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/*****************************************************************************
* McXtrace, x-ray tracing package
* Copyright, All rights reserved
* DTU Physics, Kgs. Lyngby, Denmark
* Synchrotron SOLEIL, Saint-Aubin, France
*
* Component: Pore_p
*
* %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 Pore as part of the Silicon Pore Optics (SPO) as envisioned for the ATHENA+ space telescope.
*
* %Description
* A single pore is simulated, which may have thick walls. The top and bottom are curved cylindrically
* azimuthally, and according to the Wolter I optic lengthwise (sagitally). This is the parabolic part.
* The azimuthal curvature is defined by the radius parameters. This refers to the center of the pore. I.e the top
* and bottom plates have radius of curvature <radius+yheight/2> and <radius-yheight/2> 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.
*
* %Parameters
* Input parameters:
* radius_m: [m] Ring radius of the upper (reflecting) plate of the pore at the intersection with the hyperbolic section.
* radius_p: [m] Ring radius of the upper (reflecting) plate of the pore at the edge furthest away from the focal point.
* yheight: [m] Height of the pore. (Thus the inner radius is radius_{m,h}-yehight.
* xwidth: [m] Width of the pore.
* chamferwidth: [m] Width of side walls.
* gap: [m] gap between intersection with parabolic section and actual plate.
* Z0: [m] distance between intersection plane and the focal spot( essentially the focal length).
* mirror_reflec: [ ] Data file containing reflectivities of the reflector surface (TOP).
* side_reflec: [ ] Data file containing reflectivities of the side walls (LEFT and RIGHT).
* 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.
*
* %End
*******************************************************************************/
DEFINE COMPONENT Pore_p
SETTING PARAMETERS (radius_p, radius_m, Z0, xwidth, yheight, gap=0, chamferwidth=0, zdepth=0, string mirror_reflec="", string bottom_reflec="", string side_reflec="", R_d=1, waviness=0, longw=0)
SHARE
%{
%include "read_table-lib"
#ifndef MCSPO_INTERSECT_PARABOLOID
#define MCSPO_INTERSECT_PARABOLOID 1
int intersect_paraboloid(double *l0, double x, double y, double z, double kx, double ky, double kz, double Z0, double radius, double *nx, double *ny, double *nz){
/* Intersection routine for a paraboloid as given by the paper by vanspeybroeck and Chase (appl. optics. 1972)*/
double alpha,thetap,thetah,P,d,e,C0;
alpha=0.25*atan(radius/Z0);
thetap=alpha;
thetah=alpha*3;
P=Z0*tan(4*alpha)*tan(thetap);
d=Z0*tan(4*alpha)*tan(4*alpha-thetah);
e=cos(4*alpha)*(1+tan(4*alpha)*tan(thetah));
C0=4*e*e*P*d/(e*e-1);
double kxn=kx,kyn=ky,kzn=kz;
NORM(kxn,kyn,kzn);
double A,B,C;
A=kxn*kxn + kyn*kyn;
B=2*(kxn*x + kyn*y+ P*kzn);
C=x*x + y*y -P*P - 2*P*(Z0-z) - C0;
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","Pore_p");*/
return status;
}
/*compute normal vector*/
x+=kxn* (*l0);
y+=kyn* (*l0);
z+=kzn* (*l0);
double delta_y=-P*pow(P*P+2*P*(Z0-z)+C0,-0.5);
double rp=sqrt(P*P + 2*P*(Z0-z) + C0);
/* The tilt of the normal vector perpendicular to the optical axis
* depends only on the displacement in x*/
*nx=x/rp;
*ny=y/rp;
*nz = 0 - delta_y + 0;
/* the minus sign since a negative slope in rp results in the normal tilting "forward" which
corresponds to a positive sign in z*/
NORM(*nx,*ny,*nz);
return status;
}
#endif
%}
DECLARE
%{
double nExit[3];
double wExit[3];
double nEntry[3];
double wEntry[3];
double nTop[3];
double nBottom[3];
double nRight[3];
double wRight[3];
double nLeft[3];
double wLeft[3];
double radius_1;
double radius_2;
double e_min[3];
double e_step[3];
double e_max[3];
double theta_min[3];
double theta_step[3];
double theta_max[3];
double zentry;
t_Table reflec_top_table;
t_Table reflec_bottom_table;
t_Table reflec_side_table;
t_Table wave_table[1024];
%}
INITIALIZE
%{
char *filenames[]={mirror_reflec,bottom_reflec,side_reflec};
t_Table *ref_tables[]={&reflec_top_table,&reflec_bottom_table,&reflec_side_table};
int i;
/*read data from files into tables using read_table-lib*/
for (i=0;i<3;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 for the parabolic or hyperbolic equations*/
/* the z coordinate of the entry plane*/
/*assuming the parameter xi==1*/
double alpha,thetap,thetah,P,d,e,C0,Z;
alpha=0.25*atan(radius_m/Z0);
thetap=alpha;
thetah=alpha*3;
P=Z0*tan(4*alpha)*tan(thetap);
d=Z0*tan(4*alpha)*tan(4*alpha-thetah);
e=cos(4*alpha)*(1+tan(4*alpha)*tan(thetah));
C0=4*e*e*P*d/(e*e-1);
/*solve to get the z-coordinate of the entry plane, assuming radius_1 to be bigger*/
Z=(pow(radius_p,2.0) - pow(P,2.0)- C0 ) /(2*P);
zentry=Z0-Z;
double cosa=cos(xwidth/2.0/radius_m);
double sina=sin(xwidth/2.0/radius_m);
/*side wall, entry, and exit planes*/
nLeft[0]= cosa;
nLeft[1]=-sina;
nLeft[2]=0;
wLeft[0]=radius_m*(sina);
wLeft[1]=radius_m*(1-cosa);
wLeft[2]=0;
nRight[0]=-cosa;
nRight[1]=-sina;
nRight[2]=0;
wRight[0]=-radius_m*(sina);
wRight[1]=-radius_m*(1-cosa);
wRight[2]=0;
nEntry[0]=0;
nEntry[1]=0;
nEntry[2]=-1;
wExit[0]=wExit[1]=0;wExit[2]=zentry;
nExit[0]=0;
nExit[1]=0;
nExit[2]=1;
wExit[0]=wExit[1]=wExit[2]=0;
%}
TRACE
%{
enum {LEFT, RIGHT, TOP, BOTTOM, EXIT, NONE} wall;
t_Table *reflec_table=NULL;
int hit_pore, hit_chamfer;
double R;
/*first do a test prop to see if the photon will enter the pore*/
double tmpt,tmpx,tmpy, dl;
tmpt=(zentry-z)/kz;
tmpx=x+kx*tmpt;
tmpy=y+ky*tmpt;
double psi_max,psi_min,psi;
psi_min=-xwidth*0.5/radius_m;
psi_max= xwidth*0.5/radius_m;
psi=atan2(tmpx,tmpy+radius_m);
hit_pore= ( ( tmpx*tmpx + (tmpy+radius_m)*(tmpy+radius_m) < radius_p*radius_p ) && ( tmpx*tmpx + (tmpy+radius_m)*(tmpy+radius_m) >(radius_p-yheight)*(radius_p-yheight) ) && (psi>psi_min && psi<psi_max)) ;
hit_chamfer=0;
if(hit_pore){
/*Moving photon to z=zentry. This odd way of writing this, is to handle phase and time automatically.*/
z-=zentry;
ALLOW_BACKPROP;
PROP_Z0;
z+=zentry;
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;/*index indicating which table parameter set to choose*/
/*left wall*/
intersections[LEFT]=plane_intersect(l+LEFT,x,y,z,kx,ky,kz,nLeft[0],nLeft[1],nLeft[2],wLeft[0],wLeft[1],wLeft[2]);
if (intersections[LEFT] && l[LEFT]>DBL_EPSILON && l[LEFT]<l_small) {l_small=l[LEFT];i_small=intersections[LEFT];wall=LEFT;}
/*right wall*/
intersections[RIGHT]=plane_intersect(l+RIGHT,x,y,z,kx,ky,kz,nRight[0],nRight[1],nRight[2],wRight[0],wRight[1],wRight[2]);
if (intersections[RIGHT] && l[RIGHT]>DBL_EPSILON && l[RIGHT]<l_small) {l_small=l[RIGHT];i_small=intersections[RIGHT];wall=RIGHT;}
/*exit plane*/
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_paraboloid((l+TOP),x,y+radius_m,z,kx,ky,kz,Z0,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_paraboloid((l+BOTTOM),x,y+radius_m,z,kx,ky,kz,Z0,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;}
/*sort intersections ot find the smallest positive one*/
switch (wall){
case LEFT:
/*handle left wall "reflection"*/
reflec_table=&reflec_side_table;
nx=nLeft[0];ny=nLeft[1];nz=nLeft[2];
prm_idx=2;
break;
case RIGHT:
/*handle right wall "reflection"*/
reflec_table=&reflec_side_table;
nx=nRight[0];ny=nRight[1];nz=nRight[2];
prm_idx=2;
break;
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 dth,theta,t0,t1,inner_m,inner_p;
const int N=20;
theta=xwidth/2.0/radius_m;
inner_m=radius_m-yheight;
inner_p=radius_p-yheight;
magnify("");
line(0,0,0, 0,radius_p-radius_m,zentry); /*this extra line indicates the reflecting surface*/
line( sin(theta)*radius_m, (cos(theta)-1)*radius_m, 0, sin(theta)*radius_p, cos(theta)*radius_p-radius_m, zentry);
line(-sin(theta)*radius_m, (cos(theta)-1)*radius_m, 0, -sin(theta)*radius_p, cos(theta)*radius_p-radius_m, zentry);
line( sin(theta)*inner_m, cos(theta)*inner_m-radius_m, 0, sin(theta)*inner_p, cos(theta)*inner_p-radius_m, zentry);
line(-sin(theta)*inner_m, cos(theta)*inner_m-radius_m, 0, -sin(theta)*inner_p, cos(theta)*inner_p-radius_m, zentry);
line( sin(theta)*radius_m, (cos(theta)-1)*radius_m, 0, sin(theta)*inner_m, cos(theta)*inner_m-radius_m, 0);
line(-sin(theta)*radius_m, (cos(theta)-1)*radius_m, 0, -sin(theta)*inner_m, cos(theta)*inner_m-radius_m, 0);
line( sin(theta)*radius_p, cos(theta)*radius_p-radius_m, zentry, sin(theta)*inner_p, cos(theta)*inner_p-radius_m, zentry);
line(-sin(theta)*radius_p, cos(theta)*radius_p-radius_m, zentry, -sin(theta)*inner_p, cos(theta)*inner_p-radius_m, zentry);
dth=2*theta/N;
for (k=1;k<N+1;k++){
t0=-theta+(k-1)*dth;
t1=-theta+k*dth;
line( sin(t0)*radius_m, cos(t0)*radius_m-radius_m, 0, sin(t1)*radius_m, cos(t1)*radius_m-radius_m, 0);
line( sin(t0)*inner_m, cos(t0)*inner_m-radius_m, 0, sin(t1)*inner_m, cos(t1)*inner_m-radius_m, 0);
line( sin(t0)*radius_p, cos(t0)*radius_p-radius_m, zentry, sin(t1)*radius_p, cos(t1)*radius_p-radius_m, zentry);
line( sin(t0)*inner_p, cos(t0)*inner_p-radius_m, zentry, sin(t1)*inner_p, cos(t1)*inner_p-radius_m, zentry);
}
%}
END
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