📄 gsl_sf_coulomb.h
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/* specfunc/gsl_sf_coulomb.h * * Copyright (C) 1996, 1997, 1998, 1999, 2000 Gerard Jungman * * This program 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. * * This program 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, write to the Free Software * Foundation, Inc., 51 Franklin Street, Fifth Floor, Boston, MA 02110-1301, USA. *//* Author: G. Jungman */#ifndef __GSL_SF_COULOMB_H__#define __GSL_SF_COULOMB_H__#include "gsl_mode.h"#include "gsl_sf_result.h"#include "gsl_types.h"#undef __BEGIN_DECLS#undef __END_DECLS#ifdef __cplusplus# define __BEGIN_DECLS extern "C" {# define __END_DECLS }#else# define __BEGIN_DECLS /* empty */# define __END_DECLS /* empty */#endif__BEGIN_DECLS/* Normalized hydrogenic bound states, radial dependence. *//* R_1 := 2Z sqrt(Z) exp(-Z r) */GSL_EXPORT int gsl_sf_hydrogenicR_1_e(const double Z, const double r, gsl_sf_result * result);GSL_EXPORT double gsl_sf_hydrogenicR_1(const double Z, const double r);/* R_n := norm exp(-Z r/n) (2Z/n)^l Laguerre[n-l-1, 2l+1, 2Z/n r] * * normalization such that psi(n,l,r) = R_n Y_{lm} */GSL_EXPORT int gsl_sf_hydrogenicR_e(const int n, const int l, const double Z, const double r, gsl_sf_result * result);GSL_EXPORT double gsl_sf_hydrogenicR(const int n, const int l, const double Z, const double r);/* Coulomb wave functions F_{lam_F}(eta,x), G_{lam_G}(eta,x) * and their derivatives; lam_G := lam_F - k_lam_G * * lam_F, lam_G > -0.5 * x > 0.0 * * Conventions of Abramowitz+Stegun. * * Because there can be a large dynamic range of values, * overflows are handled gracefully. If an overflow occurs, * GSL_EOVRFLW is signalled and exponent(s) are returned * through exp_F, exp_G. These are such that * * F_L(eta,x) = fc[k_L] * exp(exp_F) * G_L(eta,x) = gc[k_L] * exp(exp_G) * F_L'(eta,x) = fcp[k_L] * exp(exp_F) * G_L'(eta,x) = gcp[k_L] * exp(exp_G) */GSL_EXPORT intgsl_sf_coulomb_wave_FG_e(const double eta, const double x, const double lam_F, const int k_lam_G, gsl_sf_result * F, gsl_sf_result * Fp, gsl_sf_result * G, gsl_sf_result * Gp, double * exp_F, double * exp_G);/* F_L(eta,x) as array */GSL_EXPORT int gsl_sf_coulomb_wave_F_array( double lam_min, int kmax, double eta, double x, double * fc_array, double * F_exponent );/* F_L(eta,x), G_L(eta,x) as arrays */GSL_EXPORT int gsl_sf_coulomb_wave_FG_array(double lam_min, int kmax, double eta, double x, double * fc_array, double * gc_array, double * F_exponent, double * G_exponent );/* F_L(eta,x), G_L(eta,x), F'_L(eta,x), G'_L(eta,x) as arrays */GSL_EXPORT int gsl_sf_coulomb_wave_FGp_array(double lam_min, int kmax, double eta, double x, double * fc_array, double * fcp_array, double * gc_array, double * gcp_array, double * F_exponent, double * G_exponent );/* Coulomb wave function divided by the argument, * F(eta, x)/x. This is the function which reduces to * spherical Bessel functions in the limit eta->0. */GSL_EXPORT int gsl_sf_coulomb_wave_sphF_array(double lam_min, int kmax, double eta, double x, double * fc_array, double * F_exponent );/* Coulomb wave function normalization constant. * [Abramowitz+Stegun 14.1.8, 14.1.9] */GSL_EXPORT int gsl_sf_coulomb_CL_e(double L, double eta, gsl_sf_result * result);GSL_EXPORT int gsl_sf_coulomb_CL_array(double Lmin, int kmax, double eta, double * cl);__END_DECLS#endif /* __GSL_SF_COULOMB_H__ */
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