Presentation is loading. Please wait.

Presentation is loading. Please wait.

Implementation of Voxel Volume Projection Operators Using CUDA Applications to Iterative Cone-Beam CT reconstruction.

Similar presentations

Presentation on theme: "Implementation of Voxel Volume Projection Operators Using CUDA Applications to Iterative Cone-Beam CT reconstruction."— Presentation transcript:

1 Implementation of Voxel Volume Projection Operators Using CUDA Applications to Iterative Cone-Beam CT reconstruction

2 Three questions to keep in mind during the presentation 1.Name three differences between the GPU and CPU contributing to the observed performance improvements. 2.Scattered accumulation (a[ix] = a[ix] + b) can result in reduced performance and unexpected results in CUDA. Why? Please state two possible problems! 3.Suppose that each thread in a CUDA program is responsible for writing to one unique output element. Give one possible solution for handling odd sized output data.

3 What are voxel volume projectors? Object: f Projection data: p (line integrals through f) Forward projection: P, mapping f to p Backprojection: P T, mapping p to f X-ray source Detector f p

4 The tomography problem Given p, find an image/volume f, such that the difference between Pf and p is small in some sense, e.g. z(f)=||Pf-p|| 2 attains a minimum. Steepest descent approach: – Gradient: z(f)=2P T (Pf-p) – Update step: f k+1 =f k -2 P T (Pf k -p) We use this method only for illustration of why P and P T are needed. In practice, faster and better regularized methods are needed.

5 Why implement P and P T on the GPU? Reasonable sizes of f and p are around 2GB, implying a size of 2GBx2GB for P and P T. Although these matrices are sparse, the number of nonzero elements is approximately 2000GB, i.e., matrix-vector products involving these matrices are computationally demanding. The GPU offers many solutions that help speeding up the computations: – Massive parallelism – Hardware linear interpolation – Very high memory bandwidth – Texture caches optimized for 2D locality

6 The Joseph forward projector [1] Illustration in the 2D case: Generalization to 3D is straightforward. Instead of linear intepolation, bilinear interpolation is used. [1] Joseph, P. M., An improved algorithm for reprojecting rays through pixel images, IEEE Transactions on Medical Imaging, 1982, MI-1, L x0x0 x1x1 x2x2 x3x3 p i = L (x 0 +x 1 +x 2 +x 3 )

7 Implementation sketch for P We choose to let one thread correspond to one ray. For each ray/thread: 1.Determine the ray origin and direction. 2.Determine the ray and voxel volume intersection. 3.Step along the ray and accumulate values from the voxel volume, using the 3D-texture cache. 4.Multiply with L and store to output element.

8 Handling of odd detector sizes The x-ray detector is divided into 2D blocks corresponding to CUDA thread blocks, using a static block size (16x2). To handle the case with detector dimensions not divisible with the block size, conditional statements were used: Although this reduces efficiency due to divergent programs, the reduction is small for detectors with reasonably large number of channels and rows. // Return if outside detector if (rowIx>=Nrows) return; if (chIx>=Nch) return;

9 Implementation details 1 Calc. of source and detector positions // Calculate focus center and displacement vectors float alpha = theta + D_ALPHA(chIx); float3 fc = make_float3(Rf*cos(alpha), Rf*sin(alpha), z0+D_Z(chIx)); float3 fw = make_float3(-sin(alpha), cos(alpha), 0.f); float3 fh = make_float3(-cos(alpha)*sin(aAngle), -sin(alpha)*sin(aAngle), cos(aAngle)); // Calculate detector center and displacement vectors float3 dc = fc + (Rf+Rd) * make_float3(-cos(theta), -sin(theta), D_SLOPE(rowIx)); float3 dw = make_float3(sin(theta), -cos(theta), 0.f); float3 dh = make_float3(0.f, 0.f, 1.f); // Calculate focus position in texture index coordinates float3 f = ((fc + fOffset.x*fw + fOffset.y*fh) - origin) / spacing; // Calculate detector position in texture index coordinates float3 d = ((dc + dOffset.x*dw + dOffset.y*dh) - origin) / spacing; // Create ray struct Ray ray; ray.o = f; ray.d = normalize(d - f); Code based on NVIDIA CUDA SDK volumeRender

10 Implementation details 2 Accumulation of contributions // Accumulate contributions along ray float dValue = 0; float t = tnear; for(int i=0; i= tfar) break; } // Update detector data value dValue *= length((ray.d*spacing))*tstep; projectionData[rowIx*Nch+chIx] += dValue; Code based on NVIDIA CUDA SDK volumeRender

11 Experiments – forward projection (P) Input data dimensions: 672x24x3000 floats Output data dimensions: 512x512x257 floats Only very small differences in accuracy, without practical implications, occur between CPU and GPU implementations. Calculation times – CPU: 2500 s – GPU: 47 s Speed up factor: approximately 50x For a larger collection of problems, speedups between 20x and 50x have been observed.

12 Efficient implementation of the exact adjoint operator P T is much trickier, why? 2D illustration of the procedure: Same interpolation coefficients as for P, but with scattered accumulation instead of reading. No hardware interpolation. No 2D/3D textures. New parallelization setup is needed. One ray/one thread leads to corrupted results. pipi

13 One slow but exact implementation for the exact transpose of P Let one thread represent only one accumulation from a ray, i.e., – calculation of position in voxel volume. – calculation and multiplication with interpolation coefficients. – accumulation to the 4 voxels closest to the active ray/voxel volume plane intersection. Very short, and very many rays threads. One thread block represents a number of rays, separated so that conflicting updates do not occur: Block 0Block 1Block 2...

14 Experiments – backprojection (P T ) Input data dimensions: 512x512x257 floats Output data dimensions: 672x24x3000 floats Calculation times – CPU: 2700 s – GPU: 700 s Speed up factor: approximately 4x For a larger collection of problems, speedups between 4x and 8x have been observed.

15 Approximate implementation of the adjoint operator P T Bilinear interpolation on the detector. 2D-illustration: Parallelization is now accomplished by letting one pixel correspond to one thread. This method is approximate since the interpolation coefficients generally are different from those of P T.

16 Performance comparison Approximate versus exact P T operator Calculation times – CPU P T : 2700s – GPU P T (exact): 700s – GPU P T (approximate): 60s Axial images of Head phantom reconstructions (25HU-75HU): ExactApproximate

17 Conclusions and future research For operations such as P and P T, speedups of 4x to 50x can be obtained. The amount of speedup is highly dependent on – The possibility to efficiently read memory (coalesced or by the use of texture caches / constant memory). – The possibility to use hardware interpolation – Complexity of the kernel. Using too many registers slows down the program. Lookup tables in constant memory can help reducing the amount of registers. Although scattered write is supported by CUDA, for these problemes, it did not seem good to use it from a performance point of view. Note that this prohibits using cudaArray textures. Remark: Even if the approximate P T operator give a bad result in the example given here, there are other situations where the exact operator is superior. It is therefore of interest to find better approximations.

Download ppt "Implementation of Voxel Volume Projection Operators Using CUDA Applications to Iterative Cone-Beam CT reconstruction."

Similar presentations

Ads by Google