#include "blaswrap.h" /* -- translated by f2c (version 19990503). You must link the resulting object file with the libraries: -lf2c -lm (in that order) */ #include "f2c.h" /* Common Block Declarations */ struct { doublereal ops, itcnt; } latime_; #define latime_1 latime_ /* Subroutine */ int dlar1v_(integer *n, integer *b1, integer *bn, doublereal *sigma, doublereal *d__, doublereal *l, doublereal *ld, doublereal * lld, doublereal *gersch, doublereal *z__, doublereal *ztz, doublereal *mingma, integer *r__, integer *isuppz, doublereal *work) { /* System generated locals */ integer i__1; doublereal d__1, d__2; /* Local variables */ static integer indp, inds, from, i__, j; static doublereal s, dplus; static integer r1, r2; extern doublereal dlamch_(char *); static integer to; static logical sawnan; static integer indumn; static doublereal dminus, eps, tmp; /* -- LAPACK auxiliary routine (instru to count ops, version 3.0) -- Univ. of Tennessee, Univ. of California Berkeley, NAG Ltd., Courant Institute, Argonne National Lab, and Rice University June 30, 1999 Common block to return operation count Purpose ======= DLAR1V computes the (scaled) r-th column of the inverse of the sumbmatrix in rows B1 through BN of the tridiagonal matrix L D L^T - sigma I. The following steps accomplish this computation : (a) Stationary qd transform, L D L^T - sigma I = L(+) D(+) L(+)^T, (b) Progressive qd transform, L D L^T - sigma I = U(-) D(-) U(-)^T, (c) Computation of the diagonal elements of the inverse of L D L^T - sigma I by combining the above transforms, and choosing r as the index where the diagonal of the inverse is (one of the) largest in magnitude. (d) Computation of the (scaled) r-th column of the inverse using the twisted factorization obtained by combining the top part of the the stationary and the bottom part of the progressive transform. Arguments ========= N (input) INTEGER The order of the matrix L D L^T. B1 (input) INTEGER First index of the submatrix of L D L^T. BN (input) INTEGER Last index of the submatrix of L D L^T. SIGMA (input) DOUBLE PRECISION The shift. Initially, when R = 0, SIGMA should be a good approximation to an eigenvalue of L D L^T. L (input) DOUBLE PRECISION array, dimension (N-1) The (n-1) subdiagonal elements of the unit bidiagonal matrix L, in elements 1 to N-1. D (input) DOUBLE PRECISION array, dimension (N) The n diagonal elements of the diagonal matrix D. LD (input) DOUBLE PRECISION array, dimension (N-1) The n-1 elements L(i)*D(i). LLD (input) DOUBLE PRECISION array, dimension (N-1) The n-1 elements L(i)*L(i)*D(i). GERSCH (input) DOUBLE PRECISION array, dimension (2*N) The n Gerschgorin intervals. These are used to restrict the initial search for R, when R is input as 0. Z (output) DOUBLE PRECISION array, dimension (N) The (scaled) r-th column of the inverse. Z(R) is returned to be 1. ZTZ (output) DOUBLE PRECISION The square of the norm of Z. MINGMA (output) DOUBLE PRECISION The reciprocal of the largest (in magnitude) diagonal element of the inverse of L D L^T - sigma I. R (input/output) INTEGER Initially, R should be input to be 0 and is then output as the index where the diagonal element of the inverse is largest in magnitude. In later iterations, this same value of R should be input. ISUPPZ (output) INTEGER array, dimension (2) The support of the vector in Z, i.e., the vector Z is nonzero only in elements ISUPPZ(1) through ISUPPZ( 2 ). WORK (workspace) DOUBLE PRECISION array, dimension (4*N) Further Details =============== Based on contributions by Inderjit Dhillon, IBM Almaden, USA Osni Marques, LBNL/NERSC, USA ===================================================================== Parameter adjustments */ --work; --isuppz; --z__; --gersch; --lld; --ld; --l; --d__; /* Function Body */ eps = dlamch_("Precision"); if (*r__ == 0) { /* Eliminate the top and bottom indices from the possible values of R where the desired eigenvector is largest in magnitude. */ r1 = *b1; i__1 = *bn; for (i__ = *b1; i__ <= i__1; ++i__) { if (*sigma >= gersch[(i__ << 1) - 1] || *sigma <= gersch[i__ * 2]) { r1 = i__; goto L20; } /* L10: */ } L20: r2 = *bn; i__1 = *b1; for (i__ = *bn; i__ >= i__1; --i__) { if (*sigma >= gersch[(i__ << 1) - 1] || *sigma <= gersch[i__ * 2]) { r2 = i__; goto L40; } /* L30: */ } L40: ; } else { r1 = *r__; r2 = *r__; } indumn = *n; inds = (*n << 1) + 1; indp = *n * 3 + 1; sawnan = FALSE_; /* Compute the stationary transform (using the differential form) untill the index R2 */ if (*b1 == 1) { work[inds] = 0.; } else { work[inds] = lld[*b1 - 1]; } latime_1.ops += 1.; s = work[inds] - *sigma; i__1 = r2 - 1; for (i__ = *b1; i__ <= i__1; ++i__) { latime_1.ops += 5.; dplus = d__[i__] + s; work[i__] = ld[i__] / dplus; work[inds + i__] = s * work[i__] * l[i__]; s = work[inds + i__] - *sigma; /* L50: */ } if (! (s > 0. || s < 1.)) { /* Run a slower version of the above loop if a NaN is detected */ sawnan = TRUE_; j = *b1 + 1; L60: if (work[inds + j] > 0. || work[inds + j] < 1.) { ++j; goto L60; } work[inds + j] = lld[j]; s = work[inds + j] - *sigma; i__1 = r2 - 1; for (i__ = j + 1; i__ <= i__1; ++i__) { latime_1.ops += 3.; dplus = d__[i__] + s; work[i__] = ld[i__] / dplus; if (work[i__] == 0.) { work[inds + i__] = lld[i__]; } else { latime_1.ops += 2.; work[inds + i__] = s * work[i__] * l[i__]; } s = work[inds + i__] - *sigma; /* L70: */ } } latime_1.ops += 1.; work[indp + *bn - 1] = d__[*bn] - *sigma; i__1 = r1; for (i__ = *bn - 1; i__ >= i__1; --i__) { latime_1.ops += 5.; dminus = lld[i__] + work[indp + i__]; tmp = d__[i__] / dminus; work[indumn + i__] = l[i__] * tmp; work[indp + i__ - 1] = work[indp + i__] * tmp - *sigma; /* L80: */ } tmp = work[indp + r1 - 1]; if (! (tmp > 0. || tmp < 1.)) { /* Run a slower version of the above loop if a NaN is detected */ sawnan = TRUE_; j = *bn - 3; L90: if (work[indp + j] > 0. || work[indp + j] < 1.) { --j; goto L90; } latime_1.ops += 1.; work[indp + j] = d__[j + 1] - *sigma; i__1 = r1; for (i__ = j; i__ >= i__1; --i__) { latime_1.ops += 3.; dminus = lld[i__] + work[indp + i__]; tmp = d__[i__] / dminus; work[indumn + i__] = l[i__] * tmp; if (tmp == 0.) { latime_1.ops += 1.; work[indp + i__ - 1] = d__[i__] - *sigma; } else { latime_1.ops += 2.; work[indp + i__ - 1] = work[indp + i__] * tmp - *sigma; } /* L100: */ } } /* Find the index (from R1 to R2) of the largest (in magnitude) diagonal element of the inverse */ *mingma = work[inds + r1 - 1] + work[indp + r1 - 1]; if (*mingma == 0.) { *mingma = eps * work[inds + r1 - 1]; } *r__ = r1; i__1 = r2 - 1; for (i__ = r1; i__ <= i__1; ++i__) { latime_1.ops += 1.; tmp = work[inds + i__] + work[indp + i__]; if (tmp == 0.) { latime_1.ops += 1.; tmp = eps * work[inds + i__]; } if (abs(tmp) < abs(*mingma)) { *mingma = tmp; *r__ = i__ + 1; } /* L110: */ } /* Compute the (scaled) r-th column of the inverse */ isuppz[1] = *b1; isuppz[2] = *bn; z__[*r__] = 1.; *ztz = 1.; if (! sawnan) { from = *r__ - 1; /* Computing MAX */ i__1 = *r__ - 32; to = max(i__1,*b1); L120: if (from >= *b1) { i__1 = to; for (i__ = from; i__ >= i__1; --i__) { latime_1.ops += 3.; z__[i__] = -(work[i__] * z__[i__ + 1]); *ztz += z__[i__] * z__[i__]; /* L130: */ } if ((d__1 = z__[to], abs(d__1)) <= eps && (d__2 = z__[to + 1], abs(d__2)) <= eps) { isuppz[1] = to + 2; } else { from = to - 1; /* Computing MAX */ i__1 = to - 32; to = max(i__1,*b1); goto L120; } } from = *r__ + 1; /* Computing MIN */ i__1 = *r__ + 32; to = min(i__1,*bn); L140: if (from <= *bn) { i__1 = to; for (i__ = from; i__ <= i__1; ++i__) { latime_1.ops += 3.; z__[i__] = -(work[indumn + i__ - 1] * z__[i__ - 1]); *ztz += z__[i__] * z__[i__]; /* L150: */ } if ((d__1 = z__[to], abs(d__1)) <= eps && (d__2 = z__[to - 1], abs(d__2)) <= eps) { isuppz[2] = to - 2; } else { from = to + 1; /* Computing MIN */ i__1 = to + 32; to = min(i__1,*bn); goto L140; } } } else { i__1 = *b1; for (i__ = *r__ - 1; i__ >= i__1; --i__) { if (z__[i__ + 1] == 0.) { latime_1.ops += 2.; z__[i__] = -(ld[i__ + 1] / ld[i__]) * z__[i__ + 2]; } else if ((d__1 = z__[i__ + 1], abs(d__1)) <= eps && (d__2 = z__[ i__ + 2], abs(d__2)) <= eps) { isuppz[1] = i__ + 3; goto L170; } else { latime_1.ops += 1.; z__[i__] = -(work[i__] * z__[i__ + 1]); } latime_1.ops += 2.; *ztz += z__[i__] * z__[i__]; /* L160: */ } L170: i__1 = *bn - 1; for (i__ = *r__; i__ <= i__1; ++i__) { if (z__[i__] == 0.) { latime_1.ops += 2.; z__[i__ + 1] = -(ld[i__ - 1] / ld[i__]) * z__[i__ - 1]; } else if ((d__1 = z__[i__], abs(d__1)) <= eps && (d__2 = z__[i__ - 1], abs(d__2)) <= eps) { isuppz[2] = i__ - 2; goto L190; } else { latime_1.ops += 1.; z__[i__ + 1] = -(work[indumn + i__] * z__[i__]); } latime_1.ops += 2.; *ztz += z__[i__ + 1] * z__[i__ + 1]; /* L180: */ } L190: ; } i__1 = isuppz[1] - 3; for (i__ = *b1; i__ <= i__1; ++i__) { z__[i__] = 0.; /* L200: */ } i__1 = *bn; for (i__ = isuppz[2] + 3; i__ <= i__1; ++i__) { z__[i__] = 0.; /* L210: */ } return 0; /* End of DLAR1V */ } /* dlar1v_ */ .