546 lines
16 KiB
C
546 lines
16 KiB
C
/* -- translated by f2c (version 20240504).
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You must link the resulting object file with libf2c:
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on Microsoft Windows system, link with libf2c.lib;
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on Linux or Unix systems, link with .../path/to/libf2c.a -lm
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or, if you install libf2c.a in a standard place, with -lf2c -lm
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-- in that order, at the end of the command line, as in
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cc *.o -lf2c -lm
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Source for libf2c is in /netlib/f2c/libf2c.zip, e.g.,
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http://www.netlib.org/f2c/libf2c.zip
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*/
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#include "f2c.h"
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/* > \brief \b DLAR1V computes the (scaled) r-th column of the inverse of the submatrix in rows b1 through bn
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of the tridiagonal matrix LDLT - λI.
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=========== DOCUMENTATION ===========
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Online html documentation available at
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http://www.netlib.org/lapack/explore-html/
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> \htmlonly
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> Download DLAR1V + dependencies
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> <a href="http://www.netlib.org/cgi-bin/netlibfiles.tgz?format=tgz&filename=/lapack/lapack_routine/dlar1v.
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f">
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> [TGZ]</a>
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> <a href="http://www.netlib.org/cgi-bin/netlibfiles.zip?format=zip&filename=/lapack/lapack_routine/dlar1v.
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f">
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> [ZIP]</a>
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> <a href="http://www.netlib.org/cgi-bin/netlibfiles.txt?format=txt&filename=/lapack/lapack_routine/dlar1v.
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f">
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> [TXT]</a>
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> \endhtmlonly
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Definition:
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===========
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SUBROUTINE DLAR1V( N, B1, BN, LAMBDA, D, L, LD, LLD,
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PIVMIN, GAPTOL, Z, WANTNC, NEGCNT, ZTZ, MINGMA,
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R, ISUPPZ, NRMINV, RESID, RQCORR, WORK )
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LOGICAL WANTNC
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INTEGER B1, BN, N, NEGCNT, R
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DOUBLE PRECISION GAPTOL, LAMBDA, MINGMA, NRMINV, PIVMIN, RESID,
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$ RQCORR, ZTZ
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INTEGER ISUPPZ( * )
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DOUBLE PRECISION D( * ), L( * ), LD( * ), LLD( * ),
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$ WORK( * )
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DOUBLE PRECISION Z( * )
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> \par Purpose:
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=============
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>
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> \verbatim
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>
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> DLAR1V computes the (scaled) r-th column of the inverse of
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> the sumbmatrix in rows B1 through BN of the tridiagonal matrix
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> L D L**T - sigma I. When sigma is close to an eigenvalue, the
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> computed vector is an accurate eigenvector. Usually, r corresponds
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> to the index where the eigenvector is largest in magnitude.
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> The following steps accomplish this computation :
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> (a) Stationary qd transform, L D L**T - sigma I = L(+) D(+) L(+)**T,
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> (b) Progressive qd transform, L D L**T - sigma I = U(-) D(-) U(-)**T,
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> (c) Computation of the diagonal elements of the inverse of
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> L D L**T - sigma I by combining the above transforms, and choosing
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> r as the index where the diagonal of the inverse is (one of the)
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> largest in magnitude.
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> (d) Computation of the (scaled) r-th column of the inverse using the
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> twisted factorization obtained by combining the top part of the
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> the stationary and the bottom part of the progressive transform.
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> \endverbatim
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Arguments:
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==========
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> \param[in] N
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> \verbatim
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> N is INTEGER
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> The order of the matrix L D L**T.
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> \endverbatim
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>
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> \param[in] B1
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> \verbatim
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> B1 is INTEGER
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> First index of the submatrix of L D L**T.
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> \endverbatim
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>
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> \param[in] BN
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> \verbatim
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> BN is INTEGER
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> Last index of the submatrix of L D L**T.
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> \endverbatim
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>
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> \param[in] LAMBDA
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> \verbatim
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> LAMBDA is DOUBLE PRECISION
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> The shift. In order to compute an accurate eigenvector,
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> LAMBDA should be a good approximation to an eigenvalue
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> of L D L**T.
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> \endverbatim
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>
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> \param[in] L
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> \verbatim
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> L is DOUBLE PRECISION array, dimension (N-1)
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> The (n-1) subdiagonal elements of the unit bidiagonal matrix
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> L, in elements 1 to N-1.
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> \endverbatim
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>
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> \param[in] D
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> \verbatim
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> D is DOUBLE PRECISION array, dimension (N)
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> The n diagonal elements of the diagonal matrix D.
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> \endverbatim
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>
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> \param[in] LD
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> \verbatim
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> LD is DOUBLE PRECISION array, dimension (N-1)
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> The n-1 elements L(i)*D(i).
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> \endverbatim
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>
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> \param[in] LLD
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> \verbatim
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> LLD is DOUBLE PRECISION array, dimension (N-1)
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> The n-1 elements L(i)*L(i)*D(i).
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> \endverbatim
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>
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> \param[in] PIVMIN
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> \verbatim
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> PIVMIN is DOUBLE PRECISION
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> The minimum pivot in the Sturm sequence.
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> \endverbatim
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>
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> \param[in] GAPTOL
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> \verbatim
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> GAPTOL is DOUBLE PRECISION
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> Tolerance that indicates when eigenvector entries are negligible
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> w.r.t. their contribution to the residual.
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> \endverbatim
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>
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> \param[in,out] Z
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> \verbatim
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> Z is DOUBLE PRECISION array, dimension (N)
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> On input, all entries of Z must be set to 0.
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> On output, Z contains the (scaled) r-th column of the
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> inverse. The scaling is such that Z(R) equals 1.
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> \endverbatim
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>
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> \param[in] WANTNC
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> \verbatim
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> WANTNC is LOGICAL
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> Specifies whether NEGCNT has to be computed.
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> \endverbatim
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>
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> \param[out] NEGCNT
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> \verbatim
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> NEGCNT is INTEGER
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> If WANTNC is .TRUE. then NEGCNT = the number of pivots < pivmin
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> in the matrix factorization L D L**T, and NEGCNT = -1 otherwise.
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> \endverbatim
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>
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> \param[out] ZTZ
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> \verbatim
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> ZTZ is DOUBLE PRECISION
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> The square of the 2-norm of Z.
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> \endverbatim
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>
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> \param[out] MINGMA
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> \verbatim
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> MINGMA is DOUBLE PRECISION
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> The reciprocal of the largest (in magnitude) diagonal
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> element of the inverse of L D L**T - sigma I.
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> \endverbatim
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>
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> \param[in,out] R
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> \verbatim
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> R is INTEGER
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> The twist index for the twisted factorization used to
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> compute Z.
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> On input, 0 <= R <= N. If R is input as 0, R is set to
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> the index where (L D L**T - sigma I)^{-1} is largest
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> in magnitude. If 1 <= R <= N, R is unchanged.
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> On output, R contains the twist index used to compute Z.
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> Ideally, R designates the position of the maximum entry in the
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> eigenvector.
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> \endverbatim
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>
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> \param[out] ISUPPZ
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> \verbatim
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> ISUPPZ is INTEGER array, dimension (2)
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> The support of the vector in Z, i.e., the vector Z is
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> nonzero only in elements ISUPPZ(1) through ISUPPZ( 2 ).
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> \endverbatim
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>
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> \param[out] NRMINV
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> \verbatim
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> NRMINV is DOUBLE PRECISION
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> NRMINV = 1/SQRT( ZTZ )
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> \endverbatim
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>
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> \param[out] RESID
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> \verbatim
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> RESID is DOUBLE PRECISION
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> The residual of the FP vector.
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> RESID = ABS( MINGMA )/SQRT( ZTZ )
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> \endverbatim
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>
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> \param[out] RQCORR
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> \verbatim
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> RQCORR is DOUBLE PRECISION
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> The Rayleigh Quotient correction to LAMBDA.
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> RQCORR = MINGMA*TMP
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> \endverbatim
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>
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> \param[out] WORK
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> \verbatim
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> WORK is DOUBLE PRECISION array, dimension (4*N)
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> \endverbatim
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Authors:
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========
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> \author Univ. of Tennessee
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> \author Univ. of California Berkeley
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> \author Univ. of Colorado Denver
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> \author NAG Ltd.
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> \date September 2012
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> \ingroup doubleOTHERauxiliary
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> \par Contributors:
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==================
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>
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> Beresford Parlett, University of California, Berkeley, USA \n
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> Jim Demmel, University of California, Berkeley, USA \n
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> Inderjit Dhillon, University of Texas, Austin, USA \n
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> Osni Marques, LBNL/NERSC, USA \n
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> Christof Voemel, University of California, Berkeley, USA
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=====================================================================
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Subroutine */ int igraphdlar1v_(integer *n, integer *b1, integer *bn, doublereal
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*lambda, doublereal *d__, doublereal *l, doublereal *ld, doublereal *
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lld, doublereal *pivmin, doublereal *gaptol, doublereal *z__, logical
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*wantnc, integer *negcnt, doublereal *ztz, doublereal *mingma,
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integer *r__, integer *isuppz, doublereal *nrminv, doublereal *resid,
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doublereal *rqcorr, doublereal *work)
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{
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/* System generated locals */
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integer i__1;
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doublereal d__1, d__2, d__3;
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/* Builtin functions */
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double sqrt(doublereal);
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/* Local variables */
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integer i__;
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doublereal s;
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integer r1, r2;
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doublereal eps, tmp;
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integer neg1, neg2, indp, inds;
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doublereal dplus;
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extern doublereal igraphdlamch_(char *);
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extern logical igraphdisnan_(doublereal *);
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integer indlpl, indumn;
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doublereal dminus;
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logical sawnan1, sawnan2;
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/* -- LAPACK auxiliary routine (version 3.4.2) --
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-- LAPACK is a software package provided by Univ. of Tennessee, --
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-- Univ. of California Berkeley, Univ. of Colorado Denver and NAG Ltd..--
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September 2012
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=====================================================================
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Parameter adjustments */
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--work;
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--isuppz;
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--z__;
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--lld;
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--ld;
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--l;
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--d__;
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/* Function Body */
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eps = igraphdlamch_("Precision");
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if (*r__ == 0) {
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r1 = *b1;
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r2 = *bn;
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} else {
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r1 = *r__;
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r2 = *r__;
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}
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/* Storage for LPLUS */
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indlpl = 0;
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/* Storage for UMINUS */
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indumn = *n;
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inds = (*n << 1) + 1;
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indp = *n * 3 + 1;
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if (*b1 == 1) {
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work[inds] = 0.;
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} else {
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work[inds + *b1 - 1] = lld[*b1 - 1];
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}
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/* Compute the stationary transform (using the differential form)
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until the index R2. */
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sawnan1 = FALSE_;
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neg1 = 0;
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s = work[inds + *b1 - 1] - *lambda;
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i__1 = r1 - 1;
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for (i__ = *b1; i__ <= i__1; ++i__) {
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dplus = d__[i__] + s;
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work[indlpl + i__] = ld[i__] / dplus;
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if (dplus < 0.) {
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++neg1;
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}
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work[inds + i__] = s * work[indlpl + i__] * l[i__];
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s = work[inds + i__] - *lambda;
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/* L50: */
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}
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sawnan1 = igraphdisnan_(&s);
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if (sawnan1) {
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goto L60;
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}
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i__1 = r2 - 1;
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for (i__ = r1; i__ <= i__1; ++i__) {
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dplus = d__[i__] + s;
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work[indlpl + i__] = ld[i__] / dplus;
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work[inds + i__] = s * work[indlpl + i__] * l[i__];
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s = work[inds + i__] - *lambda;
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/* L51: */
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}
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sawnan1 = igraphdisnan_(&s);
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L60:
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if (sawnan1) {
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/* Runs a slower version of the above loop if a NaN is detected */
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neg1 = 0;
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s = work[inds + *b1 - 1] - *lambda;
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i__1 = r1 - 1;
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for (i__ = *b1; i__ <= i__1; ++i__) {
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dplus = d__[i__] + s;
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if (abs(dplus) < *pivmin) {
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dplus = -(*pivmin);
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}
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work[indlpl + i__] = ld[i__] / dplus;
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if (dplus < 0.) {
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++neg1;
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}
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work[inds + i__] = s * work[indlpl + i__] * l[i__];
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if (work[indlpl + i__] == 0.) {
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work[inds + i__] = lld[i__];
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}
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s = work[inds + i__] - *lambda;
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/* L70: */
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}
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i__1 = r2 - 1;
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for (i__ = r1; i__ <= i__1; ++i__) {
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dplus = d__[i__] + s;
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if (abs(dplus) < *pivmin) {
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dplus = -(*pivmin);
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}
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work[indlpl + i__] = ld[i__] / dplus;
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work[inds + i__] = s * work[indlpl + i__] * l[i__];
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if (work[indlpl + i__] == 0.) {
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work[inds + i__] = lld[i__];
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}
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s = work[inds + i__] - *lambda;
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/* L71: */
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}
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}
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/* Compute the progressive transform (using the differential form)
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until the index R1 */
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sawnan2 = FALSE_;
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neg2 = 0;
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work[indp + *bn - 1] = d__[*bn] - *lambda;
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i__1 = r1;
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for (i__ = *bn - 1; i__ >= i__1; --i__) {
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dminus = lld[i__] + work[indp + i__];
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tmp = d__[i__] / dminus;
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if (dminus < 0.) {
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++neg2;
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}
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work[indumn + i__] = l[i__] * tmp;
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work[indp + i__ - 1] = work[indp + i__] * tmp - *lambda;
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/* L80: */
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}
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tmp = work[indp + r1 - 1];
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sawnan2 = igraphdisnan_(&tmp);
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if (sawnan2) {
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/* Runs a slower version of the above loop if a NaN is detected */
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neg2 = 0;
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i__1 = r1;
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for (i__ = *bn - 1; i__ >= i__1; --i__) {
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dminus = lld[i__] + work[indp + i__];
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if (abs(dminus) < *pivmin) {
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dminus = -(*pivmin);
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}
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tmp = d__[i__] / dminus;
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if (dminus < 0.) {
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++neg2;
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}
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work[indumn + i__] = l[i__] * tmp;
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work[indp + i__ - 1] = work[indp + i__] * tmp - *lambda;
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if (tmp == 0.) {
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work[indp + i__ - 1] = d__[i__] - *lambda;
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}
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/* L100: */
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}
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}
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/* Find the index (from R1 to R2) of the largest (in magnitude)
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diagonal element of the inverse */
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*mingma = work[inds + r1 - 1] + work[indp + r1 - 1];
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if (*mingma < 0.) {
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++neg1;
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}
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if (*wantnc) {
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*negcnt = neg1 + neg2;
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} else {
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*negcnt = -1;
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}
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if (abs(*mingma) == 0.) {
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*mingma = eps * work[inds + r1 - 1];
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}
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*r__ = r1;
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i__1 = r2 - 1;
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for (i__ = r1; i__ <= i__1; ++i__) {
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tmp = work[inds + i__] + work[indp + i__];
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if (tmp == 0.) {
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tmp = eps * work[inds + i__];
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}
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if (abs(tmp) <= abs(*mingma)) {
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*mingma = tmp;
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*r__ = i__ + 1;
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}
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/* L110: */
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}
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/* Compute the FP vector: solve N^T v = e_r */
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isuppz[1] = *b1;
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isuppz[2] = *bn;
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z__[*r__] = 1.;
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*ztz = 1.;
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/* Compute the FP vector upwards from R */
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if (! sawnan1 && ! sawnan2) {
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i__1 = *b1;
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for (i__ = *r__ - 1; i__ >= i__1; --i__) {
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z__[i__] = -(work[indlpl + i__] * z__[i__ + 1]);
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if (((d__1 = z__[i__], abs(d__1)) + (d__2 = z__[i__ + 1], abs(
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d__2))) * (d__3 = ld[i__], abs(d__3)) < *gaptol) {
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z__[i__] = 0.;
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isuppz[1] = i__ + 1;
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goto L220;
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}
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*ztz += z__[i__] * z__[i__];
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/* L210: */
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}
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L220:
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;
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} else {
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/* Run slower loop if NaN occurred. */
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i__1 = *b1;
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for (i__ = *r__ - 1; i__ >= i__1; --i__) {
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if (z__[i__ + 1] == 0.) {
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z__[i__] = -(ld[i__ + 1] / ld[i__]) * z__[i__ + 2];
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} else {
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z__[i__] = -(work[indlpl + i__] * z__[i__ + 1]);
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}
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if (((d__1 = z__[i__], abs(d__1)) + (d__2 = z__[i__ + 1], abs(
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d__2))) * (d__3 = ld[i__], abs(d__3)) < *gaptol) {
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z__[i__] = 0.;
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isuppz[1] = i__ + 1;
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goto L240;
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}
|
|
*ztz += z__[i__] * z__[i__];
|
|
/* L230: */
|
|
}
|
|
L240:
|
|
;
|
|
}
|
|
/* Compute the FP vector downwards from R in blocks of size BLKSIZ */
|
|
if (! sawnan1 && ! sawnan2) {
|
|
i__1 = *bn - 1;
|
|
for (i__ = *r__; i__ <= i__1; ++i__) {
|
|
z__[i__ + 1] = -(work[indumn + i__] * z__[i__]);
|
|
if (((d__1 = z__[i__], abs(d__1)) + (d__2 = z__[i__ + 1], abs(
|
|
d__2))) * (d__3 = ld[i__], abs(d__3)) < *gaptol) {
|
|
z__[i__ + 1] = 0.;
|
|
isuppz[2] = i__;
|
|
goto L260;
|
|
}
|
|
*ztz += z__[i__ + 1] * z__[i__ + 1];
|
|
/* L250: */
|
|
}
|
|
L260:
|
|
;
|
|
} else {
|
|
/* Run slower loop if NaN occurred. */
|
|
i__1 = *bn - 1;
|
|
for (i__ = *r__; i__ <= i__1; ++i__) {
|
|
if (z__[i__] == 0.) {
|
|
z__[i__ + 1] = -(ld[i__ - 1] / ld[i__]) * z__[i__ - 1];
|
|
} else {
|
|
z__[i__ + 1] = -(work[indumn + i__] * z__[i__]);
|
|
}
|
|
if (((d__1 = z__[i__], abs(d__1)) + (d__2 = z__[i__ + 1], abs(
|
|
d__2))) * (d__3 = ld[i__], abs(d__3)) < *gaptol) {
|
|
z__[i__ + 1] = 0.;
|
|
isuppz[2] = i__;
|
|
goto L280;
|
|
}
|
|
*ztz += z__[i__ + 1] * z__[i__ + 1];
|
|
/* L270: */
|
|
}
|
|
L280:
|
|
;
|
|
}
|
|
|
|
/* Compute quantities for convergence test */
|
|
|
|
tmp = 1. / *ztz;
|
|
*nrminv = sqrt(tmp);
|
|
*resid = abs(*mingma) * *nrminv;
|
|
*rqcorr = *mingma * tmp;
|
|
|
|
|
|
return 0;
|
|
|
|
/* End of DLAR1V */
|
|
|
|
} /* igraphdlar1v_ */
|
|
|