DSTEVR(3)
π DSTEVR(3) π
okay bestie, this is the DSTEVR(3) page from the Library Functions Manual, and we are folding the manual name in right here because the original header line is giving βpath soupβ energy. It's the LAPACK routine in dstevr.f, and it's lowkey iconic β¨
π NAME π
/home/abuild/rpmbuild/BUILD/lapack-static-3.12.0-build/lapack-3.12.0/SRC/dstevr.f β that's the file, bestie. The manual name is DSTEVR(3), and yes, we're folding it in near the top instead of copying that funky header line. π
β¨ SYNOPSIS β¨
π¦ Functions/Subroutines π¦
Here's the whole call, no cap:
subroutine DSTEVR (jobz, range, n, d, e, vl, vu, il, iu, abstol, m, w,
z, ldz, isuppz, work, lwork, iwork, liwork, info)
and the one-liner vibe is: DSTEVR computes the eigenvalues and, optionally, the left and/or right eigenvectors for OTHER matrices. periodt π
π Function/Subroutine Documentation π
Okay so the full signature, again, because this page is thorough and we respect that:
subroutine DSTEVR (character jobz, character range, integer n, double
precision, dimension( * ) d, double precision, dimension( * ) e, double
precision vl, double precision vu, integer il, integer iu, double
precision abstol, integer m, double precision, dimension( * ) w, double
precision, dimension( ldz, * ) z, integer ldz, integer, dimension( * )
isuppz, double precision, dimension( * ) work, integer lwork, integer,
dimension( * ) iwork, integer liwork, integer info)
DSTEVR computes the eigenvalues and, optionally, the left and/or right eigenvectors for OTHER matrices. (Yes, βOTHER matricesβ is literally what it says β we're not editing the lore.) π«Ά
π₯ Purpose π₯
Okay so the actual purpose, bestie: DSTEVR computes selected eigenvalues and, optionally, eigenvectors of a real symmetric tridiagonal matrix T. Eigenvalues and eigenvectors can be selected by specifying either a range of values or a range of indices for the desired eigenvalues. π
Whenever possible, DSTEVR calls DSTEMR to compute the eigenspectrum using Relatively Robust Representations. DSTEMR computes eigenvalues by the dqds algorithm, while orthogonal eigenvectors are computed from various 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 the i-th unreduced block of T:
- (a) Compute
T - sigma_i = L_i D_i L_i^T, such thatL_i D_i L_i^Tis a relatively robust representation. - (b) Compute the eigenvalues,
lambda_j, ofL_i D_i L_i^Tto high relative accuracy by the dqds algorithm. - (c) If there is a cluster of close eigenvalues,
sigma_iclose to the cluster, and go to step (a). - (d) Given the approximate eigenvalue
lambda_jofL_i D_i L_i^T, compute the corresponding eigenvector by forming a rank-revealing twisted factorization.
The desired accuracy of the output can be specified by the input parameter ABSTOL. β¨
For more details, see , by Inderjit Dhillon, Computer Science Division Technical Report No. UCB//CSD-97-971, UC Berkeley, May 1997. (Yes, the page really has that blank spot before βbyβ β we're preserving the whole vibe.) π¦
β οΈ Note 1:DSTEVRcallsDSTEMRwhen the full spectrum is requested on machines which conform to theieee-754floating point standard.DSTEVRcallsDSTEBZandDSTEINon non-ieee machines and when partial spectrum requests are made.
π Important warning: 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.
πΈ Parameters πΈ
JOBZβJOBZisCHARACTER*1.= 'N': Compute eigenvalues only;= 'V': Compute eigenvalues and eigenvectors. πRANGEβRANGEisCHARACTER*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 will be found. ForRANGE = 'V'or'I'andIU - IL < N - 1,DSTEBZandDSTEINare called. πNβNisINTEGER. The order of the matrix.N >= 0.DβDisDOUBLE PRECISIONarray, dimension(N). On entry, thendiagonal elements of the tridiagonal matrixA. On exit,Dmay be multiplied by a constant factor chosen to avoid over/underflow in computing the eigenvalues. π«ΆEβEisDOUBLE PRECISIONarray, dimension(max(1,N-1)). On entry, the(n-1)subdiagonal elements of the tridiagonal matrixAin elements1toN-1ofE. On exit,Emay be multiplied by a constant factor chosen to avoid over/underflow in computing the eigenvalues.VLβVLisDOUBLE PRECISION. IfRANGE='V', the lower bound of the interval to be searched for eigenvalues.VL < VU. Not referenced ifRANGE = 'A'or'I'.VUβVUisDOUBLE PRECISION. IfRANGE='V', the upper bound of the interval to be searched for eigenvalues.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'.ABSTOLβABSTOLisDOUBLE PRECISION. The absolute error tolerance for the eigenvalues. An approximate 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 precision. 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. π
See by Demmel and Kahan, LAPACK Working Note #3.
If high relative accuracy is important, set ABSTOL to DLAMCH( 'Safe minimum' ). Doing so will guarantee that eigenvalues are computed to high relative accuracy 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, , LAPACK Working Note #7, for a discussion of which matrices define their eigenvalues to high relative accuracy. π₯
MβMisINTEGER. The total number of eigenvalues found.0 <= M <= N. IfRANGE = 'A',M = N, and ifRANGE = 'I',M = IU-IL+1.WβWisDOUBLE PRECISIONarray, dimension(N). The firstMelements contain the selected eigenvalues in ascending order. πZβZisDOUBLE PRECISIONarray, dimension(LDZ, max(1,M) ). IfJOBZ = 'V', then ifINFO = 0, the firstMcolumns ofZcontain the orthonormal eigenvectors of the matrixAcorresponding to the selected eigenvalues, with the i-th column ofZholding the eigenvector associated withW(i). Note: the user must ensure that at leastmax(1,M)columns are supplied in the arrayZ; ifRANGE = 'V', the exact value ofMis not known in advance and an upper bound must be used. π¦LDZβLDZisINTEGER. The leading dimension of the arrayZ.LDZ >= 1, and ifJOBZ = 'V',LDZ >= max(1,N).ISUPPZβISUPPZisINTEGERarray, dimension( 2*max(1,M) ). The support of the eigenvectors inZ, i.e., the indices indicating the nonzero elements inZ. The i-th eigenvector is nonzero only in elementsISUPPZ( 2*i-1 )throughISUPPZ( 2*i ). Implemented only forRANGE = 'A'or'I'andIU - IL = N - 1. πWORKβWORKisDOUBLE PRECISIONarray, dimension(MAX(1,LWORK)). On exit, ifINFO = 0,WORK(1)returns the optimal (and minimal)LWORK. β¨LWORKβLWORKisINTEGER. The dimension of the arrayWORK.LWORK >= max(1,20*N). IfLWORK = -1, then a workspace query is assumed; the routine only calculates the optimal sizes of theWORKandIWORKarrays, returns these values as the first entries of theWORKandIWORKarrays, and no error message related toLWORKorLIWORKis issued byXERBLA. πIWORKβIWORKisINTEGERarray, dimension(MAX(1,LIWORK)). On exit, ifINFO = 0,IWORK(1)returns the optimal (and minimal)LIWORK.LIWORKβLIWORKisINTEGER. The dimension of the arrayIWORK.LIWORK >= max(1,10*N). IfLIWORK = -1, then a workspace query is assumed; the routine only calculates the optimal sizes of theWORKandIWORKarrays, returns these values as the first entries of theWORKandIWORKarrays, and no error message related toLWORKorLIWORKis issued byXERBLA. πINFOβINFOisINTEGER.= 0: successful exit.< 0: ifINFO = -i, the i-th argument had an illegal value.> 0: Internal error. π
π Author π
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
π Contributors: π
- Inderjit Dhillon, IBM Almaden, USA
- Osni Marques, LBNL/NERSC, USA
- Ken Stanley, Computer Science Division, University of California at Berkeley, USA
Definition at line 301 of file dstevr.f.
π AUTHOR π
ok so real talk β nobody sat down and hand-typed this page, bestie. It literally says:
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So the doc-bot read the source and spat out the whole thing. That's the entire author section β no mysterious human to @, no credit to give out, just Doxygen doing its little automated thing π¦
and that's a wrap on this one π«Ά the whole page comes courtesy of LAPACK, Version 3.12.0, documented from dstevr.f(3) β that's the source file path the footer was pointing at the whole time. Version and date, right there in the fine print, slay β¨ go forth and read your eigenvalues in peace, ily, periodt π
π
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