123456789101112131415161718192021222324252627282930313233343536373839404142434445464748495051525354555657585960616263646566676869707172737475767778798081828384858687888990919293949596979899100101102103104105106107108109110111112113114115116117118119120121122123124125126127128129130131132133134135136137138139140141142143144145146147148149150151152153154155156157 |
- /* dlarra.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 "f2c.h"
- #include "blaswrap.h"
- /* Subroutine */ int dlarra_(integer *n, doublereal *d__, doublereal *e,
- doublereal *e2, doublereal *spltol, doublereal *tnrm, integer *nsplit,
- integer *isplit, integer *info)
- {
- /* System generated locals */
- integer i__1;
- doublereal d__1, d__2;
- /* Builtin functions */
- double sqrt(doublereal);
- /* Local variables */
- integer i__;
- doublereal tmp1, eabs;
- /* -- LAPACK auxiliary routine (version 3.2) -- */
- /* Univ. of Tennessee, Univ. of California Berkeley and NAG Ltd.. */
- /* November 2006 */
- /* .. Scalar Arguments .. */
- /* .. */
- /* .. Array Arguments .. */
- /* .. */
- /* Purpose */
- /* ======= */
- /* Compute the splitting points with threshold SPLTOL. */
- /* DLARRA sets any "small" off-diagonal elements to zero. */
- /* Arguments */
- /* ========= */
- /* N (input) INTEGER */
- /* The order of the matrix. N > 0. */
- /* D (input) DOUBLE PRECISION array, dimension (N) */
- /* On entry, the N diagonal elements of the tridiagonal */
- /* matrix T. */
- /* E (input/output) DOUBLE PRECISION array, dimension (N) */
- /* On entry, the first (N-1) entries contain the subdiagonal */
- /* elements of the tridiagonal matrix T; E(N) need not be set. */
- /* On exit, the entries E( ISPLIT( I ) ), 1 <= I <= NSPLIT, */
- /* are set to zero, the other entries of E are untouched. */
- /* E2 (input/output) DOUBLE PRECISION array, dimension (N) */
- /* On entry, the first (N-1) entries contain the SQUARES of the */
- /* subdiagonal elements of the tridiagonal matrix T; */
- /* E2(N) need not be set. */
- /* On exit, the entries E2( ISPLIT( I ) ), */
- /* 1 <= I <= NSPLIT, have been set to zero */
- /* SPLTOL (input) DOUBLE PRECISION */
- /* The threshold for splitting. Two criteria can be used: */
- /* SPLTOL<0 : criterion based on absolute off-diagonal value */
- /* SPLTOL>0 : criterion that preserves relative accuracy */
- /* TNRM (input) DOUBLE PRECISION */
- /* The norm of the matrix. */
- /* NSPLIT (output) INTEGER */
- /* The number of blocks T splits into. 1 <= NSPLIT <= N. */
- /* ISPLIT (output) INTEGER array, dimension (N) */
- /* The splitting points, at which T breaks up into blocks. */
- /* The first block consists of rows/columns 1 to ISPLIT(1), */
- /* the second of rows/columns ISPLIT(1)+1 through ISPLIT(2), */
- /* etc., and the NSPLIT-th consists of rows/columns */
- /* ISPLIT(NSPLIT-1)+1 through ISPLIT(NSPLIT)=N. */
- /* INFO (output) INTEGER */
- /* = 0: successful exit */
- /* Further Details */
- /* =============== */
- /* Based on contributions by */
- /* Beresford Parlett, University of California, Berkeley, USA */
- /* Jim Demmel, University of California, Berkeley, USA */
- /* Inderjit Dhillon, University of Texas, Austin, USA */
- /* Osni Marques, LBNL/NERSC, USA */
- /* Christof Voemel, University of California, Berkeley, USA */
- /* ===================================================================== */
- /* .. Parameters .. */
- /* .. */
- /* .. Local Scalars .. */
- /* .. */
- /* .. Intrinsic Functions .. */
- /* .. */
- /* .. Executable Statements .. */
- /* Parameter adjustments */
- --isplit;
- --e2;
- --e;
- --d__;
- /* Function Body */
- *info = 0;
- /* Compute splitting points */
- *nsplit = 1;
- if (*spltol < 0.) {
- /* Criterion based on absolute off-diagonal value */
- tmp1 = abs(*spltol) * *tnrm;
- i__1 = *n - 1;
- for (i__ = 1; i__ <= i__1; ++i__) {
- eabs = (d__1 = e[i__], abs(d__1));
- if (eabs <= tmp1) {
- e[i__] = 0.;
- e2[i__] = 0.;
- isplit[*nsplit] = i__;
- ++(*nsplit);
- }
- /* L9: */
- }
- } else {
- /* Criterion that guarantees relative accuracy */
- i__1 = *n - 1;
- for (i__ = 1; i__ <= i__1; ++i__) {
- eabs = (d__1 = e[i__], abs(d__1));
- if (eabs <= *spltol * sqrt((d__1 = d__[i__], abs(d__1))) * sqrt((
- d__2 = d__[i__ + 1], abs(d__2)))) {
- e[i__] = 0.;
- e2[i__] = 0.;
- isplit[*nsplit] = i__;
- ++(*nsplit);
- }
- /* L10: */
- }
- }
- isplit[*nsplit] = *n;
- return 0;
- /* End of DLARRA */
- } /* dlarra_ */
|