hbevx_2stage(3)
π hbevx_2stage(3) β Library Functions Manual π
okay so this is the hbevx_2stage(3) page β manual name folded near the top, bestie. It's {hb,sb}evx_2stage: eig, bisection, and we're in part 1 of 5. π
πΈ NAME πΈ
hbevx_2stage β {hb,sb}evx_2stage: eig, bisection
β¨ SYNOPSIS β¨
π«Ά Functions π«Ά
chbevx_2stageβ CHBEVX_2STAGE computes the eigenvalues and, optionally, the left and/or right eigenvectors for OTHER matrices
subroutine chbevx_2stage (jobz, range, uplo, n, kd, ab, ldab, q, ldq, vl, vu, il, iu, abstol, m, w, z, ldz, work, lwork, rwork, iwork, ifail, info)
dsbevx_2stageβ DSBEVX_2STAGE computes the eigenvalues and, optionally, the left and/or right eigenvectors for OTHER matrices
subroutine dsbevx_2stage (jobz, range, uplo, n, kd, ab, ldab, q, ldq, vl, vu, il, iu, abstol, m, w, z, ldz, work, lwork, iwork, ifail, info)
ssbevx_2stageβ SSBEVX_2STAGE computes the eigenvalues and, optionally, the left and/or right eigenvectors for OTHER matrices
subroutine ssbevx_2stage (jobz, range, uplo, n, kd, ab, ldab, q, ldq, vl, vu, il, iu, abstol, m, w, z, ldz, work, lwork, iwork, ifail, info)
zhbevx_2stageβ ZHBEVX_2STAGE computes the eigenvalues and, optionally, the left and/or right eigenvectors for OTHER matrices
subroutine zhbevx_2stage (jobz, range, uplo, n, kd, ab, ldab, q, ldq, vl, vu, il, iu, abstol, m, w, z, ldz, work, lwork, rwork, iwork, ifail, info)
π¦ Detailed Description π¦
(The original page doesn't add extra paragraphs here, bestie β it heads straight into the function documentation.)
π Function Documentation π
π subroutine chbevx_2stage π
subroutine chbevx_2stage (jobz, range, uplo, n, kd, ab, ldab, q, ldq, vl, vu, il, iu, abstol, m, w, z, ldz, work, lwork, rwork, iwork, ifail, info)
CHBEVX_2STAGE computes the eigenvalues and, optionally, the left and/or right eigenvectors for OTHER matrices.
π― Purpose π―
CHBEVX_2STAGE computes selected eigenvalues and, optionally, eigenvectors of a complex Hermitian band 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.
π Parameters π
JOBZβJOBZisCHARACTER*1= 'N': Compute eigenvalues only;= 'V': Compute eigenvalues and eigenvectors. Not available in this release.
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 will be found.
UPLOβUPLOisCHARACTER*1= 'U': Upper triangle of A is stored;= 'L': Lower triangle of A is stored.
NβNisINTEGER. The order of the matrix A.N >= 0.KDβKDisINTEGER. The number of superdiagonals of the matrix A ifUPLO = 'U', or the number of subdiagonals ifUPLO = 'L'.KD >= 0.ABβABisCOMPLEX array, dimension (LDAB, N). On entry, the upper or lower triangle of the Hermitian band matrix A, stored in the firstKD+1rows of the array. The j-th column of A is stored in the j-th column of the array AB as 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.
LDABβLDABisINTEGER. The leading dimension of the array AB.LDAB >= KD + 1.QβQisCOMPLEX array, dimension (LDQ, N). IfJOBZ = 'V', theN-by-Nunitary matrix used in the reduction to tridiagonal form. IfJOBZ = 'N', the array Q is not referenced.LDQβLDQisINTEGER. The leading dimension of the array Q. IfJOBZ = 'V', thenLDQ >= max(1,N).VLβVLisREAL. IfRANGE='V', the lower bound of the interval to be searched for eigenvalues.VL < VU. Not referenced ifRANGE = 'A'or'I'.VUβVUisREAL. 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'.ABSTOLβABSTOLisREAL. 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 AB to tridiagonal form.
Eigenvalues will be computed most accurately when ABSTOL is set to twice the underflow threshold 2*SLAMCH('S'), not zero. If this routine returns with INFO>0, indicating that some eigenvectors did not converge, try setting ABSTOL to 2*SLAMCH('S').
See by Demmel and Kahan, LAPACK Working Note #3.
MβMisINTEGER. The total number of eigenvalues found.0 <= M <= N. IfRANGE = 'A',M = N, and ifRANGE = 'I',M = IU-IL+1.WβWisREAL array, dimension (N). The firstMelements contain the selected eigenvalues in ascending order.ZβZisCOMPLEX array, dimension (LDZ, max(1,M)). IfJOBZ = 'V', then ifINFO = 0, the firstMcolumns 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 withW(i). If an eigenvector fails to converge, then that column of Z contains the latest approximation to the eigenvector, and the index of the eigenvector is returned inIFAIL. IfJOBZ = 'N', then Z is not referenced. Note: the user must ensure that at leastmax(1,M)columns are supplied in the array Z; ifRANGE = 'V', the exact value of M is not known in advance and an upper bound must be used.LDZβLDZisINTEGER. The leading dimension of the array Z.LDZ >= 1, and ifJOBZ = 'V',LDZ >= max(1,N).WORKβWORKisCOMPLEX array, dimension (LWORK).LWORKβLWORKisINTEGER. The length of the array WORK.LWORK >= 1, whenN <= 1; otherwise: IfJOBZ = 'N'andN > 1,LWORKmust be queried.
LWORK = MAX(1, dimension) where
dimension = (2KD+1)*N + KD*NTHREADS
where KD is the size of the band.
NTHREADS is the number of threads used when
openMP compilation is enabled, otherwise =1.
If JOBZ = 'V' and N > 1, LWORK must be queried. Not yet available.
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.
RWORKβRWORKisREAL array, dimension (7*N).IWORKβIWORKisINTEGER array, dimension (5*N).IFAILβIFAILisINTEGER array, dimension (N). IfJOBZ = 'V', then ifINFO = 0, the firstMelements ofIFAILare zero. IfINFO > 0, thenIFAILcontains the indices of the eigenvectors that failed to converge. IfJOBZ = 'N', thenIFAILis not referenced.INFOβINFOisINTEGER= 0: successful exit< 0: ifINFO = -i, the i-th argument had an illegal value> 0: ifINFO = i, then i eigenvectors failed to converge. Their indices are stored in arrayIFAIL.
π Author π
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
π Further Details π
and before we move on, here are the papers that explain all the 2stage tea βοΈπ (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 323 of file chbevx_2stage.f.
okay bestie, next up is dsbevx_2stage β she computes the eigenvalues and, optionally, the left and/or right eigenvectors for OTHER matrices, and she's literally iconic π
π₯
subroutine dsbevx_2stage (character jobz, character range, character uplo,
integer n, integer kd, double precision, dimension( ldab, * ) ab,
integer ldab, double precision, dimension( ldq, * ) q, integer ldq,
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, double precision,
dimension( * ) work, integer lwork, integer, dimension( * ) iwork,
integer, dimension( * ) ifail, integer info)
Purpose
DSBEVX_2STAGE computes selected eigenvalues and, optionally, eigenvectors of a real symmetric band 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. It's giving customizable eigenvalue realness β you pick what you want, she finds it β¨
Parameters
JOBZβJOBZ is CHARACTER*1= 'N':compute eigenvalues only;= 'V':compute eigenvalues and eigenvectors. Not available in this release π
RANGEβRANGE 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.
UPLOβUPLO is CHARACTER*1= 'U':upper triangle of A is stored;= 'L':lower triangle of A is stored.
NβN is INTEGER- The order of the matrix A.
N >= 0.
- The order of the matrix A.
KDβKD is INTEGER- The number of superdiagonals of the matrix A if
UPLO = 'U', or the number of subdiagonals ifUPLO = 'L'.KD >= 0.
- The number of superdiagonals of the matrix A if
ABβAB is DOUBLE PRECISION array, dimension (LDAB, N)- On entry, the upper or lower triangle of the symmetric band matrix A, stored in the first
KD+1rows of the array. The j-th column of A is stored in the j-th column of the array AB as follows:- if
UPLO = 'U',AB(kd+1+i-j,j) = A(i,j)formax(1,j-kd)<=i<=j; - if
UPLO = 'L',AB(1+i-j,j) = A(i,j)forj<=i<=min(n,j+kd).
- if
- 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 rowsKDandKD+1of AB, and ifUPLO = 'L', the diagonal and first subdiagonal of T are returned in the first two rows of AB.
- On entry, the upper or lower triangle of the symmetric band matrix A, stored in the first
LDABβLDAB is INTEGER- The leading dimension of the array AB.
LDAB >= KD + 1.
- The leading dimension of the array AB.
QβQ is DOUBLE PRECISION array, dimension (LDQ, N)- If
JOBZ = 'V', the N-by-N orthogonal matrix used in the reduction to tridiagonal form. - If
JOBZ = 'N', the array Q is not referenced.
- If
LDQβLDQ is INTEGER- The leading dimension of the array Q. If
JOBZ = 'V', thenLDQ >= max(1,N).
- The leading dimension of the array Q. If
VLβVL is DOUBLE PRECISION- If
RANGE='V', the lower bound of the interval to be searched for eigenvalues.VL < VU. Not referenced ifRANGE = 'A'or'I'.
- If
VUβVU is DOUBLE PRECISION- If
RANGE='V', the upper bound of the interval to be searched for eigenvalues.VL < VU. Not referenced ifRANGE = 'A'or'I'.
- If
ILβIL is INTEGER- If
RANGE='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'.
- If
IUβIU is INTEGER- If
RANGE='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'.
- If
ABSTOLβABSTOL is DOUBLE 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 toABSTOL + EPS * max( |a|,|b| ) ,whereEPSis the machine precision. IfABSTOLis less than or equal to zero, thenEPS*|T|will be used in its place, where|T|is the 1-norm of the tridiagonal matrix obtained by reducing AB to tridiagonal form. - Eigenvalues will be computed most accurately when
ABSTOLis set to twice the underflow threshold2*DLAMCH('S'), not zero. If this routine returns withINFO>0, indicating that some eigenvectors did not converge, try settingABSTOLto2*DLAMCH('S'). - See by Demmel and Kahan, LAPACK Working Note #3.
- The absolute error tolerance for the eigenvalues. An approximate eigenvalue is accepted as converged when it is determined to lie in an interval
MβM is INTEGER- The total number of eigenvalues found.
0 <= M <= N. IfRANGE = 'A',M = N, and ifRANGE = 'I',M = IU-IL+1.
- The total number of eigenvalues found.
WβW is DOUBLE PRECISION array, dimension (N)- The first
Melements contain the selected eigenvalues in ascending order.
- The first
ZβZ is DOUBLE PRECISION array, dimension (LDZ, max(1,M))- If
JOBZ = 'V', then ifINFO = 0, the firstMcolumns 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 withW(i). If an eigenvector fails to converge, then that column of Z contains the latest approximation to the eigenvector, and the index of the eigenvector is returned inIFAIL. IfJOBZ = 'N', then Z is not referenced. - Note: the user must ensure that at least
max(1,M)columns are supplied in the array Z; ifRANGE = 'V', the exact value ofMis not known in advance and an upper bound must be used.
- If
LDZβLDZ is INTEGER- The leading dimension of the array Z.
LDZ >= 1, and ifJOBZ = 'V',LDZ >= max(1,N).
- The leading dimension of the array Z.
WORKβWORK is DOUBLE PRECISION array, dimension (LWORK)LWORKβLWORK is INTEGER- The length of the array WORK.
LWORK >= 1, whenN <= 1; otherwise:- If
JOBZ = 'N'andN > 1, LWORK must be queried.
- If
- The length of the array WORK.
LWORK = MAX(1, 7*N, dimension) where
dimension = (2KD+1)*N + KD*NTHREADS + 2*N
where KD is the size of the band.
NTHREADS is the number of threads used when
openMP compilation is enabled, otherwise =1.
- If
JOBZ = 'V'andN > 1, LWORK must be queried. Not yet available.
- 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.
IWORKβIWORK is INTEGER array, dimension (5*N)IFAILβIFAIL is INTEGER array, dimension (N)- If
JOBZ = 'V', then ifINFO = 0, the firstMelements of IFAIL are zero. IfINFO > 0, then IFAIL contains the indices of the eigenvectors that failed to converge. IfJOBZ = 'N', then IFAIL is not referenced.
- If
INFOβINFO is INTEGER= 0:successful exit.< 0:ifINFO = -i, the i-th argument had an illegal value.> 0:ifINFO = i, then i eigenvectors failed to converge. Their indices are stored in array IFAIL.
Author
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
Further Details
(this section is empty in the original, but we're leaving it here for completeness π )
okay so before we jump into the next subroutine, the authors left us a whole reading list β the ~lore~ β all about the 2stage techniques. πβ¨ No cap, these are the receipts:
- 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 319 of file dsbevx_2stage.f.
π subroutine ssbevx_2stage β the single-precision sibling
subroutine ssbevx_2stage (character jobz, character range, character uplo,
integer n, integer kd, real, dimension( ldab, * ) ab, integer ldab,
real, dimension( ldq, * ) q, integer ldq, real vl, real vu, integer il,
integer iu, real abstol, integer m, real, dimension( * ) w, real,
dimension( ldz, * ) z, integer ldz, real, dimension( * ) work, integer
lwork, integer, dimension( * ) iwork, integer, dimension( * ) ifail,
integer info)
SSBEVX_2STAGE computes the eigenvalues and, optionally, the left and/or right eigenvectors for OTHER matrices π
π― Purpose
SSBEVX_2STAGE computes selected eigenvalues and, optionally, eigenvectors of a real symmetric band 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.
Translating from manpage-ese, bestie: it's the real symmetric band matrix girlie, and she uses the two-stage pipeline to get down to tridiagonal form. You can pick your eigenvalues by value range or by index range, your call πΈ
πΈ Parameters
JOBZisCHARACTER*1= 'N': compute eigenvalues only;= 'V': compute eigenvalues and eigenvectors. Not available in this release. π
RANGEisCHARACTER*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.
UPLOisCHARACTER*1= 'U': upper triangle of A is stored;= 'L': lower triangle of A is stored.
NisINTEGERβ the order of the matrix A.N >= 0.KDisINTEGERβ the number of superdiagonals of the matrix A ifUPLO = 'U', or the number of subdiagonals ifUPLO = 'L'.KD >= 0. (Think of it as how thicc the band is π)ABisREAL array, dimension (LDAB, N)- On entry: the upper or lower triangle of the symmetric band matrix A, stored in the first
KD+1rows of the array. The j-th column of A is stored in the j-th column of the array AB as 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 rowsKDandKD+1of AB, and ifUPLO = 'L', the diagonal and first subdiagonal of T are returned in the first two rows of AB. (So yeah β your input gets yeeted, plan accordingly π)
- On entry: the upper or lower triangle of the symmetric band matrix A, stored in the first
LDABisINTEGERβ the leading dimension of the array AB.LDAB >= KD + 1.QisREAL array, dimension (LDQ, N)- If
JOBZ = 'V', theN-by-Northogonal matrix used in the reduction to tridiagonal form. - If
JOBZ = 'N', the array Q is not referenced.
- If
LDQisINTEGERβ the leading dimension of the array Q. IfJOBZ = 'V', thenLDQ >= max(1,N).VLisREALβ ifRANGE='V', the lower bound of the interval to be searched for eigenvalues.VL < VU. Not referenced ifRANGE = 'A'or'I'.VUisREALβ ifRANGE='V', the upper bound of the interval to be searched for eigenvalues.VL < VU. Not referenced ifRANGE = 'A'or'I'.ILisINTEGERβ 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'.IUisINTEGERβ 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'.ABSTOLisREALβ 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 AB to tridiagonal form.
- Eigenvalues will be computed most accurately when
ABSTOLis set to twice the underflow threshold2*SLAMCH('S'), not zero. If this routine returns withINFO>0, indicating that some eigenvectors did not converge, try settingABSTOLto2*SLAMCH('S'). π₯ - See by Demmel and Kahan, LAPACK Working Note #3.
MisINTEGERβ the total number of eigenvalues found.0 <= M <= N. IfRANGE = 'A',M = N, and ifRANGE = 'I',M = IU-IL+1.WisREAL array, dimension (N)β the firstMelements contain the selected eigenvalues in ascending order. βZisREAL array, dimension (LDZ, max(1,M))- If
JOBZ = 'V', then ifINFO = 0, the firstMcolumns 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 withW(i). - If an eigenvector fails to converge, then that column of Z contains the latest approximation to the eigenvector, and the index of the eigenvector is returned in
IFAIL. - If
JOBZ = 'N', then Z is not referenced. - Note: the user must ensure that at least
max(1,M)columns are supplied in the array Z; ifRANGE = 'V', the exact value ofMis not known in advance and an upper bound must be used. (iykyk β guess big, bestie π«Ά)
- If
LDZisINTEGERβ the leading dimension of the array Z.LDZ >= 1, and ifJOBZ = 'V',LDZ >= max(1,N).WORKisREAL array, dimension (LWORK).LWORKisINTEGERβ the length of the array WORK.LWORK >= 1, whenN <= 1; otherwise:- If
JOBZ = 'N'andN > 1,LWORKmust be queried.
- If
LWORK = MAX(1, 7*N, dimension) where
dimension = (2KD+1)*N + KD*NTHREADS + 2*N
where KD is the size of the band.
NTHREADS is the number of threads used when
openMP compilation is enabled, otherwise =1.
- If
JOBZ = 'V'andN > 1,LWORKmust be queried. Not yet available π
IfLWORK = -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 toLWORKis issued byXERBLA. (the classic "just tell me how much room you need" move π
IWORKisINTEGER array, dimension (5*N).IFAILisINTEGER array, dimension (N)- If
JOBZ = 'V', then ifINFO = 0, the firstMelements ofIFAILare zero. IfINFO > 0, thenIFAILcontains the indices of the eigenvectors that failed to converge. - If
JOBZ = 'N', thenIFAILis not referenced.
- If
INFOisINTEGER= 0: successful exit. π< 0: ifINFO = -i, the i-th argument had an illegal value. π> 0: ifINFO = i, thenieigenvectors failed to converge. Their indices are stored in arrayIFAIL.
π Author
Univ. of Tennessee
Univ. of California Berkeley
Univ. of Colorado Denver
NAG Ltd.
π§ Further Details:
All details about the 2stage techniques are available in these papers, bestie β here are the receipts: π§Ύβ¨
- 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 319 of file ssbevx_2stage.f.
subroutine zhbevx_2stage (character jobz, character range, character uplo,
integer n, integer kd, complex*16, dimension( ldab, * ) ab, integer
ldab, complex*16, dimension( ldq, * ) q, integer ldq, double precision
vl, double precision vu, integer il, integer iu, double precision
abstol, integer m, double precision, dimension( * ) w, complex*16,
dimension( ldz, * ) z, integer ldz, complex*16, dimension( * ) work,
integer lwork, double precision, dimension( * ) rwork, integer,
dimension( * ) iwork, integer, dimension( * ) ifail, integer info)
ZHBEVX_2STAGE computes the eigenvalues and, optionally, the left and/or right eigenvectors for OTHER matrices ππ₯
Purpose π
Okay so ZHBEVX_2STAGE computes selected eigenvalues and, optionally, eigenvectors of a complex Hermitian band matrix A using the 2stage technique for the reduction to tridiagonal. You can pick which eigenvalues you want by specifying either a range of values or a range of indices for the desired eigenvalues β iconic flexibility, no cap. β¨
Parameters π
JOBZβCHARACTER*1.= 'N': compute eigenvalues only;= 'V': compute eigenvalues and eigenvectors. Not available in this release.RANGEβCHARACTER*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.UPLOβCHARACTER*1.= 'U': upper triangle ofAis stored;= 'L': lower triangle ofAis stored.NβINTEGER. The order of the matrixA.N >= 0.KDβINTEGER. The number of superdiagonals of the matrixAifUPLO = 'U', or the number of subdiagonals ifUPLO = 'L'.KD >= 0.ABβCOMPLEX*16array, dimension(LDAB, N). On entry, the upper or lower triangle of the Hermitian band matrixA, stored in the firstKD+1rows of the array. Thej-th column ofAis stored in thej-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,ABis overwritten by values generated during the reduction to tridiagonal form. πLDABβINTEGER. The leading dimension of the arrayAB.LDAB >= KD + 1.QβCOMPLEX*16array, dimension(LDQ, N). IfJOBZ = 'V', theN-by-Nunitary matrix used in the reduction to tridiagonal form. IfJOBZ = 'N', the arrayQis not referenced.LDQβINTEGER. The leading dimension of the arrayQ. IfJOBZ = 'V', thenLDQ >= max(1,N).VLβDOUBLE PRECISION. IfRANGE='V', the lower bound of the interval to be searched for eigenvalues.VL < VU. Not referenced ifRANGE = 'A'or'I'.VUβDOUBLE PRECISION. IfRANGE='V', the upper bound of the interval to be searched for eigenvalues.VL < VU. Not referenced ifRANGE = 'A'or'I'.ILβINTEGER. 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'.IUβINTEGER. 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'.ABSTOLβDOUBLE 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 toABSTOL + EPS * max( |a|,|b| ) ,whereEPSis the machine precision. IfABSTOLis less than or equal to zero, thenEPS*|T|will be used in its place, where|T|is the 1-norm of the tridiagonal matrix obtained by reducingABto tridiagonal form. Eigenvalues will be computed most accurately whenABSTOLis set to twice the underflow threshold2*DLAMCH('S'), not zero. If this routine returns withINFO>0, indicating that some eigenvectors did not converge, try settingABSTOLto2*DLAMCH('S'). Thereβs also the Demmel and Kahan reference, LAPACK Working Note #3. π₯MβINTEGER. The total number of eigenvalues found.0 <= M <= N. IfRANGE = 'A',M = N, and ifRANGE = 'I',M = IU-IL+1.WβDOUBLE PRECISIONarray, dimension(N). The firstMelements contain the selected eigenvalues in ascending order. πΈZβCOMPLEX*16array, dimension(LDZ, max(1,M)). IfJOBZ = 'V', then ifINFO = 0, the firstMcolumns ofZcontain the orthonormal eigenvectors of the matrixAcorresponding to the selected eigenvalues, with thei-th column ofZholding the eigenvector associated withW(i). If an eigenvector fails to converge, then that column ofZcontains the latest approximation to the eigenvector, and the index of the eigenvector is returned inIFAIL. IfJOBZ = 'N', thenZis 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. πLDZβINTEGER. The leading dimension of the arrayZ.LDZ >= 1, and ifJOBZ = 'V',LDZ >= max(1,N).WORKβCOMPLEX*16array, dimension(LWORK).LWORKβINTEGER. The length of the arrayWORK.LWORK >= 1, whenN <= 1; otherwise ifJOBZ = 'N'andN > 1,LWORKmust be queried.LWORK = MAX(1, dimension)wheredimension = (2KD+1)*N + KD*NTHREADSwhereKDis the size of the band.NTHREADSis the number of threads used when openMP compilation is enabled, otherwise=1. IfJOBZ = 'V'andN > 1,LWORKmust be queried. Not yet available. IfLWORK = -1, then a workspace query is assumed; the routine only calculates the optimal sizes of theWORK,RWORKandIWORKarrays, returns these values as the first entries of theWORK,RWORKandIWORKarrays, and no error message related toLWORKorLRWORKorLIWORKis issued byXERBLA. πRWORKβDOUBLE PRECISIONarray, dimension(7*N).IWORKβINTEGERarray, dimension(5*N).IFAILβINTEGERarray, dimension(N). IfJOBZ = 'V', then ifINFO = 0, the firstMelements ofIFAILare zero. IfINFO > 0, thenIFAILcontains the indices of the eigenvectors that failed to converge. IfJOBZ = 'N', thenIFAILis not referenced.INFOβINTEGER.= 0: successful exit.< 0: ifINFO = -i, thei-th argument had an illegal value.> 0: ifINFO = i, thenieigenvectors failed to converge. Their indices are stored in arrayIFAIL. π«Ά
Author π
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
Further Details π«Ά
This section is empty in the source β no extra lore, no hidden tea, just a blank little moment. π
Okay so real quick β the docs are like "if you wanna go DEEP, here's the reading list," and honestly? iconic of them. πβ¨ All the receipts about how the 2stage techniques actually work are in these three papers:
π the reading list (aka the receipts)
- 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
Like, three whole papers of lore, bestie. That's the deep dive if the vibes alone aren't enough for you π«Ά
And where does this beautiful little block live? Definition at line 323 of file zhbevx_2stage.f. π
π Author
Generated automatically by Doxygen for LAPACK from the source code. So like, nobody wrote this by hand, it's giving "the machine did my homework and honestly it ate." π€β¨
lowkey a slay that you made it all the way to the very last line of this page β main character energy fr fr π
Okay that's the whole thing, bestie β this was LAPACK, Version 3.12.0, and the page is literally called hbevx_2stage(3) so that's a wrap. Bye, love you, go call some routines πππ¦
π¦ where this page comes from
- arch rolling: lapack-doc 3.12.1-2 Β· custom
- π girlified by deepseek-ai/DeepSeek-V4.1-Flash-1017 on : a language model's rewrite of the original, under its terms