SRC/cheevr_2stage.f(3)
πΈ NAME πΈ
From the Library Functions Manual, bestie: this is SRC/cheevr_2stage.f(3) β the cheevr_2stage routine. π
β¨ SYNOPSIS β¨
π§ Functions/Subroutines π§
subroutine cheevr_2stage (jobz, range, uplo, n, a, lda, vl, vu, il, iu,
abstol, m, w, z, ldz, isuppz, work, lwork, rwork, lrwork, iwork,
liwork, info)
The one-liner is literally: CHEEVR_2STAGE computes the eigenvalues and, optionally, the left and/or right eigenvectors for HE matrices. π
π Function/Subroutine Documentation π
Here's the full signature in its natural habitat:
subroutine cheevr_2stage (character jobz, character range, character uplo,
integer n, complex, dimension( lda, * ) a, integer lda, real vl, real
vu, integer il, integer iu, real abstol, integer m, real, dimension( * )
w, complex, dimension( ldz, * ) z, integer ldz, integer, dimension( * )
isuppz, complex, dimension( * ) work, integer lwork, real, dimension( *
) rwork, integer lrwork, integer, dimension( * ) iwork, integer liwork,
integer info)
And the official vibe: CHEEVR_2STAGE computes the eigenvalues and, optionally, the left and/or right eigenvectors for HE matrices. β¨
π Purpose π
Okay so, CHEEVR_2STAGE computes selected eigenvalues and, optionally, eigenvectors of a complex Hermitian matrix A using the 2stage technique for the reduction to tridiagonal. Eigenvalues and eigenvectors can be selected by specifying either a range of values or a range of indices for the desired eigenvalues.
CHEEVR_2STAGE first reduces the matrix A to tridiagonal form T with a call to CHETRD. Then, whenever possible, CHEEVR_2STAGE calls CSTEMR to compute eigenspectrum using Relatively Robust Representations. CSTEMR 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 each unreduced block (submatrix) of T:
- (a) Compute
T - sigma I = L D L^T, so thatLandDdefine all the wanted eigenvalues to high relative accuracy. This means that small relative changes in the entries ofDandLcause only small relative changes in the eigenvalues and eigenvectors. The standard (unfactored) representation of the tridiagonal matrixTdoes 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 compute 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 CSTEMR's documentation and:
- Inderjit S. Dhillon and Beresford N. Parlett: Linear Algebra and its Applications, 387(1), pp. 1-28, August 2004.
- Inderjit Dhillon and Beresford Parlett: SIAM Journal on Matrix Analysis and Applications, Vol. 25, 2004. Also LAPACK Working Note 154.
- Inderjit Dhillon: , Computer Science Division Technical Report No. UCB/CSD-97-971, UC Berkeley, May 1997.
Note 1 :CHEEVR_2STAGEcallsCSTEMRwhen the full spectrum is requested on machines which conform to the ieee-754 floating point standard.CHEEVR_2STAGEcallsSSTEBZandCSTEINon non-ieee machines and when partial spectrum requests are made.
β οΈ Heads up: Normal execution of CSTEMR 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.
π¦ Parameters π¦
JOBZ
JOBZ is CHARACTER*1.
= 'N': Compute eigenvalues only;= 'V': Compute eigenvalues and eigenvectors. Not available in this release.
RANGE
RANGE is CHARACTER*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.
For RANGE = 'V' or 'I' and IU - IL < N - 1, SSTEBZ and CSTEIN are called.
UPLO
UPLO is CHARACTER*1.
= 'U': Upper triangle ofAis stored;= 'L': Lower triangle ofAis stored.
N
N is INTEGER. The order of the matrix A. N >= 0.
A
A is COMPLEX array, dimension (LDA, N).
On entry, the Hermitian 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. π
LDA
LDA is INTEGER. The leading dimension of the array A. LDA >= max(1,N).
VL
VL is REAL. If RANGE='V', the lower bound of the interval to be searched for eigenvalues. VL < VU. Not referenced if RANGE = 'A' or 'I'.
VU
VU is REAL. If RANGE='V', the upper bound of the interval to be searched for eigenvalues. VL < VU. Not referenced if RANGE = 'A' or 'I'.
IL
IL is INTEGER. If RANGE='I', the index of the smallest eigenvalue 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'.
IU
IU is INTEGER. If RANGE='I', the index of the largest eigenvalue 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
ABSTOL is REAL. 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.
See by Demmel and Kahan, LAPACK Working Note #3.
If high relative accuracy is important, set ABSTOL to SLAMCH( '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.
M
M is INTEGER. The total number of eigenvalues found. 0 <= M <= N. If RANGE = 'A', M = N, and if RANGE = 'I', M = IU-IL+1.
W
W is REAL array, dimension (N). The first M elements contain the selected eigenvalues in ascending order.
Z
Z is COMPLEX array, dimension (LDZ, max(1,M)).
If JOBZ = 'V', then if INFO = 0, the first M columns of Z contain 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 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
LDZ
LDZ is INTEGER. The leading dimension of the array Z. LDZ >= 1, and if JOBZ = 'V', LDZ >= max(1,N).
ISUPPZ
ISUPPZ is INTEGER array, dimension ( 2*max(1,M) ). The support of the eigenvectors in Z, i.e., the indices indicating the nonzero elements in Z. The i-th eigenvector is nonzero only in elements ISUPPZ( 2*i-1 ) through ISUPPZ( 2*i ). This is an output of CSTEMR (tridiagonal matrix). The support of the eigenvectors of A is typically 1:N because of the unitary transformations applied by CUNMTR. Implemented only for RANGE = 'A' or 'I' and IU - IL = N - 1.
WORK
WORK is COMPLEX array, dimension (MAX(1,LWORK)). On exit, if INFO = 0, WORK(1) returns the optimal LWORK.
LWORK
LWORK β okay bestie, LWORK is INTEGER. It's literally the dimension of the array WORK. If N <= 1, LWORK must be at least 1. If JOBZ = 'N' and N > 1, LWORK must be queried. π«Ά
LWORK = MAX(1, 26*N, dimension) where
dimension = max(stage1,stage2) + (KD+1)*N + N
= N*KD + N*max(KD+1,FACTOPTNB)
+ max(2*KD*KD, KD*NTHREADS)
+ (KD+1)*N + N
where KD is the blocking size of the reduction, FACTOPTNB is the blocking used by the QR or LQ algorithm, usually FACTOPTNB=128 is a good choice, and NTHREADS is the number of threads used when openMP compilation is enabled, otherwise =1.
IfJOBZ = 'V'andN > 1,LWORKmust be queried. Not yet available. π¨
If LWORK = -1, then a workspace query is assumed; the routine only calculates the optimal sizes of the WORK, RWORK and IWORK arrays, returns these values as the first entries of the WORK, RWORK and IWORK arrays, and no error message related to LWORK or LRWORK or LIWORK is issued by XERBLA. β¨
RWORKβRWORKisREALarray, dimension(MAX(1,LRWORK)). On exit, ifINFO = 0,RWORK(1)returns the optimal (and minimal)LRWORK. πLRWORKβLRWORKisINTEGER. The length of the arrayRWORK. IfN <= 1,LRWORK >= 1, elseLRWORK >= 24*N.
If LRWORK = -1, then a workspace query is assumed; the routine only calculates the optimal sizes of the WORK, RWORK and IWORK arrays, returns these values as the first entries of the WORK, RWORK and IWORK arrays, and no error message related to LWORK or LRWORK or LIWORK is issued by XERBLA.
IWORKβIWORKisINTEGERarray, dimension(MAX(1,LIWORK)). On exit, ifINFO = 0,IWORK(1)returns the optimal (and minimal)LIWORK. πLIWORKβLIWORKisINTEGER. The dimension of the arrayIWORK. IfN <= 1,LIWORK >= 1, elseLIWORK >= 10*N.
If LIWORK = -1, then a workspace query is assumed; the routine only calculates the optimal sizes of the WORK, RWORK and IWORK arrays, returns these values as the first entries of the WORK, RWORK and IWORK arrays, and no error message related to LWORK or LRWORK or LIWORK is issued by XERBLA.
INFOβINFOisINTEGER.= 0: successful exit β< 0: ifINFO = -i, the i-th argument had an illegal value π> 0: Internal error π
π Author
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
π Contributors:
- 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
π₯ Further Details:
All details about the 2stage techniques are available in:
Azzam Haidar, Hatem Ltaief, and Jack Dongarra. Parallel reduction to condensed forms for symmetric eigenvalue problems using aggregated fine-grained and memory-aware kernels. In Proceedings of 2011 International Conference for High Performance Computing, Networking, Storage and Analysis (SC '11), New York, NY, USA, Article 8 , 11 pages. http://doi.acm.org/10.1145/2063384.2063394
A. Haidar, J. Kurzak, P. Luszczek, 2013. An improved parallel singular value algorithm and its implementation for multicore hardware, In Proceedings of 2013 International Conference for High Performance Computing, Networking, Storage and Analysis (SC '13). Denver, Colorado, USA, 2013. Article 90, 12 pages. http://doi.acm.org/10.1145/2503210.2503292
A. Haidar, R. Solca, S. Tomov, T. Schulthess and J. Dongarra. A novel hybrid CPU-GPU generalized eigensolver for electronic structure calculations based on fine-grained memory aware tasks. International Journal of High Performance Computing Applications. Volume 28 Issue 2, Pages 196-209, May 2014. http://hpc.sagepub.com/content/28/2/196
Definition at line 405 of file cheevr_2stage.f. π
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