TESTING/LIN/dtbt05.f(3)
β¨ NAME β¨
Okay so this page is TESTING/LIN/dtbt05.f(3) from the Library Functions Manual, and the star of the show is TESTING/LIN/dtbt05.f β the Fortran test routine dtbt05. It has main character energy and it knows it. π
π°οΈ SYNOPSIS π°οΈ
π§ Functions/Subroutines
subroutine dtbt05 (uplo, trans, diag, n, kd, nrhs, ab, ldab, b, ldb, x, ldx, xact, ldxact, ferr, berr, reslts)βDTBT05
π§ͺ Function/Subroutine Documentation π§ͺ
subroutine dtbt05 (character uplo, character trans, character diag, integer
n, integer kd, integer nrhs, double precision, dimension( ldab, * ) ab,
integer ldab, double precision, dimension( ldb, * ) b, integer ldb,
double precision, dimension( ldx, * ) x, integer ldx, double precision,
dimension( ldxact, * ) xact, integer ldxact, double precision,
dimension( * ) ferr, double precision, dimension( * ) berr, double
precision, dimension( * ) reslts)
DTBT05
π― Purpose
Bestie, <rainbow>DTBT05</rainbow> tests the error bounds from iterative refinement for the computed solution to a system of equations A*X = B, where A is a triangular band matrix. That's the whole vibe.
RESLTS(1) = test of the error bound
= norm(X - XACT) / ( norm(X) * FERR )
A large value is returned if this ratio is not less than one.
RESLTS(2) = residual from the iterative refinement routine
= the maximum of BERR / ( NZ*EPS + (*) ), where
(*) = NZ*UNFL / (min_i (abs(A)*abs(X) +abs(b))_i )
and NZ = max. number of nonzeros in any row of A, plus 1
π§Ύ Parameters
UPLOβUPLO is CHARACTER*1. It specifies whether the matrixAis upper or lower triangular:'U': Upper triangular'L': Lower triangular
TRANSβTRANS is CHARACTER*1. It specifies the form of the system of equations:'N':A * X = B(No transpose)'T':A'* X = B(Transpose)'C':A'* X = B(Conjugate transpose = Transpose)
DIAGβDIAG is CHARACTER*1. It specifies whether or not the matrixAis unit triangular:'N': Non-unit triangular'U': Unit triangular
NβN is INTEGER. The number of rows of the matricesX,B, andXACT, and the order of the matrixA.N >= 0.KDβKD is INTEGER. The number of super-diagonals of the matrixAifUPLO = 'U', or the number of sub-diagonals ifUPLO = 'L'.KD >= 0.NRHSβNRHS is INTEGER. The number of columns of the matricesX,B, andXACT.NRHS >= 0.ABβAB is DOUBLE PRECISION array, dimension (LDAB,N). The upper or lower triangular band matrixA, stored in the firstkd+1rows of the array. Thej-th column ofAis stored in thej-th column of the arrayABas follows:
if UPLO = 'U', AB(kd+1+i-j,j) = A(i,j) for max(1,j-kd)<=i<=j;
if UPLO = 'L', AB(1+i-j,j) = A(i,j) for j<=i<=min(n,j+kd).
If DIAG = 'U', the diagonal elements of A are not referenced and are assumed to be 1.
LDABβLDAB is INTEGER. The leading dimension of the arrayAB.LDAB >= KD+1.BβB is DOUBLE PRECISION array, dimension (LDB,NRHS). The right hand side vectors for the system of linear equations.LDBβLDB is INTEGER. The leading dimension of the arrayB.LDB >= max(1,N).XβX is DOUBLE PRECISION array, dimension (LDX,NRHS). The computed solution vectors. Each vector is stored as a column of the matrixX.LDXβLDX is INTEGER. The leading dimension of the arrayX.LDX >= max(1,N).XACTβXACT is DOUBLE PRECISION array, dimension (LDX,NRHS). The exact solution vectors. Each vector is stored as a column of the matrixXACT.LDXACTβLDXACT is INTEGER. The leading dimension of the arrayXACT.LDXACT >= max(1,N).FERRβFERR is DOUBLE PRECISION array, dimension (NRHS). The estimated forward error bounds for each solution vectorX. IfXTRUEis the true solution,FERRbounds the magnitude of the largest entry in(X - XTRUE)divided by the magnitude of the largest entry inX.BERRβBERR is DOUBLE PRECISION array, dimension (NRHS). The componentwise relative backward error of each solution vector (i.e., the smallest relative change in any entry ofAorBthat makesXan exact solution).RESLTSβRESLTS is DOUBLE PRECISION array, dimension (2). The maximum over theNRHSsolution vectors of the ratios:
RESLTS(1) = norm(X - XACT) / ( norm(X) * FERR )
RESLTS(2) = BERR / ( NZ*EPS + (*) )
π Author
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
Definition at line 187 of file dtbt05.f.
π Author
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