OBSOLETE! See update_rhmc.c
/********** update_rhmc_omelyan.c ******************************************/
/* MIMD version 7 */
/*
See Takaishi and de Forcrand hep-lat/-0505020
Update lattice.
compute PHI for both factors in fermion determinant at beginning
update U by (epsilon/2)*lambda
compute X for light and strange quarks for each term in rational
function (or "both factors in det")
update H, by epsilon
update U by epsilon * (2-lambda)
compute X for light and strange quarks for each term in rational
function
update H, by epsilon
update U by (epsilon/2)*lambda
This routine does not refresh the antihermitian momenta.
This routine begins at "integral" time, with H and U evaluated
at same time.
"lambda" is adjustable parameter. At lambda=1 this is just two
leapfrog steps of length epsilon. Note my lambda is 4X the lambda in
Takaishi and de Forcrand and my epsilon is 1/2 theirs. This makes
epsilon the same as for the leapfrog algorithm.
Omelyan "optimum lambda" is 4*0.1932
*/
#include "ks_imp_includes.h" /* definitions files and prototypes */
#define mat_invert mat_invert_uml
/**#define mat_invert mat_invert_cg**/
int update() {
int step, iters=0;
double startaction,endaction;
Real xrandom;
int i;
su3_vector **multi_x;
su3_vector *sumvec;
Real lambda;
int iphi;
lambda = 0.8;
node0_printf("Omelyan integration, steps= %d eps= %e lambda= %e\n",steps,epsilon,lambda);
if (steps %2 != 0 ){
node0_printf("BONEHEAD! need even number of steps\n");
exit(0);
}
/* allocate space for multimass solution vectors */
multi_x = (su3_vector **)malloc(max_rat_order*sizeof(su3_vector *));
if(multi_x == NULL){
printf("update: No room for multi_x\n");
terminate(1);
}
for(i=0;i<max_rat_order;i++)
multi_x[i]=(su3_vector *)malloc( sizeof(su3_vector)*sites_on_node );
sumvec = (su3_vector *)malloc( sizeof(su3_vector)*sites_on_node );
/* refresh the momenta */
ranmom();
/* generate a pseudofermion configuration only at start*/
for(iphi = 0; iphi < n_pseudo; iphi++){
grsource_imp_rhmc( F_OFFSET(phi[iphi]), &(rparam[iphi].GR), EVEN,
multi_x,sumvec, rsqmin_gr[iphi], niter_gr[iphi]);
}
/* find action */
startaction=d_action_rhmc(multi_x,sumvec);
/* copy link field to old_link */
gauge_field_copy( F_OFFSET(link[0]), F_OFFSET(old_link[0]));
/* do "steps" microcanonical steps (one "step" = one force evaluation)" */
for(step=2; step <= steps; step+=2){
/* update U's and H's - see header comment */
update_u(0.5*epsilon*lambda);
update_h_rhmc( epsilon, multi_x);
update_u(epsilon*(2.0-lambda));
update_h_rhmc( epsilon, multi_x);
update_u(0.5*epsilon*lambda);
/* reunitarize the gauge field */
rephase( OFF );
reunitarize();
rephase( ON );
/*TEMP - monitor action*/ //if(step%6==0)d_action_rhmc(multi_x,sumvec);
} /* end loop over microcanonical steps */
/* find action */
/* do conjugate gradient to get (Madj M)inverse * phi */
endaction=d_action_rhmc(multi_x,sumvec);
/* decide whether to accept, if not, copy old link field back */
/* careful - must generate only one random number for whole lattice */
#ifdef HMC
if(this_node==0)xrandom = myrand(&node_prn);
broadcast_float(&xrandom);
if( exp( (double)(startaction-endaction) ) < xrandom ){
if(steps > 0)
gauge_field_copy( F_OFFSET(old_link[0]), F_OFFSET(link[0]) );
#ifdef FN
invalidate_all_ferm_links(&fn_links);
invalidate_all_ferm_links(&fn_links_dmdu0);
#endif
node0_printf("REJECT: delta S = %e\n", (double)(endaction-startaction));
}
else {
node0_printf("ACCEPT: delta S = %e\n", (double)(endaction-startaction));
}
#else // not HMC
node0_printf("CHECK: delta S = %e\n", (double)(endaction-startaction));
#endif // HMC
/* free multimass solution vector storage */
for(i=0;i<max_rat_order;i++)free(multi_x[i]);
free(sumvec);
if(steps > 0)return (iters/steps);
else return(-99);
}
OBSOLETE! See update_rhmc.c
/********** update.c ****************************************************/
/* MIMD version 7 */
/*
Update lattice.
compute PHI for both factors in fermion determinant at beginning
update U by (epsilon/2)
compute X for light and strange quarks for each term in rational
function ( or "both factors in det.")
update H, full step
update U to next time needed
This routine does not refresh the antihermitian momenta.
This routine begins at "integral" time, with H and U evaluated
at same time.
*/
#include "ks_imp_includes.h" /* definitions files and prototypes */
#define mat_invert mat_invert_uml
/**#define mat_invert mat_invert_cg**/
int update() {
int step, iters=0;
double startaction,endaction;
#ifdef HMC
Real xrandom;
#endif
int i;
su3_vector **multi_x;
su3_vector *sumvec;
int iphi;
node0_printf("Leapfrog integration, steps= %d eps= %e\n",steps,epsilon);
/* allocate space for multimass solution vectors */
multi_x = (su3_vector **)malloc(max_rat_order*sizeof(su3_vector *));
if(multi_x == NULL){
printf("update: No room for multi_x\n");
terminate(1);
}
for(i=0;i<max_rat_order;i++){
multi_x[i]=(su3_vector *)malloc( sizeof(su3_vector)*sites_on_node );
if(multi_x[i] == NULL){
printf("update: No room for multi_x\n");
terminate(1);
}
}
sumvec = (su3_vector *)malloc( sizeof(su3_vector)*sites_on_node );
/* refresh the momenta */
ranmom();
/* generate a pseudofermion configuration only at start*/
// NOTE used to clear xxx here. May want to clear all solutions for reversibility
for(iphi = 0; iphi < n_pseudo; iphi++){
grsource_imp_rhmc( F_OFFSET(phi[iphi]), &(rparam[iphi].GR), EVEN,
multi_x,sumvec, rsqmin_gr[iphi], niter_gr[iphi]);
}
/* find action */
startaction=d_action_rhmc(multi_x,sumvec);
/* copy link field to old_link */
gauge_field_copy( F_OFFSET(link[0]), F_OFFSET(old_link[0]));
/* do "steps" microcanonical steps" */
for(step=1; step <= steps; step++){
/* update U's to middle of interval */
update_u(0.5*epsilon);
/* now update H by full time interval */
update_h_rhmc( epsilon, multi_x);
/* update U's by half time step to get to even time */
update_u(epsilon*0.5);
/* reunitarize the gauge field */
rephase( OFF );
reunitarize();
rephase( ON );
/*TEMP - monitor action*/if(step%4==0)d_action_rhmc(multi_x,sumvec);
} /* end loop over microcanonical steps */
/* find action */
/* do conjugate gradient to get (Madj M)inverse * phi */
endaction=d_action_rhmc(multi_x,sumvec);
/* decide whether to accept, if not, copy old link field back */
/* careful - must generate only one random number for whole lattice */
#ifdef HMC
if(this_node==0)xrandom = myrand(&node_prn);
broadcast_float(&xrandom);
if( exp( (double)(startaction-endaction) ) < xrandom ){
if(steps > 0)
gauge_field_copy( F_OFFSET(old_link[0]), F_OFFSET(link[0]) );
#ifdef FN
invalidate_fermion_links(fn_links);
// invalidate_all_ferm_links(&fn_links);
// invalidate_all_ferm_links(&fn_links_dmdu0);
#endif
node0_printf("REJECT: delta S = %e\n", (double)(endaction-startaction));
}
else {
node0_printf("ACCEPT: delta S = %e\n", (double)(endaction-startaction));
}
#else // not HMC
node0_printf("CHECK: delta S = %e\n", (double)(endaction-startaction));
#endif // HMC
/* free multimass solution vector storage */
for(i=0;i<max_rat_order;i++)free(multi_x[i]);
free(sumvec);
if(steps > 0)return (iters/steps);
else return(-99);
}
