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DSYEVR(1)	      LAPACK driver routine (version 3.2)	     DSYEVR(1)

NAME
       DSYEVR - computes selected eigenvalues and, optionally, eigenvectors of
       a real symmetric matrix A

SYNOPSIS
       SUBROUTINE DSYEVR( JOBZ, RANGE, UPLO,  N,  A,  LDA,  VL,	 VU,  IL,  IU,
			  ABSTOL,  M,  W,  Z, LDZ, ISUPPZ, WORK, LWORK, IWORK,
			  LIWORK, INFO )

	   CHARACTER	  JOBZ, RANGE, UPLO

	   INTEGER	  IL, INFO, IU, LDA, LDZ, LIWORK, LWORK, M, N

	   DOUBLE	  PRECISION ABSTOL, VL, VU

	   INTEGER	  ISUPPZ( * ), IWORK( * )

	   DOUBLE	  PRECISION A( LDA, * ), W( * ), WORK( * ), Z( LDZ,  *
			  )

PURPOSE
       DSYEVR computes selected eigenvalues and, optionally, eigenvectors of a
       real symmetric matrix A.	 Eigenvalues and eigenvectors can be  selected
       by  specifying  either  a range of values or a range of indices for the
       desired eigenvalues.
       DSYEVR first reduces the matrix A to tridiagonal form T with a call  to
       DSYTRD.	 Then,	whenever  possible, DSYEVR calls DSTEMR to compute the
       eigenspectrum using Relatively Robust Representations.  DSTEMR computes
       eigenvalues  by	the  dqds algorithm, while orthogonal eigenvectors are
       computed from various "good" L D L^T  representations  (also  known  as
       Relatively  Robust  Representations). Gram-Schmidt orthogonalization is
       avoided as far as possible. More specifically, the various steps of the
       algorithm are as follows.
       For each unreduced block (submatrix) of T,
	  (a) Compute T - sigma I  = L D L^T, so that L and D
	      define all the wanted eigenvalues to high relative accuracy.
	      This means that small relative changes in the entries of D and L
	      cause only small relative changes in the eigenvalues and
	      eigenvectors. The standard (unfactored) representation of the
	      tridiagonal matrix T does not have this property in general.
	  (b) Compute the eigenvalues to suitable accuracy.
	      If the eigenvectors are desired, the algorithm attains full
	      accuracy of the computed eigenvalues only right before
	      the  corresponding vectors have to be computed, see steps c) and
       d).
	  (c) For each cluster of close eigenvalues, select a new
	      shift close to the cluster, find a new factorization, and refine
	      the shifted eigenvalues to suitable accuracy.
	  (d) For each eigenvalue with a large enough relative separation com‐
       pute
	      the  corresponding  eigenvector  by  forming  a  rank  revealing
       twisted
	      factorization. Go back to (c) for any clusters that remain.  The
       desired	accuracy of the output can be specified by the input parameter
       ABSTOL.
       For more details, see DSTEMR's documentation and:
       - Inderjit S. Dhillon and Beresford N. Parlett:	"Multiple  representa‐
       tions
	 to  compute  orthogonal  eigenvectors of symmetric tridiagonal matri‐
       ces,"
	 Linear Algebra and its Applications, 387(1), pp. 1-28,	 August	 2004.
       - Inderjit Dhillon and Beresford Parlett: "Orthogonal Eigenvectors and
	 Relative  Gaps,"  SIAM	 Journal  on Matrix Analysis and Applications,
       Vol. 25,
	 2004.	Also LAPACK Working Note 154.
       - Inderjit Dhillon: "A new O(n^2) algorithm for the symmetric
	 tridiagonal eigenvalue/eigenvector problem",
	 Computer Science Division Technical Report No. UCB/CSD-97-971,
	 UC Berkeley, May 1997.
       Note 1 : DSYEVR calls DSTEMR when the full  spectrum  is	 requested  on
       machines which conform to the ieee-754 floating point standard.	DSYEVR
       calls DSTEBZ and SSTEIN on non-ieee machines and
       when partial spectrum requests are made.
       Normal execution of DSTEMR may create NaNs and infinities and hence may
       abort  due  to  a floating point exception in environments which do not
       handle NaNs and infinities in the ieee standard default manner.

ARGUMENTS
       JOBZ    (input) CHARACTER*1
	       = 'N':  Compute eigenvalues only;
	       = 'V':  Compute eigenvalues and eigenvectors.

       RANGE   (input) CHARACTER*1
	       = 'A': all eigenvalues will be found.
	       = 'V': all eigenvalues in the half-open interval	 (VL,VU]  will
	       be  found.   = 'I': the IL-th through IU-th eigenvalues will be
	       found.

       UPLO    (input) CHARACTER*1
	       = 'U':  Upper triangle of A is stored;
	       = 'L':  Lower triangle of A is stored.

       N       (input) INTEGER
	       The order of the matrix A.  N >= 0.

       A       (input/output) DOUBLE PRECISION array, dimension (LDA, N)
	       On entry, the symmetric matrix A.  If UPLO = 'U',  the  leading
	       N-by-N upper triangular part of A contains the upper triangular
	       part of the matrix A.  If UPLO = 'L', the leading N-by-N	 lower
	       triangular  part of A contains the lower triangular part of the
	       matrix A.  On exit, the lower triangle  (if  UPLO='L')  or  the
	       upper  triangle	(if UPLO='U') of A, including the diagonal, is
	       destroyed.

       LDA     (input) INTEGER
	       The leading dimension of the array A.  LDA >= max(1,N).

       VL      (input) DOUBLE PRECISION
	       VU      (input) DOUBLE PRECISION If RANGE='V',  the  lower  and
	       upper bounds of the interval to be searched for eigenvalues. VL
	       < VU.  Not referenced if RANGE = 'A' or 'I'.

       IL      (input) INTEGER
	       IU      (input) INTEGER If RANGE='I', the indices (in ascending
	       order)  of the smallest and largest eigenvalues to be returned.
	       1 <= IL <= IU <= N, if N > 0; IL = 1 and IU = 0 if N = 0.   Not
	       referenced if RANGE = 'A' or 'V'.

       ABSTOL  (input) DOUBLE PRECISION
	       The  absolute error tolerance for the eigenvalues.  An approxi‐
	       mate eigenvalue is accepted as converged when it is  determined
	       to  lie	in  an	interval  [a,b] of width less than or equal to
	       ABSTOL + EPS *	max( |a|,|b| ) , where EPS is the machine pre‐
	       cision.	If ABSTOL is less than or equal to zero, then  EPS*|T|
	       will be used in its place, where	 |T|  is  the  1-norm  of  the
	       tridiagonal  matrix obtained by reducing A to tridiagonal form.
	       See "Computing Small Singular  Values  of  Bidiagonal  Matrices
	       with  Guaranteed	 High Relative Accuracy," by Demmel and Kahan,
	       LAPACK Working Note #3.	If high relative  accuracy  is	impor‐
	       tant,  set  ABSTOL  to DLAMCH( 'Safe minimum' ).	 Doing so will
	       guarantee that eigenvalues are computed to high relative	 accu‐
	       racy  when  possible in future releases.	 The current code does
	       not make any  guarantees	 about	high  relative	accuracy,  but
	       future  releases	 will. See J. Barlow and J. Demmel, "Computing
	       Accurate Eigensystems of Scaled Diagonally Dominant  Matrices",
	       LAPACK  Working	Note  #7,  for	a discussion of which matrices
	       define their eigenvalues to high relative accuracy.

       M       (output) INTEGER
	       The total number of eigenvalues found.  0 <= M <= N.  If	 RANGE
	       = 'A', M = N, and if RANGE = 'I', M = IU-IL+1.

       W       (output) DOUBLE PRECISION array, dimension (N)
	       The  first  M  elements	contain	 the  selected	eigenvalues in
	       ascending order.

       Z       (output) DOUBLE PRECISION array, dimension (LDZ, max(1,M))
	       If JOBZ = 'V', then if INFO = 0, the first M columns of Z  con‐
	       tain the orthonormal eigenvectors of the matrix A corresponding
	       to the selected eigenvalues, with the i-th column of Z  holding
	       the eigenvector associated with W(i).  If JOBZ = 'N', then Z is
	       not referenced.	Note: the  user	 must  ensure  that  at	 least
	       max(1,M)	 columns  are supplied in the array Z; if RANGE = 'V',
	       the exact value of M is not known in advance and an upper bound
	       must be used.  Supplying N columns is always safe.

       LDZ     (input) INTEGER
	       The  leading dimension of the array Z.  LDZ >= 1, and if JOBZ =
	       'V', LDZ >= max(1,N).

       ISUPPZ  (output) INTEGER array, dimension ( 2*max(1,M) )
	       The support of the eigenvectors in Z, i.e., the	indices	 indi‐
	       cating  the  nonzero  elements  in  Z.  The i-th eigenvector is
	       nonzero only in elements ISUPPZ( 2*i-1 ) through ISUPPZ( 2*i ).

       WORK	 (workspace/output)   DOUBLE   PRECISION   array,    dimension
       (MAX(1,LWORK))
	       On exit, if INFO = 0, WORK(1) returns the optimal LWORK.

       LWORK   (input) INTEGER
	       The  dimension  of  the array WORK.  LWORK >= max(1,26*N).  For
	       optimal efficiency, LWORK >= (NB+6)*N, where NB is the  max  of
	       the  blocksize  for  DSYTRD  and DORMTR returned by ILAENV.  If
	       LWORK = -1, then a workspace query is assumed; the routine only
	       calculates  the	optimal	 size  of the WORK array, returns this
	       value as the first entry of the WORK array, and no  error  mes‐
	       sage related to LWORK is issued by XERBLA.

       IWORK   (workspace/output) INTEGER array, dimension (MAX(1,LIWORK))
	       On exit, if INFO = 0, IWORK(1) returns the optimal LWORK.

       LIWORK  (input) INTEGER
	       The  dimension  of the array IWORK.  LIWORK >= max(1,10*N).  If
	       LIWORK = -1, then a workspace query  is	assumed;  the  routine
	       only  calculates	 the  optimal size of the IWORK array, returns
	       this value as the first entry of the IWORK array, and no	 error
	       message related to LIWORK is issued by XERBLA.

       INFO    (output) INTEGER
	       = 0:  successful exit
	       < 0:  if INFO = -i, the i-th argument had an illegal value
	       > 0:  Internal error

FURTHER DETAILS
       Based on contributions by
	  Inderjit Dhillon, IBM Almaden, USA
	  Osni Marques, LBNL/NERSC, USA
	  Ken Stanley, Computer Science Division, University of
	    California at Berkeley, USA
	  Jason Riedy, Computer Science Division, University of
	    California at Berkeley, USA

 LAPACK driver routine (version 3November 2008			     DSYEVR(1)
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