SRC/zstegr.f(3)
π SRC/zstegr.f(3) β Library Functions Manual π
okay bestie, welcome to the SRC/zstegr.f(3) page β manual name: Library Functions Manual. This is your ZSTEGR era, and yes, weβre keeping every single detail. π
πΈ NAME πΈ
SRC/zstegr.f
β¨ SYNOPSIS β¨
π§ Functions/Subroutines π§
subroutine zstegr (jobz, range, n, d, e, vl, vu, il, iu, abstol, m, w,
z, ldz, isuppz, work, lwork, iwork, liwork, info)
ZSTEGR
π Function/Subroutine Documentation π
subroutine zstegr (character jobz, character range, integer n, double
precision, dimension( * ) d, double precision, dimension( * ) e, 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, integer, dimension( * )
isuppz, double precision, dimension( * ) work, integer lwork, integer,
dimension( * ) iwork, integer liwork, integer info)
ZSTEGR
π¦ Purpose π¦
okay so ZSTEGR 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. 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. β¨
ZSTEGR is a compatibility wrapper around the improved ZSTEMR routine. See ZSTEMR for further details. π«Ά
One important change is that the ABSTOL parameter no longer provides any benefit and hence is no longer used. π
Note:ZSTEGRandZSTEMRwork 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. π
π Parameters π
JOBZβJOBZisCHARACTER*1= 'N':Compute eigenvalues only;= 'V':Compute eigenvalues and eigenvectors.
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.
NβNisINTEGER. The order of the matrix.N >= 0.DβDisDOUBLE PRECISIONarray, dimension(N). On entry, theNdiagonal elements of the tridiagonal matrixT. On exit,Dis overwritten.EβEisDOUBLE PRECISIONarray, 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.VLβVLisDOUBLE PRECISION. IfRANGE='V', the lower bound of the interval to be searched for eigenvalues.VL < VU. Not referenced ifRANGE = 'A'or'I'.VUβVUisDOUBLE PRECISION. 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. Not referenced ifRANGE = 'A'or'V'.IUβIUisINTEGER. IfRANGE='I', the index of the largest eigenvalue to be returned.1 <= IL <= IU <= N, ifN > 0. Not referenced ifRANGE = 'A'or'V'.ABSTOLβABSTOLisDOUBLE PRECISION. Unused. Was the absolute error tolerance for the eigenvalues/eigenvectors in previous versions.MβMisINTEGER. The total number of eigenvalues found.0 <= M <= N. IfRANGE = 'A',M = N, and ifRANGE = 'I',M = IU-IL+1.WβWisDOUBLE PRECISIONarray, dimension(N). The firstMelements contain the selected eigenvalues in ascending order.ZβZisCOMPLEX*16array, 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.LDZβLDZisINTEGER. The leading dimension of the arrayZ.LDZ >= 1, and ifJOBZ = 'V', thenLDZ >= max(1,N).ISUPPZβISUPPZisINTEGERarray, 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.WORKβWORKisDOUBLE PRECISIONarray, dimension(LWORK). On exit, ifINFO = 0,WORK(1)returns the optimal (and minimal)LWORK.LWORKβLWORKisINTEGER. 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.IWORKβIWORKisINTEGERarray, dimension(LIWORK). On exit, ifINFO = 0,IWORK(1)returns the optimalLIWORK.LIWORKβLIWORKisINTEGER. 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.INFOβINFOisINTEGER. On exit,INFO= 0:successful exit< 0:ifINFO = -i, thei-th argument had an illegal value> 0:ifINFO = 1X, internal error inDLARRE, ifINFO = 2X, internal error inZLARRV. Here, the digitX = ABS( IINFO ) < 10, whereIINFOis the nonzero error code returned byDLARREorZLARRV, respectively.
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 zstegr.f.
π Author π
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