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@ -59,4 +59,4 @@ docs/_build/
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target/
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# PyCharm
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.idea
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.idea/
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22
README.md
22
README.md
@ -19,7 +19,7 @@ Bloch boundary conditions are not included but wouldn't be very hard to add.
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The default solver (opencl_fdfd.cg_solver(...)) located in main.py implements
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the E-field wave operator directly (ie, as a list of OpenCL instructions
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rather than a matrix). Additionally, there is a slower (and slightly more
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versatile) sovler in csr.py which attempts to solve an arbitrary sparse
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versatile) solver in csr.py which attempts to solve an arbitrary sparse
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matrix in compressed sparse row (CSR) format using the same conjugate gradient
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method as the default solver. The CSR solver is significantly slower, but can
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be very useful for testing alternative formulations of the FDFD wave equation.
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@ -29,9 +29,29 @@ generalization to multiple GPUs should be pretty straightforward
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(ie, just copy over edge values during the matrix multiplication step).
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## Installation
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**Dependencies:**
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* python 3 (written and tested with 3.5)
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* numpy
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* pyopencl
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* jinja2
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* [fdfd_tools](https://mpxd.net/gogs/jan/fdfd_tools)
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Install with pip, via git:
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```bash
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pip install git+https://mpxd.net/gogs/jan/opencl_fdfd.git@release
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```
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## Use
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See the documentation for opencl_fdfd.cg_solver(...)
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(located in main.py) for details about how to call the solver.
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An alternate (slower) FDFD solver and a general gpu-based sparse matrix
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solver is available in csr.py . These aren't particularly well-optimized,
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and something like [MAGMA](http://icl.cs.utk.edu/magma/index.html) would
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probably be a better choice if you absolutely need to solve arbitrary
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sparse matrices and can tolerate writing and compiling C/C++ code.
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@ -19,7 +19,7 @@
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The default solver (opencl_fdfd.cg_solver(...)) located in main.py implements
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the E-field wave operator directly (ie, as a list of OpenCL instructions
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rather than a matrix). Additionally, there is a slower (and slightly more
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versatile) sovler in csr.py which attempts to solve an arbitrary sparse
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versatile) solver in csr.py which attempts to solve an arbitrary sparse
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matrix in compressed sparse row (CSR) format using the same conjugate gradient
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method as the default solver. The CSR solver is significantly slower, but can
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be very useful for testing alternative formulations of the FDFD wave equation.
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@ -1,3 +1,19 @@
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"""
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Sparse matrix solvers
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This file holds the sparse matrix solvers, as well as the
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CSRMatrix sparse matrix representation.
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The FDFD solver (fdfd_cg_solver()) solves an FDFD problem by
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creating a sparse matrix representing the problem (using
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fdfd_tools) and then passing it to cg(), which performs a
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conjugate gradient solve.
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cg() is capable of solving arbitrary sparse matrices which
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satisfy the constraints for the 'conjugate gradient' algorithm
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(positive definite, symmetric) and some that don't.
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"""
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from typing import List, Dict, Any
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import time
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@ -133,7 +149,7 @@ def cg(a: 'scipy.sparse.csr_matrix',
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return x
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def cg_solver(omega: complex,
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def fdfd_cg_solver(omega: complex,
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dxes: List[List[numpy.ndarray]],
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J: numpy.ndarray,
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epsilon: numpy.ndarray,
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@ -1,3 +1,11 @@
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"""
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Default FDFD solver
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This file holds the default FDFD solver, which uses an E-field wave
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operator implemented directly as OpenCL arithmetic (rather than as
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a matrix).
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"""
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from typing import List
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import time
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@ -1,3 +1,12 @@
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"""
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Basic PyOpenCL operations
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The functions are mostly concerned with creating and compiling OpenCL
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kernels for use by the other solvers.
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See kernels/ for any of the .cl files loaded in this file.
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"""
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from typing import List, Callable
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import numpy
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@ -8,6 +17,7 @@ import pyopencl.array
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from pyopencl.elementwise import ElementwiseKernel
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from pyopencl.reduction import ReductionKernel
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# Create jinja2 env on module load
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jinja_env = jinja2.Environment(loader=jinja2.PackageLoader(__name__, 'kernels'))
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