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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 3 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/gsl_mode.h>
+#include <gsl/gsl_sf_result.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)
+ */
+int gsl_sf_hydrogenicR_1_e(const double Z, const double r, gsl_sf_result * result);
+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}
+ */
+int gsl_sf_hydrogenicR_e(const int n, const int l, const double Z, const double r, gsl_sf_result * result);
+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)
+ */
+int
+gsl_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 */
+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 */
+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 */
+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.
+ */
+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]
+ */
+int gsl_sf_coulomb_CL_e(double L, double eta, gsl_sf_result * result);
+int gsl_sf_coulomb_CL_array(double Lmin, int kmax, double eta, double * cl);
+
+
+__END_DECLS
+
+#endif /* __GSL_SF_COULOMB_H__ */