DSBEV_2STAGE(3)
π DSBEV_2STAGE(3) π
okay so this is the Library Functions Manual entry for DSBEV_2STAGE, and bestie we are officially in LAPACK band-matrix eigenvalue territory. No cap, it's giving serious linear algebra main character energy. π¦
β¨ NAME β¨
/home/abuild/rpmbuild/BUILD/lapack-static-3.12.0-build/lapack-3.12.0/SRC/dsbev_2stage.f
that's the source-file path, exactly as listed. π
π SYNOPSIS π
π Functions/Subroutines π
subroutine DSBEV_2STAGE (jobz, uplo, n, kd, ab, ldab, w, z, ldz, work, lwork, info)β DSBEV_2STAGE computes the eigenvalues and, optionally, the left and/or right eigenvectors for OTHER matrices β¨
subroutine DSBEV_2STAGE (jobz, uplo, n, kd, ab, ldab, w, z, ldz, work,
lwork, info)
DSBEV_2STAGE computes the eigenvalues and, optionally, the left
and/or right eigenvectors for OTHER matrices
π§ Function/Subroutine Documentation π§
πΈ subroutine DSBEV_2STAGE πΈ
subroutine DSBEV_2STAGE (character jobz, character uplo, integer n, integer
kd, double precision, dimension( ldab, * ) ab, integer ldab, double
precision, dimension( * ) w, double precision, dimension( ldz, * ) z,
integer ldz, double precision, dimension( * ) work, integer lwork,
integer info)
DSBEV_2STAGE computes the eigenvalues and, optionally, the left and/or right eigenvectors for OTHER matrices π
π Purpose π
DSBEV_2STAGE computes all the eigenvalues and, optionally, eigenvectors of a real symmetric band matrix A using the 2stage technique for the reduction to tridiagonal. slay. β¨
π Parameters π
JOBZβJOBZ is CHARACTER*1;= 'N': Compute eigenvalues only;= 'V': Compute eigenvalues and eigenvectors. Not available in this release. πUPLOβUPLO is CHARACTER*1;= 'U': Upper triangle of A is stored;= 'L': Lower triangle of A is stored. π«ΆNβN is INTEGER; the order of the matrixA.N >= 0.KDβKD is INTEGER; the number of superdiagonals of the matrixAifUPLO = 'U', or the number of subdiagonals ifUPLO = 'L'.KD >= 0.ABβAB is DOUBLE PRECISION array, dimension (LDAB, N). On entry, the upper or lower triangle of the symmetric band matrixA, stored in the firstKD+1rows of the array. The j-th column ofAis stored in the j-th column of the arrayABas follows:
if UPLO = 'U', AB(kd+1+i-j,j) = A(i,j) for max(1,j-kd)<=i<=j;
if UPLO = 'L', AB(1+i-j,j) = A(i,j) for j<=i<=min(n,j+kd).
On exit, AB is overwritten by values generated during the reduction to tridiagonal form. If UPLO = 'U', the first superdiagonal and the diagonal of the tridiagonal matrix T are returned in rows KD and KD+1 of AB, and if UPLO = 'L', the diagonal and first subdiagonal of T are returned in the first two rows of AB. π₯
LDABβLDAB is INTEGER; the leading dimension of the arrayAB.LDAB >= KD + 1.WβW is DOUBLE PRECISION array, dimension (N). IfINFO = 0, the eigenvalues in ascending order. πZβZ is DOUBLE PRECISION array, dimension (LDZ, N). IfJOBZ = 'V', then ifINFO = 0,Zcontains the orthonormal eigenvectors of the matrixA, with the i-th column ofZholding the eigenvector associated withW(i). IfJOBZ = 'N', thenZis not referenced.LDZβLDZ is INTEGER; the leading dimension of the arrayZ.LDZ >= 1, and ifJOBZ = 'V',LDZ >= max(1,N).WORKβWORK is DOUBLE PRECISION array, dimension LWORK. On exit, ifINFO = 0,WORK(1)returns the optimalLWORK. β¨LWORKβLWORK is INTEGER; the length of the arrayWORK.LWORK >= 1, whenN <= 1; otherwise:- If
JOBZ = 'N'andN > 1,LWORKmust be queried. LWORK = MAX(1, dimension)wheredimension = (2KD+1)*N + KD*NTHREADS + NwhereKDis the size of the band.NTHREADSis the number of threads used when openMP compilation is enabled, otherwise=1.- If
JOBZ = 'V'andN > 1,LWORKmust be queried. Not yet available.
- If
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 message related to LWORK is issued by XERBLA. π
INFOβINFO is INTEGER:= 0: successful exit< 0: ifINFO = -i, the i-th argument had an illegal value> 0: ifINFO = i, the algorithm failed to converge; i off-diagonal elements of an intermediate tridiagonal form did not converge to zero. π
π Author π
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
π Further Details π
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
π Definition π
Definition at line 202 of file dsbev_2stage.f.
π Author π
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