ZHEEVX(3)
okay bestie, welcome to the LAPACK manual β specifically the Library Functions Manual page for zheevx.f(3). Buckle up, we're doing complex Hermitian eigenvalues π
β¨
π NAME π
This is the whole NAME vibe: /home/abuild/rpmbuild/BUILD/lapack-static-3.12.0-build/lapack-3.12.0/SRC/zheevx.f
β¨ SYNOPSIS β¨
π§ Functions/Subroutines π§
subroutine ZHEEVX (jobz, range, uplo, n, a, lda, vl, vu, il, iu, abstol,
m, w, z, ldz, work, lwork, rwork, iwork, ifail, info)
ZHEEVX computes the eigenvalues and, optionally, the left and/or right eigenvectors for HE matrices. Periodt. π
π Function/Subroutine Documentation π
Here's the full signature, same as the original, no cap:
subroutine ZHEEVX (character jobz, character range, character uplo, integer
n, complex*16, dimension( lda, * ) a, integer lda, 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)
ZHEEVX computes the eigenvalues and, optionally, the left and/or right eigenvectors for HE matrices.
π Purpose π
okay so the whole point: ZHEEVX computes selected eigenvalues and, optionally, eigenvectors of a complex Hermitian matrix A. You can pick which eigenvalues and eigenvectors you want by specifying either a range of values or a range of indices for the desired eigenvalues. Iconic selection behavior tbh. π¦
πΈ Parameters πΈ
JOBZβJOBZ is CHARACTER*1. The "what are we computing" switch:= 'N': Compute eigenvalues only;= 'V': Compute eigenvalues and eigenvectors.
RANGEβRANGE is CHARACTER*1. The selection mode, iykyk:= '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. Which triangle ofAis stored:= 'U': Upper triangle ofAis stored;= 'L': Lower triangle ofAis stored.
NβN is INTEGER. The order of the matrixA.N >= 0.AβA is COMPLEX*16 array, dimension (LDA, N). On entry, the Hermitian matrixA. IfUPLO = 'U', the leadingN-by-Nupper triangular part ofAcontains the upper triangular part of the matrixA. IfUPLO = 'L', the leadingN-by-Nlower triangular part ofAcontains the lower triangular part of the matrixA. On exit, the lower triangle (ifUPLO='L') or the upper triangle (ifUPLO='U') ofA, including the diagonal, is destroyed. π she's gone after the glow-up.LDAβLDA is INTEGER. The leading dimension of the arrayA.LDA >= max(1,N).VLβVL is DOUBLE PRECISION. IfRANGE='V', the lower bound of the interval to be searched for eigenvalues.VL < VU. Not referenced ifRANGE = 'A'or'I'.VUβVU is DOUBLE PRECISION. IfRANGE='V', the upper bound of the interval to be searched for eigenvalues.VL < VU. Not referenced ifRANGE = 'A'or'I'.ILβIL is INTEGER. 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'.IUβIU is INTEGER. 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'.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 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. Eigenvalues will be computed most accurately when ABSTOL is set to twice the underflow threshold 2*DLAMCH('S'), not zero. If this routine returns with INFO>0, indicating that some eigenvectors did not converge, try setting ABSTOL to 2*DLAMCH('S'). See by Demmel and Kahan, LAPACK Working Note #3. π
MβM is INTEGER. The total number of eigenvalues found.0 <= M <= N. IfRANGE = 'A',M = N, and ifRANGE = 'I',M = IU-IL+1.WβW is DOUBLE PRECISION array, dimension (N). On normal exit, the firstMelements contain the selected eigenvalues in ascending order. slay, ordered. β¨ZβZ is COMPLEX*16 array, dimension (LDZ, max(1,M)). IfJOBZ = 'V', then ifINFO = 0, the firstMcolumns ofZcontain the orthonormal eigenvectors of the matrixAcorresponding to the selected eigenvalues, with the i-th column ofZholding the eigenvector associated withW(i). 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. bestie pls size your array correctly πLDZβLDZ is INTEGER. The leading dimension of the arrayZ.LDZ >= 1, and ifJOBZ = 'V',LDZ >= max(1,N).WORKβWORK is COMPLEX*16 array, dimension (MAX(1,LWORK)). On exit, ifINFO = 0,WORK(1)returns the optimalLWORK.LWORKβLWORK is INTEGER. The length of the arrayWORK.LWORK >= 1, whenN <= 1; otherwise2*N. For optimal efficiency,LWORK >= (NB+1)*N, whereNBis the max of the blocksize forZHETRDand forZUNMTRas returned byILAENV. IfLWORK = -1, then a workspace query is assumed; the routine only calculates the optimal size of theWORKarray, returns this value as the first entry of theWORKarray, and no error message related toLWORKis issued byXERBLA.RWORKβRWORK is DOUBLE PRECISION array, dimension (7*N).IWORKβIWORK is INTEGER array, dimension (5*N).IFAILβIFAIL is INTEGER 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.INFOβINFO is INTEGER. The whole exit-status tea:= 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.
Definition at line 256 of file zheevx.f.
π Author π
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