SRC/cstegr.f(3)
πΈ NAME πΈ
SRC/cstegr.f β bestie, this is the file page for SRC/cstegr.f(3) from the Library Functions Manual. It's giving LAPACK subroutine energy, and we're getting into it. π
β¨ SYNOPSIS β¨
π Functions/Subroutines π
subroutine cstegr (jobz, range, n, d, e, vl, vu, il, iu, abstol, m, w,
z, ldz, isuppz, work, lwork, iwork, liwork, info)
CSTEGR
π¦ Function/Subroutine Documentation π¦
Okay so here's the full signature, literally character for character:
subroutine cstegr (character jobz, character range, integer n, real,
dimension( * ) d, real, dimension( * ) e, real vl, real vu, integer il,
integer iu, real abstol, integer m, real, dimension( * ) w, complex,
dimension( ldz, * ) z, integer ldz, integer, dimension( * ) isuppz,
real, dimension( * ) work, integer lwork, integer, dimension( * ) iwork,
integer liwork, integer info)
CSTEGR
π Purpose π
CSTEGR computes selected eigenvalues and, optionally, eigenvectors of a real symmetric tridiagonal matrix T. Any such unreduced matrix has a well defined set of pairwise different real eigenvalues, and the corresponding real eigenvectors are pairwise orthogonal. No cap. π
The spectrum may be computed either completely or partially by specifying either an interval (VL,VU] or a range of indices IL:IU for the desired eigenvalues. Very choose-your-own-adventure, honestly. β¨
CSTEGR is a compatibility wrapper around the improved CSTEMR routine. See SSTEMR for further details. π«Ά
One important change is that the ABSTOL parameter no longer provides any benefit and hence is no longer used. She's retired, bestie. π
β οΈ Note:CSTEGRandCSTEMRwork only on machines which follow IEEE-754 floating-point standard in their handling of infinities and NaNs. Normal execution may create these exceptional values and hence may abort due to a floating point exception in environments which do not conform to the IEEE-754 standard. So like, read that twice, fr fr. π
π Parameters π
JOBZβ type:CHARACTER*1= 'N': Compute eigenvalues only;= 'V': Compute eigenvalues and eigenvectors.
RANGEβ type: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.
Nβ type:INTEGER- The order of the matrix.
N >= 0.
- The order of the matrix.
Dβ type:REAL array, dimension (N)- On entry, the
Ndiagonal elements of the tridiagonal matrixT. On exit,Dis overwritten.
- On entry, the
Eβ type:REAL array, dimension (N)- On entry, the
(N-1)subdiagonal elements of the tridiagonal matrixTin elements1toN-1ofE.E(N)need not be set on input, but is used internally as workspace. On exit,Eis overwritten.
- On entry, the
VLβ type:REAL- If
RANGE='V', the lower bound of the interval to be searched for eigenvalues.VL < VU. Not referenced ifRANGE = 'A'or'I'.
- If
VUβ type:REAL- If
RANGE='V', the upper bound of the interval to be searched for eigenvalues.VL < VU. Not referenced ifRANGE = 'A'or'I'.
- If
ILβ type:INTEGER- If
RANGE='I', the index of the smallest eigenvalue to be returned.1 <= IL <= IU <= N, ifN > 0. Not referenced ifRANGE = 'A'or'V'.
- If
IUβ type:INTEGER- If
RANGE='I', the index of the largest eigenvalue to be returned.1 <= IL <= IU <= N, ifN > 0. Not referenced ifRANGE = 'A'or'V'.
- If
ABSTOLβ type:REAL- Unused. Was the absolute error tolerance for the eigenvalues/eigenvectors in previous versions. She's not doing anything here anymore, periodt. π
Mβ type: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.
Wβ type:REAL array, dimension (N)- The first
Melements contain the selected eigenvalues in ascending order.
- The first
Zβ type:COMPLEX array, dimension (LDZ, max(1,M) )- If
JOBZ = 'V', and ifINFO = 0, then the firstMcolumns ofZcontain the orthonormal eigenvectors of the matrixTcorresponding to the selected eigenvalues, with thei-th column ofZholding the eigenvector associated withW(i). - If
JOBZ = 'N', thenZis not referenced. - Note: the user must ensure that at least
max(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. SupplyingNcolumns is always safe.
- If
LDZβ type:INTEGER- The leading dimension of the array
Z.LDZ >= 1, and ifJOBZ = 'V', thenLDZ >= max(1,N).
- The leading dimension of the array
ISUPPZβ type:INTEGER array, dimension ( 2*max(1,M) )- The support of the eigenvectors in
Z, i.e., the indices indicating the nonzero elements inZ. Thei-th computed eigenvector is nonzero only in elementsISUPPZ( 2*i-1 )throughISUPPZ( 2*i ). This is relevant in the case when the matrix is split.ISUPPZis only accessed whenJOBZis'V'andN > 0.
- The support of the eigenvectors in
WORKβ type:REAL array, dimension (LWORK)- On exit, if
INFO = 0,WORK(1)returns the optimal (and minimal)LWORK.
- On exit, if
LWORKβ type:INTEGER- The dimension of the array
WORK.LWORK >= max(1,18*N)ifJOBZ = 'V', andLWORK >= max(1,12*N)ifJOBZ = 'N'. - If
LWORK = -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.
- The dimension of the array
IWORKβ type:INTEGER array, dimension (LIWORK)- On exit, if
INFO = 0,IWORK(1)returns the optimalLIWORK.
- On exit, if
LIWORKβ type:INTEGER- The dimension of the array
IWORK.LIWORK >= max(1,10*N)if the eigenvectors are desired, andLIWORK >= max(1,8*N)if only the eigenvalues are to be computed. - If
LIWORK = -1, then a workspace query is assumed; the routine only calculates the optimal size of theIWORKarray, returns this value as the first entry of theIWORKarray, and no error message related toLIWORKis issued byXERBLA.
- The dimension of the array
INFOβ type:INTEGER- On exit,
INFO = 0: successful exit< 0: ifINFO = -i, thei-th argument had an illegal value> 0: ifINFO = 1X, internal error inSLARRE, ifINFO = 2X, internal error inCLARRV. Here, the digitX = ABS( IINFO ) < 10, whereIINFOis the nonzero error code returned bySLARREorCLARRV, respectively.
- On exit,
π Author π
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
π Contributors: π
- Inderjit Dhillon, IBM Almaden, USA
- Osni Marques, LBNL/NERSC, USA
- Christof Voemel, LBNL/NERSC, USA
Definition at line 262 of file cstegr.f. π
π§ Author π§
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