TESTING/EIG/ddrvst.f(3)
okay so bestie, welcome to TESTING/EIG/ddrvst.f β this one lives in the Library Functions Manual and it's lowkey a whole vibe check for the symmetric eigenvalue drivers. π¦
πΈ NAME πΈ
TESTING/EIG/ddrvst.f
β¨ SYNOPSIS β¨
π Functions/Subroutines π
subroutine ddrvst (nsizes, nn, ntypes, dotype, iseed, thresh, nounit, a,
lda, d1, d2, d3, d4, eveigs, wa1, wa2, wa3, u, ldu, v, tau, z, work,
lwork, iwork, liwork, result, info)
DDRVST
π Function/Subroutine Documentation π
π subroutine ddrvst π
subroutine ddrvst (integer nsizes, integer, dimension( * ) nn, integer
ntypes, logical, dimension( * ) dotype, integer, dimension( 4 ) iseed,
double precision thresh, integer nounit, double precision, dimension(
lda, * ) a, integer lda, double precision, dimension( * ) d1, double
precision, dimension( * ) d2, double precision, dimension( * ) d3,
double precision, dimension( * ) d4, double precision, dimension( * )
eveigs, double precision, dimension( * ) wa1, double precision,
dimension( * ) wa2, double precision, dimension( * ) wa3, double
precision, dimension( ldu, * ) u, integer ldu, double precision,
dimension( ldu, * ) v, double precision, dimension( * ) tau, double
precision, dimension( ldu, * ) z, double precision, dimension( * ) work,
integer lwork, integer, dimension( * ) iwork, integer liwork, double
precision, dimension( * ) result, integer info)
DDRVST
π Purpose π
okay so DDRVST checks the symmetric eigenvalue problem drivers, and it is so thorough about it. π
Here's the driver lineup it's putting through the tests:
DSTEVβ computes all eigenvalues and, optionally, eigenvectors of a real symmetric tridiagonal matrix.DSTEVXβ computes selected eigenvalues and, optionally, eigenvectors of a real symmetric tridiagonal matrix.DSTEVRβ computes selected eigenvalues and, optionally, eigenvectors of a real symmetric tridiagonal matrix using the Relatively Robust Representation where it can.DSYEVβ computes all eigenvalues and, optionally, eigenvectors of a real symmetric matrix.DSYEVXβ computes selected eigenvalues and, optionally, eigenvectors of a real symmetric matrix.DSYEVRβ computes selected eigenvalues and, optionally, eigenvectors of a real symmetric matrix using the Relatively Robust Representation where it can.DSPEVβ computes all eigenvalues and, optionally, eigenvectors of a real symmetric matrix in packed storage.DSPEVXβ computes selected eigenvalues and, optionally, eigenvectors of a real symmetric matrix in packed storage.DSBEVβ computes all eigenvalues and, optionally, eigenvectors of a real symmetric band matrix.DSBEVXβ computes selected eigenvalues and, optionally, eigenvectors of a real symmetric band matrix.DSYEVDβ computes all eigenvalues and, optionally, eigenvectors of a real symmetric matrix using a divide and conquer algorithm.DSPEVDβ computes all eigenvalues and, optionally, eigenvectors of a real symmetric matrix in packed storage, using a divide and conquer algorithm.DSBEVDβ computes all eigenvalues and, optionally, eigenvectors of a real symmetric band matrix, using a divide and conquer algorithm.
When DDRVST is called, a number of matrix sizes (NSIZES) and a number of matrix types (NTYPES) are specified. For each size (NN(j)) and each type of matrix, one matrix will be generated and used to test the appropriate drivers. For each matrix and each driver routine called, the following tests will be performed:
| A - Z D Z' | / ( |A| n ulp )| I - Z Z' | / ( n ulp )| D1 - D2 | / ( |D1| ulp )
where Z is the matrix of eigenvectors returned when the eigenvector option is given, and D1 and D2 are the eigenvalues returned with and without the eigenvector option.
The sizes are specified by an array NN(1:NSIZES); the value of each element NN(j) specifies one size. The types are specified by a logical array DOTYPE( 1:NTYPES ); if DOTYPE(j) is .TRUE., then matrix type j will be generated. Currently, the list of possible types is:
- The zero matrix.
- The identity matrix.
- A diagonal matrix with evenly spaced eigenvalues
1, ..., ULPand random signs. (ULP = (first number larger than 1) - 1) - A diagonal matrix with geometrically spaced eigenvalues
1, ..., ULPand random signs. - A diagonal matrix with eigenvalues
1, ULP, ..., ULPand random signs. - Same as (4), but multiplied by
SQRT( overflow threshold ). - Same as (4), but multiplied by
SQRT( underflow threshold ). - A matrix of the form
U' D U, whereUis orthogonal andDhas evenly spaced entries1, ..., ULPwith random signs on the diagonal. - A matrix of the form
U' D U, whereUis orthogonal andDhas geometrically spaced entries1, ..., ULPwith random signs on the diagonal. - A matrix of the form
U' D U, whereUis orthogonal andDhas entries1, ULP,..., ULPwith random signs on the diagonal. - Same as (8), but multiplied by
SQRT( overflow threshold ). - Same as (8), but multiplied by
SQRT( underflow threshold ). - Symmetric matrix with random entries chosen from
(-1,1). - Same as (13), but multiplied by
SQRT( overflow threshold ). - Same as (13), but multiplied by
SQRT( underflow threshold ). - A band matrix with half bandwidth randomly chosen between
0andN-1, with evenly spaced eigenvalues1, ..., ULPwith random signs. - Same as (16), but multiplied by
SQRT( overflow threshold ). - Same as (16), but multiplied by
SQRT( underflow threshold ).
okay so, the argument list keeps going and every single one of these matters, bestie β no skipping π
NSIZESβINTEGERπΈ the number of matrix sizes to use. If it's zero,DDRVSTliterally does nothing. It must be at least zero. Not modified.NNβINTEGER array, dimension (NSIZES)π an array holding the sizes used for the matrices. Zero values get skipped. The values must be at least zero. Not modified.NTYPESβINTEGERβ¨ the number of elements inDOTYPE. If it's zero,DDRVSTdoes nothing. It must be at least zero. And there's a spicy special case: if it'sMAXTYP+1andNSIZESis1, then an additional type,MAXTYP+1, is defined, which is to use whatever matrix is inA. This is only useful ifDOTYPE(1:MAXTYP)is.FALSE.andDOTYPE(MAXTYP+1)is.TRUE.. Not modified.DOTYPEβLOGICAL array, dimension (NTYPES)π¦ ifDOTYPE(j)is.TRUE., then for each size inNNa matrix of that size and of typejwill be generated. IfNTYPESis smaller than the maximum number of types defined (PARAMETER MAXTYP), then typesNTYPES+1throughMAXTYPwill not be generated. IfNTYPESis larger thanMAXTYP,DOTYPE(MAXTYP+1)throughDOTYPE(NTYPES)will be ignored. Not modified.ISEEDβINTEGER array, dimension (4)π on entry,ISEEDspecifies the seed of the random number generator. The array elements should be between0and4095; if not, they will be reduced mod4096. Also,ISEED(4)must be odd. The random number generator uses a linear congruential sequence limited to small integers, and so should produce machine independent random numbers. The values ofISEEDare changed on exit, and can be used in the next call toDDRVSTto continue the same random number sequence. Modified.THRESHβDOUBLE PRECISIONπ a test will count as a fail if the error, computed as described above, exceedsTHRESH. Note that the error is scaled to beO(1), soTHRESHshould be a reasonably small multiple of1, e.g.,10or100. In particular, it should not depend on the precision (single vs. double) or the size of the matrix. It must be at least zero. Not modified.NOUNITβINTEGERπ the FORTRAN unit number for printing out error messages (e.g., if a routine returnsIINFOnot equal to0.). Not modified.AβDOUBLE PRECISION array, dimension (LDA , max(NN))π₯ used to hold the matrix whose eigenvalues are to be computed. On exit,Acontains the last matrix actually used. Modified.LDAβINTEGERπ the leading dimension ofA. It must be at least1and at leastmax( NN ). Not modified.D1βDOUBLE PRECISION array, dimension (max(NN))β¨ the eigenvalues ofA, as computed byDSTEQRsimultaneously withZ. On exit, the eigenvalues inD1correspond with the matrix inA. Modified.D2βDOUBLE PRECISION array, dimension (max(NN))π the eigenvalues ofA, as computed byDSTEQRifZis not computed. On exit, the eigenvalues inD2correspond with the matrix inA. Modified.D3βDOUBLE PRECISION array, dimension (max(NN))β the eigenvalues ofA, as computed byDSTERF. On exit, the eigenvalues inD3correspond with the matrix inA. Modified.D4βDOUBLE PRECISION array, dimensionπ« that's genuinely all the dimension info this page gives, so I'm not inventing numbers here.EVEIGSβDOUBLE PRECISION array, dimension (max(NN))π§ the eigenvalues as computed byDSTEV('N', ... ). And the author literally says: βI reserve the right to change this to the output of whichever algorithm computes the most accurate eigenvalues.β πWA1βDOUBLE PRECISION array, dimensionπΈ again, the page just saysdimensionand leaves it there.WA2βDOUBLE PRECISION array, dimensionπ same energy, no size listed.WA3βDOUBLE PRECISION array, dimensionπ¦ same thing, bestie.UβDOUBLE PRECISION array, dimension (LDU, max(NN))π the orthogonal matrix computed byDSYTRD+DORGTR. Modified.LDUβINTEGERπ₯ the leading dimension ofU,Z, andV. It must be at least1and at leastmax( NN ). Not modified.VβDOUBLE PRECISION array, dimension (LDU, max(NN))π the Housholder vectors computed byDSYTRDin reducingAto tridiagonal form. Modified.TAUβDOUBLE PRECISION array, dimension (max(NN))π the Householder factors computed byDSYTRDin reducingAto tridiagonal form. Modified.ZβDOUBLE PRECISION array, dimension (LDU, max(NN))β the orthogonal matrix of eigenvectors computed byDSTEQR,DPTEQR, andDSTEIN. Modified.WORKβDOUBLE PRECISION array, dimension (LWORK)π workspace. Modified.LWORKβINTEGERπ§ the number of entries inWORK. This must be at least1 + 4 * Nmax + 2 * Nmax * lg Nmax + 4 * Nmax**2whereNmax = max( NN(j), 2 )andlg = log base 2. Not modified.IWORKβINTEGER array, dimension (6 + 6*Nmax + 5 * Nmax * lg Nmax )πΈ whereNmax = max( NN(j), 2 )andlg = log base 2. Workspace. Modified.RESULTβDOUBLE PRECISION array, dimension (105)π the values computed by the tests described above. The values are currently limited to1/ulp, to avoid overflow. Modified.INFOβINTEGERπ if0, then everything ran OK. Otherwise:-1:NSIZES < 0-2: SomeNN(j) < 0-3:NTYPES < 0-5:THRESH < 0-9:LDA < 1orLDA < NMAX, whereNMAXismax( NN(j) ).-16:LDU < 1orLDU < NMAX.-21:LWORKtoo small.
If DLATMR, DLATMS, DSYTRD, DORGTR, DSTEQR, DSTERF, or DORMTR returns an error code, the absolute value of it is returned. Modified.
Some Local Variables and Parameters: π«Ά
ZERO,ONEβ real0and1.MAXTYPβ the number of types defined.NTESTβ the number of tests performed, or which can be performed so far, for the current matrix.NTESTTβ the total number of tests performed so far.NMAXβ largest value inNN.NMATSβ the number of matrices generated so far.NERRSβ the number of tests which have exceededTHRESHso far (computed byDLAFTS).COND,IMODEβ values to be passed to the matrix generators.ANORMβ norm ofA; passed to matrix generators.OVFL,UNFLβ overflow and underflow thresholds.ULP,ULPINVβ finest relative precision and its inverse.RTOVFL,RTUNFLβ square roots of the previous 2 values.
The following four arrays decode JTYPE:
KTYPE(j)β the general type (1-10) for type .KMODE(j)β theMODEvalue to be passed to the matrix generator for type .KMAGN(j)β the order of magnitude (O(1),O(overflow^(1/2) ),O(underflow^(1/2) ))
and here's the test roster β literally every test, routine included, no cap π₯
The tests performed are: Routine tested
1= | A - U S U' | / ( |A| n ulp ) DSTEV('V', ... )
2= | I - U U' | / ( n ulp ) DSTEV('V', ... )
3= |D(with Z) - D(w/o Z)| / (|D| ulp) DSTEV('N', ... )
4= | A - U S U' | / ( |A| n ulp ) DSTEVX('V','A', ... )
5= | I - U U' | / ( n ulp ) DSTEVX('V','A', ... )
6= |D(with Z) - EVEIGS| / (|D| ulp) DSTEVX('N','A', ... )
7= | A - U S U' | / ( |A| n ulp ) DSTEVR('V','A', ... )
8= | I - U U' | / ( n ulp ) DSTEVR('V','A', ... )
9= |D(with Z) - EVEIGS| / (|D| ulp) DSTEVR('N','A', ... )
10= | A - U S U' | / ( |A| n ulp ) DSTEVX('V','I', ... )
11= | I - U U' | / ( n ulp ) DSTEVX('V','I', ... )
12= |D(with Z) - D(w/o Z)| / (|D| ulp) DSTEVX('N','I', ... )
13= | A - U S U' | / ( |A| n ulp ) DSTEVX('V','V', ... )
14= | I - U U' | / ( n ulp ) DSTEVX('V','V', ... )
15= |D(with Z) - D(w/o Z)| / (|D| ulp) DSTEVX('N','V', ... )
16= | A - U S U' | / ( |A| n ulp ) DSTEVD('V', ... )
17= | I - U U' | / ( n ulp ) DSTEVD('V', ... )
18= |D(with Z) - EVEIGS| / (|D| ulp) DSTEVD('N', ... )
19= | A - U S U' | / ( |A| n ulp ) DSTEVR('V','I', ... )
20= | I - U U' | / ( n ulp ) DSTEVR('V','I', ... )
21= |D(with Z) - D(w/o Z)| / (|D| ulp) DSTEVR('N','I', ... )
22= | A - U S U' | / ( |A| n ulp ) DSTEVR('V','V', ... )
23= | I - U U' | / ( n ulp ) DSTEVR('V','V', ... )
24= |D(with Z) - D(w/o Z)| / (|D| ulp) DSTEVR('N','V', ... )
25= | A - U S U' | / ( |A| n ulp ) DSYEV('L','V', ... )
26= | I - U U' | / ( n ulp ) DSYEV('L','V', ... )
27= |D(with Z) - D(w/o Z)| / (|D| ulp) DSYEV('L','N', ... )
okay so the test list continues from 28, and it's giving extensive π β every single line is a whole vibe check for the eigensolvers, fr fr:
!> 28= | A - U S U' | / ( |A| n ulp ) DSYEVX('L','V','A', ... )
!> 29= | I - U U' | / ( n ulp ) DSYEVX('L','V','A', ... )
!> 30= |D(with Z) - D(w/o Z)| / (|D| ulp) DSYEVX('L','N','A', ... )
!> 31= | A - U S U' | / ( |A| n ulp ) DSYEVX('L','V','I', ... )
!> 32= | I - U U' | / ( n ulp ) DSYEVX('L','V','I', ... )
!> 33= |D(with Z) - D(w/o Z)| / (|D| ulp) DSYEVX('L','N','I', ... )
!> 34= | A - U S U' | / ( |A| n ulp ) DSYEVX('L','V','V', ... )
!> 35= | I - U U' | / ( n ulp ) DSYEVX('L','V','V', ... )
!> 36= |D(with Z) - D(w/o Z)| / (|D| ulp) DSYEVX('L','N','V', ... )
!> 37= | A - U S U' | / ( |A| n ulp ) DSPEV('L','V', ... )
!> 38= | I - U U' | / ( n ulp ) DSPEV('L','V', ... )
!> 39= |D(with Z) - D(w/o Z)| / (|D| ulp) DSPEV('L','N', ... )
!> 40= | A - U S U' | / ( |A| n ulp ) DSPEVX('L','V','A', ... )
!> 41= | I - U U' | / ( n ulp ) DSPEVX('L','V','A', ... )
!> 42= |D(with Z) - D(w/o Z)| / (|D| ulp) DSPEVX('L','N','A', ... )
!> 43= | A - U S U' | / ( |A| n ulp ) DSPEVX('L','V','I', ... )
!> 44= | I - U U' | / ( n ulp ) DSPEVX('L','V','I', ... )
!> 45= |D(with Z) - D(w/o Z)| / (|D| ulp) DSPEVX('L','N','I', ... )
!> 46= | A - U S U' | / ( |A| n ulp ) DSPEVX('L','V','V', ... )
!> 47= | I - U U' | / ( n ulp ) DSPEVX('L','V','V', ... )
!> 48= |D(with Z) - D(w/o Z)| / (|D| ulp) DSPEVX('L','N','V', ... )
!> 49= | A - U S U' | / ( |A| n ulp ) DSBEV('L','V', ... )
!> 50= | I - U U' | / ( n ulp ) DSBEV('L','V', ... )
!> 51= |D(with Z) - D(w/o Z)| / (|D| ulp) DSBEV('L','N', ... )
!> 52= | A - U S U' | / ( |A| n ulp ) DSBEVX('L','V','A', ... )
!> 53= | I - U U' | / ( n ulp ) DSBEVX('L','V','A', ... )
!> 54= |D(with Z) - D(w/o Z)| / (|D| ulp) DSBEVX('L','N','A', ... )
!> 55= | A - U S U' | / ( |A| n ulp ) DSBEVX('L','V','I', ... )
!> 56= | I - U U' | / ( n ulp ) DSBEVX('L','V','I', ... )
!> 57= |D(with Z) - D(w/o Z)| / (|D| ulp) DSBEVX('L','N','I', ... )
!> 58= | A - U S U' | / ( |A| n ulp ) DSBEVX('L','V','V', ... )
!> 59= | I - U U' | / ( n ulp ) DSBEVX('L','V','V', ... )
!> 60= |D(with Z) - D(w/o Z)| / (|D| ulp) DSBEVX('L','N','V', ... )
!> 61= | A - U S U' | / ( |A| n ulp ) DSYEVD('L','V', ... )
!> 62= | I - U U' | / ( n ulp ) DSYEVD('L','V', ... )
!> 63= |D(with Z) - D(w/o Z)| / (|D| ulp) DSYEVD('L','N', ... )
!> 64= | A - U S U' | / ( |A| n ulp ) DSPEVD('L','V', ... )
!> 65= | I - U U' | / ( n ulp ) DSPEVD('L','V', ... )
!> 66= |D(with Z) - D(w/o Z)| / (|D| ulp) DSPEVD('L','N', ... )
!> 67= | A - U S U' | / ( |A| n ulp ) DSBEVD('L','V', ... )
!> 68= | I - U U' | / ( n ulp ) DSBEVD('L','V', ... )
!> 69= |D(with Z) - D(w/o Z)| / (|D| ulp) DSBEVD('L','N', ... )
!> 70= | A - U S U' | / ( |A| n ulp ) DSYEVR('L','V','A', ... )
!> 71= | I - U U' | / ( n ulp ) DSYEVR('L','V','A', ... )
!> 72= |D(with Z) - D(w/o Z)| / (|D| ulp) DSYEVR('L','N','A', ... )
!> 73= | A - U S U' | / ( |A| n ulp ) DSYEVR('L','V','I', ... )
!> 74= | I - U U' | / ( n ulp ) DSYEVR('L','V','I', ... )
!> 75= |D(with Z) - D(w/o Z)| / (|D| ulp) DSYEVR('L','N','I', ... )
!> 76= | A - U S U' | / ( |A| n ulp ) DSYEVR('L','V','V', ... )
!> 77= | I - U U' | / ( n ulp ) DSYEVR('L','V','V', ... )
!> 78= |D(with Z) - D(w/o Z)| / (|D| ulp) DSYEVR('L','N','V', ... )
!>
!> Tests 25 through 78 are repeated (as tests 79 through 132)
!> with UPLO='U'
!>
!> To be added in 1999
!>
!> 79= | A - U S U' | / ( |A| n ulp ) DSPEVR('L','V','A', ... )
!> 80= | I - U U' | / ( n ulp ) DSPEVR('L','V','A', ... )
!> 81= |D(with Z) - D(w/o Z)| / (|D| ulp) DSPEVR('L','N','A', ... )
!> 82= | A - U S U' | / ( |A| n ulp ) DSPEVR('L','V','I', ... )
!> 83= | I - U U' | / ( n ulp ) DSPEVR('L','V','I', ... )
!> 84= |D(with Z) - D(w/o Z)| / (|D| ulp) DSPEVR('L','N','I', ... )
!> 85= | A - U S U' | / ( |A| n ulp ) DSPEVR('L','V','V', ... )
!> 86= | I - U U' | / ( n ulp ) DSPEVR('L','V','V', ... )
!> 87= |D(with Z) - D(w/o Z)| / (|D| ulp) DSPEVR('L','N','V', ... )
!> 88= | A - U S U' | / ( |A| n ulp ) DSBEVR('L','V','A', ... )
!> 89= | I - U U' | / ( n ulp ) DSBEVR('L','V','A', ... )
!> 90= |D(with Z) - D(w/o Z)| / (|D| ulp) DSBEVR('L','N','A', ... )
!> 91= | A - U S U' | / ( |A| n ulp ) DSBEVR('L','V','I', ... )
!> 92= | I - U U' | / ( n ulp ) DSBEVR('L','V','I', ... )
!> 93= |D(with Z) - D(w/o Z)| / (|D| ulp) DSBEVR('L','N','I', ... )
!> 94= | A - U S U' | / ( |A| n ulp ) DSBEVR('L','V','V', ... )
!> 95= | I - U U' | / ( n ulp ) DSBEVR('L','V','V', ... )
!> 96= |D(with Z) - D(w/o Z)| / (|D| ulp) DSBEVR('L','N','V', ... )
!>
and bestie, notice the βTo be added in 1999β line β yes, this list is vintage π, and the note about tests 25 through 78 being repeated as 79 through 132 with UPLO='U' is literally right there. Not me being obsessed with the historical accuracy π
Author π
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
Definition at line 449 of file ddrvst.f.
Author (the man-page one) β¨
Generated automatically by Doxygen for LAPACK from the source code.
and thatβs the whole page, bestie! π«Ά This masterpiece was auto-generated by Doxygen for LAPACK, and youβre looking at TESTING/EIG/ddrvst.f β LAPACK Version 3.12.0, no cap. πβ¨π
π¦ where this page comes from
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