Field-theoretical EOS with scalar-isovector meson,
.
More...
#include <eos_had_rmf_delta.h>
This essentially follows the notation in Kubis97, except that our definitions of b and c follow their
and
, respectively.
Also discussed in Gaitanos04, where they take
MeV.
The full Lagragian is:
where the additional terms are
The new field equation for the delta meson is
Definition at line 95 of file eos_had_rmf_delta.h.
Public Member Functions | |
| virtual int | calc_e (fermion &ne, fermion &pr, thermo <h) |
| Equation of state as a function of density. | |
| virtual int | calc_p (fermion &neu, fermion &p, double sig, double ome, double rho, double delta, double &f1, double &f2, double &f3, double &f4, thermo &th) |
| Equation of state as a function of chemical potentials. | |
| int | calc_temp_p (fermion &ne, fermion &pr, double temper, double sig, double ome, double lrho, double delta, double &f1, double &f2, double &f3, double &f4, thermo <h) |
| Finite temperature (unfinished) | |
| virtual int | set_fields (double sig, double ome, double lrho, double delta) |
| Set a guess for the fields for the next call to calc_e(), calc_p(), or saturation() | |
| virtual int | saturation () |
| Calculate saturation properties for nuclear matter at the saturation density. More... | |
Public Member Functions inherited from o2scl::eos_had_rmf | |
| virtual int | calc_p (fermion &ne, fermion &pr, thermo <h) |
| Equation of state as a function of chemical potential. More... | |
| virtual int | calc_eq_p (fermion &neu, fermion &p, double sig, double ome, double rho, double &f1, double &f2, double &f3, thermo &th) |
| Equation of state and meson field equations as a function of chemical potentials. More... | |
| virtual int | calc_eq_temp_p (fermion &ne, fermion &pr, double temper, double sig, double ome, double rho, double &f1, double &f2, double &f3, thermo &th) |
| Equation of state and meson field equations as a function of chemical potentials at finite temperature. More... | |
| virtual int | calc_temp_p (fermion &ne, fermion &pr, double T, thermo <h) |
| Equation of state as a function of chemical potential. More... | |
| int | calc_temp_e (fermion &ne, fermion &pr, double T, thermo <h) |
| Equation of state as a function of densities at finite temperature. | |
| int | fix_saturation (double guess_cs=4.0, double guess_cw=3.0, double guess_b=0.001, double guess_c=-0.001) |
| Calculate cs, cw, cr, b, and c from the saturation properties. More... | |
| double | fesym_fields (double sig, double ome, double nb) |
| Calculate symmetry energy assuming the field equations have already been solved. More... | |
| double | fcomp_fields (double sig, double ome, double nb) |
| Calculate the compressibility assuming the field equations have already been solved. More... | |
| void | fkprime_fields (double sig, double ome, double nb, double &k, double &kprime) |
Calculate compressibilty and kprime assuming the field equations have already been solved. More... | |
| int | field_eqs (size_t nv, const ubvector &x, ubvector &y) |
| A function for solving the field equations. More... | |
| int | field_eqsT (size_t nv, const ubvector &x, ubvector &y) |
| A function for solving the field equations at finite temperature. More... | |
| int | get_fields (double &sig, double &ome, double &lrho) |
| Return the most recent values of the meson fields. More... | |
| virtual const char * | type () |
| Return string denoting type ("eos_had_rmf") | |
| eos_had_rmf () | |
| virtual int | set_sat_mroot (mroot< mm_funct, ubvector, jac_funct > &mrx) |
| Set class mroot object for use calculating saturation density. | |
| void | check_naturalness (eos_had_rmf &re) |
| Set the coefficients of a eos_had_rmf object to their limits from naturalness. More... | |
| void | naturalness_limits (double value, eos_had_rmf &re) |
| Provide the maximum values of the couplings assuming a limit on naturalness. More... | |
Public Member Functions inherited from o2scl::eos_had_temp_base | |
| virtual int | calc_liqgas_dens_temp_e (fermion &n1, fermion &p1, fermion &n2, fermion &p2, double T, thermo &th1, thermo &th2) |
| Compute liquid-gas phase transition densities using eos_had_temp_base::calc_temp_e() . More... | |
| virtual int | calc_liqgas_temp_e (fermion &n1, fermion &p1, fermion &n2, fermion &p2, double nB, double Ye, double T, thermo &th1, thermo &th2, double &chi) |
| Compute the liquid-gas phase transition using eos_had_temp_base::calc_temp_e() . More... | |
| virtual int | calc_liqgas_beta_temp_e (fermion &n1, fermion &p1, fermion &n2, fermion &p2, double nB, double T, thermo &th1, thermo &th2, double &Ye, double &chi) |
| Compute the liquid-gas phase transition in beta-equilibrium using eos_had_temp_base::calc_temp_e() . More... | |
| virtual double | fesym_T (double nb, double T, double delta=0.0) |
| Compute the symmetry energy at finite temperature. | |
| virtual double | fsyment_T (double nb, double T, double delta=0.0) |
| Compute the symmetry entropy at finite temperature. | |
| virtual double | calc_temp_mun_e (double nn, double np, double T) |
| Neutron chemical potential as a function of the densities. | |
| virtual double | calc_temp_mup_e (double nn, double np, double T) |
| Proton chemical potential as a function of the densities. | |
| virtual double | calc_temp_nn_p (double mun, double mup, double T) |
| Neutron density as a function of the chemical potentials. | |
| virtual double | calc_temp_np_p (double mun, double mup, double T) |
| Proton density as a function of the chemical potentials. | |
| double | calc_fr (double nn, double np, double T) |
| Compute the free energy as a function of the temperature and the densities. | |
| virtual void | f_number_suscept_T (double mun, double mup, double T, double &dPdnn, double &dPdnp, double &dPdpp) |
Compute the number susceptibilities as a function of the chemical potentials, at a fixed temperature. | |
| virtual void | f_inv_number_suscept_T (double mun, double mup, double T, double &dednn, double &dednp, double &dedpp) |
Compute the 'inverse' number susceptibilities as a function of the densities, at a fixed temperature. | |
| void | check_en (fermion &n, fermion &p, double T, thermo &th, double &en_deriv, double &en_err) |
| Check the entropy by computing the derivative numerically. | |
| void | check_mu_T (fermion &n, fermion &p, double T, thermo &th, double &mun_deriv, double &mup_deriv, double &mun_err, double &mup_err) |
| Check the chemical potentials at finite temperature by computing the derivative numerically. | |
| virtual void | set_fermion_thermo (fermion_thermo &f) |
| Computing finite-temperature integrals. More... | |
Public Member Functions inherited from o2scl::eos_had_base | |
| virtual double | fcomp (double nb, double delta=0.0) |
Calculate the incompressibility in using calc_e() More... | |
| virtual double | fcomp_err (double nb, double delta, double &unc) |
| Compute the incompressibility and its uncertainty. More... | |
| virtual double | feoa (double nb, double delta=0.0) |
Calculate the energy per baryon in using calc_e() More... | |
| virtual double | fesym (double nb, double delta=0.0) |
Calculate symmetry energy of matter in using calc_dmu_delta() . More... | |
| virtual double | fesym_err (double nb, double delta, double &unc) |
Calculate symmetry energy of matter and its uncertainty in . More... | |
| virtual double | fesym_slope (double nb, double delta=0.0) |
The symmetry energy slope parameter in . More... | |
| virtual double | fesym_curve (double nb, double delta=0.0) |
The curvature of the symmetry energy in . | |
| virtual double | fesym_skew (double nb, double delta=0.0) |
The skewness of the symmetry energy in . | |
| virtual double | fesym_diff (double nb) |
Calculate symmetry energy of matter as energy of neutron matter minus the energy of nuclear matter in . More... | |
| virtual double | feta (double nb) |
| The strength parameter for quartic terms in the symmetry energy. | |
| virtual double | feta_prime (double nb) |
| The derivative of the strength parameter for quartic terms in the symmetry energy. | |
| virtual double | fkprime (double nb, double delta=0.0) |
Calculate skewness of nuclear matter in using calc_e() More... | |
| virtual double | fmsom (double nb, double delta=0.0) |
| Calculate reduced neutron effective mass using calc_e() More... | |
| virtual double | f_effm_neut (double nb, double delta=0.0) |
| Neutron (reduced) effective mass. | |
| virtual double | f_effm_prot (double nb, double delta=0.0) |
| Proton (reduced) effective mass. | |
| virtual double | f_effm_scalar (double nb, double delta=0.0) |
| Scalar effective mass. More... | |
| virtual double | f_effm_vector (double nb, double delta=1.0) |
| Vector effective mass. More... | |
| virtual double | fn0 (double delta, double &leoa) |
| Calculate saturation density using calc_e() More... | |
| virtual void | f_number_suscept (double mun, double mup, double &dPdnn, double &dPdnp, double &dPdpp) |
Compute the number susceptibilities as a function of the chemical potentials, . | |
| virtual void | f_inv_number_suscept (double mun, double mup, double &dednn, double &dednp, double &dedpp) |
Compute the 'inverse' number susceptibilities as a function of the densities, . | |
| double | calc_mun_e (double nn, double np) |
| Compute the neutron chemical potential at fixed density. More... | |
| double | calc_ed (double nn, double np) |
| Compute the energy density as a function of the nucleon densities. | |
| double | calc_pr (double nn, double np) |
| Compute the pressure as a function of the nucleon chemical potentials. | |
| double | calc_mup_e (double nn, double np) |
| Compute the proton chemical potential at fixed density. More... | |
| double | calc_nn_p (double mun, double mup) |
| Compute the neutron density at fixed chemical potential. More... | |
| double | calc_np_p (double mun, double mup) |
| Compute the proton density at fixed chemical potential. More... | |
| double | calc_dmu_delta (double delta, double nb) |
| Compute the difference between neutron and proton chemical potentials as a function of the isospin asymmetry. More... | |
| double | calc_musum_delta (double delta, double nb) |
| Compute the sum of the neutron and proton chemical potentials as a function of the isospin asymmetry. More... | |
| double | calc_pressure_nb (double nb, double delta=0.0) |
| Compute the pressure as a function of baryon density at fixed isospin asymmetry. More... | |
| double | calc_edensity_nb (double nb, double delta=0.0) |
| Compute the energy density as a function of baryon density at fixed isospin asymmetry. More... | |
| void | const_pf_derivs (double nb, double pf, double &dednb_pf, double &dPdnb_pf) |
| Compute derivatives at constant proton fraction. | |
| double | calc_press_over_den2 (double nb, double delta=0.0) |
| Calculate pressure / baryon density squared in nuclear matter as a function of baryon density at fixed isospin asymmetry. More... | |
| double | calc_edensity_delta (double delta, double nb) |
| Calculate energy density as a function of the isospin asymmetry at fixed baryon density. More... | |
| int | nuc_matter_p (size_t nv, const ubvector &x, ubvector &y, double nn0, double np0) |
| Solve for the chemical potentials given the densities. More... | |
| int | nuc_matter_e (size_t nv, const ubvector &x, ubvector &y, double mun0, double mup0) |
| Solve for the densities given the chemical potentials. More... | |
| void | gradient_qij (fermion &n, fermion &p, thermo &th, double &qnn, double &qnp, double &qpp, double &dqnndnn, double &dqnndnp, double &dqnpdnn, double &dqnpdnp, double &dqppdnn, double &dqppdnp) |
| Calculate coefficients for gradient part of Hamiltonian. More... | |
| virtual void | set_mroot (mroot<> &mr) |
| Set class mroot object for use in calculating chemical potentials from densities. More... | |
| virtual void | set_sat_root (root<> &mr) |
| Set class mroot object for use calculating saturation density. More... | |
| virtual void | set_sat_deriv (deriv_base<> &de) |
| Set deriv_base object to use to find saturation properties. | |
| virtual void | set_sat_deriv2 (deriv_base<> &de) |
| Set the second deriv_base object to use to find saturation properties. More... | |
| virtual void | set_n_and_p (fermion &n, fermion &p) |
| Set neutron and proton. | |
| void | check_mu (fermion &n, fermion &p, thermo &th, double &mun_deriv, double &mup_deriv, double &mun_err, double &mup_err) |
| Check the chemical potentials by computing the derivatives numerically. | |
| void | check_den (fermion &n, fermion &p, thermo &th, double &nn_deriv, double &np_deriv, double &nn_err, double &np_err) |
| Check the densities by computing the derivatives numerically. | |
Public Member Functions inherited from o2scl::eos_base | |
| virtual void | set_thermo (thermo &th) |
| Set class thermo object. | |
| virtual const thermo & | get_thermo () |
| Get class thermo object. | |
Public Attributes | |
| double | md |
| The mass of the scalar-isovector field. | |
| double | cd |
| The coupling of the scalar-isovector field to the nucleons. | |
| double | del |
| The value of the scalar-isovector field. | |
Public Attributes inherited from o2scl::eos_had_rmf | |
| size_t | calc_e_steps |
The number of separate calls to the solver that the calc_e functions take (default 20) More... | |
| bool | calc_e_relative |
| If true, solve for relative densities rather than absolute densities (default false) More... | |
| bool | zm_mode |
| Modifies method of calculating effective masses (default false) | |
| int | verbose |
| Verbosity parameter. More... | |
| bool | err_nonconv |
| If true, throw exceptions when the function calc_e() does not converge (default true) | |
| double | mnuc |
The scale . More... | |
| double | ms |
mass (in ) | |
| double | mw |
mass (in ) | |
| double | mr |
mass (in ) | |
| double | cs |
| double | cw |
| double | cr |
| double | b |
| double | c |
| double | zeta |
| double | xi |
| double | a1 |
| double | a2 |
| double | a3 |
| double | a4 |
| double | a5 |
| double | a6 |
| double | b1 |
| double | b2 |
| double | b3 |
| mroot_hybrids | def_sat_mroot |
| The default solver for calculating the saturation density. More... | |
Public Attributes inherited from o2scl::eos_had_temp_base | |
| fermion_eff | def_fet |
| Default fermion thermodynamics object. | |
Public Attributes inherited from o2scl::eos_had_base | |
| double | eoa |
Binding energy (without the rest mass) in . More... | |
| double | comp |
Compression modulus in . | |
| double | esym |
Symmetry energy in . | |
| double | n0 |
Saturation density in . | |
| double | msom |
| Effective mass (neutron) | |
| double | kprime |
Skewness in . | |
| bool | err_nonconv |
| If true, call the error handler if msolve() or msolve_de() does not converge (default true) | |
| deriv_gsl | def_deriv |
| The default object for derivatives. More... | |
| deriv_gsl | def_deriv2 |
| The second default object for derivatives. More... | |
| mroot_hybrids | def_mroot |
| The default solver. More... | |
| root_cern | def_sat_root |
| The default solver for calculating the saturation density. More... | |
| fermion | def_neutron |
| The defaut neutron. More... | |
| fermion | def_proton |
| The defaut proton. More... | |
Public Attributes inherited from o2scl::eos_base | |
| thermo | def_thermo |
| The default thermo object. | |
Protected Member Functions | |
| virtual int | calc_e_solve_fun (size_t nv, const ubvector &ex, ubvector &ey) |
| The function for calc_e() | |
| virtual int | zero_pressure (size_t nv, const ubvector &ex, ubvector &ey) |
| Compute matter at zero pressure (for saturation()) | |
Protected Member Functions inherited from o2scl::eos_had_rmf | |
| int | fix_saturation_fun (size_t nv, const ubvector &x, ubvector &y) |
| The function for fix_saturation() | |
| virtual int | calc_temp_e_solve_fun (size_t nv, const ubvector &ex, ubvector &ey) |
| The function for calc_temp_e() | |
| int | calc_cr (double sig, double ome, double nb) |
Calculate the cr coupling given sig and ome at the density 'nb'. More... | |
Protected Member Functions inherited from o2scl::eos_had_temp_base | |
| int | nuc_matter_temp_e (size_t nv, const ubvector &x, ubvector &y, double nn0, double np0, double T) |
| Solve for nuclear matter at finite temperature given density. | |
| int | nuc_matter_temp_p (size_t nv, const ubvector &x, ubvector &y, double mun0, double mup0, double T) |
| Solve for nuclear matter at finite temperature given mu. | |
| int | liqgas_dens_solve (size_t nv, const ubvector &x, ubvector &y, fermion &n1, fermion &p1, fermion &n2, fermion &p2, double T, thermo &th1, thermo &th2) |
| Solve for the liquid gas phase transition as a function of the densities. | |
| int | liqgas_solve (size_t nv, const ubvector &x, ubvector &y, fermion &n1, fermion &p1, fermion &n2, fermion &p2, double nB0, double Ye0, double T, thermo &th1, thermo &th2) |
| Solve for the liquid-gas phase transition at fixed baryon density and electron fraction. More... | |
| int | liqgas_beta_solve (size_t nv, const ubvector &x, ubvector &y, fermion &n1, fermion &p1, fermion &n2, fermion &p2, double nB0, double T, thermo &th1, thermo &th2, fermion &e) |
| Solve for the liquid-gas phase transition in beta-equilibrium. | |
| double | calc_entropy_delta (double delta, double nb, double T) |
| Compute the entropy. | |
| double | calc_dmu_delta_T (double delta, double nb, double T) |
| Compute the difference between the neutron and proton chemical potentials. More... | |
Protected Member Functions inherited from o2scl::eos_had_base | |
| double | t1_fun (double barn) |
| Compute t1 for gradient_qij(). | |
| double | t2_fun (double barn) |
| Compute t2 for gradient_qij(). | |
Private Member Functions | |
| virtual int | set_fields (double sig, double ome, double lrho) |
| Forbid setting the guesses to the fields unless all four fields are specified. | |
Additional Inherited Members | |
Public Types inherited from o2scl::eos_had_base | |
| typedef boost::numeric::ublas::vector< double > | ubvector |
Protected Attributes inherited from o2scl::eos_had_rmf | |
| double | n_baryon |
| Temporary baryon density. | |
| double | n_charge |
| Temporary charge density. More... | |
| double | sigma |
| double | omega |
| double | rho |
| double | fe_temp |
| Temperature for solving field equations at finite temperature. | |
| bool | ce_neut_matter |
| For calc_e(), if true, then solve for neutron matter. | |
| bool | ce_prot_matter |
| For calc_e(), if true, then solve for proton matter. | |
| bool | guess_set |
| True if a guess for the fields has been given. | |
| mroot< mm_funct, ubvector, jac_funct > * | sat_mroot |
| The solver to compute saturation properties. | |
| double | ce_temp |
| Temperature storage for calc_temp_e() | |
Protected Attributes inherited from o2scl::eos_had_temp_base | |
| fermion_thermo * | fet |
| Fermion thermodynamics (default is def_fet) | |
Protected Attributes inherited from o2scl::eos_had_base | |
| mroot * | eos_mroot |
| The EOS solver. | |
| root * | sat_root |
| The solver to compute saturation properties. | |
| deriv_base * | sat_deriv |
| The derivative object for saturation properties. | |
| deriv_base * | sat_deriv2 |
| The second derivative object for saturation properties. | |
| fermion * | neutron |
| The neutron object. | |
| fermion * | proton |
| The proton object. | |
Protected Attributes inherited from o2scl::eos_base | |
| thermo * | eos_thermo |
| A pointer to the thermo object. | |
|
virtual |
This requires initial guesses to the chemical potentials, etc.
Reimplemented from o2scl::eos_had_rmf.
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