// The original code, of which work was not DANSE funded,
// was provided by J. Cho.
#if !defined(o_h)
#define refl_adv_h
/**
* Structure definition for sphere parameters
*/
//[PYTHONCLASS] = ReflAdvModel
//[DISP_PARAMS] = thick_inter0
//[DESCRIPTION] =Calculate neutron reflectivity using the Parratt iterative formula
// Parameters:
// background:background
// scale: scale factor
// sld_bottom0: the SLD of the substrate
// sld_medium: the SLD of the incident medium
// or superstrate
// sld_flatN: the SLD of the flat region of
// the N'th layer
// thick_flatN: the thickness of the flat
// region of the N'th layer
// func_interN: the function used to describe
// the interface of the N'th layer
// nu_interN: the coefficient for the func_interN
// thick_interN: the thickness of the interface
// of the N'th layer
// Note: the layer number starts to increase
// from the bottom (substrate) to the top.
//
//[FIXED]=
//[NON_FITTABLE_PARAMS]= n_layers;func_inter0;func_inter1;func_inter2;func_inter3;func_inter4;func_inter5;func_inter5;func_inter7;func_inter8;func_inter9;func_inter10
//[ORIENTATION_PARAMS]=
typedef struct {
/// number of layers
// [DEFAULT]=n_layers=1
int n_layers;
/// Scale factor
// [DEFAULT]=scale= 1.0
double scale;
/// thick_inter0 [A]
// [DEFAULT]=thick_inter0=50.0 [A]
double thick_inter0;
/// func_inter0
// [DEFAULT]=func_inter0= 0
double func_inter0;
/// sld_bottom0 [1/A^(2)]
// [DEFAULT]=sld_bottom0= 2.07e-6 [1/A^(2)]
double sld_bottom0;
/// sld_medium [1/A^(2)]
// [DEFAULT]=sld_medium= 1.0e-6 [1/A^(2)]
double sld_medium;
/// Background
// [DEFAULT]=background=0
double background;
// [DEFAULT]=sld_flat1=4.0e-06 [1/A^(2)]
double sld_flat1;
// [DEFAULT]=sld_flat2=3.5e-06 [1/A^(2)]
double sld_flat2;
// [DEFAULT]=sld_flat3=4.0e-06 [1/A^(2)]
double sld_flat3;
// [DEFAULT]=sld_flat4=3.5e-06 [1/A^(2)]
double sld_flat4;
// [DEFAULT]=sld_flat5=4.0e-06 [1/A^(2)]
double sld_flat5;
// [DEFAULT]=sld_flat6=3.5e-06 [1/A^(2)]
double sld_flat6;
// [DEFAULT]=sld_flat7=4.0e-06 [1/A^(2)]
double sld_flat7;
// [DEFAULT]=sld_flat8=3.5e-06 [1/A^(2)]
double sld_flat8;
// [DEFAULT]=sld_flat9=4.0e-06 [1/A^(2)]
double sld_flat9;
// [DEFAULT]=sld_flat10=3.5e-06 [1/A^(2)]
double sld_flat10;
// [DEFAULT]=thick_inter1=50 [A]
double thick_inter1;
// [DEFAULT]=thick_inter2=50 [A]
double thick_inter2;
// [DEFAULT]=thick_inter3=50 [A]
double thick_inter3;
// [DEFAULT]=thick_inter4=50 [A]
double thick_inter4;
// [DEFAULT]=thick_inter5=50 [A]
double thick_inter5;
// [DEFAULT]=thick_inter6=50 [A]
double thick_inter6;
// [DEFAULT]=thick_inter7=50 [A]
double thick_inter7;
// [DEFAULT]=thick_inter8=50 [A]
double thick_inter8;
// [DEFAULT]=thick_inter9=50 [A]
double thick_inter9;
// [DEFAULT]=thick_inter10=50 [A]
double thick_inter10;
// [DEFAULT]=thick_flat1=100 [A]
double thick_flat1;
// [DEFAULT]=thick_flat2=100 [A]
double thick_flat2;
// [DEFAULT]=thick_flat3=100 [A]
double thick_flat3;
// [DEFAULT]=thick_flat4=100 [A]
double thick_flat4;
// [DEFAULT]=thick_flat5=100 [A]
double thick_flat5;
// [DEFAULT]=thick_flat6=100 [A]
double thick_flat6;
// [DEFAULT]=thick_flat7=100 [A]
double thick_flat7;
// [DEFAULT]=thick_flat8=100 [A]
double thick_flat8;
// [DEFAULT]=thick_flat9=100 [A]
double thick_flat9;
// [DEFAULT]=thick_flat10=100 [A]
double thick_flat10;
// [DEFAULT]=func_inter1=0
double func_inter1;
// [DEFAULT]=func_inter2=0
double func_inter2;
// [DEFAULT]=func_inter3=0
double func_inter3;
// [DEFAULT]=func_inter4=0
double func_inter4;
// [DEFAULT]=func_inter5=0
double func_inter5;
// [DEFAULT]=func_inter6=0
double func_inter6;
// [DEFAULT]=func_inter7=0
double func_inter7;
// [DEFAULT]=func_inter8=0
double func_inter8;
// [DEFAULT]=func_inter9=0
double func_inter9;
// [DEFAULT]=func_inter10=0
double func_inter10;
// [DEFAULT]=sldIM_flat1=0 [1/A^(2)]
double sldIM_flat1;
// [DEFAULT]=sldIM_flat2=0 [1/A^(2)]
double sldIM_flat2;
// [DEFAULT]=sldIM_flat3=0 [1/A^(2)]
double sldIM_flat3;
// [DEFAULT]=sldIM_flat4=0 [1/A^(2)]
double sldIM_flat4;
// [DEFAULT]=sldIM_flat5=0 [1/A^(2)]
double sldIM_flat5;
// [DEFAULT]=sldIM_flat6=0 [1/A^(2)]
double sldIM_flat6;
// [DEFAULT]=sldIM_flat7=0 [1/A^(2)]
double sldIM_flat7;
// [DEFAULT]=sldIM_flat8=0 [1/A^(2)]
double sldIM_flat8;
// [DEFAULT]=sldIM_flat9=0 [1/A^(2)]
double sldIM_flat9;
// [DEFAULT]=sldIM_flat10=0 [1/A^(2)]
double sldIM_flat10;
// [DEFAULT]=nu_inter1=2.5
double nu_inter1;
// [DEFAULT]=nu_inter2=2.5
double nu_inter2;
// [DEFAULT]=nu_inter3=2.5
double nu_inter3;
// [DEFAULT]=nu_inter4=2.5
double nu_inter4;
// [DEFAULT]=nu_inter5=2.5
double nu_inter5;
// [DEFAULT]=nu_inter6=2.5
double nu_inter6;
// [DEFAULT]=nu_inter7=2.5
double nu_inter7;
// [DEFAULT]=nu_inter8=2.5
double nu_inter8;
// [DEFAULT]=nu_inter9=2.5
double nu_inter9;
// [DEFAULT]=nu_inter10=2.5
double nu_inter10;
// [DEFAULT]=sldIM_sub0=0
double sldIM_sub0;
// [DEFAULT]=sldIM_medium=0
double sldIM_medium;
// [DEFAULT]=npts_inter=21.0
double npts_inter;
// [DEFAULT]=nu_inter0=2.5
double nu_inter0;
} ReflAdvParameters;
double re_adv_kernel(double dq[], double q);
/// 1D scattering function
double refl_adv_analytical_1D(ReflAdvParameters *pars, double q);
/// 2D scattering function
double refl_adv_analytical_2D(ReflAdvParameters *pars, double q, double phi);
double refl_adv_analytical_2DXY(ReflAdvParameters *pars, double qx, double qy);
#endif