SRC/dlarrd.f(3)
π¦ SRC/dlarrd.f π¦
okay so bestie, this is a page from the Library Functions Manual, and it's literally all about one little subroutine called dlarrd. she's an icon, she's a workhorse, and she lives in SRC/dlarrd.f. let's get into it π
β¨ SYNOPSIS β¨
πΈ Functions/Subroutines
subroutine dlarrd (range, order, n, vl, vu, il, iu, gers, reltol, d, e,
e2, pivmin, nsplit, isplit, m, w, werr, wl, wu, iblock, indexw,
work, iwork, info)
DLARRD computes the eigenvalues of a symmetric tridiagonal matrix to suitable accuracy. no cap, that's the whole vibe π
π₯ Function/Subroutine Documentation π₯
π subroutine dlarrd
the full signature, in all her glory:
subroutine dlarrd (character range, character order, integer n, double
precision vl, double precision vu, integer il, integer iu, double
precision, dimension( * ) gers, double precision reltol, double
precision, dimension( * ) d, double precision, dimension( * ) e, double
precision, dimension( * ) e2, double precision pivmin, integer nsplit,
integer, dimension( * ) isplit, integer m, double precision, dimension(
* ) w, double precision, dimension( * ) werr, double precision wl,
double precision wu, integer, dimension( * ) iblock, integer, dimension(
* ) indexw, double precision, dimension( * ) work, integer, dimension( *
) iwork, integer info)
DLARRD computes the eigenvalues of a symmetric tridiagonal matrix to suitable accuracy.
π Purpose:
DLARRD computes the eigenvalues of a symmetric tridiagonal matrix T to suitable accuracy. she's an auxiliary code β meaning she's the supporting character who gets called from DSTEMR. main character energy, honestly π«Ά
the user may ask for all eigenvalues, all eigenvalues in the half-open interval (VL, VU], or the IL-th through IU-th eigenvalues.
β οΈ overflow warning, fr fr: to avoid overflow, the matrix must be scaled so that its largest element is no greater than overflow**(1/2) * underflow**(1/4) in absolute value. and for greatest accuracy, it should not be much smaller than that. careful with her π
see W. Kahan, Report CS41, Computer Science Dept., Stanford University, July 21, 1966. iconic citation, we love a reference π
π Parameters
RANGEβRANGEisCHARACTER*1= 'A': ()all eigenvalues will be found.= 'V': ()all eigenvalues in the half-open interval(VL, VU]will be found.= 'I': ()theIL-th throughIU-th eigenvalues (of the entire matrix) will be found.
ORDERβORDERisCHARACTER*1= 'B': ()the eigenvalues will be grouped by split-off block (seeIBLOCK,ISPLIT) and ordered from smallest to largest within the block.= 'E': ()the eigenvalues for the entire matrix will be ordered from smallest to largest.
NβNisINTEGER. the order of the tridiagonal matrix T.N >= 0.VLβVLisDOUBLE PRECISION. ifRANGE='V', the lower bound of the interval to be searched for eigenvalues. eigenvalues less than or equal toVL, or greater thanVU, will not be returned.VL < VU. not referenced ifRANGE = 'A'or'I'.VUβVUisDOUBLE PRECISION. ifRANGE='V', the upper bound of the interval to be searched for eigenvalues. eigenvalues less than or equal toVL, or greater thanVU, will not be returned.VL < VU. not referenced ifRANGE = 'A'or'I'.ILβILisINTEGER. ifRANGE='I', the index of the smallest eigenvalue to be returned.1 <= IL <= IU <= N, ifN > 0;IL = 1andIU = 0ifN = 0. not referenced ifRANGE = 'A'or'V'.IUβIUisINTEGER. ifRANGE='I', the index of the largest eigenvalue to be returned.1 <= IL <= IU <= N, ifN > 0;IL = 1andIU = 0ifN = 0. not referenced ifRANGE = 'A'or'V'.GERSβGERSisDOUBLE PRECISIONarray, dimension(2*N). theNGerschgorin intervals β the i-th Gerschgorin interval is(GERS(2*i-1), GERS(2*i)).RELTOLβRELTOLisDOUBLE PRECISION. the minimum relative width of an interval. when an interval is narrower thanRELTOLtimes the larger (in magnitude) endpoint, then it is considered to be sufficiently small, i.e., converged. note: this should always be at leastradix*machine epsilon. bestie, do not skip that note πDβDisDOUBLE PRECISIONarray, dimension(N). thendiagonal elements of the tridiagonal matrix T.EβEisDOUBLE PRECISIONarray, dimension(N-1). the(n-1)off-diagonal elements of the tridiagonal matrix T.E2βE2isDOUBLE PRECISIONarray, dimension(N-1). the(n-1)squared off-diagonal elements of the tridiagonal matrix T.PIVMINβPIVMINisDOUBLE PRECISION. the minimum pivot allowed in the Sturm sequence for T.NSPLITβNSPLITisINTEGER. the number of diagonal blocks in the matrix T.1 <= NSPLIT <= N.ISPLITβISPLITisINTEGERarray, dimension(N). the splitting points, at which T breaks up into submatrices. the first submatrix consists of rows/columns1toISPLIT(1), the second of rows/columnsISPLIT(1)+1throughISPLIT(2), etc., and theNSPLIT-th consists of rows/columnsISPLIT(NSPLIT-1)+1throughISPLIT(NSPLIT)=N. (only the firstNSPLITelements will actually be used, but since the user cannot know a priori what valueNSPLITwill have,Nwords must be reserved forISPLIT.) π yeah she's a little greedy with memory, that's just how it isMβMisINTEGER. the actual number of eigenvalues found.0 <= M <= N. (see also the description ofINFO=2,3.)WβWisDOUBLE PRECISIONarray, dimension(N). on exit, the firstMelements ofWwill contain the eigenvalue approximations. DLARRD computes an intervalI_j = (a_j, b_j]that includes eigenvaluej. the eigenvalue approximation is given as the interval midpointW(j)= ( a_j + b_j)/2. the corresponding error is bounded byWERR(j) = abs( a_j - b_j)/2. midpoints ate, honestly πWERRβWERRisDOUBLE PRECISIONarray, dimension(N). the error bound on the corresponding eigenvalue approximation inW.WLβWLisDOUBLE PRECISION.WUβWUisDOUBLE PRECISION. the interval(WL, WU]contains all the wanted eigenvalues.- if
RANGE='V', thenWL=VLandWU=VU. - if
RANGE='A', thenWLandWUare the global Gerschgorin bounds on the spectrum. - if
RANGE='I', thenWLandWUare computed byDLAEBZfrom the index range specified.
- if
IBLOCKβIBLOCKisINTEGERarray, dimension(N). at each row/columnjwhereE(j)is zero or small, the matrix T is considered to split into a block diagonal matrix. on exit, ifINFO = 0,IBLOCK(i)specifies to which block (from 1 to the number of blocks) the eigenvalueW(i)belongs. (DLARRD may use the remainingN-Melements as workspace.) sneaky little workspace thief πINDEXWβINDEXWisINTEGERarray, dimension(N). the indices of the eigenvalues within each block (submatrix); for example,INDEXW(i)= jandIBLOCK(i)=kimply that the i-th eigenvalueW(i)is the j-th eigenvalue in blockk.WORKβWORKisDOUBLE PRECISIONarray, dimension(4*N).IWORKβIWORKisINTEGERarray, dimension(3*N).INFOβINFOisINTEGER= 0: successful exit π< 0: ifINFO = -i, the i-th argument had an illegal value> 0: some or all of the eigenvalues failed to converge or were not computed:=1 or 3: bisection failed to converge for some eigenvalues; these eigenvalues are flagged by a negative block number. the effect is that the eigenvalues may not be as accurate as the absolute and relative tolerances. this is generally caused by unexpectedly inaccurate arithmetic.=2 or 3:RANGE='I'only: not all of the eigenvaluesIL:IUwere found.- Effect:
M < IU+1-IL - Cause: non-monotonic arithmetic, causing the Sturm sequence to be non-monotonic.
- Cure: recalculate, using
RANGE='A', and pick out eigenvaluesIL:IU. in some cases, increasing thePARAMETERmay make things work.
- Effect:
= 4:RANGE='I', and the Gershgorin interval initially used was too small. no eigenvalues were computed.- Probable cause: your machine has sloppy floating-point arithmetic.
- Cure: increase the
PARAMETER, recompile, and try again.
π§ Internal Parameters:
(bestie hold that thought β there's more coming in part 2 π)
FUDGEβDOUBLE PRECISION,default = 2β¨ it's theAto widen the Gershgorin intervals. Ideally, a value of1should work, but on machines with sloppy arithmetic, this needs to be larger. The default for publicly released versions should be large enough to handle the worst machine around. Note that this has no effect on accuracy of the solution. π«Ά
πΈ Contributors: πΈ
- W. Kahan, University of California, Berkeley, USA
- 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
π Author π
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
Definition at line 325 of file dlarrd.f.
Author Generated automatically by Doxygen for LAPACK from the source code.
π okay that's literally the whole page, bestie β footer info is LAPACK Version 3.12.0, source SRC/dlarrd.f(3), and the date isn't in this snippet so I'm not inventing one, periodt π
π¦ where this page comes from
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