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/*******************************************************************************
*
* McXtrace, x-ray tracing package
* Copyright, All rights reserved
* DTU Physics, Kgs. Lyngby, Denmark
* Synchrotron SOLEIL, Saint-Aubin, France
*
* Component: Shell_c
*
* %Identification
*
* Written by: Erik B Knudsen and Desiree D. M. Ferreira
* Date: Feb. 2016
* Version: 1.0
* Release: McXtrace 1.2
* Origin: DTU Physics, DTU Space
*
* Single conical shell as part of a Wolter optic.
*
* %Description
* A single shell is simulated. The top and bottom are curved cylindrically
* azimuthally, whereas they are straight sagitally. The primary parameter specifies whether this is a
* primary or secondary mirror.
* The azimuthal curvature is defined by the parameter radius. This refers to the top plate of the shell. I.e the top
* and bottom plates have radius of curvature <radius> and <radius-yheight> respectively.
*
* To intersect the Wolter I plates we take advatage of the azimuthal symmetry and only consider the radial component
* of the photon's wavevector.
*
* Example: Shell_c( radius_m=0.535532,Z0=12,yheight=1e-2,length=0.5,primary=0, R_d=1)
*
* %Parameters
* Input parameters:
* radius_m: [m] Ring radius of the upper (reflecting) plate of the shell at the optic centre.
* yheight: [m] Height of the shell.
* chamferwidth: [m] Width of side walls.
* gap: [m] Gap between the plate and the intersection plane with the hyperbolic section. (currently ignored)
* Z0: [m] Distance between optics centre plane and focal spot (essentially focal length).
* mirror_reflec: [ ] Data file containing reflectivities of the reflector surface (TOP).
* bottom_reflec: [ ] Data file containing reflectivities of the bottom surface (BOTTOM).
* R_d: [ ] Default reflectivity value to use if no reflectivity file is given. Useful f.i. is one surface is reflecting and the others absorbing.
* primary: [ ] If non-zero, the shell is considered a primary reflector, and extends towards negative z. I.e. the entry plane is behind the z=0-plane. If zero, the shell is considered secondary
* and extends from the z=0-plane and towards positive z.
* dalpha: [deg] Offset to the alpha angle computed from the focal length. Useful for targeting the modified conical geometry (currently ignored).
* waviness: [rad] Waviness of the shell reflecting surface. The slope error is assumed to be uniformly distributed in the interval [-waviness:waviness].
* longw: [ ] If non-zero, waviness is 1D and along the shell axis.
* %End
*******************************************************************************/
DEFINE COMPONENT Shell_c
SETTING PARAMETERS (radius_m, Z0, yheight, gap=0, chamferwidth=0, length=0, string mirror_reflec="", string bottom_reflec="", R_d=1, primary=1, dalpha=0, waviness=0, longw=0)
SHARE
%{
#ifndef MCSPO_INTERSECT_CONE
#define MCSPO_INTERSECT_CONE 1
int intersect_cone(double *l0, double x, double y, double z, double kx, double ky, double kz, double alpha, double radius, double *nx, double *ny, double *nz){
double kxn=kx,kyn=ky,kzn=kz;
NORM(kxn,kyn,kzn);
double c=tan(alpha);
double z0=radius/c;
double c2=c*c;
double A,B,C;
A=kxn*kxn + kyn*kyn - c2*kzn*kzn;
B=2*(kxn*x + kyn*y - c2*kzn*(z-z0));
C=x*x + y*y - c2*(z-z0)*(z-z0);
int status;
double l1;
if ( (status=solve_2nd_order(l0,&l1,A,B,C))==0 ){
/*note that if l1->NULL only the smallest positive solution is returned*/
//fprintf(stderr,"Error(%s): No solution to second order eq.\n","Shell_c");
return status;
}
/*compute normal vector here*/
x+=kxn* (*l0);
y+=kyn* (*l0);
z+=kzn* (*l0);
double vn=sqrt(x*x+y*y);
*nx=x/vn;
*ny=y/vn;
*nz=1;
*nx *= cos(alpha);
*ny *= cos(alpha);
*nz *= sin(alpha);
return status;
}
#endif
%}
DECLARE
%{
double nExit[3];
double wExit[3];
double nEntry[3];
double wEntry[3];
double nTop[3];
double nBottom[3];
double alpha;
double radius_1;
double radius_2;
double e_min[2];
double e_step[2];
double e_max[2];
double theta_min[2];
double theta_step[2];
double theta_max[2];
double zentry;
double zexit;
t_Table reflec_top_table;
t_Table reflec_bottom_table;
%}
INITIALIZE
%{
/*read data from files into tables using read_table-lib*/
char *filenames[2]={mirror_reflec,bottom_reflec};
t_Table *ref_tables[2]={&reflec_top_table,&reflec_bottom_table};
int i;
/*read data from files into tables using read_table-lib*/
for (i=0;i<2;i++){
char *reflec=filenames[i];
t_Table *tp=ref_tables[i];
if (reflec && strlen(reflec)) {
char **header_parsed;
/* read 1st block data from file into tp */
if (Table_Read(tp, reflec, 1) <= 0)
{
exit(fprintf(stderr,"Error(%s): can not read file %s\n",NAME_CURRENT_COMP, reflec));
}
header_parsed = Table_ParseHeader(tp->header,
"e_min=","e_max=","e_step=","theta_min=","theta_max=","theta_step=",NULL);
if (header_parsed[0] && header_parsed[1] && header_parsed[2] &&
header_parsed[3] && header_parsed[4] && header_parsed[5])
{
e_min[i]=strtod(header_parsed[0],NULL);
e_max[i]=strtod(header_parsed[1],NULL);
e_step[i]=strtod(header_parsed[2],NULL);
theta_min[i]=strtod(header_parsed[3],NULL);
theta_max[i]=strtod(header_parsed[4],NULL);
theta_step[i]=strtod(header_parsed[5],NULL);
} else {
exit(fprintf(stderr,"Error (%s): wrong/missing header line(s) in file %s\n", NAME_CURRENT_COMP, reflec));
}
if (!((int)(e_max[i]-e_min[i]) == (int)((tp->rows-1)*e_step[i])))
{
exit(fprintf(stderr,"Error (%s): e_step does not match e_min and e_max in file %s\n",NAME_CURRENT_COMP, reflec));
}
if (!((int)(theta_max[i]-theta_min[i]) == (int)((tp->columns-1)*theta_step[i])))
{
exit(fprintf(stderr,"Error (%s): theta_step does not match theta_min and theta_max in file %s\n",NAME_CURRENT_COMP, reflec));
}
}else{
/*mark the table as unread by setting "rows" to -1
This will trigger the default reflectivity.*/
tp->rows=-1;
}
}
/* compute some pore parameters*/
alpha=0.25*atan(radius_m/Z0);
double D,Z0p;
if (primary){
Z0p=radius_m/tan(alpha);
D=sqrt(radius_m*radius_m + Z0p*Z0p);
zentry=Z0p*(1-(D+length)/D);
zexit=0;
radius_1=(D+length)/D*radius_m;
radius_2=radius_m;
}else{
alpha*=3.0;
Z0p=radius_m/tan(alpha);
D=sqrt(radius_m*radius_m + Z0p*Z0p);
zentry=0;
zexit=Z0p*(1-(D-length)/D);
radius_1=radius_m;
radius_2=(D-length)/D*radius_m;
}
nEntry[0]=nEntry[1]=0; nEntry[2]=-1;
wEntry[0]=wEntry[1]=0; wEntry[2]=zentry;
nExit[0]=nExit[1]=0; nExit[2]=1;
wExit[0]=wExit[1]=0; wExit[2]=zexit;
%}
TRACE
%{
enum {LEFT, RIGHT, TOP, BOTTOM, EXIT, NONE} wall;
t_Table *reflec_table=NULL;
int hit_shell, hit_chamfer;
double R;
/*Moving photon to z=-zentry. This odd way of writing this is to handle phase and time automatically.
Note that zentry is z<0, hence the sign convention.*/
z-=zentry;
ALLOW_BACKPROP;
PROP_Z0;
z+=zentry;
hit_shell= ( ( x*x + y*y < radius_1*radius_1 ) && ( x*x + y*y >(radius_1-yheight)*(radius_1-yheight) ) ) ;
hit_chamfer=0;
if(hit_shell){
SCATTER;
int exit=0;
int intersections[5]={0,0,0,0,0};
int i_small;
double l[5]={100000.0, 100000.0, 100000.0, 100000.0, 100000.0};
double l_small;
double nx,ny,nz;
while (!exit){
l_small=DBL_MAX;
wall=NONE;
double nx,ny,nz;
double wx,wy,wz;
int prm_idx;
intersections[EXIT]=plane_intersect(l+EXIT,x,y,z,kx,ky,kz,nExit[0],nExit[1],nExit[2],wExit[0],wExit[1],wExit[2]);
if (intersections[EXIT] && l[EXIT]>DBL_EPSILON && l[EXIT]<l_small) {l_small=l[EXIT];i_small=intersections[EXIT];wall=EXIT;}
/*top surface - the real reflecting surface*/
intersections[TOP]=intersect_cone((l+TOP),x,y,z,kx,ky,kz,alpha,radius_m,&(nTop[0]),&(nTop[1]),&(nTop[2]));
if (intersections[TOP] && l[TOP]>DBL_EPSILON && l[TOP]<l_small) {l_small=l[TOP];i_small=intersections[TOP];wall=TOP;}
/*bottom surface*/
intersections[BOTTOM]=intersect_cone((l+BOTTOM),x,y,z,kx,ky,kz,alpha,radius_m-yheight,&(nBottom[0]),&(nBottom[1]),&(nBottom[2]));
if (intersections[BOTTOM] && l[BOTTOM]>DBL_EPSILON && l[BOTTOM]<l_small) {l_small=l[BOTTOM];i_small=intersections[BOTTOM];wall=BOTTOM;}
switch (wall){
case TOP:
/*handle top wall reflection*/
reflec_table=&reflec_top_table;
nx=nTop[0];ny=nTop[1];nz=nTop[2];
prm_idx=0;
break;
case BOTTOM:
/*handle bottom wall "reflection"*/
reflec_table=&reflec_bottom_table;
nx=nBottom[0];ny=nBottom[1];nz=nBottom[2];
prm_idx=1;
break;
case EXIT:
/*photon will exit pore*/
exit=1;
break;
}
if(exit){
continue;
}
PROP_DL(l_small);
double kix=kx,kiy=ky,kiz=kz;
double k=sqrt(kx*kx+ ky*ky + kz*kz);
double e=K2E*k;
double s=scalar_prod(kx,ky,kz,nx,ny,nz);
double theta=RAD2DEG*(M_PI_2-acos(s/k)); /*pi_2 since theta is supposed to be the grazing angle*/
/*if we have waviness alter the normal vector slightly*/
if(waviness!=0){
/*assuming theta to be small we might disregard atan*/
if(longw){
double dtheta;
if(theta<waviness){
dtheta=rand01()*(theta+waviness)-theta;
}else{
dtheta=randpm1()*waviness;
}
double tx,ty,tz;
vec_prod(tx,ty,tz,0,0,1,nx,ny,nz);
rotate(nx,ny,nz, nx,ny,nz, dtheta, tx,ty,tz);
}else{
/*waviness is also transversal but isotropic*/
double radius;
if(theta<waviness){
radius=atan(waviness);
randvec_target_circle(&nx,&ny,&nz,NULL,nx,ny,nx,radius);
}else{
radius=(atan(theta)+atan(waviness))/2.0;
randvec_target_circle(&nx,&ny,&nz,NULL,nx,ny,nx+radius-atan(theta),radius);
}
NORM(nx,ny,nz);
}
/*recompute theta*/
theta=RAD2DEG*0.5*acos(scalar_prod(kx,ky,kz,kix,kiy,kiz)/k/k);
}
/*reflect the photon through the surface normal*/
if(s!=0){
kx-=2*s*nx;
ky-=2*s*ny;
kz-=2*s*nz;
}
SCATTER;
if(reflec_table==NULL || reflec_table->rows==-1){
R=R_d;
}else{
R=Table_Value2d(*reflec_table,(e-e_min[prm_idx])/e_step[prm_idx], (theta-theta_min[prm_idx])/theta_step[prm_idx]);
}
p*=R;
}
}else if (hit_chamfer){
ABSORB;
}else{
/*no hit*/
ABSORB;
}
%}
MCDISPLAY
%{
int k;
double zo,zm,radius_o;
magnify("");
zm=0;
double D,Z0p;
Z0p=radius_m/tan(alpha);
D=sqrt(radius_m*radius_m + Z0p*Z0p);
if (primary){
zo=Z0p*(1-(D+length)/D);
radius_o=(Z0p-zo)/Z0p*radius_m;
}else{
zo=Z0p*(1-(D-length)/D);
radius_o=(Z0p-zexit)/Z0p*radius_m;
}
circle("xy",0,0,zm,radius_m);
circle("xy",0,0,zm,radius_m-yheight);
circle("xy",0,0,zo,radius_o);
circle("xy",0,0,zo,radius_o-yheight);
%}
END
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