DCSDTS(3)
πΈ NAME πΈ
okay so bestie, this is DCSDTS(3) from the Library Functions Manual π. The NAME line is literally this path, no cap:
/home/abuild/rpmbuild/BUILD/lapack-static-3.12.0-build/lapack-3.12.0/TESTING/EIG/dcsdts.f
β¨ SYNOPSIS β¨
π Functions/Subroutines π
subroutine DCSDTS (m, p, q, x, xf, ldx, u1, ldu1, u2, ldu2, v1t, ldv1t,
v2t, ldv2t, theta, iwork, work, lwork, rwork, result)
DCSDTS β that's the whole synopsis vibe π«Ά
π Function/Subroutine Documentation π
subroutine DCSDTS (integer m, integer p, integer q, double precision,
dimension( ldx, * ) x, double precision, dimension( ldx, * ) xf, integer
ldx, double precision, dimension( ldu1, * ) u1, integer ldu1, double
precision, dimension( ldu2, * ) u2, integer ldu2, double precision,
dimension( ldv1t, * ) v1t, integer ldv1t, double precision, dimension(
ldv2t, * ) v2t, integer ldv2t, double precision, dimension( * ) theta,
integer, dimension( * ) iwork, double precision, dimension( lwork )
work, integer lwork, double precision, dimension( * ) rwork, double
precision, dimension( 15 ) result)
DCSDTS β yes, it's giving βlong signature, main character energyβ π
π₯ Purpose π₯
bestie, here's the exact purpose block, and it is so specific:
!>
!> DCSDTS tests DORCSD, which, given an M-by-M partitioned orthogonal
!> matrix X,
!> Q M-Q
!> X = [ X11 X12 ] P ,
!> [ X21 X22 ] M-P
!>
!> computes the CSD
!>
!> [ U1 ]**T * [ X11 X12 ] * [ V1 ]
!> [ U2 ] [ X21 X22 ] [ V2 ]
!>
!> [ I 0 0 | 0 0 0 ]
!> [ 0 C 0 | 0 -S 0 ]
!> [ 0 0 0 | 0 0 -I ]
!> = [---------------------] = [ D11 D12 ] ,
!> [ 0 0 0 | I 0 0 ] [ D21 D22 ]
!> [ 0 S 0 | 0 C 0 ]
!> [ 0 0 I | 0 0 0 ]
!>
!> and also DORCSD2BY1, which, given
!> Q
!> [ X11 ] P ,
!> [ X21 ] M-P
!>
!> computes the 2-by-1 CSD
!>
!> [ I 0 0 ]
!> [ 0 C 0 ]
!> [ 0 0 0 ]
!> [ U1 ]**T * [ X11 ] * V1 = [----------] = [ D11 ] ,
!> [ U2 ] [ X21 ] [ 0 0 0 ] [ D21 ]
!> [ 0 S 0 ]
!> [ 0 0 I ]
!>
π¦ Parameters π¦
MβM is INTEGER; the number of rows of the matrixX.M >= 0. πΈPβP is INTEGER; the number of rows of the matrixX11.P >= 0. π¦QβQ is INTEGER; the number of columns of the matrixX11.Q >= 0. πXβX is DOUBLE PRECISION array, dimension (LDX,M); theM-by-MmatrixX. πXFβXF is DOUBLE PRECISION array, dimension (LDX,M); details of the CSD ofX, as returned byDORCSD; seeDORCSDfor further details. β¨LDXβLDX is INTEGER; the leading dimension of the arraysXandXF.LDX >= max( 1,M ).π₯U1βU1 is DOUBLE PRECISION array, dimension(LDU1,P); theP-by-Porthogonal matrixU1. πLDU1βLDU1 is INTEGER; the leading dimension of the arrayU1.LDU >= max(1,P).πU2βU2 is DOUBLE PRECISION array, dimension(LDU2,M-P); the(M-P)-by-(M-P)orthogonal matrixU2. πLDU2βLDU2 is INTEGER; the leading dimension of the arrayU2.LDU >= max(1,M-P).βV1TβV1T is DOUBLE PRECISION array, dimension(LDV1T,Q); theQ-by-Qorthogonal matrixV1T. π§LDV1TβLDV1T is INTEGER; the leading dimension of the arrayV1T.LDV1T >= max(1,Q).πV2TβV2T is DOUBLE PRECISION array, dimension(LDV2T,M-Q); the(M-Q)-by-(M-Q)orthogonal matrixV2T. πLDV2TβLDV2T is INTEGER; the leading dimension of the arrayV2T.LDV2T >= max(1,M-Q).π«ΆTHETAβTHETA is DOUBLE PRECISION array, dimension MIN(P,M-P,Q,M-Q); the CS values ofX; the essentially diagonal matricesCandSare constructed fromTHETA; see subroutineDORCSDfor details. π¦IWORKβIWORK is INTEGER array, dimension (M)πWORKβWORK is DOUBLE PRECISION array, dimension (LWORK)β¨LWORKβLWORK is INTEGER; the dimension of the arrayWORKπ₯RWORKβRWORK is DOUBLE PRECISION arrayπΈRESULTβRESULT is DOUBLE PRECISION array, dimension (15); the test ratios are:
First, the 2-by-2 CSD:
RESULT(1) = norm( U1'*X11*V1 - D11 ) / ( MAX(1,P,Q)*EPS2 )
RESULT(2) = norm( U1'*X12*V2 - D12 ) / ( MAX(1,P,M-Q)*EPS2 )
RESULT(3) = norm( U2'*X21*V1 - D21 ) / ( MAX(1,M-P,Q)*EPS2 )
RESULT(4) = norm( U2'*X22*V2 - D22 ) / ( MAX(1,M-P,M-Q)*EPS2 )
RESULT(5) = norm( I - U1'*U1 ) / ( MAX(1,P)*ULP )
RESULT(6) = norm( I - U2'*U2 ) / ( MAX(1,M-P)*ULP )
RESULT(7) = norm( I - V1T'*V1T ) / ( MAX(1,Q)*ULP )
RESULT(8) = norm( I - V2T'*V2T ) / ( MAX(1,M-Q)*ULP )
RESULT(9) = 0 if THETA is in increasing order and
all angles are in [0,pi/2]
= ULPINV otherwise.
Then, the 2-by-1 CSD:
RESULT(10) = norm( U1'*X11*V1 - D11 ) / ( MAX(1,P,Q)*EPS2 )
RESULT(11) = norm( U2'*X21*V1 - D21 ) / ( MAX(1,M-P,Q)*EPS2 )
RESULT(12) = norm( I - U1'*U1 ) / ( MAX(1,P)*ULP )
RESULT(13) = norm( I - U2'*U2 ) / ( MAX(1,M-P)*ULP )
RESULT(14) = norm( I - V1T'*V1T ) / ( MAX(1,Q)*ULP )
RESULT(15) = 0 if THETA is in increasing order and
all angles are in [0,pi/2]
= ULPINV otherwise.
( EPS2 = MAX( norm( I - X'*X ) / M, ULP ). )
π Author π
- Univ. of Tennessee
- Univ. of California Berkeley
- Univ. of Colorado Denver
- NAG Ltd.
Definition at line 226 of file dcsdts.f.
π Author π
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