diff options
author | Thomas White <taw@physics.org> | 2010-03-01 17:10:41 +0100 |
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committer | Thomas White <taw@physics.org> | 2010-03-01 17:52:03 +0100 |
commit | f213d4dc787d4d6edb8981c41138f4ace1e2f324 (patch) | |
tree | b9e3b4d59993474a6c5e4c769d3d4f75638b04c1 /data/diffraction.cl | |
parent | 8c01976e4bc6670c6f824479357c42caa18fb2ff (diff) |
Use a lookup table for sinc values in GPU calculation
Diffstat (limited to 'data/diffraction.cl')
-rw-r--r-- | data/diffraction.cl | 47 |
1 files changed, 23 insertions, 24 deletions
diff --git a/data/diffraction.cl b/data/diffraction.cl index ebacb416..cc3e91bd 100644 --- a/data/diffraction.cl +++ b/data/diffraction.cl @@ -15,6 +15,15 @@ #define M_PI ((float)(3.14159265)) #endif + +const sampler_t sampler_a = CLK_NORMALIZED_COORDS_TRUE | CLK_ADDRESS_REPEAT + | CLK_FILTER_LINEAR; +const sampler_t sampler_b = CLK_NORMALIZED_COORDS_TRUE | CLK_ADDRESS_REPEAT + | CLK_FILTER_LINEAR; +const sampler_t sampler_c = CLK_NORMALIZED_COORDS_TRUE | CLK_ADDRESS_REPEAT + | CLK_FILTER_LINEAR; + + float4 quat_rot(float4 q, float4 z) { float4 res; @@ -80,36 +89,23 @@ float range(float a) } -float lattice_factor(float16 cell, float4 q, int4 ncells) +float lattice_factor(float16 cell, float4 q, + read_only image2d_t func_a, + read_only image2d_t func_b, + read_only image2d_t func_c) { float f1, f2, f3, v; float4 Udotq; - const int na = ncells.s0; - const int nb = ncells.s1; - const int nc = ncells.s2; 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 */ - v = M_PI*Udotq.x; - f1 = sin(v*(float)na) / sin(v); - f1 = isnan(f1) ? na : f1; - - /* At exact Bragg condition, f2 = nb */ - v = M_PI*Udotq.y; - f2 = sin(v*(float)nb) / sin(v); - f2 = isnan(f2) ? nb : f2; - - /* At exact Bragg condition, f3 = nc */ - v = M_PI*Udotq.z; - f3 = sin(v*(float)nc) / sin(v); - f3 = isnan(f3) ? nc : f3; + /* Look up values from precalculated sinc() table */ + f1 = read_imagef(func_a, sampler_a, (float2)(Udotq.x, 0.0)).s0; + f2 = read_imagef(func_b, sampler_b, (float2)(Udotq.y, 0.0)).s0; + f3 = read_imagef(func_c, sampler_c, (float2)(Udotq.z, 0.0)).s0; - /* 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; } @@ -148,9 +144,12 @@ float2 get_sfac(global float2 *sfacs, float16 cell, float4 q) kernel void diffraction(global float *diff, global float *tt, float klow, int w, float cx, float cy, float res, float clen, float16 cell, - global float2 *sfacs, float4 z, int4 ncells, + global float2 *sfacs, float4 z, int xmin, int ymin, int sampling, local float *tmp, - float kstep) + float kstep, + read_only image2d_t func_a, + read_only image2d_t func_b, + read_only image2d_t func_c) { float ttv; const int x = get_global_id(0) + (xmin*sampling); @@ -169,7 +168,7 @@ kernel void diffraction(global float *diff, global float *tt, float klow, /* Calculate value */ q = get_q(x, y, cx, cy, res, clen, k, &ttv, z, sampling); - f_lattice = lattice_factor(cell, q, ncells); + f_lattice = lattice_factor(cell, q, func_a, func_b, func_c); f_molecule = get_sfac(sfacs, cell, q); /* Write the value to local memory */ |