
*sigma += eta;
i__1 = *n;
for (j = 1; j <= i__1; ++j) {
work[j] += eta;
delta[j] -= eta;
/* L170: */
}
/* Evaluate PSI and the derivative DPSI */
dpsi = 0.f;
psi = 0.f;
erretm = 0.f;
i__1 = iim1;
for (j = 1; j <= i__1; ++j) {
temp = z__[j] / (work[j] * delta[j]);
psi += z__[j] * temp;
dpsi += temp * temp;
erretm += psi;
/* L180: */
}
erretm = dabs(erretm);
/* Evaluate PHI and the derivative DPHI */
dphi = 0.f;
phi = 0.f;
i__1 = iip1;
for (j = *n; j >= i__1; --j) {
temp = z__[j] / (work[j] * delta[j]);
phi += z__[j] * temp;
dphi += temp * temp;
erretm += phi;
/* L190: */
}
temp = z__[ii] / (work[ii] * delta[ii]);
dw = dpsi + dphi + temp * temp;
temp = z__[ii] * temp;
w = rhoinv + phi + psi + temp;
erretm = (phi - psi) * 8.f + erretm + rhoinv * 2.f + dabs(temp) * 3.f
+ dabs(tau) * dw;
if (w <= 0.f) {
sg2lb = dmax(sg2lb,tau);
} else {
sg2ub = dmin(sg2ub,tau);
}
swtch = FALSE_;
if (orgati) {
if (-w > dabs(prew) / 10.f) {
swtch = TRUE_;
}
} else {
if (w > dabs(prew) / 10.f) {
swtch = TRUE_;
}
}
/* Main loop to update the values of the array DELTA and WORK */
iter = niter + 1;
for (niter = iter; niter <= 20; ++niter) {
/* Test for convergence */
if (dabs(w) <= eps * erretm) {
goto L240;
}
/* Calculate the new step */
if (! swtch3) {
dtipsq = work[ip1] * delta[ip1];
dtisq = work[*i__] * delta[*i__];
if (! swtch) {
if (orgati) {
/* Computing 2nd power */
r__1 = z__[*i__] / dtisq;
c__ = w - dtipsq * dw + delsq * (r__1 * r__1);
} else {
/* Computing 2nd power */
r__1 = z__[ip1] / dtipsq;
c__ = w - dtisq * dw - delsq * (r__1 * r__1);
}
} else {
temp = z__[ii] / (work[ii] * delta[ii]);
if (orgati) {
dpsi += temp * temp;
} else {
dphi += temp * temp;
}
c__ = w - dtisq * dpsi - dtipsq * dphi;
}
a = (dtipsq + dtisq) * w - dtipsq * dtisq * dw;
b = dtipsq * dtisq * w;
if (c__ == 0.f) {
if (a == 0.f) {
if (! swtch) {
if (orgati) {
a = z__[*i__] * z__[*i__] + dtipsq * dtipsq *
(dpsi + dphi);
} else {
a = z__[ip1] * z__[ip1] + dtisq * dtisq * (
dpsi + dphi);
}
} else {
a = dtisq * dtisq * dpsi + dtipsq * dtipsq * dphi;
}
}
eta = b / a;
} else if (a <= 0.f) {
eta = (a - sqrt((r__1 = a * a - b * 4.f * c__, dabs(r__1))
)) / (c__ * 2.f);
} else {
eta = b * 2.f / (a + sqrt((r__1 = a * a - b * 4.f * c__,
dabs(r__1))));
}
} else {
/* Interpolation using THREE most relevant poles */
dtiim = work[iim1] * delta[iim1];
dtiip = work[iip1] * delta[iip1];
temp = rhoinv + psi + phi;
if (swtch) {
c__ = temp - dtiim * dpsi - dtiip * dphi;
zz[0] = dtiim * dtiim * dpsi;
zz[2] = dtiip * dtiip * dphi;
} else {
if (orgati) {
temp1 = z__[iim1] / dtiim;
temp1 *= temp1;
temp2 = (d__[iim1] - d__[iip1]) * (d__[iim1] + d__[
iip1]) * temp1;
c__ = temp - dtiip * (dpsi + dphi) - temp2;
zz[0] = z__[iim1] * z__[iim1];
if (dpsi < temp1) {
zz[2] = dtiip * dtiip * dphi;
} else {
zz[2] = dtiip * dtiip * (dpsi - temp1 + dphi);
}
} else {
temp1 = z__[iip1] / dtiip;
temp1 *= temp1;
temp2 = (d__[iip1] - d__[iim1]) * (d__[iim1] + d__[
iip1]) * temp1;
c__ = temp - dtiim * (dpsi + dphi) - temp2;
if (dphi < temp1) {
zz[0] = dtiim * dtiim * dpsi;
} else {
zz[0] = dtiim * dtiim * (dpsi + (dphi - temp1));
}
zz[2] = z__[iip1] * z__[iip1];
}
}
dd[0] = dtiim;
dd[1] = delta[ii] * work[ii];
dd[2] = dtiip;
slaed6_(&niter, &orgati, &c__, dd, zz, &w, &eta, info);
if (*info != 0) {
goto L240;
}
}
/* Note, eta should be positive if w is negative, and */
/* eta should be negative otherwise. However, */
/* if for some reason caused by roundoff, eta*w > 0, */
/* we simply use one Newton step instead. This way */
/* will guarantee eta*w < 0. */
if (w * eta >= 0.f) {
eta = -w / dw;
}
if (orgati) {
temp1 = work[*i__] * delta[*i__];
temp = eta - temp1;
} else {
temp1 = work[ip1] * delta[ip1];
temp = eta - temp1;
}
if (temp > sg2ub || temp < sg2lb) {
if (w < 0.f) {
eta = (sg2ub - tau) / 2.f;
} else {
eta = (sg2lb - tau) / 2.f;
}
}
tau += eta;
eta /= *sigma + sqrt(*sigma * *sigma + eta);
*sigma += eta;
i__1 = *n;
for (j = 1; j <= i__1; ++j) {
work[j] += eta;
delta[j] -= eta;
/* L200: */
}
prew = w;
/* Evaluate PSI and the derivative DPSI */
dpsi = 0.f;
psi = 0.f;
erretm = 0.f;
i__1 = iim1;
for (j = 1; j <= i__1; ++j) {
temp = z__[j] / (work[j] * delta[j]);
psi += z__[j] * temp;
dpsi += temp * temp;
erretm += psi;
/* L210: */
}
erretm = dabs(erretm);
/* Evaluate PHI and the derivative DPHI */
dphi = 0.f;
phi = 0.f;
i__1 = iip1;
for (j = *n; j >= i__1; --j) {
temp = z__[j] / (work[j] * delta[j]);
phi += z__[j] * temp;
dphi += temp * temp;
erretm += phi;
/* L220: */
}
temp = z__[ii] / (work[ii] * delta[ii]);
dw = dpsi + dphi + temp * temp;
temp = z__[ii] * temp;
w = rhoinv + phi + psi + temp;
erretm = (phi - psi) * 8.f + erretm + rhoinv * 2.f + dabs(temp) *
3.f + dabs(tau) * dw;
if (w * prew > 0.f && dabs(w) > dabs(prew) / 10.f) {
swtch = ! swtch;
}
if (w <= 0.f) {
sg2lb = dmax(sg2lb,tau);
} else {
sg2ub = dmin(sg2ub,tau);
}
/* L230: */
}
/* Return with INFO = 1, NITER = MAXIT and not converged */
*info = 1;
}
L240:
return 0;
/* End of SLASD4 */
} /* slasd4_ */