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libflame
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Functions | |
| FLA_Error | FLA_UDdate_UT_unb_var1 (FLA_Obj R, FLA_Obj C, FLA_Obj D, FLA_Obj T) |
References FLA_Apply_HUD_UT(), FLA_Cont_with_1x3_to_1x2(), FLA_Cont_with_3x3_to_2x2(), FLA_Herk_external(), FLA_Househ3UD_UT(), FLA_MINUS_ONE, FLA_Obj_min_dim(), FLA_ONE, FLA_ONE_HALF, FLA_Part_1x2(), FLA_Part_2x2(), FLA_Repart_1x2_to_1x3(), FLA_Repart_2x2_to_3x3(), FLA_Scale_diag(), and FLA_Set_to_identity().
Referenced by FLA_UDdate_UT_internal().
{
FLA_Obj RTL, RTR, R00, r01, R02,
RBL, RBR, r10t, rho11, r12t,
R20, r21, R22;
FLA_Obj CL, CR, C0, c1, C2;
FLA_Obj DL, DR, D0, d1, D2;
FLA_Obj TTL, TTR, T00, t01, T02,
TBL, TBR, t10t, tau11, w12t,
T20, t21, T22;
FLA_Part_2x2( R, &RTL, &RTR,
&RBL, &RBR, 0, 0, FLA_TL );
FLA_Part_1x2( C, &CL, &CR, 0, FLA_LEFT );
FLA_Part_1x2( D, &DL, &DR, 0, FLA_LEFT );
FLA_Part_2x2( T, &TTL, &TTR,
&TBL, &TBR, 0, 0, FLA_TL );
while ( FLA_Obj_min_dim( RBR ) > 0 ){
FLA_Repart_2x2_to_3x3( RTL, /**/ RTR, &R00, /**/ &r01, &R02,
/* ************* */ /* ************************** */
&r10t, /**/ &rho11, &r12t,
RBL, /**/ RBR, &R20, /**/ &r21, &R22,
1, 1, FLA_BR );
FLA_Repart_1x2_to_1x3( CL, /**/ CR, &C0, /**/ &c1, &C2,
1, FLA_RIGHT );
FLA_Repart_1x2_to_1x3( DL, /**/ DR, &D0, /**/ &d1, &D2,
1, FLA_RIGHT );
FLA_Repart_2x2_to_3x3( TTL, /**/ TTR, &T00, /**/ &t01, &T02,
/* ************* */ /* ************************ */
&t10t, /**/ &tau11, &w12t,
TBL, /**/ TBR, &T20, /**/ &t21, &T22,
1, 1, FLA_BR );
/*------------------------------------------------------------*/
// Compute tau11, u1, and v2 from rho11, c1, and d1 such that tau11, u1,
// and v1 determine an up/downdating UT Householder transform H such that
// applying H from the left to the column vector consisting of rho11, c1,
// and d1 annihilates the entries in c1 and d1 (and updates rho11).
FLA_Househ3UD_UT( rho11,
c1,
d1, tau11 );
// / r12t \ / r12t \
// | C2 | = H' | C2 |
// \ D2 / \ D2 /
//
// where H is formed from tau11, u1 (stored in c1) and v1 (stored in d1).
FLA_Apply_HUD_UT( FLA_LEFT,
tau11, w12t,
r12t,
c1, C2,
d1, D2 );
/*------------------------------------------------------------*/
FLA_Cont_with_3x3_to_2x2( &RTL, /**/ &RTR, R00, r01, /**/ R02,
r10t, rho11, /**/ r12t,
/* ************** */ /* ************************ */
&RBL, /**/ &RBR, R20, r21, /**/ R22,
FLA_TL );
FLA_Cont_with_1x3_to_1x2( &CL, /**/ &CR, C0, c1, /**/ C2,
FLA_LEFT );
FLA_Cont_with_1x3_to_1x2( &DL, /**/ &DR, D0, d1, /**/ D2,
FLA_LEFT );
FLA_Cont_with_3x3_to_2x2( &TTL, /**/ &TTR, T00, t01, /**/ T02,
t10t, tau11, /**/ w12t,
/* ************** */ /* ********************** */
&TBL, /**/ &TBR, T20, t21, /**/ T22,
FLA_TL );
}
// T = I + C' * C - D' * D;
// T = striu( T ) + 0.5*diag( T );
// NOTE: The only reason this 'herk' method of computing T works is because
// up-and-downdating is used to up/downdate a system that is being solved
// either by QR factorization, or the method of normal equations (Cholesky
// factorization on A' * A), and in either case, R will have a real diagonal.
FLA_Set_to_identity( T );
FLA_Herk_external( FLA_UPPER_TRIANGULAR, FLA_CONJ_TRANSPOSE,
FLA_ONE, C, FLA_ONE, T );
FLA_Herk_external( FLA_UPPER_TRIANGULAR, FLA_CONJ_TRANSPOSE,
FLA_MINUS_ONE, D, FLA_ONE, T );
FLA_Scale_diag( FLA_NO_CONJUGATE, FLA_ONE_HALF, T );
return FLA_SUCCESS;
}
1.7.6.1