/*******************************************************************************
*
* McStas, neutron ray-tracing package
*         Copyright (C) 1997-2006, All rights reserved
*         Risoe National Laboratory, Roskilde, Denmark
*         Institut Laue Langevin, Grenoble, France
*
* Component: Monochromator_anisotropic
*
* %I
*
* Written by: Kristian Nielsen
* Date: 1999
* Version: $Revision: 1.11 $
* Origin: Risoe
* Release: McStas 1.9.1
* Modified by: EF, 2004. Renamed as Monochromator_flat
*
* Flat Mosaic crystal with anisotropic mosaic.
*
* %D
* Flat, infinitely thin mosaic crystal, useful as a monochromator or analyzer.
* For an unrotated monochromator component, the crystal surface lies in the Y-Z
* plane (ie. parallel to the beam).
* The mosaic is anisotropic gaussian, with different FWHMs in the Y and Z
* directions. The scattering vector is perpendicular to the surface.
* OBSOLETE: rather use optics/Monochromator_flat
*
* Example: Mosaic_anisotropic(zmin=-0.1, zmax=0.1, ymin=-0.1, ymax=0.1,
*           mosaich=30.0, mosaicv=30.0, r0=0.7, Q=1.8734)
*
* %P
* INPUT PARAMETERS:
*
* zmin:    Lower z-bound of crystal (m)
* zmax:    Upper z-bound of crystal (m)
* ymin:    Lower y-bound of crystal (m)
* ymax:    Upper y-bound of crystal (m)
* mosaich: Horisontal mosaic (in Z direction) (FWHM) (arc minutes)
* mosaicv: Vertical mosaic (in Y direction) (FWHM) (arc minutes)
* r0:      Maximum reflectivity (1)
* Q:       Magnitude of scattering vector (AA-1)
*
* optional parameters
* DM:      monochromator d-spacing (Angstrom) instead of Q = 2*pi/DM
*
* %E
*******************************************************************************/

DEFINE COMPONENT Mosaic_anisotropic
DEFINITION PARAMETERS ()
SETTING PARAMETERS (zmin, zmax, ymin, ymax, mosaich=30.0, mosaicv=30.0, r0=0.7, Q=1.8734, DM=0)
OUTPUT PARAMETERS (mos_rms_y, mos_rms_z, mos_rms_max, mono_Q)
STATE PARAMETERS (x,y,z,vx,vy,vz,t,s1,s2,p)

SHARE
%{
#ifndef GAUSS
  /* Define these arrays only once for all instances. */
  /* Values for Gauss quadrature. Taken from Brice Carnahan, H. A. Luther and
     James O Wilkes, "Applied numerical methods", Wiley, 1996, page 103. */
  double Gauss_X[] = {-0.987992518020485, 0.937273392400706, 0.848206583410427,
                0.724417731360170, 0.570972172608539, 0.394151347077563,
                0.201194093997435, 0, 0.201194093997435,
                0.394151347077563, 0.570972172608539, 0.724417731360170,
                0.848206583410427, 0.937273392400706, 0.987992518020485};
  double Gauss_W[] = {0.030753241996117, 0.070366047488108, 0.107159220467172,
                0.139570677926154, 0.166269205816994, 0.186161000115562,
                0.198431485327111, 0.202578241925561, 0.198431485327111,
                0.186161000115562, 0.166269205816994, 0.139570677926154,
                0.107159220467172, 0.070366047488108, 0.030753241996117};


#define GAUSS(x,mean,rms) \
  (exp(-((x)-(mean))*((x)-(mean))/(2*(rms)*(rms)))/(sqrt(2*PI)*(rms)))
#endif
%}

DECLARE
%{
  double mos_rms_y; /* root-mean-square of mosaic, in radians */
  double mos_rms_z;
  double mos_rms_max;
  double mono_Q;
%}

INITIALIZE
%{
  mos_rms_y = MIN2RAD*mosaich/sqrt(8*log(2));
  mos_rms_z = MIN2RAD*mosaicv/sqrt(8*log(2));
  mos_rms_max = mos_rms_y > mos_rms_z ? mos_rms_y : mos_rms_z;

  mono_Q = Q;
  if (DM != 0) mono_Q = 2*PI/DM;
%}

TRACE
%{
  double y1,z1,t1,dt,kix,kiy,kiz,ratio,order,q0x,k,q0,theta;
  double bx,by,bz,kux,kuy,kuz,ax,ay,az,phi;
  double cos_2theta,k_sin_2theta,cos_phi,sin_phi,kfx,kfy,kfz,q_x,q_y,q_z;
  double delta,p_reflect,total,c1x,c1y,c1z,width,mos_sample;
  int i;

  if(vx != 0.0 && (dt = -x/vx) >= 0.0)
  {                             /* Moving towards crystal? */
    y1 = y + vy*dt;             /* Propagate to crystal plane */
    z1 = z + vz*dt;
    t1 = t + dt;
    if (z1>zmin && z1<zmax && y1>ymin && y1<ymax)
    {                           /* Intersect the crystal? */
      kix = V2K*vx;             /* Initial wave vector */
      kiy = V2K*vy;
      kiz = V2K*vz;
      /* Get reflection order and corresponding nominal scattering vector q0
         of correct length and direction. Only the order with the closest
         scattering vector is considered */
      ratio = -2*kix/mono_Q;
      order = floor(ratio + .5);
      if(order == 0.0)
        order = ratio < 0 ? -1 : 1;
      /* Order will be negative when the neutron enters from the back, in
         which case the direction of Q0 is flipped. */
      if(order < 0)
        order = -order;
      /* Make sure the order is small enough to allow Bragg scattering at the
         given neutron wavelength */
      k = sqrt(kix*kix + kiy*kiy + kiz*kiz);
      kux = kix/k;              /* Unit vector along ki */
      kuy = kiy/k;
      kuz = kiz/k;
      if(order > 2*k/mono_Q)
        order--;
      if(order > 0)             /* Bragg scattering possible? */
      {
        q0  = order*mono_Q;
        q0x = ratio < 0 ? -q0 : q0;
        theta = asin(q0/(2*k)); /* Actual bragg angle */
        /* Make MC choice: reflect or transmit? */
        delta = asin(fabs(kux)) - theta;
        p_reflect = r0*exp(-kiz*kiz/(kiy*kiy + kiz*kiz)*(delta*delta)/
                           (2*mos_rms_y*mos_rms_y))*
                       exp(-kiy*kiy/(kiy*kiy + kiz*kiz)*(delta*delta)/
                           (2*mos_rms_z*mos_rms_z));
        if(rand01() < p_reflect)
        {                       /* Reflect */
          cos_2theta = cos(2*theta);
          k_sin_2theta = k*sin(2*theta);
          /* Get unit normal to plane containing ki and most probable kf */
          vec_prod(bx, by, bz, kix, kiy, kiz, q0x, 0, 0);
          NORM(bx,by,bz);
          bx *= k_sin_2theta;
          by *= k_sin_2theta;
          bz *= k_sin_2theta;
          /* Get unit vector normal to ki and b */
          vec_prod(ax, ay, az, bx, by, bz, kux, kuy, kuz);
          /* Compute the total scattering probability at this ki */
          total = 0;
          /* Choose width of Gaussian distribution to sample the angle
           * phi on the Debye-Scherrer cone for the scattered neutron.
           * The radius of the Debye-Scherrer cone is smaller by a
           * factor 1/cos(theta) than the radius of the (partial) sphere
           * describing the possible orientations of Q due to mosaicity, so we
           * start with a width 1/cos(theta) greater than the largest of
           * the two mosaics. */
          mos_sample = mos_rms_max/cos(theta);
          c1x = kix*(cos_2theta-1);
          c1y = kiy*(cos_2theta-1);
          c1z = kiz*(cos_2theta-1);
          /* Loop, repeatedly reducing the sample width until it is small
           * enough to avoid sampling scattering directions with
           * ridiculously low scattering probability.
           * Use a cut-off at 5 times the gauss width for considering
           * scattering probability as well as for integration limits
           * when integrating the sampled distribution below. */
          for(;;) {
            width = 5*mos_sample;
            cos_phi = cos(width);
            sin_phi = sin(width);
            q_x = c1x + cos_phi*ax + sin_phi*bx;
            q_y = (c1y + cos_phi*ay + sin_phi*by)/mos_rms_z;
            q_z = (c1z + cos_phi*az + sin_phi*bz)/mos_rms_y;
            /* Stop when we get near a factor of 25=5^2. */
            if(q_z*q_z + q_y*q_y < (25/(2.0/3.0))*(q_x*q_x))
              break;
            mos_sample *= (2.0/3.0);
          }
          /* Now integrate the chosen sampling distribution, using a
           * cut-off at five times sigma. */
          for(i = 0; i < (sizeof(Gauss_X)/sizeof(double)); i++)
          {
            phi = width*Gauss_X[i];
            cos_phi = cos(phi);
            sin_phi = sin(phi);
            q_x = c1x + cos_phi*ax + sin_phi*bx;
            q_y = c1y + cos_phi*ay + sin_phi*by;
            q_z = c1z + cos_phi*az + sin_phi*bz;
            p_reflect = GAUSS((q_z/q_x),0,mos_rms_y)*
                        GAUSS((q_y/q_x),0,mos_rms_z);
            total += Gauss_W[i]*p_reflect;
          }
          total *= width;
          /* Choose point on Debye-Scherrer cone. Sample from a Gaussian of
           * width 1/cos(theta) greater than the mosaic and correct for any
           * error by adjusting the neutron weight later. */
          phi = mos_sample*randnorm();
          /* Compute final wave vector kf and scattering vector q = ki - kf */
          cos_phi = cos(phi);
          sin_phi = sin(phi);
          q_x = c1x + cos_phi*ax + sin_phi*bx;
          q_y = c1y + cos_phi*ay + sin_phi*by;
          q_z = c1z + cos_phi*az + sin_phi*bz;
          p_reflect = GAUSS((q_z/q_x),0,mos_rms_y)*
                      GAUSS((q_y/q_x),0,mos_rms_z);
          x = 0;
          y = y1;
          z = z1;
          t = t1;
          vx = K2V*(kix+q_x);
          vy = K2V*(kiy+q_y);
          vz = K2V*(kiz+q_z);
          p *= p_reflect/(total*GAUSS(phi,0,mos_sample));
          SCATTER;
        } /* End MC choice to reflect or transmit neutron */
      } /* End bragg scattering possible */
    } /* End intersect the crystal */
  } /* End neutron moving towards crystal */
%}

MCDISPLAY
%{
  magnify("zy");
  multiline(5, 0.0, (double)ymin, (double)zmin,
               0.0, (double)ymax, (double)zmin,
               0.0, (double)ymax, (double)zmax,
               0.0, (double)ymin, (double)zmax,
               0.0, (double)ymin, (double)zmin);
%}

END
