          SUBROUTINE DLARRE( RANGE, N, VL, VU, IL, IU, D, E, E2,
         $                    RTOL1, RTOL2, SPLTOL, NSPLIT, ISPLIT, M,
         $                    W, WERR, WGAP, IBLOCK, INDEXW, GERS, PIVMIN,
         $                    WORK, IWORK, INFO )
          IMPLICIT NONE
    *
    *  -- LAPACK auxiliary routine (version 3.1) --
    *     Univ. of Tennessee, Univ. of California Berkeley and NAG Ltd..
    *     November 2006
    *
    *     .. Scalar Arguments ..
          CHARACTER          RANGE
          INTEGER            IL, INFO, IU, M, N, NSPLIT
          DOUBLE PRECISION  PIVMIN, RTOL1, RTOL2, SPLTOL, VL, VU
    *     ..
    *     .. Array Arguments ..
          INTEGER            IBLOCK( * ), ISPLIT( * ), IWORK( * ),
         $                   INDEXW( * )
          DOUBLE PRECISION   D( * ), E( * ), E2( * ), GERS( * ),
         $                   W( * ),WERR( * ), WGAP( * ), WORK( * )
    *     ..
    *
    *  Purpose
    *  =======
    *
    *  To find the desired eigenvalues of a given real symmetric
    *  tridiagonal matrix T, DLARRE sets any "small" off-diagonal
    *  elements to zero, and for each unreduced block T_i, it finds
    *  (a) a suitable shift at one end of the block's spectrum,
    *  (b) the base representation, T_i - sigma_i I = L_i D_i L_i^T, and
    *  (c) eigenvalues of each L_i D_i L_i^T.
    *  The representations and eigenvalues found are then used by
    *  DSTEMR to compute the eigenvectors of T.
    *  The accuracy varies depending on whether bisection is used to
    *  find a few eigenvalues or the dqds algorithm (subroutine DLASQ2) to
    *  conpute all and then discard any unwanted one.
    *  As an added benefit, DLARRE also outputs the n
    *  Gerschgorin intervals for the matrices L_i D_i L_i^T.
    *
    *  Arguments
    *  =========
    *
    *  RANGE   (input) CHARACTER
    *          = 'A': ("All")   all eigenvalues will be found.
    *          = 'V': ("Value") all eigenvalues in the half-open interval
    *                           (VL, VU] will be found.
    *          = 'I': ("Index") the IL-th through IU-th eigenvalues (of the
    *                           entire matrix) will be found.
    *
    *  N       (input) INTEGER
    *          The order of the matrix. N > 0.
    *
    *  VL      (input/output) DOUBLE PRECISION
    *  VU      (input/output) DOUBLE PRECISION
    *          If RANGE='V', the lower and upper bounds for the eigenvalues.
    *          Eigenvalues less than or equal to VL, or greater than VU,
    *          will not be returned.  VL < VU.
    *          If RANGE='I' or ='A', DLARRE computes bounds on the desired
    *          part of the spectrum.
    *
    *  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.
    *
    *  D       (input/output) DOUBLE PRECISION array, dimension (N)
    *          On entry, the N diagonal elements of the tridiagonal
    *          matrix T.
    *          On exit, the N diagonal elements of the diagonal
    *          matrices D_i.
    *
    *  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, E contains the subdiagonal elements of the unit
    *          bidiagonal matrices L_i. The entries E( ISPLIT( I ) ),
    *          1 <= I <= NSPLIT, contain the base points sigma_i on output.
    *
    *  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
    *
    *  RTOL1   (input) DOUBLE PRECISION
    *  RTOL2   (input) DOUBLE PRECISION
    *           Parameters for bisection.
    *           An interval [LEFT,RIGHT] has converged if
    *           RIGHT-LEFT.LT.MAX( RTOL1*GAP, RTOL2*MAX(|LEFT|,|RIGHT|) )
    *
    *  SPLTOL (input) DOUBLE PRECISION
    *          The threshold for splitting.
    *
    *  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.
    *
    *  M       (output) INTEGER
    *          The total number of eigenvalues (of all L_i D_i L_i^T)
    *          found.
    *
    *  W       (output) DOUBLE PRECISION array, dimension (N)
    *          The first M elements contain the eigenvalues. The
    *          eigenvalues of each of the blocks, L_i D_i L_i^T, are
    *          sorted in ascending order ( DLARRE may use the
    *          remaining N-M elements as workspace).
    *
    *  WERR    (output) DOUBLE PRECISION array, dimension (N)
    *          The error bound on the corresponding eigenvalue in W.
    *
    *  WGAP    (output) DOUBLE PRECISION array, dimension (N)
    *          The separation from the right neighbor eigenvalue in W.
    *          The gap is only with respect to the eigenvalues of the same block
    *          as each block has its own representation tree.
    *          Exception: at the right end of a block we store the left gap
    *
    *  IBLOCK  (output) INTEGER array, dimension (N)
    *          The indices of the blocks (submatrices) associated with the
    *          corresponding eigenvalues in W; IBLOCK(i)=1 if eigenvalue
    *          W(i) belongs to the first block from the top, =2 if W(i)
    *          belongs to the second block, etc.
    *
    *  INDEXW  (output) INTEGER array, dimension (N)
    *          The indices of the eigenvalues within each block (submatrix);
    *          for example, INDEXW(i)= 10 and IBLOCK(i)=2 imply that the
    *          i-th eigenvalue W(i) is the 10-th eigenvalue in block 2
    *
    *  GERS    (output) DOUBLE PRECISION array, dimension (2*N)
    *          The N Gerschgorin intervals (the i-th Gerschgorin interval
    *          is (GERS(2*i-1), GERS(2*i)).
    *
    *  PIVMIN  (output) DOUBLE PRECISION
    *          The minimum pivot in the Sturm sequence for T.
    *
    *  WORK    (workspace) DOUBLE PRECISION array, dimension (6*N)
    *          Workspace.
    *
    *  IWORK   (workspace) INTEGER array, dimension (5*N)
    *          Workspace.
    *
    *  INFO    (output) INTEGER
    *          = 0:  successful exit
    *          > 0:  A problem occured in DLARRE.
    *          < 0:  One of the called subroutines signaled an internal problem.
    *                Needs inspection of the corresponding parameter IINFO
    *                for further information.
    *
    *          =-1:  Problem in DLARRD.
    *          = 2:  No base representation could be found in MAXTRY iterations.
    *                Increasing MAXTRY and recompilation might be a remedy.
    *          =-3:  Problem in DLARRB when computing the refined root
    *                representation for DLASQ2.
    *          =-4:  Problem in DLARRB when preforming bisection on the
    *                desired part of the spectrum.
    *          =-5:  Problem in DLASQ2.
    *          =-6:  Problem in DLASQ2.
    *
    *  Further Details
    *  The base representations are required to suffer very little
    *  element growth and consequently define all their eigenvalues to
    *  high relative accuracy.
    *  ===============
    *
    *  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 ..
          DOUBLE PRECISION   FAC, FOUR, FOURTH, FUDGE, HALF, HNDRD,
         $                   MAXGROWTH, ONE, PERT, TWO, ZERO
          PARAMETER          ( ZERO = 0.0D0, ONE = 1.0D0,
         $                     TWO = 2.0D0, FOUR=4.0D0,
         $                     HNDRD = 100.0D0,
         $                     PERT = 8.0D0,
         $                     HALF = ONE/TWO, FOURTH = ONE/FOUR, FAC= HALF,
         $                     MAXGROWTH = 64.0D0, FUDGE = 2.0D0 )
          INTEGER            MAXTRY, ALLRNG, INDRNG, VALRNG
          PARAMETER          ( MAXTRY = 6, ALLRNG = 1, INDRNG = 2,
         $                     VALRNG = 3 )
    *     ..
    *     .. Local Scalars ..
          LOGICAL            FORCEB, NOREP, USEDQD
          INTEGER            CNT, CNT1, CNT2, I, IBEGIN, IDUM, IEND, IINFO,
         $                   IN, INDL, INDU, IRANGE, J, JBLK, MB, MM,
         $                   WBEGIN, WEND
          DOUBLE PRECISION   AVGAP, BSRTOL, CLWDTH, DMAX, DPIVOT, EABS,
         $                   EMAX, EOLD, EPS, GL, GU, ISLEFT, ISRGHT, RTL,
         $                   RTOL, S1, S2, SAFMIN, SGNDEF, SIGMA, SPDIAM,
         $                   TAU, TMP, TMP1

    *     ..
    *     .. Local Arrays ..
          INTEGER            ISEED( 4 )
    *     ..
    *     .. External Functions ..
          LOGICAL            LSAME
          DOUBLE PRECISION            DLAMCH
          EXTERNAL           DLAMCH, LSAME

    *     ..
    *     .. External Subroutines ..
          EXTERNAL           DCOPY, DLARNV, DLARRA, DLARRB, DLARRC, DLARRD,
         $                   DLASQ2
    *     ..
    *     .. Intrinsic Functions ..
          INTRINSIC          ABS, MAX, MIN

    *     ..
    *     .. Executable Statements ..
    *

          INFO = 0

    *
    *     Decode RANGE
    *
          IF( LSAME( RANGE, 'A' ) ) THEN
             IRANGE = ALLRNG
          ELSE IF( LSAME( RANGE, 'V' ) ) THEN
             IRANGE = VALRNG
          ELSE IF( LSAME( RANGE, 'I' ) ) THEN
             IRANGE = INDRNG
          END IF

          M = 0

    *     Get machine constants
          SAFMIN = DLAMCH( 'S' )
          EPS = DLAMCH( 'P' )

    *     Set parameters
          RTL = SQRT(EPS)
          BSRTOL = SQRT(EPS)

    *     Treat case of 1x1 matrix for quick return
          IF( N.EQ.1 ) THEN
             IF( (IRANGE.EQ.ALLRNG).OR.
         $       ((IRANGE.EQ.VALRNG).AND.(D(1).GT.VL).AND.(D(1).LE.VU)).OR.
         $       ((IRANGE.EQ.INDRNG).AND.(IL.EQ.1).AND.(IU.EQ.1)) ) THEN
                M = 1
                W(1) = D(1)
    *           The computation error of the eigenvalue is zero
                WERR(1) = ZERO
                WGAP(1) = ZERO
                IBLOCK( 1 ) = 1
                INDEXW( 1 ) = 1
                GERS(1) = D( 1 )
                GERS(2) = D( 1 )
             ENDIF
    *        store the shift for the initial RRR, which is zero in this case
             E(1) = ZERO
             RETURN
          END IF

    *     General case: tridiagonal matrix of order > 1
    *
    *     Init WERR, WGAP. Compute Gerschgorin intervals and spectral diameter.
    *     Compute maximum off-diagonal entry and pivmin.
          GL = D(1)
          GU = D(1)
          EOLD = ZERO
          EMAX = ZERO
          E(N) = ZERO
          DO 5 I = 1,N
             WERR(I) = ZERO
             WGAP(I) = ZERO
             EABS = ABS( E(I) )
             IF( EABS .GE. EMAX ) THEN
                EMAX = EABS
             END IF
             TMP1 = EABS + EOLD
             GERS( 2*I-1) = D(I) - TMP1
             GL =  MIN( GL, GERS( 2*I - 1))
             GERS( 2*I ) = D(I) + TMP1
             GU = MAX( GU, GERS(2*I) )
             EOLD  = EABS
     5    CONTINUE
    *     The minimum pivot allowed in the Sturm sequence for T
          PIVMIN = SAFMIN * MAX( ONE, EMAX**2 )
    *     Compute spectral diameter. The Gerschgorin bounds give an
    *     estimate that is wrong by at most a factor of SQRT(2)
          SPDIAM = GU - GL

    *     Compute splitting points
          CALL DLARRA( N, D, E, E2, SPLTOL, SPDIAM,
         $                    NSPLIT, ISPLIT, IINFO )

    *     Can force use of bisection instead of faster DQDS.
    *     Option left in the code for future multisection work.
          FORCEB = .FALSE.

          IF( (IRANGE.EQ.ALLRNG) .AND. (.NOT. FORCEB) ) THEN
    *        Set interval [VL,VU] that contains all eigenvalues
             VL = GL
             VU = GU
          ELSE
    *        We call DLARRD to find crude approximations to the eigenvalues
    *        in the desired range. In case IRANGE = INDRNG, we also obtain the
    *        interval (VL,VU] that contains all the wanted eigenvalues.
    *        An interval [LEFT,RIGHT] has converged if
    *        RIGHT-LEFT.LT.RTOL*MAX(ABS(LEFT),ABS(RIGHT))
    *        DLARRD needs a WORK of size 4*N, IWORK of size 3*N
             CALL DLARRD( RANGE, 'B', N, VL, VU, IL, IU, GERS,
         $                    BSRTOL, D, E, E2, PIVMIN, NSPLIT, ISPLIT,
         $                    MM, W, WERR, VL, VU, IBLOCK, INDEXW,
         $                    WORK, IWORK, IINFO )
             IF( IINFO.NE.0 ) THEN
                INFO = -1
                RETURN
             ENDIF
    *        Make sure that the entries M+1 to N in W, WERR, IBLOCK, INDEXW are 0
             DO 14 I = MM+1,N
                W( I ) = ZERO
                WERR( I ) = ZERO
                IBLOCK( I ) = 0
                INDEXW( I ) = 0
     14      CONTINUE
          END IF

    ***
    *     Loop over unreduced blocks
          IBEGIN = 1
          WBEGIN = 1
          DO 170 JBLK = 1, NSPLIT
             IEND = ISPLIT( JBLK )
             IN = IEND - IBEGIN + 1

    *        1 X 1 block
             IF( IN.EQ.1 ) THEN
                IF( (IRANGE.EQ.ALLRNG).OR.( (IRANGE.EQ.VALRNG).AND.
         $         ( D( IBEGIN ).GT.VL ).AND.( D( IBEGIN ).LE.VU ) )
         $        .OR. ( (IRANGE.EQ.INDRNG).AND.(IBLOCK(WBEGIN).EQ.JBLK))
         $        ) THEN
                   M = M + 1
                   W( M ) = D( IBEGIN )
                   WERR(M) = ZERO
    *              The gap for a single block doesn't matter for the later
    *              algorithm and is assigned an arbitrary large value
                   WGAP(M) = ZERO
                   IBLOCK( M ) = JBLK
                   INDEXW( M ) = 1
                   WBEGIN = WBEGIN + 1
                ENDIF
    *           E( IEND ) holds the shift for the initial RRR
                E( IEND ) = ZERO
                IBEGIN = IEND + 1
                GO TO 170
             END IF
    *
    *        Blocks of size larger than 1x1
    *
    *        E( IEND ) will hold the shift for the initial RRR, for now set it =0
             E( IEND ) = ZERO
    *
    *        Find local outer bounds GL,GU for the block
             GL = D(IBEGIN)
             GU = D(IBEGIN)
             DO 15 I = IBEGIN , IEND
                GL = MIN( GERS( 2*I-1 ), GL )
                GU = MAX( GERS( 2*I ), GU )
     15      CONTINUE
             SPDIAM = GU - GL

             IF(.NOT. ((IRANGE.EQ.ALLRNG).AND.(.NOT.FORCEB)) ) THEN
    *           Count the number of eigenvalues in the current block.
                MB = 0
                DO 20 I = WBEGIN,MM
                   IF( IBLOCK(I).EQ.JBLK ) THEN
                      MB = MB+1
                   ELSE
                      GOTO 21
                   ENDIF
     20         CONTINUE
     21         CONTINUE

                IF( MB.EQ.0) THEN
    *              No eigenvalue in the current block lies in the desired range
    *              E( IEND ) holds the shift for the initial RRR
                   E( IEND ) = ZERO
                   IBEGIN = IEND + 1
                   GO TO 170
                ELSE

    *              Decide whether dqds or bisection is more efficient
                   USEDQD = ( (MB .GT. FAC*IN) .AND. (.NOT.FORCEB) )
                   WEND = WBEGIN + MB - 1
    *              Calculate gaps for the current block
    *              In later stages, when representations for individual
    *              eigenvalues are different, we use SIGMA = E( IEND ).
                   SIGMA = ZERO
                   DO 30 I = WBEGIN, WEND - 1
                      WGAP( I ) = MAX( ZERO,
         $                        W(I+1)-WERR(I+1) - (W(I)+WERR(I)) )
     30            CONTINUE
                   WGAP( WEND ) = MAX( ZERO,
         $                     VU - SIGMA - (W( WEND )+WERR( WEND )))
    *              Find local index of the first and last desired evalue.
                   INDL = INDEXW(WBEGIN)
                   INDU = INDEXW( WEND )
                ENDIF
             ENDIF
             IF(( (IRANGE.EQ.ALLRNG) .AND. (.NOT. FORCEB) ).OR.USEDQD) THEN
    *           Case of DQDS
    *           Find approximations to the extremal eigenvalues of the block
                CALL DLARRK( IN, 1, GL, GU, D(IBEGIN),
         $               E2(IBEGIN), PIVMIN, RTL, TMP, TMP1, IINFO )
                IF( IINFO.NE.0 ) THEN
                   INFO = -1
                   RETURN
                ENDIF
                ISLEFT = MAX(GL, TMP - TMP1
         $               - HNDRD * EPS* ABS(TMP - TMP1))

                CALL DLARRK( IN, IN, GL, GU, D(IBEGIN),
         $               E2(IBEGIN), PIVMIN, RTL, TMP, TMP1, IINFO )
                IF( IINFO.NE.0 ) THEN
                   INFO = -1
                   RETURN
                ENDIF
                ISRGHT = MIN(GU, TMP + TMP1
         $                 + HNDRD * EPS * ABS(TMP + TMP1))
    *           Improve the estimate of the spectral diameter
                SPDIAM = ISRGHT - ISLEFT
             ELSE
    *           Case of bisection
    *           Find approximations to the wanted extremal eigenvalues
                ISLEFT = MAX(GL, W(WBEGIN) - WERR(WBEGIN)
         $                  - HNDRD * EPS*ABS(W(WBEGIN)- WERR(WBEGIN) ))
                ISRGHT = MIN(GU,W(WEND) + WERR(WEND)
         $                  + HNDRD * EPS * ABS(W(WEND)+ WERR(WEND)))
             ENDIF

    *        Decide whether the base representation for the current block
    *        L_JBLK D_JBLK L_JBLK^T = T_JBLK - sigma_JBLK I
    *        should be on the left or the right end of the current block.
    *        The strategy is to shift to the end which is "more populated"
    *        Furthermore, decide whether to use DQDS for the computation of
    *        the eigenvalue approximations at the end of DLARRE or bisection.
    *        dqds is chosen if all eigenvalues are desired or the number of
    *        eigenvalues to be computed is large compared to the blocksize.
             IF( ( IRANGE.EQ.ALLRNG ) .AND. (.NOT.FORCEB) ) THEN
    *           If all the eigenvalues have to be computed, we use dqd
                USEDQD = .TRUE.
    *           INDL is the local index of the first eigenvalue to compute
                INDL = 1
                INDU = IN
    *           MB =  number of eigenvalues to compute
                MB = IN
                WEND = WBEGIN + MB - 1
    *           Define 1/4 and 3/4 points of the spectrum
                S1 = ISLEFT + FOURTH * SPDIAM
                S2 = ISRGHT - FOURTH * SPDIAM
             ELSE
    *           DLARRD has computed IBLOCK and INDEXW for each eigenvalue
    *           approximation.
    *           choose sigma
                IF( USEDQD ) THEN
                   S1 = ISLEFT + FOURTH * SPDIAM
                   S2 = ISRGHT - FOURTH * SPDIAM
                ELSE
                   TMP = MIN(ISRGHT,VU) -  MAX(ISLEFT,VL)
                   S1 =  MAX(ISLEFT,VL) + FOURTH * TMP
                   S2 =  MIN(ISRGHT,VU) - FOURTH * TMP
                ENDIF
             ENDIF

    *        Compute the negcount at the 1/4 and 3/4 points
             IF(MB.GT.1) THEN
                CALL DLARRC( 'T', IN, S1, S2, D(IBEGIN),
         $                    E(IBEGIN), PIVMIN, CNT, CNT1, CNT2, IINFO)
             ENDIF

             IF(MB.EQ.1) THEN
                SIGMA = GL
                SGNDEF = ONE
             ELSEIF( CNT1 - INDL .GE. INDU - CNT2 ) THEN
                IF( ( IRANGE.EQ.ALLRNG ) .AND. (.NOT.FORCEB) ) THEN
                   SIGMA = MAX(ISLEFT,GL)
                ELSEIF( USEDQD ) THEN
    *              use Gerschgorin bound as shift to get pos def matrix
    *              for dqds
                   SIGMA = ISLEFT
                ELSE
    *              use approximation of the first desired eigenvalue of the
    *              block as shift
                   SIGMA = MAX(ISLEFT,VL)
                ENDIF
                SGNDEF = ONE
             ELSE
                IF( ( IRANGE.EQ.ALLRNG ) .AND. (.NOT.FORCEB) ) THEN
                   SIGMA = MIN(ISRGHT,GU)
                ELSEIF( USEDQD ) THEN
    *              use Gerschgorin bound as shift to get neg def matrix
    *              for dqds
                   SIGMA = ISRGHT
                ELSE
    *              use approximation of the first desired eigenvalue of the
    *              block as shift
                   SIGMA = MIN(ISRGHT,VU)
                ENDIF
                SGNDEF = -ONE
             ENDIF

    *        An initial SIGMA has been chosen that will be used for computing
    *        T - SIGMA I = L D L^T
    *        Define the increment TAU of the shift in case the initial shift
    *        needs to be refined to obtain a factorization with not too much
    *        element growth.
             IF( USEDQD ) THEN
    *           The initial SIGMA was to the outer end of the spectrum
    *           the matrix is definite and we need not retreat.
                TAU = SPDIAM*EPS*N + TWO*PIVMIN
             ELSE
                IF(MB.GT.1) THEN
                   CLWDTH = W(WEND) + WERR(WEND) - W(WBEGIN) - WERR(WBEGIN)
                   AVGAP = ABS(CLWDTH / DBLE(WEND-WBEGIN))
                   IF( SGNDEF.EQ.ONE ) THEN
                      TAU = HALF*MAX(WGAP(WBEGIN),AVGAP)
                      TAU = MAX(TAU,WERR(WBEGIN))
                   ELSE
                      TAU = HALF*MAX(WGAP(WEND-1),AVGAP)
                      TAU = MAX(TAU,WERR(WEND))
                   ENDIF
                ELSE
                   TAU = WERR(WBEGIN)
                ENDIF
             ENDIF
    *
             DO 80 IDUM = 1, MAXTRY
    *           Compute L D L^T factorization of tridiagonal matrix T - sigma I.
    *           Store D in WORK(1:IN), L in WORK(IN+1:2*IN), and reciprocals of
    *           pivots in WORK(2*IN+1:3*IN)
                DPIVOT = D( IBEGIN ) - SIGMA
                WORK( 1 ) = DPIVOT
                DMAX = ABS( WORK(1) )
                J = IBEGIN
                DO 70 I = 1, IN - 1
                   WORK( 2*IN+I ) = ONE / WORK( I )
                   TMP = E( J )*WORK( 2*IN+I )
                   WORK( IN+I ) = TMP
                   DPIVOT = ( D( J+1 )-SIGMA ) - TMP*E( J )
                   WORK( I+1 ) = DPIVOT
                   DMAX = MAX( DMAX, ABS(DPIVOT) )
                   J = J + 1
     70         CONTINUE
    *           check for element growth
                IF( DMAX .GT. MAXGROWTH*SPDIAM ) THEN
                   NOREP = .TRUE.
                ELSE
                   NOREP = .FALSE.
                ENDIF
                IF( USEDQD .AND. .NOT.NOREP ) THEN
    *              Ensure the definiteness of the representation
    *              All entries of D (of L D L^T) must have the same sign
                   DO 71 I = 1, IN
                      TMP = SGNDEF*WORK( I )
                      IF( TMP.LT.ZERO ) NOREP = .TRUE.
     71            CONTINUE
                ENDIF
                IF(NOREP) THEN
    *              Note that in the case of IRANGE=ALLRNG, we use the Gerschgorin
    *              shift which makes the matrix definite. So we should end up
    *              here really only in the case of IRANGE = VALRNG or INDRNG.
                   IF( IDUM.EQ.MAXTRY-1 ) THEN
                      IF( SGNDEF.EQ.ONE ) THEN
    *                    The fudged Gerschgorin shift should succeed
                         SIGMA =
         $                    GL - FUDGE*SPDIAM*EPS*N - FUDGE*TWO*PIVMIN
                      ELSE
                         SIGMA =
         $                    GU + FUDGE*SPDIAM*EPS*N + FUDGE*TWO*PIVMIN
                      END IF
                   ELSE
                      SIGMA = SIGMA - SGNDEF * TAU
                      TAU = TWO * TAU
                   END IF
                ELSE
    *              an initial RRR is found
                   GO TO 83
                END IF
     80      CONTINUE
    *        if the program reaches this point, no base representation could be
    *        found in MAXTRY iterations.
             INFO = 2
             RETURN

     83      CONTINUE
    *        At this point, we have found an initial base representation
    *        T - SIGMA I = L D L^T with not too much element growth.
    *        Store the shift.
             E( IEND ) = SIGMA
    *        Store D and L.
             CALL DCOPY( IN, WORK, 1, D( IBEGIN ), 1 )
             CALL DCOPY( IN-1, WORK( IN+1 ), 1, E( IBEGIN ), 1 )

             IF(MB.GT.1 ) THEN
    *
    *           Perturb each entry of the base representation by a small
    *           (but random) relative amount to overcome difficulties with
    *           glued matrices.
    *
                DO 122 I = 1, 4
                   ISEED( I ) = 1
     122        CONTINUE

                CALL DLARNV(2, ISEED, 2*IN-1, WORK(1))
                DO 125 I = 1,IN-1
                   D(IBEGIN+I-1) = D(IBEGIN+I-1)*(ONE+EPS*PERT*WORK(I))
                   E(IBEGIN+I-1) = E(IBEGIN+I-1)*(ONE+EPS*PERT*WORK(IN+I))
     125        CONTINUE
                D(IEND) = D(IEND)*(ONE+EPS*FOUR*WORK(IN))
    *
             ENDIF
    *
    *        Don't update the Gerschgorin intervals because keeping track
    *        of the updates would be too much work in DLARRV.
    *        We update W instead and use it to locate the proper Gerschgorin
    *        intervals.

    *        Compute the required eigenvalues of L D L' by bisection or dqds
             IF ( .NOT.USEDQD ) THEN
    *           If DLARRD has been used, shift the eigenvalue approximations
    *           according to their representation. This is necessary for
    *           a uniform DLARRV since dqds computes eigenvalues of the
    *           shifted representation. In DLARRV, W will always hold the
    *           UNshifted eigenvalue approximation.
                DO 134 J=WBEGIN,WEND
                   W(J) = W(J) - SIGMA
                   WERR(J) = WERR(J) + ABS(W(J)) * EPS
     134        CONTINUE
    *           call DLARRB to reduce eigenvalue error of the approximations
    *           from DLARRD
                DO 135 I = IBEGIN, IEND-1
                   WORK( I ) = D( I ) * E( I )**2
     135        CONTINUE
    *           use bisection to find EV from INDL to INDU
                CALL DLARRB(IN, D(IBEGIN), WORK(IBEGIN),
         $                  INDL, INDU, RTOL1, RTOL2, INDL-1,
         $                  W(WBEGIN), WGAP(WBEGIN), WERR(WBEGIN),
         $                  WORK( 2*N+1 ), IWORK, PIVMIN, SPDIAM,
         $                  IN, IINFO )
                IF( IINFO .NE. 0 ) THEN
                   INFO = -4
                   RETURN
                END IF
    *           DLARRB computes all gaps correctly except for the last one
    *           Record distance to VU/GU
                WGAP( WEND ) = MAX( ZERO,
         $           ( VU-SIGMA ) - ( W( WEND ) + WERR( WEND ) ) )
                DO 138 I = INDL, INDU
                   M = M + 1
                   IBLOCK(M) = JBLK
                   INDEXW(M) = I
     138        CONTINUE
             ELSE
    *           Call dqds to get all eigs (and then possibly delete unwanted
    *           eigenvalues).
    *           Note that dqds finds the eigenvalues of the L D L^T representation
    *           of T to high relative accuracy. High relative accuracy
    *           might be lost when the shift of the RRR is subtracted to obtain
    *           the eigenvalues of T. However, T is not guaranteed to define its
    *           eigenvalues to high relative accuracy anyway.
    *           Set RTOL to the order of the tolerance used in DLASQ2
    *           This is an ESTIMATED error, the worst case bound is 4*N*EPS
    *           which is usually too large and requires unnecessary work to be
    *           done by bisection when computing the eigenvectors
                RTOL = LOG(DBLE(IN)) * FOUR * EPS
                J = IBEGIN
                DO 140 I = 1, IN - 1
                   WORK( 2*I-1 ) = ABS( D( J ) )
                   WORK( 2*I ) = E( J )*E( J )*WORK( 2*I-1 )
                   J = J + 1
      140       CONTINUE
                WORK( 2*IN-1 ) = ABS( D( IEND ) )
                WORK( 2*IN ) = ZERO
                CALL DLASQ2( IN, WORK, IINFO )
                IF( IINFO .NE. 0 ) THEN
    *              If IINFO = -5 then an index is part of a tight cluster
    *              and should be changed. The index is in IWORK(1) and the
    *              gap is in WORK(N+1)
                   INFO = -5
                   RETURN
                ELSE
    *              Test that all eigenvalues are positive as expected
                   DO 149 I = 1, IN
                      IF( WORK( I ).LT.ZERO ) THEN
                         INFO = -6
                         RETURN
                      ENDIF
     149           CONTINUE
                END IF
                IF( SGNDEF.GT.ZERO ) THEN
                   DO 150 I = INDL, INDU
                      M = M + 1
                      W( M ) = WORK( IN-I+1 )
                      IBLOCK( M ) = JBLK
                      INDEXW( M ) = I
     150           CONTINUE
                ELSE
                   DO 160 I = INDL, INDU
                      M = M + 1
                      W( M ) = -WORK( I )
                      IBLOCK( M ) = JBLK
                      INDEXW( M ) = I
     160           CONTINUE
                END IF

                DO 165 I = M - MB + 1, M
    *              the value of RTOL below should be the tolerance in DLASQ2
                   WERR( I ) = RTOL * ABS( W(I) )
     165        CONTINUE
                DO 166 I = M - MB + 1, M - 1
    *              compute the right gap between the intervals
                   WGAP( I ) = MAX( ZERO,
         $                          W(I+1)-WERR(I+1) - (W(I)+WERR(I)) )
     166        CONTINUE
                WGAP( M ) = MAX( ZERO,
         $           ( VU-SIGMA ) - ( W( M ) + WERR( M ) ) )
             END IF
    *        proceed with next block
             IBEGIN = IEND + 1
             WBEGIN = WEND + 1
     170  CONTINUE
    *

          RETURN
    *
    *     end of DLARRE
    *
          END