boson_star_equil.C

/*
 * Method Boson_star::equilibrium
 *
 *    (see file boson_star.h for documentation).
 */
 
/*
 *   Copyright (c) 2012 Claire Some, Eric Gourgoulhon
 *
 *   This file is part of LORENE.
 *
 *   LORENE is free software; you can redistribute it and/or modify
 *   it under the terms of the GNU General Public License as published by
 *   the Free Software Foundation; either version 2 of the License, or
 *   (at your option) any later version.
 *
 *   LORENE is distributed in the hope that it will be useful,
 *   but WITHOUT ANY WARRANTY; without even the implied warranty of
 *   MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE.  See the
 *   GNU General Public License for more details.
 *
 *   You should have received a copy of the GNU General Public License
 *   along with LORENE; if not, write to the Free Software
 *   Foundation, Inc., 59 Temple Place, Suite 330, Boston, MA  02111-1307  USA
 *
 */
 
 
 
 
/*
 * $Id: boson_star_equil.C,v 1.7 2016/12/05 16:17:49 j_novak Exp $
 * $Log: boson_star_equil.C,v $
 * Revision 1.7  2016/12/05 16:17:49  j_novak
 * Suppression of some global variables (file names, loch, ...) to prevent redefinitions
 *
 * Revision 1.6  2014/10/13 08:52:49  j_novak
 * Lorene classes and functions now belong to the namespace Lorene.
 *
 * Revision 1.5  2014/10/06 15:13:04  j_novak
 * Modified #include directives to use c++ syntax.
 *
 * Revision 1.4  2013/04/03 12:10:13  e_gourgoulhon
 * Added member kk to Compobj; suppressed tkij
 *
 * Revision 1.3  2012/12/03 15:27:30  c_some
 * Small changes
 *
 * Revision 1.2  2012/11/23 15:43:05  c_some
 * Small changes
 *
 * Revision 1.1  2012/11/22 16:04:12  c_some
 * New class Boson_star
 *
 *
 * $Header: /cvsroot/Lorene/C++/Source/Compobj/boson_star_equil.C,v 1.7 2016/12/05 16:17:49 j_novak Exp $
 *
 */
 
// Headers C
#include <cmath>
 
// Headers Lorene
#include "boson_star.h"
#include "param.h"
#include "tenseur.h"
 
#include "graphique.h"
#include "utilitaires.h"
#include "unites.h"
 
namespace Lorene {
void Boson_star::equilibrium(double, double,
                 int nzadapt, const Tbl& phi_limit, const Itbl& icontrol,
                 const Tbl& control, Tbl& diff, Param*) {
                 
    // Fundamental constants and units
    // -------------------------------
 
    using namespace Unites ;        
    
    // For the display 
    // ---------------
    char display_bold[]="x[1m" ; display_bold[0] = 27 ;
    char display_normal[] = "x[0m" ; display_normal[0] = 27 ;
 
    // Grid parameters
    // ---------------
    
    const Mg3d* mg = mp.get_mg() ; 
    int nz = mg->get_nzone() ;      // total number of domains
    
    // The following is required to initialize mp_prev as a Map_et:
    Map_et& mp_et = dynamic_cast<Map_et&>(mp) ; 
        
    // Index of the point at phi=0, theta=pi/2 at the surface of the star:
 
    int nzet = nzadapt ; //## to be checked 
    
    assert(mg->get_type_t() == SYM) ; 
    int l_b = nzet - 1 ; 
    int j_b = mg->get_nt(l_b) - 1 ; 
    int k_b = 0 ; 
    
    // Value of the enthalpy defining the surface of the star
    // double ent_b = phi_limit(nzet-1) ;
    
    // Parameters to control the iteration
    // -----------------------------------
    
    int mer_max = icontrol(0) ; 
//    int mer_rot = icontrol(1) ;
//    int mer_change_omega = icontrol(2) ; 
//    int mer_fix_omega = icontrol(3) ; 
//##    int mer_mass = icontrol(4) ; 
    int mermax_poisson = icontrol(5) ; 
    int mer_triax = icontrol(6) ; 
//##    int delta_mer_kep = icontrol(7) ; 
 
 
    double precis = control(0) ; 
//    double omega_ini = control(1) ; 
    double relax = control(2) ;
    double relax_prev = double(1) - relax ;  
    double relax_poisson = control(3) ; 
//    double thres_adapt = control(4) ; 
    double ampli_triax = control(5) ; 
    double precis_adapt = control(6) ; 
 
 
    // Error indicators
    // ----------------
    
    diff.set_etat_qcq() ; 
    double& diff_phi = diff.set(0) ; 
    double& diff_nuf = diff.set(1) ; 
    double& diff_nuq = diff.set(2) ; 
//    double& diff_dzeta = diff.set(3) ; 
//    double& diff_ggg = diff.set(4) ; 
    double& diff_shift_x = diff.set(5) ; 
    double& diff_shift_y = diff.set(6) ; 
    double& vit_triax = diff.set(7) ; 
    
    // Parameters for the function Map_et::adapt
    // -----------------------------------------
    
    Param par_adapt ; 
    int nitermax = 100 ;  
    int niter ; 
    int adapt_flag = 1 ;    //  1 = performs the full computation, 
                //  0 = performs only the rescaling by 
                //      the factor alpha_r
    int nz_search = nzet + 1 ;  // Number of domains for searching the enthalpy
                //  isosurfaces
    double alpha_r ; 
    double reg_map = 1. ; // 1 = regular mapping, 0 = contracting mapping
 
    par_adapt.add_int(nitermax, 0) ; // maximum number of iterations to
                     // locate zeros by the secant method
    par_adapt.add_int(nzadapt, 1) ; // number of domains where the adjustment 
                    // to the isosurfaces of ent is to be 
                    // performed
    par_adapt.add_int(nz_search, 2) ;   // number of domains to search for
                    // the enthalpy isosurface
    par_adapt.add_int(adapt_flag, 3) ; //  1 = performs the full computation, 
                       //  0 = performs only the rescaling by 
                       //      the factor alpha_r
    par_adapt.add_int(j_b, 4) ; //  theta index of the collocation point 
                    //  (theta_*, phi_*)
    par_adapt.add_int(k_b, 5) ; //  theta index of the collocation point 
                    //  (theta_*, phi_*)
 
    par_adapt.add_int_mod(niter, 0) ;  //  number of iterations actually used in 
                       //  the secant method
    
    par_adapt.add_double(precis_adapt, 0) ; // required absolute precision in 
                         // the determination of zeros by 
                         // the secant method
    par_adapt.add_double(reg_map, 1)    ;  // 1. = regular mapping, 0 = contracting mapping
    
    par_adapt.add_double(alpha_r, 2) ;  // factor by which all the radial 
                       // distances will be multiplied 
           
    par_adapt.add_tbl(phi_limit, 0) ;   // array of values of the field Phi
                        // to define the isosurfaces.              
 
    // Parameters for the function Map_et::poisson for nuf
    // ----------------------------------------------------
 
    double precis_poisson = 1.e-16 ;     
 
    // Preparations 
    // ------------
    
    // Cartesian components of the shift vector are required
    beta.change_triad( mp.get_bvect_cart() ) ; 
 
 
    Cmp cssjm1_nuf(ssjm1_nuf) ; 
    Cmp cssjm1_nuq(ssjm1_nuq) ; 
    Cmp cssjm1_tggg(ssjm1_tggg) ; 
    Cmp cssjm1_khi(ssjm1_khi) ; 
    Tenseur cssjm1_wshift(mp, 1, CON, mp.get_bvect_cart() ) ;
    cssjm1_wshift.set_etat_qcq() ;
    for (int i=1; i<=3; i++) {
    cssjm1_wshift.set(i-1) = ssjm1_wshift(i) ; 
    }
 
    Tenseur cshift(mp, 1, CON, mp.get_bvect_cart() ) ;
    cshift.set_etat_qcq() ;
    for (int i=1; i<=3; i++) {
      cshift.set(i-1) = -beta(i) ; 
    }
 
    Tenseur cw_shift(mp, 1, CON, mp.get_bvect_cart() ) ;
    cw_shift.set_etat_qcq() ;
    for (int i=1; i<=3; i++) {
      cw_shift.set(i-1) = w_shift(i) ; 
    }
 
    Tenseur ckhi_shift(mp) ;
    ckhi_shift.set_etat_qcq() ;
    ckhi_shift.set() = khi_shift ; 
 
    Param par_poisson_nuf ; 
    par_poisson_nuf.add_int(mermax_poisson,  0) ;  // maximum number of iterations
    par_poisson_nuf.add_double(relax_poisson,  0) ; // relaxation parameter
    par_poisson_nuf.add_double(precis_poisson, 1) ; // required precision
    par_poisson_nuf.add_int_mod(niter, 0) ;  //  number of iterations actually used 
    par_poisson_nuf.add_cmp_mod( cssjm1_nuf ) ; 
                       
    Param par_poisson_nuq ; 
    par_poisson_nuq.add_int(mermax_poisson,  0) ;  // maximum number of iterations
    par_poisson_nuq.add_double(relax_poisson,  0) ; // relaxation parameter
    par_poisson_nuq.add_double(precis_poisson, 1) ; // required precision
    par_poisson_nuq.add_int_mod(niter, 0) ;  //  number of iterations actually used 
    par_poisson_nuq.add_cmp_mod( cssjm1_nuq ) ; 
                       
    Param par_poisson_tggg ; 
    par_poisson_tggg.add_int(mermax_poisson,  0) ;  // maximum number of iterations
    par_poisson_tggg.add_double(relax_poisson,  0) ; // relaxation parameter
    par_poisson_tggg.add_double(precis_poisson, 1) ; // required precision
    par_poisson_tggg.add_int_mod(niter, 0) ;  //  number of iterations actually used 
    par_poisson_tggg.add_cmp_mod( cssjm1_tggg ) ; 
    double lambda_tggg ;
    par_poisson_tggg.add_double_mod( lambda_tggg ) ; 
    
    Param par_poisson_dzeta ; 
    double lbda_grv2 ;
    par_poisson_dzeta.add_double_mod( lbda_grv2 ) ; 
                       
    // Parameters for the function Scalar::poisson_vect
    // -------------------------------------------------
 
    Param par_poisson_vect ; 
 
    par_poisson_vect.add_int(mermax_poisson,  0) ;  // maximum number of iterations
    par_poisson_vect.add_double(relax_poisson,  0) ; // relaxation parameter
    par_poisson_vect.add_double(precis_poisson, 1) ; // required precision
    par_poisson_vect.add_cmp_mod( cssjm1_khi ) ; 
    par_poisson_vect.add_tenseur_mod( cssjm1_wshift ) ; 
    par_poisson_vect.add_int_mod(niter, 0) ;   
 
                       
    // Initializations
    // ---------------
 
    //## Spherical components of the shift vector are restored
    beta.change_triad( mp.get_bvect_spher() ) ; 
    update_metric() ; 
    //## Back to Cartesian components 
    beta.change_triad( mp.get_bvect_cart() ) ; 
    
 
    // Quantities at the previous step :    
    Map_et mp_prev = mp_et ; 
    Scalar rphi_prev = rphi ;       
    Scalar logn_prev = logn ;       
    Scalar dzeta_prev = dzeta ;     
    
    // Creation of uninitialized tensors:
    Scalar source_nuf(mp) ;    // source term in the equation for nuf
    Scalar source_nuq(mp) ;    // source term in the equation for nuq
    Scalar source_dzf(mp) ; // matter source term in the eq. for dzeta
    Scalar source_dzq(mp) ; // quadratic source term in the eq. for dzeta
    Scalar source_tggg(mp) ;    // source term in the eq. for tggg
    Vector source_shift(mp, CON, mp.get_bvect_cart()) ;  
                            // source term for shift
    
            
    ofstream fichconv("convergence.d") ;    // Output file for diff_phi
    fichconv << "#     diff_phi     GRV2       max_triax      vit_triax" << endl ; 
    
    
    ofstream fichevol("evolution.d") ;    // Output file for various quantities
    fichevol << 
    "#       |dH/dr_eq/dH/dr_pole|      r_pole/r_eq rphi_c" 
    << endl ; 
    
    diff_phi = 1 ; 
    double err_grv2 = 1 ; 
    double max_triax_prev = 0 ;     // Triaxial amplitude at previous step
 
    //=========================================================================
    //          Start of iteration
    //=========================================================================
 
    for(int mer=0 ; (diff_phi > precis) && (mer<mer_max) ; mer++ ) {
 
    cout << "-----------------------------------------------" << endl ;
    cout << "step: " << mer << endl ;
    cout << "diff_phi = " << display_bold << diff_phi << display_normal
         << endl ;    
    cout << "err_grv2 = " << err_grv2 << endl ;    
    fichconv << mer ;
    fichevol << mer ;
 
 
    //-----------------------------------------------
    //  Sources of the Poisson equations
    //-----------------------------------------------
    
    // Source for nu
    // -------------
    Scalar bet = log(bbb) ; 
    bet.std_spectral_base() ; 
 
    Vector d_logn = logn.derive_cov( mp.flat_met_spher() ) ; 
    Vector d_bet = bet.derive_cov( mp.flat_met_spher() ) ; 
 
    Scalar s_euler = stress_euler.trace(gamma) ; 
    source_nuf =  qpig * a_car *( ener_euler + s_euler ) ; 
 
    source_nuq = ak_car - d_logn(1)*(d_logn(1)+d_bet(1))
        - d_logn(2)*(d_logn(2)+d_bet(2))
        - d_logn(3)*(d_logn(3)+d_bet(3)) ; 
 
    source_nuf.std_spectral_base() ;    
    source_nuq.std_spectral_base() ;    
 
    // Source for dzeta
    // ----------------
    source_dzf = 2 * qpig * a_car * b_car * stress_euler(3,3) ;
    source_dzf.std_spectral_base() ; 
  
    source_dzq = 1.5 * ak_car 
        - d_logn(1)*d_logn(1) - d_logn(2)*d_logn(2) - d_logn(3)*d_logn(3) ;     
    source_dzq.std_spectral_base() ;    
    
    // Source for tggg
    // ---------------
    
    source_tggg = 2 * qpig * nn * a_car * bbb * (s_euler - b_car * stress_euler(3,3)) ;
    source_tggg.std_spectral_base() ; 
    
    source_tggg.mult_rsint() ; 
    
 
    // Source for shift
    // ----------------
        
    // Matter term: 
    Vector mom_euler_cart = mom_euler ;
    mom_euler_cart.change_triad(mp.get_bvect_cart()) ;
    source_shift = (-4*qpig) * nn * a_car  * mom_euler_cart ;
 
    // Quadratic terms:
    Vector vtmp =  6 * bet.derive_con( mp.flat_met_spher() ) 
        - 2 * logn.derive_con( mp.flat_met_spher() ) ;
 
    Vector squad  = nn * contract(kk, 1, vtmp, 0) / b_car ; 
    squad.change_triad(mp.get_bvect_cart()) ;
    
    source_shift = source_shift + squad.up(0, mp.flat_met_cart() ) ; 
 
    //----------------------------------------------
    // Resolution of the Poisson equation for nuf 
    //----------------------------------------------
 
    source_nuf.poisson(par_poisson_nuf, nuf) ; 
    
    cout << "Test of the Poisson equation for nuf :" << endl ; 
    Tbl err = source_nuf.test_poisson(nuf, cout, true) ; 
    diff_nuf = err(0, 0) ; 
 
    //---------------------------------------
    // Triaxial perturbation of nuf
    //---------------------------------------
    
    if (mer == mer_triax) {
    
        if ( mg->get_np(0) == 1 ) {
        cout << 
        "Boson_star::equilibrium: np must be stricly greater than 1"
        << endl << " to set a triaxial perturbation !" << endl ; 
        abort() ; 
        }
    
        const Coord& phi = mp.phi ; 
        const Coord& sint = mp.sint ; 
        Scalar perturb(mp) ; 
        perturb = 1 + ampli_triax * sint*sint * cos(2*phi) ;
        nuf = nuf * perturb ;  
        
        nuf.std_spectral_base() ;    // set the bases for spectral expansions
                    //  to be the standard ones for a 
                    //  scalar field
 
    }
    
    // Monitoring of the triaxial perturbation
    // ---------------------------------------
    
    const Valeur& va_nuf = nuf.get_spectral_va() ; 
    va_nuf.coef() ;     // Computes the spectral coefficients
    double max_triax = 0 ; 
 
    if ( mg->get_np(0) > 1 ) {
 
        for (int l=0; l<nz; l++) {  // loop on the domains
        for (int j=0; j<mg->get_nt(l); j++) {
            for (int i=0; i<mg->get_nr(l); i++) {
        
            // Coefficient of cos(2 phi) : 
            double xcos2p = (*(va_nuf.c_cf))(l, 2, j, i) ; 
 
            // Coefficient of sin(2 phi) : 
            double xsin2p = (*(va_nuf.c_cf))(l, 3, j, i) ; 
            
            double xx = sqrt( xcos2p*xcos2p + xsin2p*xsin2p ) ; 
            
            max_triax = ( xx > max_triax ) ? xx : max_triax ;           
            }
        } 
        }
        
    }
    
    cout << "Triaxial part of nuf : " << max_triax << endl ; 
 
        //----------------------------------------------
        // Resolution of the Poisson equation for nuq 
        //----------------------------------------------
 
        source_nuq.poisson(par_poisson_nuq, nuq) ; 
        
        cout << "Test of the Poisson equation for nuq :" << endl ; 
        err = source_nuq.test_poisson(nuq, cout, true) ;
        diff_nuq = err(0, 0) ; 
    
        //---------------------------------------------------------
        // Resolution of the vector Poisson equation for the shift
        //---------------------------------------------------------
 
 
        for (int i=1; i<=3; i++) {
          if(source_shift(i).get_etat() != ETATZERO) {
            if(source_shift(i).dz_nonzero()) {
            assert( source_shift(i).get_dzpuis() == 4 ) ; 
            }
            else{
            (source_shift.set(i)).set_dzpuis(4) ; 
            }
        }
        }
 
        double lambda_shift = double(1) / double(3) ; 
 
        if ( mg->get_np(0) == 1 ) {
        lambda_shift = 0 ; 
        }
    
        Tenseur csource_shift(mp, 1, CON, mp.get_bvect_cart() ) ;
        csource_shift.set_etat_qcq() ;
        for (int i=1; i<=3; i++) {
        csource_shift.set(i-1) = source_shift(i) ; 
        }
        csource_shift.set(2).set_etat_zero() ;  //## bizarre...
 
        csource_shift.poisson_vect(lambda_shift, par_poisson_vect, 
                          cshift, cw_shift, ckhi_shift) ;           
 
        for (int i=1; i<=3; i++) {
        beta.set(i) = - cshift(i-1) ;
        beta.set(i).set_dzpuis(0) ;     //## bizarre...
        w_shift.set(i) = cw_shift(i-1) ; 
        }
        khi_shift = ckhi_shift() ; 
 
        cout << "Test of the Poisson equation for shift_x :" << endl ; 
        err = source_shift(1).test_poisson(-beta(1), cout, true) ;
        diff_shift_x = err(0, 0) ; 
    
        cout << "Test of the Poisson equation for shift_y :" << endl ; 
        err = source_shift(2).test_poisson(-beta(2), cout, true) ;
        diff_shift_y = err(0, 0) ; 
        
        // Computation of tnphi and nphi from the Cartesian components
        //  of the shift
        // -----------------------------------------------------------
        
        fait_nphi() ; 
    
 
 
    //----------------------------------------------------
    // Adaptation of the mapping to the new enthalpy field
    //----------------------------------------------------
    
    // Shall the adaptation be performed ?
    // ---------------------------------
    
    adapt_flag = 0 ;    // No adaptation of the mapping 
 
    mp_prev = mp_et ; 
 
    
    //---------------------------------------------------------
    // Matter source terms in the gravitational field equations 
    //---------------------------------------------------------
 
    //## Computation of tnphi and nphi from the Cartesian components
    //  of the shift for the test in hydro_euler():
        
    fait_nphi() ; 
 
    // Update of the energy-momentum tensor
    update_ener_mom() ; 
    
 
        //-------------------------------------------------------
        //  2-D Poisson equation for tggg
        //-------------------------------------------------------
 
        Cmp csource_tggg(source_tggg) ; 
        Cmp ctggg(tggg) ; 
        mp.poisson2d(csource_tggg, mp.cmp_zero(), par_poisson_tggg,
             ctggg) ; 
        tggg = ctggg ; 
 
        
        //-------------------------------------------------------
        //  2-D Poisson equation for dzeta
        //-------------------------------------------------------
 
        Cmp csource_dzf(source_dzf) ; 
        Cmp csource_dzq(source_dzq) ; 
        Cmp cdzeta(dzeta) ; 
        mp.poisson2d(csource_dzf, csource_dzq, par_poisson_dzeta,
             cdzeta) ;
        dzeta = cdzeta ; 
        
        err_grv2 = lbda_grv2 - 1; 
        cout << "GRV2: " << err_grv2 << endl ; 
        
 
    //---------------------------------------
    // Computation of the metric coefficients (except for N^phi)
    //---------------------------------------
 
    // Relaxations on nu and dzeta :  
 
    if (mer >= 10) {
        logn = relax * logn + relax_prev * logn_prev ;
 
        dzeta = relax * dzeta + relax_prev * dzeta_prev ; 
    }
 
    // Update of the metric coefficients N, A, B and computation of K_ij :
 
    //## Spherical components of the shift vector are restored
    beta.change_triad( mp.get_bvect_spher() ) ; 
    update_metric() ; 
    //## Back to Cartesian components 
    beta.change_triad( mp.get_bvect_cart() ) ; 
    
    //-----------------------
    //  Informations display
    //-----------------------
 
    cout << *this << endl ; 
 
 
    //------------------------------------------------------------
    //  Relative change in Phi with respect to previous step 
    //------------------------------------------------------------
 
    Tbl diff_phi_tbl = diffrel( rphi, rphi_prev ) ; 
    diff_phi = diff_phi_tbl(0) ; 
    for (int l=1; l<nzet; l++) {
        diff_phi += diff_phi_tbl(l) ; 
    }
    diff_phi /= nzet ; 
    
    fichconv << "  " << log10( fabs(diff_phi) + 1.e-16 ) ;
    fichconv << "  " << log10( fabs(err_grv2) + 1.e-16 ) ;
    fichconv << "  " << log10( fabs(max_triax) + 1.e-16 ) ;
 
    vit_triax = 0 ;
    if ( (mer > mer_triax+1) && (max_triax_prev > 1e-13) ) {
        vit_triax = (max_triax - max_triax_prev) / max_triax_prev ; 
    }
 
    fichconv << "  " << vit_triax ;
    
    //------------------------------
    //  Recycling for the next step
    //------------------------------
    
    rphi_prev = rphi ; 
    logn_prev = logn ; 
    dzeta_prev = dzeta ; 
    max_triax_prev = max_triax ; 
    
    fichconv << endl ;
    fichevol << endl ;
    fichconv.flush() ; 
    fichevol.flush() ; 
    
    } // End of main loop
    
    //=========================================================================
    //          End of iteration
    //=========================================================================
 
    ssjm1_nuf = cssjm1_nuf ; 
    ssjm1_nuq = cssjm1_nuq ; 
    ssjm1_tggg = cssjm1_tggg ; 
    ssjm1_khi = cssjm1_khi ; 
    for (int i=1; i<=3; i++) {
        ssjm1_wshift.set(i) = cssjm1_wshift(i-1) ; 
    }
 
    // Spherical components of the shift vector are restored
    beta.change_triad( mp.get_bvect_spher() ) ; 
 
    fichconv.close() ; 
    fichevol.close() ; 
    
}
}