diff options
author | Thomas White <taw@physics.org> | 2010-02-09 17:24:16 +0100 |
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committer | Thomas White <taw@physics.org> | 2010-02-17 10:33:13 +0100 |
commit | 0f6ebe5649902dea9456c6598bc28e694c422336 (patch) | |
tree | 3ce031ca3c8ecf4fb132fa90aeae7373e0d5b0b6 /data | |
parent | 89bd4cc23c5ac40dd0060d362f663819a5f4ae22 (diff) |
Use OpenCL for much faster diffraction calculation
Diffstat (limited to 'data')
-rw-r--r-- | data/Makefile.am | 2 | ||||
-rw-r--r-- | data/diffraction.cl | 106 |
2 files changed, 107 insertions, 1 deletions
diff --git a/data/Makefile.am b/data/Makefile.am index b4cebb2d..b55597f0 100644 --- a/data/Makefile.am +++ b/data/Makefile.am @@ -2,4 +2,4 @@ hdfseedir = $(datadir)/hdfsee hdfsee_DATA = displaywindow.ui crystfeldir = $(datadir)/crystfel -crystfel_DATA = sfac/* +crystfel_DATA = sfac/* diffraction.cl diff --git a/data/diffraction.cl b/data/diffraction.cl new file mode 100644 index 00000000..5c75d70b --- /dev/null +++ b/data/diffraction.cl @@ -0,0 +1,106 @@ +/* + * diffraction.cl + * + * GPU calculation kernel for truncated lattice diffraction + * + * (c) 2006-2010 Thomas White <taw@physics.org> + * + * Part of CrystFEL - crystallography with a FEL + * + */ + + +#define INDMAX 30 +#define IDIM (INDMAX*2 +1) + + +float4 get_q(int x, int y, float cx, float cy, float res, float clen, float k, + float *ttp) +{ + float rx, ry, r; + float ttx, tty, tt; + + rx = ((float)x - cx)/res; + ry = ((float)y - cy)/res; + + r = sqrt(pow(rx, 2.0) + pow(ry, 2.0)); + + ttx = atan2(rx, clen); + tty = atan2(ry, clen); + tt = atan2(r, clen); + + *ttp = tt; + + return (float4)(k*sin(ttx), k*sin(tty), k-k*cos(tt), 0.0); +} + + +float lattice_factor(float16 cell, float4 q) +{ + float f1, f2, f3; + float4 Udotq; + const int na = 8; + const int nb = 8; + const int nc = 8; + + Udotq.x = cell.s0*q.x + cell.s1*q.y + cell.s2*q.z; + Udotq.y = cell.s3*q.x + cell.s4*q.y + cell.s5*q.z; + Udotq.z = cell.s6*q.x + cell.s7*q.y + cell.s8*q.z; + + /* At exact Bragg condition, f1 = na */ + f1 = sin(M_PI*(float)na*Udotq.x) / sin(M_PI*Udotq.x); + + /* At exact Bragg condition, f2 = nb */ + f2 = sin(M_PI*(float)nb*Udotq.y) / sin(M_PI*Udotq.y); + + /* At exact Bragg condition, f3 = nc */ + f3 = sin(M_PI*(float)nc*Udotq.z) / sin(M_PI*Udotq.z); + + /* At exact Bragg condition, this will multiply the molecular + * part of the structure factor by the number of unit cells, + * as desired (more scattering from bigger crystal!) */ + return f1 * f2 * f3; +} + + +float2 get_sfac(global float2 *sfacs, float16 cell, float4 q) +{ + signed int h, k, l; + int idx; + + h = rint(cell.s0*q.x + cell.s1*q.y + cell.s2*q.z); /* h */ + k = rint(cell.s3*q.x + cell.s4*q.y + cell.s5*q.z); /* k */ + l = rint(cell.s6*q.x + cell.s7*q.y + cell.s8*q.z); /* l */ + + if ( (abs(h) > INDMAX) || (abs(k) > INDMAX) || (abs(l) > INDMAX) ) { + return 100.0; + } + + if ( h < 0 ) h += IDIM; + if ( k < 0 ) k += IDIM; + if ( l < 0 ) l += IDIM; + + idx = h + (IDIM*k) + (IDIM*IDIM*l); + return sfacs[idx]; +} + + +kernel void diffraction(global float2 *diff, global float *tt, float k, + int w, float cx, float cy, + float res, float clen, float16 cell, + global float2 *sfacs) +{ + float ttv; + const int x = get_global_id(0); + const int y = get_global_id(1); + float f_lattice; + float2 f_molecule; + + float4 q = get_q(x, y, cx, cy, res, clen, k, &ttv); + + f_lattice = lattice_factor(cell, q); + f_molecule = get_sfac(sfacs, cell, q); + + diff[x+w*y] = f_molecule*f_lattice; + tt[x+w*y] = ttv; +} |