/* 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_ */