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libflame
revision_anchor
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Functions | |
| FLA_Error | FLA_Tevd_eigval_n_opt_var1 (FLA_Obj G, FLA_Obj d, FLA_Obj e, FLA_Obj k) |
| FLA_Error | FLA_Tevd_eigval_n_ops_var1 (int m_A, int n_G, float *buff_d, int inc_d, float *buff_e, int inc_e, int *n_iter) |
| FLA_Error | FLA_Tevd_eigval_n_opd_var1 (int m_A, int n_G, double *buff_d, int inc_d, double *buff_e, int inc_e, int *n_iter) |
| FLA_Error FLA_Tevd_eigval_n_opd_var1 | ( | int | m_A, |
| int | n_G, | ||
| double * | buff_d, | ||
| int | inc_d, | ||
| double * | buff_e, | ||
| int | inc_e, | ||
| int * | n_iter | ||
| ) |
References FLA_Mach_params_opd(), FLA_Tevd_francis_n_opd_var1(), and FLA_Wilkshift_tridiag_opd().
Referenced by FLA_Tevd_eigval_n_opt_var1(), and FLA_Tevd_iteracc_n_opd_var1().
{
FLA_Error r_val;
double eps2;
double safmin;
double* e_last;
double* d_last;
double* d_last_m1;
double shift;
int k;
int n_iter_allowed = n_G;
// Query epsilon and safmin, which are used in the test for convergence.
eps2 = FLA_Mach_params_opd( FLA_MACH_EPS2 );
safmin = FLA_Mach_params_opd( FLA_MACH_SFMIN );
// Initialize a pointer to the last sub-diagonal element and two
// more to the last and second last
e_last = &buff_e[ (m_A-2)*inc_e ];
d_last_m1 = &buff_d[ (m_A-2)*inc_d ];
d_last = &buff_d[ (m_A-1)*inc_d ];
for ( k = 0; k < n_iter_allowed; ++k )
{
/*------------------------------------------------------------*/
// If we've converged, record k and return index of eigenvalue found.
// The reason we check before the Francis step (rather than after)
// is so we correctly handle situations where the last diagonal
// element has already converged from previous eigenvalue searches
// and thus no iteration is necessary. If we checked after the
// Francis step, we would have unnecessarily executed an additional
// Francis step's worth of rotations with a sub-optimal shift (since
// it would be using a 2x2 that was not "centered" properly).
if ( MAC_Tevd_eigval_converged2_opd( eps2, safmin, *d_last_m1, *e_last, *d_last ) )
{
*e_last = 0.0;
*n_iter = k;
return m_A - 1;
}
//if ( (n_iter_allowed - k) % 2 == 0 )
// Compute a Wilkinson shift with the last 2x2 matrix.
FLA_Wilkshift_tridiag_opd( *d_last_m1,
*e_last,
*d_last,
&shift );
//else
// shift = *d_last;
// Perform a Francis step.
r_val = FLA_Tevd_francis_n_opd_var1( m_A,
&shift,
buff_d, inc_d,
buff_e, inc_e );
// Check for internal deflation.
if ( r_val != FLA_SUCCESS )
{
#ifdef PRINTF
printf( "FLA_Tevd_eigval_n_opt_var1: Internal deflation in col %d, eig %d\n", r_val, m_A - 1 );
printf( "FLA_Tevd_eigval_n_opt_var1: alpha11 = %23.19e\n", buff_d[r_val*inc_d] );
printf( "FLA_Tevd_eigval_n_opt_var1: alpha21 alpha22 = %23.19e %23.19e\n", buff_e[r_val*inc_e], buff_d[(r_val+1)*inc_d] );
#endif
// Set the off-diagonal element to zero.
buff_e[ r_val*inc_e ] = 0.0;
*n_iter = k + 1;
return r_val;
}
/*------------------------------------------------------------*/
}
*n_iter = n_iter_allowed;
return FLA_FAILURE;
}
| FLA_Error FLA_Tevd_eigval_n_ops_var1 | ( | int | m_A, |
| int | n_G, | ||
| float * | buff_d, | ||
| int | inc_d, | ||
| float * | buff_e, | ||
| int | inc_e, | ||
| int * | n_iter | ||
| ) |
Referenced by FLA_Tevd_eigval_n_opt_var1().
{
return FLA_SUCCESS;
}
References FLA_Obj_datatype(), FLA_Obj_vector_dim(), FLA_Obj_vector_inc(), FLA_Obj_width(), FLA_Tevd_eigval_n_opd_var1(), and FLA_Tevd_eigval_n_ops_var1().
{
FLA_Datatype datatype;
int m_A, n_G;
int inc_d;
int inc_e;
datatype = FLA_Obj_datatype( d );
m_A = FLA_Obj_vector_dim( d );
n_G = FLA_Obj_width( G );
inc_d = FLA_Obj_vector_inc( d );
inc_e = FLA_Obj_vector_inc( e );
switch ( datatype )
{
case FLA_FLOAT:
{
float* buff_d = FLA_FLOAT_PTR( d );
float* buff_e = FLA_FLOAT_PTR( e );
int* buff_k = FLA_INT_PTR( k );
FLA_Tevd_eigval_n_ops_var1( m_A,
n_G,
buff_d, inc_d,
buff_e, inc_e,
buff_k );
break;
}
case FLA_DOUBLE:
{
double* buff_d = FLA_DOUBLE_PTR( d );
double* buff_e = FLA_DOUBLE_PTR( e );
int* buff_k = FLA_INT_PTR( k );
FLA_Tevd_eigval_n_opd_var1( m_A,
n_G,
buff_d, inc_d,
buff_e, inc_e,
buff_k );
break;
}
}
return FLA_SUCCESS;
}
1.7.6.1