void eo_fermion_force_rhmc( Real eps, params_ratfunc *rf,
su3_vector **multi_x, field_offset phi_off,
Real my_rsqmin, int my_niter,
int cg_prec, int ff_prec, fermion_links_t *fl)
{
// at different time steps
Real final_rsq;
int j;
int order = rf->order;
Real *residues = rf->res;
Real *roots = rf->pole;
imp_ferm_links_t **fn;
// Compute ( M^\dagger M)^{-1} in xxx_even
// Then compute M*xxx in temporary vector xxx_odd
/* See long comment at end of file */
/* The diagonal term in M doesn't matter */
// load_ferm_links(fn);
restore_fermion_links_from_site(fl, cg_prec);
fn = get_fm_links(fl);
/* Do the inversion for zero Naik term epsilon */
ks_ratinv( phi_off, multi_x, roots, order, my_niter,
my_rsqmin, cg_prec, EVEN, &final_rsq, fn[0], 0, 0. );
/* Do dslash for zero Naik term epsilon */
for(j=0;j<order;j++){ dslash_field( multi_x[j], multi_x[j], ODD, fn[0] ); }
eo_fermion_force_multi( eps, &(residues[1]), multi_x, order, ff_prec, fl );
}
// fermion force update grouping pseudofermions with the same path coeffs
int update_h_fermion( Real eps, su3_vector **multi_x ){
int iphi,jphi;
Real final_rsq;
int i,j,n;
int order, tmporder;
Real *residues,*allresidues;
Real *roots;
int iters = 0;
imp_ferm_links_t **fn;
/* Algorithm sketch: assemble multi_x with all |X> fields,
then call force routine for each part (so far we have to parts:
zero correction to Naik and non-zero correction to Naik */
allresidues = (Real *)malloc(n_order_naik_total*sizeof(Real));
// Group the fermion force calculation according to sets of like
// path coefficients.
tmporder = 0;
iphi = 0;
#if ( FERM_ACTION == HISQ || FERM_ACTION == HYPISQ )
n = fermion_links_get_n_naiks(fn_links);
#else
n = 1;
#endif
for( i=0; i<n; i++ ) {
for( jphi=0; jphi<n_pseudo_naik[i]; jphi++ ) {
restore_fermion_links_from_site(fn_links, prec_md[iphi]);
fn = get_fm_links(fn_links);
// Add the current pseudofermion to the current set
order = rparam[iphi].MD.order;
residues = rparam[iphi].MD.res;
roots = rparam[iphi].MD.pole;
// Compute ( M^\dagger M)^{-1} in xxx_even
// Then compute M*xxx in temporary vector xxx_odd
/* See long comment at end of file */
/* The diagonal term in M doesn't matter */
iters += ks_ratinv( F_OFFSET(phi[iphi]), multi_x+tmporder, roots, order,
niter_md[iphi], rsqmin_md[iphi], prec_md[iphi], EVEN,
&final_rsq, fn[i],
i, rparam[iphi].naik_term_epsilon );
for(j=0;j<order;j++){
dslash_field( multi_x[tmporder+j], multi_x[tmporder+j], ODD,
fn[i]);
allresidues[tmporder+j] = residues[j+1];
// remember that residues[0] is constant, no force contribution.
}
tmporder += order;
iphi++;
}
}
#ifdef MILC_GLOBAL_DEBUG
node0_printf("update_h_rhmc: MULTI_X ASSEMBLED\n");fflush(stdout);
node0_printf("update_h_rhmc: n_distinct_Naik=%d\n",n);
for(j=0;j<n;j++)
node0_printf("update_h_rhmc: orders[%d]=%d\n",j,n_orders_naik[j]);
#if ( FERM_ACTION == HISQ || FERM_ACTION == HYPISQ )
for(j=0;j<n;j++)
node0_printf("update_h_rhmc: masses_Naik[%d]=%f\n",j,fn_links.hl.eps_naik[j]);
#endif
fflush(stdout);
#endif /* MILC_GLOBAL_DEBUG */
restore_fermion_links_from_site(fn_links, prec_ff);
eo_fermion_force_multi( eps, allresidues, multi_x,
n_order_naik_total, prec_ff, fn_links );
free(allresidues);
return iters;
} /* update_h_fermion */
