SRC/sstegr.f(3)
π NAME π
okay bestie, welcome to the SRC/sstegr.f(3) page from the Library Functions Manual β yes, the whole NAME section is literally just SRC/sstegr.f, and we love a minimal icon π
β¨ SYNOPSIS β¨
π¦ Functions/Subroutines π¦
subroutine sstegr (jobz, range, n, d, e, vl, vu, il, iu, abstol, m, w,
z, ldz, isuppz, work, lwork, iwork, liwork, info)
SSTEGR
π Function/Subroutine Documentation π
πΈ subroutine sstegr πΈ
subroutine sstegr (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, real,
dimension( ldz, * ) z, integer ldz, integer, dimension( * ) isuppz,
real, dimension( * ) work, integer lwork, integer, dimension( * ) iwork,
integer liwork, integer info)
SSTEGR
π Purpose π
okay so SSTEGR 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. iconic behavior, no cap β¨
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. bestie gets options π
SSTEGR is a compatibility wrapper around the improved SSTEMR routine. See SSTEMR for further details.
One important change is that the ABSTOL parameter no longer provides any benefit and hence is no longer used. rip bozo, but make a note π
Note:SSTEGRandSSTEMRwork 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 likeβ¦ check your machine's vibe before sending it π
π Parameters π
JOBZβJOBZ is CHARACTER*1.= 'N': compute eigenvalues only;= 'V': compute eigenvalues and eigenvectors. pick your fighter, bestie πRANGEβRANGE 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. the range girlies stay winning β¨NβN is INTEGER. The order of the matrix.N >= 0.DβD is REAL array, dimension (N). On entry, theNdiagonal elements of the tridiagonal matrixT. On exit,Dis overwritten. she gets replaced, periodt πEβE is 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.VLβVL is REAL. IfRANGE='V', the lower bound of the interval to be searched for eigenvalues.VL < VU. Not referenced ifRANGE = 'A'or'I'.VUβVU is REAL. 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. 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. Not referenced ifRANGE = 'A'or'V'.ABSTOLβABSTOL is REAL. Unused. Was the absolute error tolerance for the eigenvalues/eigenvectors in previous versions. she's retired, let her rest π«ΆMβM is INTEGER. The total number of eigenvalues found.0 <= M <= N. IfRANGE = 'A',M = N, and ifRANGE = 'I',M = IU-IL+1.WβW is REAL array, dimension (N). The firstMelements contain the selected eigenvalues in ascending order. organized queen πZβZ is REAL array, dimension (LDZ, max(1,M) ). IfJOBZ = '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). 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. SupplyingNcolumns is always safe. literally plan ahead bestie πLDZβLDZ is INTEGER. The leading dimension of the arrayZ.LDZ >= 1, and ifJOBZ = 'V', thenLDZ >= max(1,N).ISUPPZβISUPPZ is INTEGER array, dimension ( 2*max(1,M) ). The support of the eigenvectors inZ, 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. support system but make it math πWORKβWORK is REAL array, dimension (LWORK). On exit, ifINFO = 0,WORK(1)returns the optimal (and minimal)LWORK.LWORKβLWORK is INTEGER. The dimension of the arrayWORK.LWORK >= max(1,18*N)ifJOBZ = 'V', andLWORK >= max(1,12*N)ifJOBZ = 'N'. 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.IWORKβIWORK is INTEGER array, dimension (LIWORK). On exit, ifINFO = 0,IWORK(1)returns the optimalLIWORK.LIWORKβLIWORK is INTEGER. The dimension of the arrayIWORK.LIWORK >= max(1,10*N)if the eigenvectors are desired, andLIWORK >= max(1,8*N)if only the eigenvalues are to be computed. IfLIWORK = -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.INFOβINFO is 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 inSLARRV. Here, the digitX = ABS( IINFO ) < 10, whereIINFOis the nonzero error code returned bySLARREorSLARRV, respectively. so ifINFOis being weird, that's the lore π
π Author π
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
πΈ Contributors πΈ
- Inderjit Dhillon, IBM Almaden, USA
- Osni Marques, LBNL/NERSC, USA
- Christof Voemel, LBNL/NERSC, USA
Definition at line 262 of file sstegr.f.
π§ Author π§
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