Man page - heevr_2stage(3)
Packages contains this manual
- hptrd(3)
- potri(3)
- xerbla_array(3)
- ggsvd_driver_grp(3)
- hfrk(3)
- getsqr_comp_grp(3)
- laed6(3)
- gtrfs(3)
- lasdq(3)
- gglse(3)
- la_xisnan_la_isnan(3)
- unmr2(3)
- hetrs_aa(3)
- tpttr(3)
- gerz_comp_grp(3)
- potrf(3)
- hegv_driver(3)
- laqps(3)
- ggqr_comp_grp(3)
- ilalc(3)
- ung2r(3)
- heevd(3)
- pstf2(3)
- lacn2(3)
- ptrfs(3)
- ungrq(3)
- gelqf(3)
- ppsv_comp(3)
- blas2_full(3)
- gemlqt(3)
- unml2(3)
- tplqt(3)
- tpcon(3)
- getf2(3)
- ggbak(3)
- bdsvd_driver(3)
- lamch(3)
- gelq(3)
- gebal(3)
- laqr1(3)
- ptsvx(3)
- lahr2(3)
- larscl2(3)
- geqrt(3)
- larfb(3)
- gtsv_comp(3)
- gesvd_aux(3)
- hbevx_2stage(3)
- hbgvx(3)
- tprfs(3)
- params_grp(3)
- lahef(3)
- laqr_group(3)
- unmqr(3)
- tgsy2(3)
- tfsv_comp(3)
- ggls_driver_grp(3)
- geev(3)
- latrd(3)
- unbdb4(3)
- bbcsd(3)
- lange(3)
- gelq_comp3(3)
- gttrs(3)
- lasy2(3)
- hetf2_rook(3)
- gtsv(3)
- lalsd(3)
- lanhb(3)
- laqhb(3)
- hgeqz(3)
- gesvj(3)
- gsvj0(3)
- ungtsqr_row(3)
- gelq_comp1(3)
- gemmtr(3)
- pbequ(3)
- heev_driver(3)
- unhr_col(3)
- syconvf_rook(3)
- getc2(3)
- syconv(3)
- norm_grp(3)
- larrc(3)
- laqr4(3)
- posv_comp(3)
- geev_driver_grp(3)
- heev_comp(3)
- pfsv(3)
- trevc3(3)
- gesv_driver_grp(3)
- reflector_aux_grp(3)
- langt(3)
- lacrt(3)
- latdf(3)
- hetrs_aa_2stage(3)
- lamc1(3)
- hpev_driver(3)
- hegvd(3)
- pptri(3)
- geqrt3(3)
- gelqt3(3)
- lasd5(3)
- laeda(3)
- geqr(3)
- lamtsqr(3)
- heev(3)
- hpev_comp(3)
- larfg(3)
- blas2_grp(3)
- hesv_rook(3)
- laexc(3)
- hetrd(3)
- geesx(3)
- ppsvx(3)
- blas_top(3)
- gtts2(3)
- la_herpvgrw(3)
- hpevx(3)
- ggevx(3)
- lahqr(3)
- gelq_comp_grp(3)
- hesv_comp_v3(3)
- tplqt2(3)
- hpev(3)
- hbtrd(3)
- getrs(3)
- hecon_3(3)
- lasrt(3)
- lanhe(3)
- gesv_comp(3)
- gbequ(3)
- hetrf_rk(3)
- laqr3(3)
- heev_comp_grp(3)
- ungtsqr(3)
- ppcon(3)
- ggrq_comp_grp(3)
- larmm(3)
- ieeeck(3)
- geqrf(3)
- solve_aux_grp(3)
- herfs(3)
- posvx(3)
- posvxx(3)
- gges3(3)
- hbgvd(3)
- lantb(3)
- lasd_comp_grp(3)
- hpgvx(3)
- lapy2(3)
- lauu2(3)
- copy(3)
- getsqrhrt(3)
- stev_comp_grp(3)
- laev2(3)
- larfb_gett(3)
- trti2(3)
- laqz4(3)
- hegv_driver_grp(3)
- la_porfsx_extended(3)
- laruv(3)
- ggsvd_comp_grp(3)
- dot(3)
- gehd2(3)
- lanhf(3)
- hetri_rook(3)
- pfsv_comp(3)
- gbtrf(3)
- hpgst(3)
- getri(3)
- trevc(3)
- unmrz(3)
- hsein(3)
- lsamen(3)
- lasd6(3)
- trtri(3)
- ggglm(3)
- las2(3)
- latrs(3)
- lapll(3)
- gemlq(3)
- geqpf_comp_grp(3)
- stemr(3)
- rotm(3)
- disna(3)
- ggrqf(3)
- pptrf(3)
- lasd0(3)
- lals0(3)
- laqz2(3)
- hbev_driver2(3)
- geswlq_comp_grp(3)
- laqr0(3)
- trttp(3)
- stedc(3)
- lasq4(3)
- geev_comp_grp(3)
- ungbr(3)
- lanv2(3)
- hpsv(3)
- pprfs(3)
- gehrd(3)
- ppsv(3)
- lagtm(3)
- hpgv(3)
- trsv_comp(3)
- larfx(3)
- gesv_driver(3)
- gerfsx(3)
- la_geamv(3)
- laed9(3)
- tpqrt2(3)
- uncsd(3)
- gecs_comp_grp(3)
- bdsqr(3)
- hegv_comp_grp(3)
- labad(3)
- geqp3(3)
- gesvdq(3)
- tfttp(3)
- laln2(3)
- uncsd2by1(3)
- blas2_like_grp(3)
- latbs(3)
- hbgst(3)
- larrv(3)
- ilaenv2stage(3)
- bdsvdx(3)
- hegs2(3)
- lasq_comp_grp(3)
- hpr2(3)
- laqhe(3)
- larra(3)
- gemqrt(3)
- hbmv(3)
- hpsv_driver(3)
- lacp2(3)
- lapmt(3)
- gecon(3)
- unbdb5(3)
- la_gerpvgrw(3)
- tgex2(3)
- laqhp(3)
- tftri(3)
- getrf2(3)
- porfs(3)
- lartg(3)
- lagts(3)
- ggev_comp_grp(3)
- lasd3(3)
- geqr_comp2(3)
- laqz_group(3)
- pftri(3)
- hetri2x(3)
- lahef_aa(3)
- svd_driver_grp(3)
- gbsv_driver(3)
- hesv_comp_aasen2(3)
- laqtr(3)
- lag2(3)
- la_porcond(3)
- hbev(3)
- pbtrf(3)
- lascl(3)
- larr_comp_grp(3)
- hecon(3)
- pttrs(3)
- lasd8(3)
- lsame(3)
- unm2l(3)
- potrs(3)
- tptrs(3)
- lartv(3)
- trtrs(3)
- gsvj1(3)
- sum1(3)
- larrj(3)
- gbmv(3)
- posv(3)
- gghd3(3)
- geev_top(3)
- geqr_comp_grp(3)
- laset(3)
- hesvxx(3)
- posv_comp_grp(3)
- lahef_rk(3)
- lasd1(3)
- tprfb(3)
- potf2(3)
- laein(3)
- lamc4(3)
- stevd(3)
- gtsv_driver(3)
- gesvd_comp_grp(3)
- la_constants(3)
- gesvx(3)
- hseqr(3)
- launhr_col_getrfnp2(3)
- trcon(3)
- larre(3)
- gelsy(3)
- ptsv(3)
- lacon(3)
- laed_comp_grp(3)
- hpsvx(3)
- gemm(3)
- poequ(3)
- laesy(3)
- lagtf(3)
- trrfs(3)
- ggev3(3)
- pbstf(3)
- poequb(3)
- heevr(3)
- lanhp(3)
- unbdb3(3)
- tgsyl(3)
- lamc5(3)
- geqr2p(3)
- ungqr(3)
- laqz3(3)
- imax1(3)
- gels_top(3)
- hesv(3)
- gelqt(3)
- pfsv_driver(3)
- stegr(3)
- gerqf(3)
- laisnan(3)
- ilatrans(3)
- gbsv_comp(3)
- pbrfs(3)
- lascl2(3)
- larz(3)
- la_hercond(3)
- tgexc(3)
- ggesx(3)
- unbdb6(3)
- ungl2(3)
- laed_comp2(3)
- rscl(3)
- hegv(3)
- gelst(3)
- gbtrs(3)
- pftrf(3)
- langb(3)
- lantr(3)
- laqgb(3)
- ggsvp3(3)
- bdsdc(3)
- ladiv(3)
- laqge(3)
- iparmq(3)
- ggbal(3)
- hb2st_kernels(3)
- lartgs(3)
- lartgp(3)
- rot(3)
- ppequ(3)
- laed3(3)
- her(3)
- hptri(3)
- stevx(3)
- upgtr(3)
- lar2v(3)
- hbev_2stage(3)
- gejsv(3)
- ppsv_driver(3)
- unm22(3)
- gesvxx(3)
- laqz0(3)
- unmtr(3)
- laed5(3)
- tptri(3)
- laed0(3)
- heev_driver2(3)
- hpcon(3)
- lasd4(3)
- hetrf_aa(3)
- geqr_comp3(3)
- rot_aux_grp(3)
- aux_grp(3)
- laebz(3)
- trsyl3(3)
- gges(3)
- gesdd(3)
- trexc(3)
- ung2l(3)
- gesv(3)
- laed4(3)
- md__r_e_a_d_m_e(3)
- blas3_like_grp(3)
- laed1(3)
- larcm(3)
- hbevx(3)
- hesv_driver_grp(3)
- hetrs(3)
- hbevd_2stage(3)
- blas1_grp(3)
- laic1(3)
- geql_comp_grp(3)
- heev_2stage(3)
- hpmv(3)
- pbtf2(3)
- hetrf_aa_2stage(3)
- hbgv(3)
- pptrs(3)
- lapmr(3)
- tpqr_comp_grp(3)
- larfy(3)
- gedmd(3)
- lasr(3)
- hetrd_2stage(3)
- gerfs(3)
- ungtr(3)
- porfsx(3)
- tpmv(3)
- lasd_comp2(3)
- unmbr(3)
- tbtrs(3)
- hetd2(3)
- trsv_comp_grp(3)
- lapy3(3)
- ptts2(3)
- unmhr(3)
- hbev_driver(3)
- lalsa(3)
- tbsv_comp(3)
- hesv_comp_v1(3)
- geql2(3)
- sterf(3)
- larrd(3)
- larft(3)
- lagv2(3)
- gttrf(3)
- tpqrt(3)
- la_lin_berr(3)
- rotg(3)
- solve_top(3)
- lacgv(3)
- larrf(3)
- tbmv(3)
- trsyl(3)
- geequ(3)
- upmtr(3)
- hpgv_driver(3)
- tbsv(3)
- hesvx(3)
- latrz(3)
- tfttr(3)
- gesv_comp_grp(3)
- xerbla_grp(3)
- tpsv(3)
- blas3_grp(3)
- gesvd_driver(3)
- geqr_comp1(3)
- ggev_driver_grp(3)
- la_gbamv(3)
- tpmlqt(3)
- trttf(3)
- larzb(3)
- unmr3(3)
- hecon_rook(3)
- stebz(3)
- lantp(3)
- laqz1(3)
- hesv_rk(3)
- tbcon(3)
- xerbla(3)
- posv_mixed(3)
- latps(3)
- hesv_aa_driver(3)
- gemqr(3)
- larrr(3)
- gebrd(3)
- tgsna(3)
- la_gercond(3)
- gbsv(3)
- hesv_comp_grp(3)
- gesv_mixed(3)
- gghrd(3)
- gbrfs(3)
- tpmqrt(3)
- lasq3(3)
- tpsv_comp(3)
- largv(3)
- gelsd(3)
- pftrs(3)
- asum(3)
- launhr_col_getrfnp(3)
- hptrf(3)
- lacpy(3)
- gesc2(3)
- lasda(3)
- second(3)
- hprfs(3)
- hpsv_comp(3)
- lamrg(3)
- pbsv_comp(3)
- hegv_2stage(3)
- gerq2(3)
- lasdt(3)
- abs1(3)
- hbevd(3)
- hbev_comp(3)
- trsv(3)
- la_porpvgrw(3)
- la_gbrpvgrw(3)
- hbgv_driver(3)
- tgsja(3)
- gebd2(3)
- geqr2(3)
- unm2r(3)
- unmql(3)
- la_gbrfsx_extended(3)
- gelq_comp2(3)
- iparam2stage(3)
- ger(3)
- larf(3)
- ilaprec(3)
- labrd(3)
- unbdb1(3)
- unmlq(3)
- geequb(3)
- la_herfsx_extended(3)
- unbdb2(3)
- lapack_top(3)
- ptsv_driver(3)
- hetrs2(3)
- geqr_comp4(3)
- pbsv(3)
- posv_driver(3)
- steqr(3)
- gels(3)
- lar1v(3)
- hemv(3)
- la_transtype(3)
- hesv_aa(3)
- lacrm(3)
- stevr(3)
- hetf2_rk(3)
- blas2_banded(3)
- stein(3)
- unmrq(3)
- larrk(3)
- hetri2(3)
- hesv_aa_2stage(3)
- pttrf(3)
- gelss(3)
- pbsv_driver(3)
- lasq5(3)
- heevx_2stage(3)
- hetri(3)
- lasd2(3)
- laed2(3)
- pbcon(3)
- ptcon(3)
- laed7(3)
- gels_aux_grp(3)
- hpgvd(3)
- hetf2(3)
- tzrzf(3)
- hpr(3)
- unitary_top(3)
- latsqr(3)
- ungql(3)
- her2(3)
- hetri_3x(3)
- hetrd_hb2st(3)
- tgsen(3)
- ggsvd3(3)
- lasq6(3)
- set_grp(3)
- larfgp(3)
- gels_driver_grp(3)
- pbtrs(3)
- lamswlq(3)
- lanht(3)
- gbsvxx(3)
- tgevc(3)
- ilaenv(3)
- swap(3)
- lae2(3)
- iladiag(3)
- lasq2(3)
- la_heamv(3)
- blas_like_top(3)
- la_gerfsx_extended(3)
- hegst(3)
- tfsm(3)
- gesvd(3)
- ungr2(3)
- ggev(3)
- aux_top(3)
- blas2_packed(3)
- geqlf(3)
- hetrs_rook(3)
- gelq2(3)
- geqrfp(3)
- gbequb(3)
- stev(3)
- lauum(3)
- potrf2(3)
- lamc3(3)
- gbrfsx(3)
- gerq_comp_grp(3)
- pocon(3)
- tbrfs(3)
- heswapr(3)
- lamc2(3)
- hpevd(3)
- hesv_comp_aasen(3)
- scalar_grp(3)
- gemv(3)
- lasv2(3)
- lanhs(3)
- svd_top(3)
- gbsvx(3)
- gesvdx(3)
- tplq_comp_grp(3)
- hesv_driver(3)
- hesv_comp_v2(3)
- trsen(3)
- syconvf(3)
- lasd7(3)
- gbcon(3)
- unbdb(3)
- heev_driver_grp(3)
- ggqrf(3)
- heevx(3)
- gtsvx(3)
- lahef_rook(3)
- hetrf_rook(3)
- hetrf(3)
- trsna(3)
- gebak(3)
- larnv(3)
- ptsv_comp(3)
- laswlq(3)
- lags2(3)
- laed8(3)
- laswp(3)
- hptrs(3)
- unglq(3)
- la_wwaddw(3)
- getrf(3)
- gees(3)
- gbtf2(3)
- hegvx(3)
- latrs3(3)
- roundup_lwork(3)
- unghr(3)
- iamax(3)
- larzt(3)
- pteqr(3)
- ilaver(3)
- trmv(3)
- la_gbrcond(3)
- blas0_like_grp(3)
- nrm2(3)
- heev_top(3)
- gtcon(3)
- heevr_2stage(3)
- pstrf(3)
- rot_comp(3)
- laqr5(3)
- heevd_2stage(3)
- getsls(3)
- hetrd_he2hb(3)
- heequb(3)
- laqp2(3)
- axpy(3)
- blast_aux(3)
- rotmg(3)
- pbsvx(3)
- ilauplo(3)
- herfsx(3)
- laqr2(3)
- blas1_like_grp(3)
- lassq(3)
- larrb(3)
- stev_driver(3)
- geevx(3)
- tpttf(3)
- scal(3)
- laneg(3)
- posv_driver_grp(3)
- lasq1(3)
- hetrs_3(3)
- geqrt2(3)
- gbbrd(3)
- ilalr(3)
- hetri_3(3)
apt-get install liblapack-doc
Manual
heevr_2stage
NAMESYNOPSIS
Functions
Detailed Description
Function Documentation
subroutine cheevr_2stage (character jobz, character range, character uplo,integer n, complex, dimension( lda, * ) a, integer lda, real vl, realvu, 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, integerliwork, integer info)
subroutine dsyevr_2stage (character jobz, character range, character uplo,integer n, double precision, dimension( lda, * ) a, integer lda, doubleprecision vl, double precision vu, integer il, integer iu, doubleprecision abstol, integer m, double precision, dimension( * ) w, doubleprecision, dimension( ldz, * ) z, integer ldz, integer, dimension( * )isuppz, double precision, dimension( * ) work, integer lwork, integer,dimension( * ) iwork, integer liwork, integer info)
subroutine ssyevr_2stage (character jobz, character range, character uplo,integer n, real, dimension( lda, * ) a, integer lda, real vl, real vu,integer il, integer iu, real abstol, integer m, real, dimension( * ) w,real, dimension( ldz, * ) z, integer ldz, integer, dimension( * )isuppz, real, dimension( * ) work, integer lwork, integer, dimension( *) iwork, integer liwork, integer info)
subroutine zheevr_2stage (character jobz, character range, character uplo,integer n, complex*16, dimension( lda, * ) a, integer lda, doubleprecision vl, double precision vu, integer il, integer iu, doubleprecision abstol, integer m, double precision, dimension( * ) w,complex*16, dimension( ldz, * ) z, integer ldz, integer, dimension( * )isuppz, complex*16, dimension( * ) work, integer lwork, doubleprecision, dimension( * ) rwork, integer lrwork, integer, dimension( *) iwork, integer liwork, integer info)
Author
NAME
heevr_2stage - {he,sy}evr_2stage: eig, MRRR
SYNOPSIS
Functions
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)
CHEEVR_2STAGE computes the eigenvalues and, optionally, the
left and/or right eigenvectors for HE matrices
subroutine
dsyevr_2stage
(jobz, range, uplo, n, a,
lda, vl, vu, il, iu, abstol, m, w, z, ldz, isuppz, work,
lwork, iwork, liwork, info)
DSYEVR_2STAGE computes the eigenvalues and, optionally, the
left and/or right eigenvectors for SY matrices
subroutine
ssyevr_2stage
(jobz, range, uplo, n, a,
lda, vl, vu, il, iu, abstol, m, w, z, ldz, isuppz, work,
lwork, iwork, liwork, info)
SSYEVR_2STAGE computes the eigenvalues and, optionally, the
left and/or right eigenvectors for SY matrices
subroutine
zheevr_2stage
(jobz, range, uplo, n, a,
lda, vl, vu, il, iu, abstol, m, w, z, ldz, isuppz, work,
lwork, rwork, lrwork, iwork, liwork, info)
ZHEEVR_2STAGE computes the eigenvalues and, optionally, the
left and/or right eigenvectors for HE matrices
Detailed Description
Function Documentation
subroutine cheevr_2stage (character jobz, character range, character uplo,integer n, complex, dimension( lda, * ) a, integer lda, real vl, realvu, 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, integerliwork, integer info)
CHEEVR_2STAGE computes the eigenvalues and, optionally, the left and/or right eigenvectors for HE matrices
Purpose:
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 ’good’ L
D LˆT 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 LˆT, so that L and D
define all the wanted eigenvalues to high relative accuracy.
This means that small relative changes in the entries of D
and L
cause only small relative changes in the eigenvalues and
eigenvectors. The standard (unfactored) representation of
the
tridiagonal matrix T does 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:
’Multiple representations
to compute orthogonal eigenvectors of symmetric tridiagonal
matrices,’
Linear Algebra and its Applications, 387(1), pp. 1-28,
August 2004.
- Inderjit Dhillon and Beresford Parlett: ’Orthogonal
Eigenvectors and
Relative Gaps,’ SIAM Journal on Matrix Analysis and
Applications, Vol. 25,
2004. Also LAPACK Working Note 154.
- Inderjit Dhillon: ’A new O(nˆ2) algorithm for
the symmetric
tridiagonal eigenvalue/eigenvector problem’,
Computer Science Division Technical Report No.
UCB/CSD-97-971,
UC Berkeley, May 1997.
Note 1 :
CHEEVR_2STAGE calls CSTEMR when the full spectrum is
requested
on machines which conform to the ieee-754 floating point
standard.
CHEEVR_2STAGE calls SSTEBZ and CSTEIN on non-ieee machines
and
when partial spectrum requests are made.
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.
Parameters
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’: the IL-th through IU-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 of A is stored;
= ’L’: Lower triangle of A is 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.
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
’Computing Small Singular Values of Bidiagonal
Matrices
with Guaranteed High Relative Accuracy,’ 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,
’Computing Accurate Eigensystems of Scaled Diagonally
Dominant Matrices’, 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 least max(1,M) columns
are
supplied in the array Z; if RANGE = ’V’, the
exact value of M
is not known in advance and an upper bound must be used.
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 is
INTEGER
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.
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
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.
RWORK
RWORK is REAL
array, dimension (MAX(1,LRWORK))
On exit, if INFO = 0, RWORK(1) returns the optimal
(and minimal) LRWORK.
LRWORK
LRWORK is
INTEGER
The length of the array RWORK.
If N <= 1, LRWORK >= 1, else LRWORK >= 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.
IWORK
IWORK is
INTEGER array, dimension (MAX(1,LIWORK))
On exit, if INFO = 0, IWORK(1) returns the optimal
(and minimal) LIWORK.
LIWORK
LIWORK is
INTEGER
The dimension of the array IWORK.
If N <= 1, LIWORK >= 1, else LIWORK >= 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.
INFO
INFO is INTEGER
= 0: successful exit
< 0: if INFO = -i, the i-th argument had an illegal value
> 0: Internal error
Author
Univ. of Tennessee
Univ. of California Berkeley
Univ. of Colorado Denver
NAG Ltd.
Contributors:
Inderjit
Dhillon, IBM Almaden, USA \n
Osni Marques, LBNL/NERSC, USA \n
Ken Stanley, Computer Science Division, University of
California at Berkeley, USA \n
Jason Riedy, Computer Science Division, University of
California at Berkeley, USA \n
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
subroutine dsyevr_2stage (character jobz, character range, character uplo,integer n, double precision, dimension( lda, * ) a, integer lda, doubleprecision vl, double precision vu, integer il, integer iu, doubleprecision abstol, integer m, double precision, dimension( * ) w, doubleprecision, dimension( ldz, * ) z, integer ldz, integer, dimension( * )isuppz, double precision, dimension( * ) work, integer lwork, integer,dimension( * ) iwork, integer liwork, integer info)
DSYEVR_2STAGE computes the eigenvalues and, optionally, the left and/or right eigenvectors for SY matrices
Purpose:
DSYEVR_2STAGE
computes selected eigenvalues and, optionally, eigenvectors
of a real symmetric 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.
DSYEVR_2STAGE
first reduces the matrix A to tridiagonal form T with a call
to DSYTRD. Then, whenever possible, DSYEVR_2STAGE calls
DSTEMR to compute
the eigenspectrum using Relatively Robust Representations.
DSTEMR
computes eigenvalues by the dqds algorithm, while orthogonal
eigenvectors are computed from various ’good’ L
D LˆT 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 LˆT, so that L and D
define all the wanted eigenvalues to high relative accuracy.
This means that small relative changes in the entries of D
and L
cause only small relative changes in the eigenvalues and
eigenvectors. The standard (unfactored) representation of
the
tridiagonal matrix T does 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 DSTEMR’s documentation and:
- Inderjit S. Dhillon and Beresford N. Parlett:
’Multiple representations
to compute orthogonal eigenvectors of symmetric tridiagonal
matrices,’
Linear Algebra and its Applications, 387(1), pp. 1-28,
August 2004.
- Inderjit Dhillon and Beresford Parlett: ’Orthogonal
Eigenvectors and
Relative Gaps,’ SIAM Journal on Matrix Analysis and
Applications, Vol. 25,
2004. Also LAPACK Working Note 154.
- Inderjit Dhillon: ’A new O(nˆ2) algorithm for
the symmetric
tridiagonal eigenvalue/eigenvector problem’,
Computer Science Division Technical Report No.
UCB/CSD-97-971,
UC Berkeley, May 1997.
Note 1 :
DSYEVR_2STAGE calls DSTEMR when the full spectrum is
requested
on machines which conform to the ieee-754 floating point
standard.
DSYEVR_2STAGE calls DSTEBZ and SSTEIN on non-ieee machines
and
when partial spectrum requests are made.
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.
Parameters
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’: the IL-th through IU-th eigenvalues will
be found.
For RANGE = ’V’ or ’I’ and IU - IL
< N - 1, DSTEBZ and
DSTEIN are called
UPLO
UPLO is
CHARACTER*1
= ’U’: Upper triangle of A is stored;
= ’L’: Lower triangle of A is stored.
N
N is INTEGER
The order of the matrix A. N >= 0.
A
A is DOUBLE
PRECISION array, dimension (LDA, N)
On entry, the symmetric 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.
LDA
LDA is INTEGER
The leading dimension of the array A. LDA >=
max(1,N).
VL
VL is DOUBLE
PRECISION
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 DOUBLE
PRECISION
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
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 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
’Computing Small Singular Values of Bidiagonal
Matrices
with Guaranteed High Relative Accuracy,’ 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,
’Computing Accurate Eigensystems of Scaled Diagonally
Dominant Matrices’, 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 DOUBLE
PRECISION array, dimension (N)
The first M elements contain the selected eigenvalues in
ascending order.
Z
Z is DOUBLE
PRECISION 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 least max(1,M) columns
are
supplied in the array Z; if RANGE = ’V’, the
exact value of M
is not known in advance and an upper bound must be used.
Supplying N columns is always safe.
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 DSTEMR (tridiagonal
matrix). The support of the eigenvectors of A is typically
1:N because of the orthogonal transformations applied by
DORMTR.
Implemented only for RANGE = ’A’ or
’I’ and IU - IL = N - 1
WORK
WORK is DOUBLE
PRECISION array, dimension (MAX(1,LWORK))
On exit, if INFO = 0, WORK(1) returns the optimal LWORK.
LWORK
LWORK is
INTEGER
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.
LWORK = MAX(1, 26*N, dimension) where
dimension = max(stage1,stage2) + (KD+1)*N + 5*N
= N*KD + N*max(KD+1,FACTOPTNB)
+ max(2*KD*KD, KD*NTHREADS)
+ (KD+1)*N + 5*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
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 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.
IWORK
IWORK is
INTEGER array, dimension (MAX(1,LIWORK))
On exit, if INFO = 0, IWORK(1) returns the optimal
LIWORK.
LIWORK
LIWORK is
INTEGER
The dimension of the array IWORK.
If N <= 1, LIWORK >= 1, else LIWORK >= 10*N.
If LIWORK = -1,
then a workspace query is assumed; the
routine only calculates the optimal size of the IWORK array,
returns this value as the first entry of the IWORK array,
and
no error message related to LIWORK is issued by XERBLA.
INFO
INFO is INTEGER
= 0: successful exit
< 0: if INFO = -i, the i-th argument had an illegal value
> 0: Internal error
Author
Univ. of Tennessee
Univ. of California Berkeley
Univ. of Colorado Denver
NAG Ltd.
Contributors:
Inderjit
Dhillon, IBM Almaden, USA \n
Osni Marques, LBNL/NERSC, USA \n
Ken Stanley, Computer Science Division, University of
California at Berkeley, USA \n
Jason Riedy, Computer Science Division, University of
California at Berkeley, USA \n
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
subroutine ssyevr_2stage (character jobz, character range, character uplo,integer n, real, dimension( lda, * ) a, integer lda, real vl, real vu,integer il, integer iu, real abstol, integer m, real, dimension( * ) w,real, dimension( ldz, * ) z, integer ldz, integer, dimension( * )isuppz, real, dimension( * ) work, integer lwork, integer, dimension( *) iwork, integer liwork, integer info)
SSYEVR_2STAGE computes the eigenvalues and, optionally, the left and/or right eigenvectors for SY matrices
Purpose:
SSYEVR_2STAGE
computes selected eigenvalues and, optionally, eigenvectors
of a real symmetric 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.
SSYEVR_2STAGE
first reduces the matrix A to tridiagonal form T with a call
to SSYTRD. Then, whenever possible, SSYEVR_2STAGE calls
SSTEMR to compute
the eigenspectrum using Relatively Robust Representations.
SSTEMR
computes eigenvalues by the dqds algorithm, while orthogonal
eigenvectors are computed from various ’good’ L
D LˆT 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 LˆT, so that L and D
define all the wanted eigenvalues to high relative accuracy.
This means that small relative changes in the entries of D
and L
cause only small relative changes in the eigenvalues and
eigenvectors. The standard (unfactored) representation of
the
tridiagonal matrix T does 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 SSTEMR’s documentation and:
- Inderjit S. Dhillon and Beresford N. Parlett:
’Multiple representations
to compute orthogonal eigenvectors of symmetric tridiagonal
matrices,’
Linear Algebra and its Applications, 387(1), pp. 1-28,
August 2004.
- Inderjit Dhillon and Beresford Parlett: ’Orthogonal
Eigenvectors and
Relative Gaps,’ SIAM Journal on Matrix Analysis and
Applications, Vol. 25,
2004. Also LAPACK Working Note 154.
- Inderjit Dhillon: ’A new O(nˆ2) algorithm for
the symmetric
tridiagonal eigenvalue/eigenvector problem’,
Computer Science Division Technical Report No.
UCB/CSD-97-971,
UC Berkeley, May 1997.
Note 1 :
SSYEVR_2STAGE calls SSTEMR when the full spectrum is
requested
on machines which conform to the ieee-754 floating point
standard.
SSYEVR_2STAGE calls SSTEBZ and SSTEIN on non-ieee machines
and
when partial spectrum requests are made.
Normal
execution of SSTEMR 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.
Parameters
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’: the IL-th through IU-th eigenvalues will
be found.
For RANGE = ’V’ or ’I’ and IU - IL
< N - 1, SSTEBZ and
SSTEIN are called
UPLO
UPLO is
CHARACTER*1
= ’U’: Upper triangle of A is stored;
= ’L’: Lower triangle of A is stored.
N
N is INTEGER
The order of the matrix A. N >= 0.
A
A is REAL
array, dimension (LDA, N)
On entry, the symmetric 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.
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
’Computing Small Singular Values of Bidiagonal
Matrices
with Guaranteed High Relative Accuracy,’ 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,
’Computing Accurate Eigensystems of Scaled Diagonally
Dominant Matrices’, 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 REAL
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 least max(1,M) columns
are
supplied in the array Z; if RANGE = ’V’, the
exact value of M
is not known in advance and an upper bound must be used.
Supplying N columns is always safe.
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 SSTEMR (tridiagonal
matrix). The support of the eigenvectors of A is typically
1:N because of the orthogonal transformations applied by
SORMTR.
Implemented only for RANGE = ’A’ or
’I’ and IU - IL = N - 1
WORK
WORK is REAL
array, dimension (MAX(1,LWORK))
On exit, if INFO = 0, WORK(1) returns the optimal LWORK.
LWORK
LWORK is
INTEGER
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.
LWORK = MAX(1, 26*N, dimension) where
dimension = max(stage1,stage2) + (KD+1)*N + 5*N
= N*KD + N*max(KD+1,FACTOPTNB)
+ max(2*KD*KD, KD*NTHREADS)
+ (KD+1)*N + 5*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
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 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.
IWORK
IWORK is
INTEGER array, dimension (MAX(1,LIWORK))
On exit, if INFO = 0, IWORK(1) returns the optimal
LIWORK.
LIWORK
LIWORK is
INTEGER
The dimension of the array IWORK.
If N <= 1, LIWORK >= 1, else LIWORK >= 10*N.
If LIWORK = -1,
then a workspace query is assumed; the
routine only calculates the optimal size of the IWORK array,
returns this value as the first entry of the IWORK array,
and
no error message related to LIWORK is issued by XERBLA.
INFO
INFO is INTEGER
= 0: successful exit
< 0: if INFO = -i, the i-th argument had an illegal value
> 0: Internal error
Author
Univ. of Tennessee
Univ. of California Berkeley
Univ. of Colorado Denver
NAG Ltd.
Contributors:
Inderjit
Dhillon, IBM Almaden, USA \n
Osni Marques, LBNL/NERSC, USA \n
Ken Stanley, Computer Science Division, University of
California at Berkeley, USA \n
Jason Riedy, Computer Science Division, University of
California at Berkeley, USA \n
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
subroutine zheevr_2stage (character jobz, character range, character uplo,integer n, complex*16, dimension( lda, * ) a, integer lda, doubleprecision vl, double precision vu, integer il, integer iu, doubleprecision abstol, integer m, double precision, dimension( * ) w,complex*16, dimension( ldz, * ) z, integer ldz, integer, dimension( * )isuppz, complex*16, dimension( * ) work, integer lwork, doubleprecision, dimension( * ) rwork, integer lrwork, integer, dimension( *) iwork, integer liwork, integer info)
ZHEEVR_2STAGE computes the eigenvalues and, optionally, the left and/or right eigenvectors for HE matrices
Purpose:
ZHEEVR_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.
ZHEEVR_2STAGE
first reduces the matrix A to tridiagonal form T with a call
to ZHETRD. Then, whenever possible, ZHEEVR_2STAGE calls
ZSTEMR to compute
eigenspectrum using Relatively Robust Representations.
ZSTEMR
computes eigenvalues by the dqds algorithm, while orthogonal
eigenvectors are computed from various ’good’ L
D LˆT 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 LˆT, so that L and D
define all the wanted eigenvalues to high relative accuracy.
This means that small relative changes in the entries of D
and L
cause only small relative changes in the eigenvalues and
eigenvectors. The standard (unfactored) representation of
the
tridiagonal matrix T does 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 ZSTEMR’s documentation and:
- Inderjit S. Dhillon and Beresford N. Parlett:
’Multiple representations
to compute orthogonal eigenvectors of symmetric tridiagonal
matrices,’
Linear Algebra and its Applications, 387(1), pp. 1-28,
August 2004.
- Inderjit Dhillon and Beresford Parlett: ’Orthogonal
Eigenvectors and
Relative Gaps,’ SIAM Journal on Matrix Analysis and
Applications, Vol. 25,
2004. Also LAPACK Working Note 154.
- Inderjit Dhillon: ’A new O(nˆ2) algorithm for
the symmetric
tridiagonal eigenvalue/eigenvector problem’,
Computer Science Division Technical Report No.
UCB/CSD-97-971,
UC Berkeley, May 1997.
Note 1 :
ZHEEVR_2STAGE calls ZSTEMR when the full spectrum is
requested
on machines which conform to the ieee-754 floating point
standard.
ZHEEVR_2STAGE calls DSTEBZ and ZSTEIN on non-ieee machines
and
when partial spectrum requests are made.
Normal
execution of ZSTEMR 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.
Parameters
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’: the IL-th through IU-th eigenvalues will
be found.
For RANGE = ’V’ or ’I’ and IU - IL
< N - 1, DSTEBZ and
ZSTEIN are called
UPLO
UPLO is
CHARACTER*1
= ’U’: Upper triangle of A is stored;
= ’L’: Lower triangle of A is stored.
N
N is INTEGER
The order of the matrix A. N >= 0.
A
A is COMPLEX*16
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.
LDA
LDA is INTEGER
The leading dimension of the array A. LDA >=
max(1,N).
VL
VL is DOUBLE
PRECISION
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 DOUBLE
PRECISION
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
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 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
’Computing Small Singular Values of Bidiagonal
Matrices
with Guaranteed High Relative Accuracy,’ 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,
’Computing Accurate Eigensystems of Scaled Diagonally
Dominant Matrices’, 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 DOUBLE
PRECISION array, dimension (N)
The first M elements contain the selected eigenvalues in
ascending order.
Z
Z is COMPLEX*16
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 least max(1,M) columns
are
supplied in the array Z; if RANGE = ’V’, the
exact value of M
is not known in advance and an upper bound must be used.
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 ZSTEMR (tridiagonal
matrix). The support of the eigenvectors of A is typically
1:N because of the unitary transformations applied by
ZUNMTR.
Implemented only for RANGE = ’A’ or
’I’ and IU - IL = N - 1
WORK
WORK is
COMPLEX*16 array, dimension (MAX(1,LWORK))
On exit, if INFO = 0, WORK(1) returns the optimal LWORK.
LWORK
LWORK is
INTEGER
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.
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
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.
RWORK
RWORK is DOUBLE
PRECISION array, dimension (MAX(1,LRWORK))
On exit, if INFO = 0, RWORK(1) returns the optimal
(and minimal) LRWORK.
LRWORK
LRWORK is
INTEGER
The length of the array RWORK.
If N <= 1, LRWORK >= 1, else LRWORK >= 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.
IWORK
IWORK is
INTEGER array, dimension (MAX(1,LIWORK))
On exit, if INFO = 0, IWORK(1) returns the optimal
(and minimal) LIWORK.
LIWORK
LIWORK is
INTEGER
The dimension of the array IWORK.
If N <= 1, LIWORK >= 1, else LIWORK >= 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.
INFO
INFO is INTEGER
= 0: successful exit
< 0: if INFO = -i, the i-th argument had an illegal value
> 0: Internal error
Author
Univ. of Tennessee
Univ. of California Berkeley
Univ. of Colorado Denver
NAG Ltd.
Contributors:
Inderjit
Dhillon, IBM Almaden, USA \n
Osni Marques, LBNL/NERSC, USA \n
Ken Stanley, Computer Science Division, University of
California at Berkeley, USA \n
Jason Riedy, Computer Science Division, University of
California at Berkeley, USA \n
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
Author
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