// This file is part of monofonIC (MUSIC2) // A software package to generate ICs for cosmological simulations // Copyright (C) 2020 by Oliver Hahn & Bruno Marcos (this file) // // monofonIC 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 3 of the License, or // (at your option) any later version. // // monofonIC 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 this program. If not, see . // // NOTE: part of this code, notably the translation into the first Brillouin // zone (FBZ), was adapted from Fortran code written by Bruno Marcos // #pragma once #include #include // for unlink #include #include #include #include #include #include #include #include #include inline double Hypergeometric2F1( double a, double b, double c, double x ) { return gsl_sf_hyperg_2F1( a, b, c, x); } #define PRODUCTION namespace particle{ //! implement Joyce, Marcos et al. PLT calculation class lattice_gradient{ private: const real_t boxlen_, aini_; const size_t ngmapto_, ngrid_, ngrid32_; const real_t mapratio_;//, XmL_; Grid_FFT D_xx_, D_xy_, D_xz_, D_yy_, D_yz_, D_zz_; Grid_FFT grad_x_, grad_y_, grad_z_; std::vector> vectk_; std::vector> ico_, vecitk_; bool is_even( int i ){ return (i%2)==0; } bool is_in( int i, int j, int k, const mat3_t& M ){ vec3_t v({i,j,k}); auto vv = M * v; return is_even(vv.x)&&is_even(vv.y)&&is_even(vv.z); } void init_D( lattice lattice_type ) { constexpr real_t pi = M_PI; constexpr real_t twopi = 2.0*M_PI; constexpr real_t fourpi = 4.0*M_PI; const real_t sqrtpi = std::sqrt(M_PI); const real_t pi32 = std::pow(M_PI,1.5); //! === vectors, reciprocals and normals for the SC lattice === const int charge_fac_sc = 1; const mat3_t mat_bravais_sc{ real_t{1.0}, real_t{0.0}, real_t{0.0}, real_t{0.0}, real_t{1.0}, real_t{0.0}, real_t{0.0}, real_t{0.0}, real_t{1.0}, }; const mat3_t mat_reciprocal_sc{ twopi, real_t{0.0}, real_t{0.0}, real_t{0.0}, twopi, real_t{0.0}, real_t{0.0}, real_t{0.0}, twopi, }; const mat3_t mat_invrecip_sc{ 2, 0, 0, 0, 2, 0, 0, 0, 2, }; const std::vector> normals_sc{ {pi,real_t{0.},real_t{0.}},{-pi,real_t{0.},real_t{0.}}, {real_t{0.},pi,real_t{0.}},{real_t{0.},-pi,real_t{0.}}, {real_t{0.},real_t{0.},pi},{real_t{0.},real_t{0.},-pi}, }; //! === vectors, reciprocals and normals for the BCC lattice === const int charge_fac_bcc = 2; const mat3_t mat_bravais_bcc{ real_t{1.0}, real_t{0.0}, real_t{0.5}, real_t{0.0}, real_t{1.0}, real_t{0.5}, real_t{0.0}, real_t{0.0}, real_t{0.5}, }; const mat3_t mat_reciprocal_bcc{ twopi, real_t{0.0}, real_t{0.0}, real_t{0.0}, twopi, real_t{0.0}, -twopi, -twopi, fourpi, }; const mat3_t mat_invrecip_bcc{ 2, 0, 0, 0, 2, 0, 1, 1, 1, }; const std::vector> normals_bcc{ {real_t{0.0},pi,pi},{real_t{0.0},-pi,pi},{real_t{0.0},pi,-pi},{real_t{0.0},-pi,-pi}, {pi,real_t{0.0},pi},{-pi,real_t{0.0},pi},{pi,real_t{0.0},-pi},{-pi,real_t{0.0},-pi}, {pi,pi,real_t{0.0}},{-pi,pi,real_t{0.0}},{pi,-pi,real_t{0.0}},{-pi,-pi,real_t{0.0}} }; //! === vectors, reciprocals and normals for the FCC lattice === const int charge_fac_fcc = 4; const mat3_t mat_bravais_fcc{ real_t{0.0}, real_t{0.5}, real_t{0.0}, real_t{0.5}, real_t{0.0}, real_t{1.0}, real_t{0.5}, real_t{0.5}, real_t{0.0}, }; const mat3_t mat_reciprocal_fcc{ -fourpi, fourpi, twopi, real_t{0.0}, real_t{0.0}, twopi, fourpi, real_t{0.0}, -twopi, }; const mat3_t mat_invrecip_fcc{ 0, 1, 1, 1, 0, 1, 0, 2, 0, }; const std::vector> normals_fcc{ {twopi,real_t{0.0},real_t{0.0}},{-twopi,real_t{0.0},real_t{0.0}}, {real_t{0.0},twopi,real_t{0.0}},{real_t{0.0},-twopi,real_t{0.0}}, {real_t{0.0},real_t{0.0},twopi},{real_t{0.0},real_t{0.0},-twopi}, {+pi,+pi,+pi},{+pi,+pi,-pi}, {+pi,-pi,+pi},{+pi,-pi,-pi}, {-pi,+pi,+pi},{-pi,+pi,-pi}, {-pi,-pi,+pi},{-pi,-pi,-pi}, }; //! select the properties for the chosen lattice const int ilat = lattice_type; // 0 = sc, 1 = bcc, 2 = fcc const auto mat_bravais = (ilat==2)? mat_bravais_fcc : (ilat==1)? mat_bravais_bcc : mat_bravais_sc; const auto mat_reciprocal = (ilat==2)? mat_reciprocal_fcc : (ilat==1)? mat_reciprocal_bcc : mat_reciprocal_sc; const auto mat_invrecip = (ilat==2)? mat_invrecip_fcc : (ilat==1)? mat_invrecip_bcc : mat_invrecip_sc; const auto normals = (ilat==2)? normals_fcc : (ilat==1)? normals_bcc : normals_sc; const auto charge_fac = (ilat==2)? charge_fac_fcc : (ilat==1)? charge_fac_bcc : charge_fac_sc; const ptrdiff_t nlattice = ngrid_; const real_t dx = 1.0/real_t(nlattice); const real_t eta = 4.0; // Ewald cutoff shall be 4 cells const real_t alpha = 1.0/std::sqrt(2)/eta; const real_t alpha2 = alpha*alpha; const real_t alpha3 = alpha2*alpha; const real_t charge = 1.0/std::pow(real_t(nlattice),3)/charge_fac; const real_t fft_norm = 1.0/std::pow(real_t(nlattice),3.0); const real_t fft_norm12 = 1.0/std::pow(real_t(nlattice),1.5); //! just a Kronecker \delta_ij auto kronecker = []( int i, int j ) -> real_t { return (i==j)? 1.0 : 0.0; }; //! Ewald summation: short-range Green's function auto add_greensftide_sr = [&]( mat3_t& D, const vec3_t& d ) -> void { auto r = d.norm(); if( r< 1e-14 ) return; // return zero for r=0 const real_t r2(r*r), r3(r2*r), r5(r3*r2); const real_t K1( -alpha3/pi32 * std::exp(-alpha2*r2)/r2 ); const real_t K2( (std::erfc(alpha*r) + 2.0*alpha/sqrtpi*std::exp(-alpha2*r2)*r)/fourpi ); for( int mu=0; mu<3; ++mu ){ for( int nu=mu; nu<3; ++nu ){ real_t dd( d[mu]*d[nu] * K1 + (kronecker(mu,nu)/r3 - 3.0 * (d[mu]*d[nu])/r5) * K2 ); D(mu,nu) += dd; D(nu,mu) += (mu!=nu)? dd : 0.0; } } }; //! Ewald summation: long-range Green's function auto add_greensftide_lr = [&]( mat3_t& D, const vec3_t& k, const vec3_t& r ) -> void { real_t kmod2 = k.norm_squared(); real_t term = std::exp(-kmod2/(4*alpha2))*std::cos(k.dot(r)) / kmod2 * fft_norm; for( int mu=0; mu<3; ++mu ){ for( int nu=mu; nu<3; ++nu ){ auto dd = k[mu] * k[nu] * term; D(mu,nu) += dd; D(nu,mu) += (mu!=nu)? dd : 0.0; } } }; //! checks if 'vec' is in the FBZ with FBZ normal vectors given in 'normals' auto check_FBZ = []( const auto& normals, const auto& vec ) -> bool { for( const auto& n : normals ){ if( n.dot( vec ) > 1.0001 * n.dot(n) ){ return false; } } return true; }; constexpr ptrdiff_t lnumber = 3, knumber = 3; const int numb = 1; //!< search radius when shifting vectors into FBZ vectk_.assign(D_xx_.memsize(),vec3_t()); ico_.assign(D_xx_.memsize(),vec3_t()); vecitk_.assign(D_xx_.memsize(),vec3_t()); #pragma omp parallel { //... temporary to hold values of the dynamical matrix mat3_t matD(real_t(0.0)); #pragma omp for for( ptrdiff_t i=0; i x_ijk({dx*real_t(i),dx*real_t(j),dx*real_t(k)}); const vec3_t ar = (mat_bravais * x_ijk).wrap_abs(); //... zero temporary matrix matD.zero(); // add real-space part of dynamical matrix, periodic copies for( ptrdiff_t ix=-lnumber; ix<=lnumber; ix++ ){ for( ptrdiff_t iy=-lnumber; iy<=lnumber; iy++ ){ for( ptrdiff_t iz=-lnumber; iz<=lnumber; iz++ ){ const vec3_t n_ijk({real_t(ix),real_t(iy),real_t(iz)}); const vec3_t dr(ar - mat_bravais * n_ijk); add_greensftide_sr(matD, dr); } } } // add k-space part of dynamical matrix for( ptrdiff_t ix=-knumber; ix<=knumber; ix++ ){ for( ptrdiff_t iy=-knumber; iy<=knumber; iy++ ){ for( ptrdiff_t iz=-knumber; iz<=knumber; iz++ ){ if(std::abs(ix)+std::abs(iy)+std::abs(iz) != 0){ const vec3_t k_ijk({real_t(ix)/nlattice,real_t(iy)/nlattice,real_t(iz)/nlattice}); const vec3_t ak( mat_reciprocal * k_ijk); add_greensftide_lr(matD, ak, ar ); } } } } D_xx_.relem(i,j,k) = matD(0,0) * charge; D_xy_.relem(i,j,k) = matD(0,1) * charge; D_xz_.relem(i,j,k) = matD(0,2) * charge; D_yy_.relem(i,j,k) = matD(1,1) * charge; D_yz_.relem(i,j,k) = matD(1,2) * charge; D_zz_.relem(i,j,k) = matD(2,2) * charge; } } } } // end omp parallel region // fix r=0 with background density (added later in Fourier space) D_xx_.relem(0,0,0) = 1.0/3.0; D_xy_.relem(0,0,0) = 0.0; D_xz_.relem(0,0,0) = 0.0; D_yy_.relem(0,0,0) = 1.0/3.0; D_yz_.relem(0,0,0) = 0.0; D_zz_.relem(0,0,0) = 1.0/3.0; D_xx_.FourierTransformForward(); D_xy_.FourierTransformForward(); D_xz_.FourierTransformForward(); D_yy_.FourierTransformForward(); D_yz_.FourierTransformForward(); D_zz_.FourierTransformForward(); #ifndef PRODUCTION if (CONFIG::MPI_task_rank == 0) unlink("debug.hdf5"); D_xx_.Write_to_HDF5("debug.hdf5","Dxx"); D_xy_.Write_to_HDF5("debug.hdf5","Dxy"); D_xz_.Write_to_HDF5("debug.hdf5","Dxz"); D_yy_.Write_to_HDF5("debug.hdf5","Dyy"); D_yz_.Write_to_HDF5("debug.hdf5","Dyz"); D_zz_.Write_to_HDF5("debug.hdf5","Dzz"); std::ofstream ofs2("test_brillouin.txt"); #endif using map_t = std::map,size_t>; map_t iimap; //!=== Make temporary copies before resorting to std. Fourier grid ========!// Grid_FFT temp1({ngrid_, ngrid_, ngrid_}, {1.0,1.0,1.0}), temp2({ngrid_, ngrid_, ngrid_}, {1.0,1.0,1.0}), temp3({ngrid_, ngrid_, ngrid_}, {1.0,1.0,1.0}); temp1.FourierTransformForward(false); temp2.FourierTransformForward(false); temp3.FourierTransformForward(false); #pragma omp parallel for for( size_t i=0; i D; vec3_t eval, evec1, evec2, evec3_t; #pragma omp for for( size_t i=0; i kv = D_xx_.get_k(i,j,k); // put matrix elements into actual matrix D(0,0) = std::real(temp1.kelem(i,j,k)) / fft_norm12; D(0,1) = D(1,0) = std::imag(temp1.kelem(i,j,k)) / fft_norm12; D(0,2) = D(2,0) = std::real(temp2.kelem(i,j,k)) / fft_norm12; D(1,1) = std::imag(temp2.kelem(i,j,k)) / fft_norm12; D(1,2) = D(2,1) = std::real(temp3.kelem(i,j,k)) / fft_norm12; D(2,2) = std::imag(temp3.kelem(i,j,k)) / fft_norm12; // compute eigenstructure of matrix D.eigen(eval, evec1, evec2, evec3_t); evec3_t /= (twopi*ngrid_); // now determine to which modes on the regular lattice this contributes vec3_t ar = kv / (twopi*ngrid_); vec3_t a(mat_reciprocal * ar); // translate the k-vectors into the "candidate" FBZ for( int l1=-numb; l1<=numb; ++l1 ){ for( int l2=-numb; l2<=numb; ++l2 ){ for( int l3=-numb; l3<=numb; ++l3 ){ // need both halfs of Fourier space since we use real transforms for( int isign=0; isign<=1; ++isign ){ const real_t sign = 2.0*real_t(isign)-1.0; const vec3_t vshift({real_t(l1),real_t(l2),real_t(l3)}); vec3_t vectk = sign * a + mat_reciprocal * vshift; if( check_FBZ( normals, vectk ) ) { int ix = std::round(vectk.x*(ngrid_)/twopi); int iy = std::round(vectk.y*(ngrid_)/twopi); int iz = std::round(vectk.z*(ngrid_)/twopi); #pragma omp critical {iimap.insert( std::pair,size_t>({ix,iy,iz}, D_xx_.get_idx(i,j,k)) );} temp1.kelem(i,j,k) = ccomplex_t(eval[2],eval[1]); temp2.kelem(i,j,k) = ccomplex_t(eval[0],evec3_t.x); temp3.kelem(i,j,k) = ccomplex_t(evec3_t.y,evec3_t.z); } }//sign } //l3 } //l2 } //l1 } //k } //j } //i } D_xx_.kelem(0,0,0) = 1.0; D_xy_.kelem(0,0,0) = 0.0; D_xz_.kelem(0,0,0) = 0.0; D_yy_.kelem(0,0,0) = 1.0; D_yz_.kelem(0,0,0) = 0.0; D_zz_.kelem(0,0,0) = 0.0; //... approximate infinite lattice by inerpolating to sites not convered by current resolution... #pragma omp parallel for for( size_t i=0; inlattice/2)? int(i)-nlattice : int(i); int jj = (int(j)>nlattice/2)? int(j)-nlattice : int(j); int kk = (int(k)>nlattice/2)? int(k)-nlattice : int(k); vec3_t kv({real_t(ii),real_t(jj),real_t(kk)}); auto align_with_k = [&]( const vec3_t& v ) -> vec3_t{ return v*((v.dot(kv)<0.0)?-1.0:1.0); }; vec3_t v, l; map_t::iterator it; if( !is_in(i,j,k,mat_invrecip) ){ auto average_lv = [&]( const auto& t1, const auto& t2, const auto& t3, vec3_t& v, vec3_t& l ) { v = vec3_t(0.0); l = vec3_t(0.0); int count(0); auto add_lv = [&]( auto it ) -> void { auto q = it->second;++count; l += vec3_t({std::real(t1.kelem(q)),std::imag(t1.kelem(q)),std::real(t2.kelem(q))}); v += align_with_k(vec3_t({std::imag(t2.kelem(q)),std::real(t3.kelem(q)),std::imag(t3.kelem(q))})); }; map_t::iterator it; if( (it = iimap.find({ii-1,jj,kk}))!=iimap.end() ){ add_lv(it); } if( (it = iimap.find({ii+1,jj,kk}))!=iimap.end() ){ add_lv(it); } if( (it = iimap.find({ii,jj-1,kk}))!=iimap.end() ){ add_lv(it); } if( (it = iimap.find({ii,jj+1,kk}))!=iimap.end() ){ add_lv(it); } if( (it = iimap.find({ii,jj,kk-1}))!=iimap.end() ){ add_lv(it); } if( (it = iimap.find({ii,jj,kk+1}))!=iimap.end() ){ add_lv(it); } l/=real_t(count); v/=real_t(count); }; average_lv(temp1,temp2,temp3,v,l); }else{ if( (it = iimap.find({ii,jj,kk}))!=iimap.end() ){ auto q = it->second; l = vec3_t({std::real(temp1.kelem(q)),std::imag(temp1.kelem(q)),std::real(temp2.kelem(q))}); v = align_with_k(vec3_t({std::imag(temp2.kelem(q)),std::real(temp3.kelem(q)),std::imag(temp3.kelem(q))})); } } D_xx_.kelem(i,j,k) = l[0]; D_xy_.kelem(i,j,k) = l[1]; D_xz_.kelem(i,j,k) = l[2]; D_yy_.kelem(i,j,k) = v[0]; D_yz_.kelem(i,j,k) = v[1]; D_zz_.kelem(i,j,k) = v[2]; } } } #ifdef PRODUCTION #pragma omp parallel for for( size_t i=0; i kv = D_xx_.get_k(i,j,k); double mu1 = std::real(D_xx_.kelem(i,j,k)); // double mu2 = std::real(D_xy_.kelem(i,j,k)); // double mu3 = std::real(D_xz_.kelem(i,j,k)); vec3_t evec1({std::real(D_yy_.kelem(i,j,k)),std::real(D_yz_.kelem(i,j,k)),std::real(D_zz_.kelem(i,j,k))}); evec1 /= evec1.norm(); // /////////////////////////////////// // // project onto spherical coordinate vectors real_t kr = kv.norm(), kphi = kr>0.0? std::atan2(kv.y,kv.x) : real_t(0.0), ktheta = kr>0.0? std::acos( kv.z / kr ): real_t(0.0); real_t st = std::sin(ktheta), ct = std::cos(ktheta), sp = std::sin(kphi), cp = std::cos(kphi); vec3_t e_r( st*cp, st*sp, ct), e_theta( ct*cp, ct*sp, -st), e_phi( -sp, cp, real_t(0.0) ); // re-normalise to that longitudinal amplitude is exact double renorm = evec1.dot( e_r ); if( renorm < 0.01 ) renorm = 1.0; // -- store in diagonal components of D_ij D_xx_.kelem(i,j,k) = 1.0; D_yy_.kelem(i,j,k) = evec1.dot( e_theta ) / renorm; D_zz_.kelem(i,j,k) = evec1.dot( e_phi ) / renorm; // spatially dependent correction to vfact = \dot{D_+}/D_+ D_xy_.kelem(i,j,k) = 1.0/(0.25*(std::sqrt(1.+24*mu1)-1.)); } } } D_xy_.kelem(0,0,0) = 1.0; D_xx_.kelem(0,0,0) = 1.0; D_yy_.kelem(0,0,0) = 0.0; D_zz_.kelem(0,0,0) = 0.0; // unlink("debug.hdf5"); // D_xy_.Write_to_HDF5("debug.hdf5","mu1"); // D_xx_.Write_to_HDF5("debug.hdf5","e1x"); // D_yy_.Write_to_HDF5("debug.hdf5","e1y"); // D_zz_.Write_to_HDF5("debug.hdf5","e1z"); #else D_xx_.Write_to_HDF5("debug.hdf5","mu1"); D_xy_.Write_to_HDF5("debug.hdf5","mu2"); D_xz_.Write_to_HDF5("debug.hdf5","mu3"); D_yy_.Write_to_HDF5("debug.hdf5","e1x"); D_yz_.Write_to_HDF5("debug.hdf5","e1y"); D_zz_.Write_to_HDF5("debug.hdf5","e1z"); #endif } public: // real_t boxlen, size_t ngridother explicit lattice_gradient( config_file& the_config, size_t ngridself=64 ) : boxlen_( the_config.get_value("setup", "BoxLength") ), aini_ ( 1.0/(1.0+the_config.get_value("setup", "zstart")) ), ngmapto_( the_config.get_value("setup", "GridRes") ), ngrid_( ngridself ), ngrid32_( std::pow(ngrid_, 1.5) ), mapratio_(real_t(ngrid_)/real_t(ngmapto_)), //XmL_ ( the_config.get_value("cosmology", "Omega_L") / the_config.get_value("cosmology", "Omega_m") ), D_xx_({ngrid_, ngrid_, ngrid_}, {1.0,1.0,1.0}), D_xy_({ngrid_, ngrid_, ngrid_}, {1.0,1.0,1.0}), D_xz_({ngrid_, ngrid_, ngrid_}, {1.0,1.0,1.0}), D_yy_({ngrid_, ngrid_, ngrid_}, {1.0,1.0,1.0}), D_yz_({ngrid_, ngrid_, ngrid_}, {1.0,1.0,1.0}), D_zz_({ngrid_, ngrid_, ngrid_}, {1.0,1.0,1.0}), grad_x_({ngrid_, ngrid_, ngrid_}, {1.0,1.0,1.0}), grad_y_({ngrid_, ngrid_, ngrid_}, {1.0,1.0,1.0}), grad_z_({ngrid_, ngrid_, ngrid_}, {1.0,1.0,1.0}) { music::ilog << "-------------------------------------------------------------------------------" << std::endl; std::string lattice_str = the_config.get_value_safe("setup","ParticleLoad","sc"); const lattice lattice_type = ((lattice_str=="bcc")? lattice_bcc : ((lattice_str=="fcc")? lattice_fcc : ((lattice_str=="rsc")? lattice_rsc : lattice_sc))); music::ilog << "PLT corrections for " << lattice_str << " lattice will be computed on " << ngrid_ << "**3 mesh" << std::endl; double wtime = get_wtime(); music::ilog << std::setw(40) << std::setfill('.') << std::left << "Computing PLT eigenmodes "<< std::flush; init_D( lattice_type ); // init_D__old(); music::ilog << std::setw(20) << std::setfill(' ') << std::right << "took " << get_wtime()-wtime << "s" << std::endl; } inline ccomplex_t gradient( const int idim, std::array ijk ) const { real_t ix = ijk[0]*mapratio_, iy = ijk[1]*mapratio_, iz = ijk[2]*mapratio_; auto kv = D_xx_.get_k( ix, iy, iz ); auto kmod = kv.norm() / mapratio_ / boxlen_; // // project onto spherical coordinate vectors auto D_r = std::real(D_xx_.get_cic_kspace({ix,iy,iz})); auto D_theta = std::real(D_yy_.get_cic_kspace({ix,iy,iz})); auto D_phi = std::real(D_zz_.get_cic_kspace({ix,iy,iz})); real_t kr = kv.norm(), kphi = kr>0.0? std::atan2(kv.y,kv.x) : 0.0, ktheta = kr>0.0? std::acos( kv.z / kr ) : 0.0; real_t st = std::sin(ktheta), ct = std::cos(ktheta), sp = std::sin(kphi), cp = std::cos(kphi); if( idim == 0 ){ return ccomplex_t(0.0, kmod*(D_r * st * cp + D_theta * ct * cp - D_phi * sp)); } else if( idim == 1 ){ return ccomplex_t(0.0, kmod*(D_r * st * sp + D_theta * ct * sp + D_phi * cp)); } return ccomplex_t(0.0, kmod*(D_r * ct - D_theta * st)); } inline real_t vfac_corr( std::array ijk ) const { real_t ix = ijk[0]*mapratio_, iy = ijk[1]*mapratio_, iz = ijk[2]*mapratio_; const real_t alpha = 1.0/std::real(D_xy_.get_cic_kspace({ix,iy,iz})); return 1.0/alpha; // // below is for LCDM, but it is a tiny correction for typical starting redshifts: //! X = \Omega_\Lambda / \Omega_m // return 1.0 / (alpha - (2*std::pow(aini_,3)*alpha*(2 + alpha)*XmL_*Hypergeometric2F1((3 + alpha)/3.,(5 + alpha)/3., // (13 + 4*alpha)/6.,-(std::pow(aini_,3)*XmL_)))/ // ((7 + 4*alpha)*Hypergeometric2F1(alpha/3.,(2 + alpha)/3.,(7 + 4*alpha)/6.,-(std::pow(aini_,3)*XmL_)))); } }; }