TESTING/EIG/dglmts.f(3)
π TESTING/EIG/dglmts.f π
okay bestie, welcome to the Library Functions Manual page for TESTING/EIG/dglmts.f β yes, the filename is the whole vibe. we're about to get into dglmts, and I promise we're keeping every tiny detail. no cap. π
πΈ NAME πΈ
TESTING/EIG/dglmts.f
β¨ SYNOPSIS β¨
π«Ά Functions/Subroutines π«Ά
subroutine dglmts (n, m, p, a, af, lda, b, bf, ldb, d, df, x, u, work,
lwork, rwork, result)
DGLMTS
π§ Function/Subroutine Documentation π§
subroutine dglmts (integer n, integer m, integer p, double precision,
dimension( lda, * ) a, double precision, dimension( lda, * ) af, integer
lda, double precision, dimension( ldb, * ) b, double precision,
dimension( ldb, * ) bf, integer ldb, double precision, dimension( * ) d,
double precision, dimension( * ) df, double precision, dimension( * ) x,
double precision, dimension( * ) u, double precision, dimension( lwork )
work, integer lwork, double precision, dimension( * ) rwork, double
precision result)
DGLMTS
πΈ Purpose πΈ
DGLMTS tests DGGGLM - a subroutine for solving the generalized linear model problem. that's the whole purpose, and honestly it ate. π
π Parameters π
NβINTEGER. the number of rows of the matricesAandB.N >= 0.MβINTEGER. the number of columns of the matrixA.M >= 0.PβINTEGER. the number of columns of the matrixB.P >= 0.AβDOUBLE PRECISIONarray, dimension(LDA,M). theN-by-MmatrixA.AFβDOUBLE PRECISIONarray, dimension(LDA,M). that's the whole note for this one in the original, bestie.LDAβINTEGER. the leading dimension of the arraysA,AF.LDA >= max(M,N).BβDOUBLE PRECISIONarray, dimension(LDB,P). theN-by-PmatrixA. (yes, really β preserving the source exactly π)BFβDOUBLE PRECISIONarray, dimension(LDB,P). no extra description in the source, just vibes.LDBβINTEGER. the leading dimension of the arraysB,BF.LDB >= max(P,N).DβDOUBLE PRECISIONarray, dimension( N ). on input, the left hand side of the GLM.DFβDOUBLE PRECISIONarray, dimension( N ). no extra description in the source.XβDOUBLE PRECISIONarray, dimension( M ). solution vectorXin the GLM problem.UβDOUBLE PRECISIONarray, dimension( P ). solution vectorUin the GLM problem.WORKβDOUBLE PRECISIONarray, dimension(LWORK). no extra description in the source.LWORKβINTEGER. the dimension of the arrayWORK.RWORKβDOUBLE PRECISIONarray, dimension(M). no extra description in the source.RESULTβDOUBLE PRECISION. the test ratio:
norm( d - A*x - B*u )
RESULT = -----------------------------------------
(norm(A)+norm(B))*(norm(x)+norm(u))*EPS
π Author π
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
π Definition at line π
144 of file dglmts.f.
π Author π
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