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// Header Lorene:
#include "nbr_spx.h"
#include "utilitaires.h"
#include "graphique.h"
#include "math.h"
#include "metric.h"
#include "param.h"
#include "param_elliptic.h"
#include "tensor.h"
#include "diff.h"
#include "proto.h"
namespace Lorene {
// Resolution of tensorial equation (N^2/Psi^4)Delta(hij) - LbLbhij = Sij, using degenerate elliptic solver.
// Here assumption is made that no boundary condition has to be enforced, mainly Beta^i*s_i = N/psi^2
Sym_tensor boundfree_tensBC ( Sym_tensor source, Vector Beta, Scalar Psi, Scalar Nn, Sym_tensor hij_guess, double precision, int loopmax) {
cout << "================================================================" << endl;
cout << "STARTING THE SUBITERATION FOR THE CONFORMAL METRIC" << endl;
cout << " iteration parameters are the following: " << endl;
cout << " convergence precision required:" << precision << endl;
cout << " max number of global steps :" << loopmax << endl;
cout << "================================================================" << endl;
// Construction of a multi-grid (Mg3d)
// -----------------------------------
const int nz = (*source.get_mp().get_mg()).get_nzone(); // Number of domains
int nr = (*source.get_mp().get_mg()).get_nr(1); // Number of collocation points in r in each domain
const Coord& rr = source.get_mp().r;
Scalar rrr (source.get_mp()) ;
rrr = rr ;
rrr.std_spectral_base();
const Metric_flat& mets = (source.get_mp()).flat_met_spher() ;
//// Initialisation of iteration variables.
Sym_tensor hij = hij_guess;
Sym_tensor hij_new = hij;
Scalar n2sp4 = (Nn/(Psi*Psi))*(Nn/(Psi*Psi)) ; // Scale factor in front of Poisson Equation.
n2sp4.std_spectral_base();
// Resolution variables
Scalar khi = hij(1,1);
if (khi.get_etat() == ETATZERO) {
khi.annule_hard() ;
khi.set_dzpuis(4) ;
khi.std_spectral_base() ;
}
khi.set_spectral_va().ylm();
khi.mult_r();
khi.mult_r_dzpuis(1);
Scalar mmu = hij.mu();
if (mmu.get_etat() == ETATZERO) {
mmu.annule_hard() ;
mmu.std_spectral_base() ;
}
mmu.set_spectral_va().ylm();
Scalar etta = hij.eta();
if (etta.get_etat() == ETATZERO) {
etta.annule_hard() ;
etta.std_spectral_base() ;
}
etta.set_spectral_va().ylm();
Scalar Aa = hij.compute_A();
if (Aa.get_etat() == ETATZERO) {
Aa.annule_hard() ;
Aa.std_spectral_base() ;
}
Aa.set_spectral_va().ylm();
Scalar Bt = hij.compute_tilde_B();
if (Bt.get_etat() == ETATZERO) {
Bt.annule_hard() ;
Bt.std_spectral_base() ;
}
Bt.set_spectral_va().ylm();
Scalar hh = hij.trace(mets);
if (hh.get_etat() == ETATZERO) {
hh.annule_hard() ;
hh.std_spectral_base() ;
}
//Fitting scalar
Scalar fit1(source.get_mp()); fit1.set_etat_qcq();
// For storing the result of inversion
Scalar Aanew (source.get_mp()); Aanew.annule_hard(); Aanew.std_spectral_base();
Scalar Btnew (source.get_mp()); Btnew.annule_hard(); Btnew.std_spectral_base();
// Construction of sources for the next iteration
Sym_tensor LbLbhij = (hij.derive_lie(Beta)).derive_lie(Beta);
hij.annule_domain(0);
LbLbhij.annule_domain(0);
LbLbhij.inc_dzpuis(1);
Sym_tensor source_hij = source/n2sp4;
Scalar sourcetrace = source_hij.trace(mets);
Scalar Bttrace = source_hij.compute_tilde_B();
Sym_tensor source_hij2 = LbLbhij/n2sp4;
Scalar Btsource2 = source_hij2.compute_tilde_B();
Scalar source_Bt2 = Bttrace + Btsource2;
source_hij = source_hij + source_hij2;
Scalar r2LbLbrr = LbLbhij(1,1);
r2LbLbrr.mult_r();
r2LbLbrr.mult_r();
Scalar LbLbmu = LbLbhij.mu();
Scalar source_khi2 = source_hij(1,1);
source_khi2.mult_r();
source_khi2.mult_r();
Scalar source_mu2 = source_hij.mu();
Scalar source_eta2 = source_hij.eta();
Scalar source_A2 = source_hij.compute_A();
source_khi2.annule_domain(0);
source_mu2.annule_domain(0);
source_A2.annule_domain(0);
source_Bt2.annule_domain(0);
source_eta2.annule_domain(0);
// source_A2.set_spectral_va().set_base( Aa.set_spectral_va().get_base());
// source_Bt2.set_spectral_va().set_base( Bt.set_spectral_va().get_base());
//////////////// // Approximation of (Beta/(N^/psi^4))^2, for input in degenerate operator parameters.
Scalar Betacarre = (Beta(1)*Beta(1))/n2sp4 ;
double fitd1 = (Betacarre.val_grid_point(1,0,0,nr-1) - Betacarre.val_grid_point(1,0,0,0))/(rrr.val_grid_point(1,0,0,nr-1) - rrr.val_grid_point(1,0,0,0)) ;
// double error = 0.; // Voluntary error on fit.
// fitd1 += error;
int nrint = (nr-1)/2 ;
double ampl_r = (rrr.val_grid_point(1,0,0, nr -1) - rrr.val_grid_point(1,0,0 ,0))/2.;
Scalar approx(source.get_mp());
approx.annule_hard();
approx.std_spectral_base();
fit1 = fitd1*(rrr-1.) +1.;
// First order approximation
approx.set_domain(1)= fit1.set_domain(1); // MAKE PARTICULAR FOR ETATUN; DECLARE FIT1?2?3 FIRST TO BE CLEAN.
//Second order approximation
Scalar firststep = Betacarre - approx;
double ampli = firststep.val_grid_point(1,0,0,nrint);
double fit2d1 = - ampli/(ampl_r* ampl_r);
approx.set_domain(1) += (fit2d1*(rrr - 1.)*(rrr - rrr.val_grid_point(1,0,0,nr-1))).set_domain(1);
double fit0d2 = approx.val_grid_point(1,0,0,nr -1);
double fit1d2 = (Betacarre.val_grid_point(2,0,0,nr-1) - fit0d2)/(rrr.val_grid_point(2,0,0,nr-1)- rrr.val_grid_point(2,0,0,0));
double fit0d3 = Betacarre.val_grid_point(3,0,0,0);
double fit1d3 = ( - fit0d3)/(rrr.val_grid_point(3,0,0,nr-1)- rrr.val_grid_point(3,0,0,0));
approx.set_domain(2) = (fit0d2 + fit1d2*(rrr - rrr.val_grid_point(2,0,0,0))).set_domain(2);
approx.set_domain(3) = (fit0d3 + fit1d3*(rrr - rrr.val_grid_point(3,0,0,0))).set_domain(3);
for(int ii=1; ii<=3; ii++){
source_khi2.set_domain(ii) += (-approx*(khi.dsdr().dsdr())).set_domain(ii);
source_mu2.set_domain(ii) += (-approx*(mmu.dsdr().dsdr())).set_domain(ii);
source_eta2.set_domain(ii) += (-approx*(etta.dsdr().dsdr())).set_domain(ii);
source_A2.set_domain(ii) += (-approx*(Aa.dsdr().dsdr())).set_domain(ii);
source_Bt2.set_domain(ii) += (-approx*(Bt.dsdr().dsdr())).set_domain(ii);
}
// Convergence markers
Scalar Aa_old(source.get_mp());
Scalar Bt_old(source.get_mp());
// Parameters for the iteration
cout <<"==================================================================================" << endl;
cout << "amplitude for the tensor equation source (used as scaling for convergence marker)" << endl;
cout <<"==================================================================================" << endl;
double scale = max(maxabs(source));
double diff_ent = 0.15 ; // Initialisation of the difference marker between two iterations on some value
/////////////////////////////////////////////////////////////////////////////////////
///////////////// ITERATION ///////////////////////////////////////////////////////
/////////////////////////////////////////////////////////////////////////////////////
//////////////////////////////////////////////////////////////////////////////////////
for (int mer = 0; (diff_ent>precision) && (mer< loopmax) ; mer++) {
double relax = 0.15; // Global relaxation parameter
// Rsolution for variables A and tilde(B)
tensorelliptic (source_A2, Aanew , fitd1, fit2d1, fit0d2, fit1d2, fit0d3, fit1d3);
tensorellipticBt (source_Bt2, Btnew, fitd1, fit2d1, fit0d2, fit1d2, fit0d3, fit1d3);
Aa = Aanew ;
Bt = Btnew ; // No relaxation on these variables; it will be done globally on the tensor.
/////////////////////////////////////////////////////////////////////////////////
//// Resolution tests
Scalar essaiA = Aanew.laplacian() - approx*(Aanew.dsdr().dsdr());
essaiA.annule_domain(0);
Scalar bobofA = essaiA -source_A2 ;
bobofA.set_spectral_va().ylm() ;
// maxabs (bobofA);
// bobofA.spectral_display();
bobofA.set_spectral_va().ylm_i();
////////////////////////////////////////////////////////////////////////////////////
//-------------------------------------------
// Retrieving the tensor hij by Dirac inversion
//------------------------------------------
/////////////
// Magnetic part
Scalar mmuA = mmu;
Scalar mmuAsr = mmuA; mmuAsr.div_r();
Scalar xxA(source.get_mp()); xxA.annule_hard(); xxA.std_spectral_base();
const Scalar AA = Aa;
Param* par_bc = 0x0;
Sym_tensor_trans hijt(source.get_mp(), source.get_mp().get_bvect_spher(), mets);
hijt = hij;
hijt.sol_Dirac_A2 ( AA , mmuAsr, xxA, source_mu2, par_bc);
// Monitoring A and Hmu;
Scalar musrsr = mmuAsr; musrsr.div_r_dzpuis(2);
Aanew = xxA.dsdr() - musrsr;
Scalar xxsr = xxA; xxsr.div_r_dzpuis(2);
// Scalar Hmut = 3.*musrsr + mmuAsr.dsdr() + 2.*xxsr + xxsr.lapang();
////////////
//Electric part
Scalar hrrBC (source.get_mp()); hrrBC.annule_hard();
Scalar wwBC(source.get_mp()); wwBC.annule_hard();
Scalar tilde_etaBC(source.get_mp()); tilde_etaBC.annule_hard();
Scalar source_khi3 = source_khi2;
source_khi3.annule_domain(nz-1);
source_khi3 += 2*hh;
source_khi3.set_spectral_va().ylm();
hijt.sol_Dirac_BC3( Bt, hh, hrrBC , tilde_etaBC , wwBC , source_khi3, source_eta2, par_bc, par_bc) ;
// Tensor reconstruction
hij_new.set_auxiliary(hrrBC, tilde_etaBC, mmuAsr, wwBC, xxA, hh -hrrBC);
hij= relax*hij_new + (1 - relax)*hij ; // Global relaxation (opposite to relaxation on resolution variables).
// Calculation of updated trace.
hh = (1 + hij(1,1))*( hij(2,3)*hij(2,3) - hij(2,2)*hij(3,3) )
+ hij(1,2)*hij(1,2)*(1 + hij(3,3))
+ hij(1,3)*hij(1,3)*(1 + hij(2,2))
- hij(1,1)*(hij(2,2) + hij(3,3)) - 2*hij(1,2)*hij(1,3)*hij(2,3) ;
khi = hij(1,1);
khi.mult_r();
khi.mult_r_dzpuis(0);
mmu = hij.mu();
etta = hij.eta();
Aa = hij.compute_A();
Bt = hij.compute_tilde_B();
if (mer >=1){
Aa.set_spectral_va().ylm();
Bt.set_spectral_va().ylm();
Aa_old.set_spectral_va().ylm();
Bt_old.set_spectral_va().ylm();
diff_ent = max(maxabs (Bt - Bt_old))/scale; // Convergence marker
}
Aa_old = Aa;
Bt_old = Bt;
// Update of sources for the next loop
LbLbhij = (hij.derive_lie(Beta)).derive_lie(Beta);
LbLbhij.inc_dzpuis(1);
r2LbLbrr = LbLbhij(1,1);
r2LbLbrr.mult_r();
r2LbLbrr.mult_r();
LbLbmu = LbLbhij.mu();
source_hij = source/n2sp4;
Bttrace = source_hij.compute_tilde_B();
source_hij2 = LbLbhij/n2sp4;
Btsource2 = source_hij2.compute_tilde_B();
source_Bt2 = Bttrace + Btsource2;
source_hij = source_hij + source_hij2;
source_khi2 = source_hij(1,1);
source_khi2.mult_r();
source_khi2.mult_r();
source_mu2 = source_hij.mu();
source_eta2 = source_hij.eta();
source_A2= source_hij.compute_A();
source_A2.set_spectral_va().set_base( Aa.set_spectral_va().get_base());
source_Bt2.set_spectral_va().set_base( Bt.set_spectral_va().get_base());
for(int ii=1; ii<=3; ii++){
source_khi2.set_domain(ii) += (-approx*(khi.dsdr().dsdr())).set_domain(ii);
source_mu2.set_domain(ii) += (-approx*(mmu.dsdr().dsdr())).set_domain(ii);
source_eta2.set_domain(ii) += (-approx*(etta.dsdr().dsdr())).set_domain(ii);
source_A2.set_domain(ii) += (-approx*(Aa.dsdr().dsdr())).set_domain(ii);
source_Bt2.set_domain(ii) += (-approx*(Bt.dsdr().dsdr())).set_domain(ii);
}
source_khi2.annule_domain(0);
source_mu2.annule_domain(0);
source_eta2.annule_domain(0);
source_A2.annule_domain(0);
source_Bt2.annule_domain(0);
// cout << "real A resolution?" << endl;
// Sym_tensor mucorrect = LbLbhij + source;
// mucorrect = mucorrect/n2sp4;
// Scalar AAs = mucorrect.compute_A();
// AAs.annule_domain(nz-1);
// Aa.annule_domain(nz-1);
// Scalar Aa2 = Aa.laplacian();
// Scalar voirA = AAs - Aa2;
// voirA.set_spectral_va().ylm_i();
// // des_meridian(voirA, 1.00001*Rhor, Rout,"diffA", 1);
// voirA.set_spectral_va().ylm();
// maxabs (voirA);
// voirA.spectral_display("voirA", 1.e-9);
cout << "diff_ent" << diff_ent << endl;
cout << mer << endl;
}
return hij;
}
}
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