Revert "Add restrict keyword to pointers (not sharing the same memory for multiple fields)"

This reverts commit 60b70bb332.

It appears to have minimal performance impact, and fails to compile on
nvidia cards.

.gitignore

@@ -1,5 +1,9 @@
 .idea/
-__pycache__
 *.h5
-*.pyc
+
+__pycache__
+*.py[cod]
+build/
+dist/
+*.egg-info/
 

README.md

@@ -27,14 +27,16 @@ electromagnetic simulations on parallel compute hardware (mainly GPUs).
 * numpy
 * pyopencl
 * jinja2
+* [fdfd_tools](https://mpxd.net/code/jan/fdfd_tools)
+
+Optional (used for examples):
 * dill (for file output)
-* [gridlock](https://mpxd.net/gogs/jan/gridlock)
-* [masque](https://mpxd.net/gogs/jan/masque)
-* [fdfd_tools](https://mpxd.net/gogs/jan/fdfd_tools)
+* [gridlock](https://mpxd.net/code/jan/gridlock)
+* [masque](https://mpxd.net/code/jan/masque)
 
 To get the code, just clone this repository:
 ```bash
-git clone https://mpxd.net/gogs/jan/opencl_fdtd.git
+git clone https://mpxd.net/code/jan/opencl_fdtd.git
 ```
 
 You can install the requirements and their dependencies easily with

fdtd.py

@@ -6,12 +6,13 @@ See main() for simulation setup.
 
 import sys
 import time
+import logging
 
 import numpy
-import lzma 
+import lzma
 import dill
 
-from fdtd.simulation import Simulation
+from opencl_fdtd import Simulation
 from masque import Pattern, shapes
 import gridlock
 import pcgen
@@ -20,6 +21,9 @@ import fdfd_tools
 
 __author__ = 'Jan Petykiewicz'
 
+logging.basicConfig(level=logging.DEBUG)
+logger = logging.getLogger(__name__)
+
 
 def perturbed_l3(a: float, radius: float, **kwargs) -> Pattern:
     """
@@ -120,9 +124,13 @@ def main():
                        eps=n_air**2,
                        polygons=mask.as_polygons())
 
-    print('grid shape: {}'.format(grid.shape))
+    logger.info('grid shape: {}'.format(grid.shape))
     # #### Create the simulation grid ####
-    sim = Simulation(grid.grids, do_poynting=True, pml_thickness=8)
+    pmls = [{'axis': a, 'polarity': p, 'thickness': pml_thickness}
+            for a in 'xyz' for p in 'np']
+    #bloch = [{'axis': a, 'real': 1, 'imag': 0} for a in 'x']
+    bloch = []
+    sim = Simulation(grid.grids, do_poynting=True, pmls=pmls, bloch_boundaries=bloch)
 
     # Source parameters and function
     w = 2 * numpy.pi * dx / wl
@@ -133,31 +141,41 @@ def main():
     def field_source(i):
         t0 = i * sim.dt - delay
         return numpy.sin(w * t0) * numpy.exp(-alpha * t0**2)
-   
+
     with open('sources.c', 'w') as f:
         f.write(sim.sources['E'])
-        f.write('\n==========================================\n')
+        f.write('\n====================H======================\n')
         f.write(sim.sources['H'])
         if sim.update_S:
-            f.write('\n==========================================\n')
+            f.write('\n=====================S=====================\n')
             f.write(sim.sources['S'])
+        if bloch:
+            f.write('\n=====================F=====================\n')
+            f.write(sim.sources['F'])
+            f.write('\n=====================G=====================\n')
+            f.write(sim.sources['G'])
 
     # #### Run a bunch of iterations ####
     # event = sim.whatever([prev_event]) indicates that sim.whatever should be queued
     #  immediately and run once prev_event is finished.
     start = time.perf_counter()
     for t in range(max_t):
-        sim.update_E([]).wait()
+        e = sim.update_E([])
+        if bloch:
+            e = sim.update_F([e])
+        e.wait()
 
         ind = numpy.ravel_multi_index(tuple(grid.shape//2), dims=grid.shape, order='C') + numpy.prod(grid.shape)
         sim.E[ind] += field_source(t)
         e = sim.update_H([])
+        if bloch:
+            e = sim.update_G([e])
         if sim.update_S:
             e = sim.update_S([e])
         e.wait()
 
         if t % 100 == 0:
-            print('iteration {}: average {} iterations per sec'.format(t, (t+1)/(time.perf_counter()-start)))
+            logger.info('iteration {}: average {} iterations per sec'.format(t, (t+1)/(time.perf_counter()-start)))
             sys.stdout.flush()
 
     with lzma.open('saved_simulation', 'wb') as f:
@@ -172,5 +190,6 @@ def main():
             d['S'] = unvec(sim.S.get())
         dill.dump(d, f)
 
+
 if __name__ == '__main__':
     main()

fdtd/kernels/update_e.cl

@@ -1,78 +0,0 @@
-/*
- *  Update E-field, including any PMLs.
- *  
- *  Template parameters:
- *   common_header: Rendered contents of common.cl
- *   pmls: [('x', 'n'), ('z', 'p'),...] list of pml axes and polarities
- *   pml_thickness: Number of cells (integer)
- *   
- *  OpenCL args:
- *   E, H, dt, eps, [p{01}e{np}, Psi_{xyz}{np}_E]
- */
-
-{{common_header}}
-
-////////////////////////////////////////////////////////////////////////////
-
-__global ftype *epsx = eps + XX;
-__global ftype *epsy = eps + YY;
-__global ftype *epsz = eps + ZZ;
-
-{% if pmls -%}
-const int pml_thickness = {{pml_thickness}};
-{%- endif %}
-
-/*
- *   Precalclate derivatives
- */
-ftype dHxy = Hx[i] - Hx[i + my];
-ftype dHxz = Hx[i] - Hx[i + mz];
-
-ftype dHyx = Hy[i] - Hy[i + mx];
-ftype dHyz = Hy[i] - Hy[i + mz];
-
-ftype dHzx = Hz[i] - Hz[i + mx];
-ftype dHzy = Hz[i] - Hz[i + my];
-
-/*
- *   PML Update
- */
-// PML effects on E
-ftype pExi = 0;
-ftype pEyi = 0;
-ftype pEzi = 0;
-
-{% for r, p in pmls -%}
-    {%- set u, v = ['x', 'y', 'z'] | reject('equalto', r) -%}
-    {%- set psi = 'Psi_' ~ r ~ p ~ '_E' -%}
-    {%- if r != 'y' -%}
-        {%- set se, sh = '-', '+' -%}
-    {%- else -%}
-        {%- set se, sh = '+', '-' -%}
-    {%- endif -%}
-
-    {%- if p == 'n' %}
-
-if ( {{r}} < pml_thickness ) {
-    const size_t ir = {{r}};                          // index into pml parameters
-
-    {%- elif p == 'p' %}
-
-if ( s{{r}} > {{r}} && {{r}} >= s{{r}} - pml_thickness ) {
-    const size_t ir = (s{{r}} - 1) - {{r}};                     // index into pml parameters
-
-    {%- endif %}
-    const size_t ip = {{v}} + {{u}} * s{{v}} + ir * s{{v}} * s{{u}};  // linear index into Psi
-    {{psi ~ u}}[ip] = p0e{{p}}[ir] * {{psi ~ u}}[ip] + p1e{{p}}[ir] * dH{{v ~ r}};
-    {{psi ~ v}}[ip] = p0e{{p}}[ir] * {{psi ~ v}}[ip] + p1e{{p}}[ir] * dH{{u ~ r}};
-    pE{{u}}i {{se}}= {{psi ~ u}}[ip];
-    pE{{v}}i {{sh}}= {{psi ~ v}}[ip];
-}
-{%- endfor %}
-
-/*
- *  Update E
- */
-Ex[i] += dt / epsx[i] * (dHzy - dHyz + pExi);
-Ey[i] += dt / epsy[i] * (dHxz - dHzx + pEyi);
-Ez[i] += dt / epsz[i] * (dHyx - dHxy + pEzi);

fdtd/simulation.py

@@ -1,238 +0,0 @@
-"""
-Class for constructing and holding the basic FDTD operations and fields
-"""
-
-from typing import List, Dict, Callable
-from collections import OrderedDict
-import numpy
-import jinja2
-import warnings
-
-import pyopencl
-import pyopencl.array
-from pyopencl.elementwise import ElementwiseKernel
-
-from fdfd_tools import vec
-
-
-__author__ = 'Jan Petykiewicz'
-
-
-# Create jinja2 env on module load
-jinja_env = jinja2.Environment(loader=jinja2.PackageLoader(__name__, 'kernels'))
-
-
-class Simulation(object):
-    """
-    Constructs and holds the basic FDTD operations and related fields
-    """
-    E = None    # type: List[pyopencl.array.Array]
-    H = None    # type: List[pyopencl.array.Array]
-    S = None    # type: List[pyopencl.array.Array]
-    eps = None  # type: List[pyopencl.array.Array]
-    dt = None   # type: float
-
-    arg_type = None     # type: numpy.float32 or numpy.float64
-
-    context = None      # type: pyopencl.Context
-    queue = None        # type: pyopencl.CommandQueue
-
-    update_E = None     # type: Callable[[],pyopencl.Event]
-    update_H = None     # type: Callable[[],pyopencl.Event]
-    update_S = None     # type: Callable[[],pyopencl.Event]
-    sources = None      # type: Dict[str, str]
-
-    def __init__(self,
-                 epsilon: List[numpy.ndarray],
-                 dt: float = .99/numpy.sqrt(3),
-                 initial_E: List[numpy.ndarray] = None,
-                 initial_H: List[numpy.ndarray] = None,
-                 context: pyopencl.Context = None,
-                 queue: pyopencl.CommandQueue = None,
-                 float_type: numpy.float32 or numpy.float64 = numpy.float32,
-                 pml_thickness: int = 10,
-                 pmls: List[List[str]] = None,
-                 do_poynting: bool = True):
-        """
-        Initialize the simulation.
-
-        :param epsilon: List containing [eps_r,xx, eps_r,yy, eps_r,zz], where each element is a Yee-shifted ndarray
-                spanning the simulation domain. Relative epsilon is used.
-        :param dt: Time step. Default is the Courant factor.
-        :param initial_E: Initial E-field (default is 0 everywhere). Same format as epsilon.
-        :param initial_H: Initial H-field (default is 0 everywhere). Same format as epsilon.
-        :param context: pyOpenCL context. If not given, pyopencl.create_some_context(False) is called.
-        :param queue: pyOpenCL command queue. If not given, pyopencl.CommandQueue(context) is called.
-        :param float_type: numpy.float32 or numpy.float64. Default numpy.float32.
-        """
-
-        if len(epsilon) != 3:
-            Exception('Epsilon must be a list with length of 3')
-        if not all((e.shape == epsilon[0].shape for e in epsilon[1:])):
-            Exception('All epsilon grids must have the same shape. Shapes are {}', [e.shape for e in epsilon])
-
-        if context is None:
-            self.context = pyopencl.create_some_context()
-        else:
-            self.context = context
-
-        if queue is None:
-            self.queue = pyopencl.CommandQueue(self.context)
-        else:
-            self.queue = queue
-
-        if dt > .99/numpy.sqrt(3):
-            warnings.warn('Warning: unstable dt: {}'.format(dt))
-        elif dt <= 0:
-            raise Exception('Invalid dt: {}'.format(dt))
-        else:
-            self.dt = dt
-
-        self.arg_type = float_type
-        self.sources = {}
-        self.eps = pyopencl.array.to_device(self.queue, vec(epsilon).astype(float_type))
-
-        if initial_E is None:
-            self.E = pyopencl.array.zeros_like(self.eps)
-        else:
-            if len(initial_E) != 3:
-                Exception('Initial_E must be a list of length 3')
-            if not all((E.shape == epsilon[0].shape for E in initial_E)):
-                Exception('Initial_E list elements must have same shape as epsilon elements')
-            self.E = pyopencl.array.to_device(self.queue, vec(E).astype(float_type))
-
-        if initial_H is None:
-            self.H = pyopencl.array.zeros_like(self.eps)
-        else:
-            if len(initial_H) != 3:
-                Exception('Initial_H must be a list of length 3')
-            if not all((H.shape == epsilon[0].shape for H in initial_H)):
-                Exception('Initial_H list elements must have same shape as epsilon elements')
-            self.H = pyopencl.array.to_device(self.queue, vec(H).astype(float_type))
-
-        if pmls is None:
-            pmls = [[d, p] for d in 'xyz' for p in 'np']
-
-        ctype = type_to_C(self.arg_type)
-
-        def ptr(arg: str) -> str:
-            return ctype + ' *' + arg
-
-        base_fields = OrderedDict()
-        base_fields[ptr('E')] = self.E
-        base_fields[ptr('H')] = self.H
-        base_fields[ctype + ' dt'] = self.dt
-
-        eps_field = OrderedDict()
-        eps_field[ptr('eps')] = self.eps
-
-        common_source = jinja_env.get_template('common.cl').render(
-                ftype=ctype,
-                shape=epsilon[0].shape,
-                )
-        jinja_args = {
-                'common_header': common_source,
-                'pml_thickness': pml_thickness,
-                'pmls': pmls,
-                'do_poynting': do_poynting,
-                }
-        E_source = jinja_env.get_template('update_e.cl').render(**jinja_args)
-        H_source = jinja_env.get_template('update_h.cl').render(**jinja_args)
-
-        self.sources['E'] = E_source
-        self.sources['H'] = H_source
-
-        if do_poynting:
-            S_source = jinja_env.get_template('update_s.cl').render(**jinja_args)
-            self.sources['S'] = S_source
-
-            self.oS = pyopencl.array.zeros(self.queue, self.E.shape + (2,), dtype=float_type)
-            self.S = pyopencl.array.zeros_like(self.E)
-            S_fields = OrderedDict()
-            S_fields[ptr('oS')] = self.oS
-            S_fields[ptr('S')] = self.S
-        else:
-            S_fields = OrderedDict() 
-
-        '''
-        PML
-        '''
-        m = (3.5, 1)
-        sigma_max = 0.8 * (m[0] + 1) / numpy.sqrt(1.0) # TODO: epsilon_eff (not 1.0)
-        alpha_max = 0  # TODO: Decide what to do about non-zero alpha
-
-        def par(x):
-            sigma = ((x / pml_thickness) ** m[0]) * sigma_max
-            alpha = ((1 - x / pml_thickness) ** m[1]) * alpha_max
-            p0 = numpy.exp(-(sigma + alpha) * dt)
-            p1 = sigma / (sigma + alpha) * (p0 - 1)
-            return p0, p1
-        
-        xen, xep, xhn, xhp = (numpy.arange(1, pml_thickness + 1, dtype=float_type)[::-1] for _ in range(4))
-        xep -= 0.5
-        xhn -= 0.5
-
-        pml_p_names = [['p' + a + eh + np for np in 'np' for a in '01'] for eh in 'eh']
-        pml_e_fields = OrderedDict()
-        pml_h_fields = OrderedDict()
-        for ne, nh, pe, ph in zip(*pml_p_names, par(xen) + par(xep), par(xhn) + par(xhp)):
-            pml_e_fields[ptr(ne)] = pyopencl.array.to_device(self.queue, pe)
-            pml_h_fields[ptr(nh)] = pyopencl.array.to_device(self.queue, ph)
-
-        for pml in pmls:
-            uv = 'xyz'.replace(pml[0], '')
-            psi_base = 'Psi_' + ''.join(pml) + '_'
-            psi_names = [[psi_base + eh + c for c in uv] for eh in 'EH']
-
-            psi_shape = list(epsilon[0].shape)
-            psi_shape['xyz'.find(pml[0])] = pml_thickness
-
-            for ne, nh in zip(*psi_names):
-                pml_e_fields[ptr(ne)] = pyopencl.array.zeros(self.queue, tuple(psi_shape), dtype=self.arg_type)
-                pml_h_fields[ptr(nh)] = pyopencl.array.zeros(self.queue, tuple(psi_shape), dtype=self.arg_type)
-        
-        self.pml_e_fields = pml_e_fields
-        self.pml_h_fields = pml_h_fields
-
-
-        '''
-        Create operations
-        '''
-        E_args = OrderedDict()
-        [E_args.update(d) for d in (base_fields, eps_field, pml_e_fields)]
-        E_update = ElementwiseKernel(self.context, operation=E_source,
-                                     arguments=', '.join(E_args.keys()))
-
-        H_args = OrderedDict()
-        [H_args.update(d) for d in (base_fields, pml_h_fields, S_fields)]
-        H_update = ElementwiseKernel(self.context, operation=H_source,
-                                     arguments=', '.join(H_args.keys()))
-        self.update_E = lambda e: E_update(*E_args.values(), wait_for=e)
-        self.update_H = lambda e: H_update(*H_args.values(), wait_for=e)
-
-        if do_poynting:
-            S_args = OrderedDict()
-            [S_args.update(d) for d in (base_fields, S_fields)]
-            S_update = ElementwiseKernel(self.context, operation=S_source,
-                                         arguments=', '.join(S_args.keys()))
-
-            self.update_S = lambda e: S_update(*S_args.values(), wait_for=e)
-
-
-def type_to_C(float_type) -> str:
-    """
-    Returns a string corresponding to the C equivalent of a numpy type.
-    Only works for float16, float32, float64.
-
-    :param float_type: e.g. numpy.float32
-    :return: string containing the corresponding C type (eg. 'double')
-    """
-    if float_type == numpy.float16:
-        arg_type = 'half'
-    elif float_type == numpy.float32:
-        arg_type = 'float'
-    elif float_type == numpy.float64:
-        arg_type = 'double'
-    else:
-        raise Exception('Unsupported type')
-    return arg_type

opencl_fdtd/__init__.py

@@ -0,0 +1,5 @@
+from .simulation import Simulation, type_to_C
+
+__author__ = 'Jan Petykiewicz'
+
+version = '0.4'

opencl_fdtd/kernels/common.cl

@@ -2,7 +2,7 @@
 /* Common code for E, H updates
  *
  * Template parameters:
- *  ftype	type name (e.g. float or double)
+ *  ftype       type name (e.g. float or double)
  *  shape       list of 3 ints specifying shape of fields
  */
 #}
@@ -73,12 +73,13 @@ __global ftype *Hz = H + ZZ;
  * the cell x_{+1} == 0 instead, ie. px = -(sx - 1) * dix .
  */
 {% for r in 'xyz' %}
-int m{{r}} = -di{{r}};
-int p{{r}} = +di{{r}};
-int wrap_{{r}} = (s{{r}} - 1) * di{{r}};
+int m{{r}} = - (int) di{{r}};
+int p{{r}} = + (int) di{{r}};
+int wrap_{{r}} = (s{{r}} - 1) * (int) di{{r}};
 if ( {{r}} == 0 ) {
   m{{r}} = wrap_{{r}};
-} else if ( {{r}} == s{{r}} - 1 ) {
+}
+if ( {{r}} == s{{r}} - 1 ) {
   p{{r}} = -wrap_{{r}};
-} 
+}
 {% endfor %}

opencl_fdtd/kernels/update_e.cl

@@ -0,0 +1,107 @@
+/*
+ *  Update E-field, including any PMLs.
+ *
+ *  Template parameters:
+ *   common_header: Rendered contents of common.cl
+ *   pmls: [{'axis': 'x', 'polarity': 'n', 'thickness': 8}, ...] list of pml dicts containing
+ *      axes, polarities, and thicknesses.
+ *   uniform_dx: If grid is uniform, uniform_dx should be the grid spacing.
+ *      Otherwise, uniform_dx should be False and [inv_dh{xyz}] arrays must be supplied as
+ *      OpenCL args.
+ *
+ *  OpenCL args:
+ *   E, H, dt, eps, [p{012}e{np}, Psi_{xyz}{np}_E], [inv_dh{xyz}]
+ */
+
+{{common_header}}
+
+////////////////////////////////////////////////////////////////////////////
+
+__global ftype *epsx = eps + XX;
+__global ftype *epsy = eps + YY;
+__global ftype *epsz = eps + ZZ;
+
+
+{%- if uniform_dx %}
+ftype inv_dx = 1.0 / {{uniform_dx}};
+ftype inv_dy = 1.0 / {{uniform_dx}};
+ftype inv_dz = 1.0 / {{uniform_dx}};
+{%- else %}
+ftype inv_dx = inv_dhx[x];
+ftype inv_dy = inv_dhy[y];
+ftype inv_dz = inv_dhz[z];
+{%- endif %}
+
+
+/*
+ *   Precalculate derivatives
+ */
+ftype dHxy = (Hx[i] - Hx[i + my]) * inv_dy;
+ftype dHxz = (Hx[i] - Hx[i + mz]) * inv_dz;
+
+ftype dHyx = (Hy[i] - Hy[i + mx]) * inv_dx;
+ftype dHyz = (Hy[i] - Hy[i + mz]) * inv_dz;
+
+ftype dHzx = (Hz[i] - Hz[i + mx]) * inv_dx;
+ftype dHzy = (Hz[i] - Hz[i + my]) * inv_dy;
+
+{% for bloch in bloch_boundaries -%}
+    {%- set r = bloch['axis'] -%}
+    {%- set u, v = ['x', 'y', 'z'] | reject('equalto', r) -%}
+if ({{r}} == 0) {
+    ftype bloch_im = {{bloch['real']}};
+    ftype bloch_re = {{bloch['imag']}};
+    dH{{u ~ r}} = bloch_re * dH{{v ~ r}} + bloch_im * (G{{u}}[i] - G{{u}}[i + m{{u}}]);
+    dH{{v ~ r}} = bloch_re * dH{{v ~ r}} + bloch_im * (G{{v}}[i] - G{{v}}[i + m{{v}}]);
+}
+{%- endfor %}
+
+
+/*
+ *   PML Update
+ */
+// PML effects on E
+ftype pExi = 0;
+ftype pEyi = 0;
+ftype pEzi = 0;
+
+{% for pml in pmls -%}
+    {%- set r = pml['axis'] -%}
+    {%- set p = pml['polarity'] -%}
+    {%- set u, v = ['x', 'y', 'z'] | reject('equalto', r) -%}
+    {%- set psi = 'Psi_' ~ r ~ p ~ '_E' -%}
+    {%- if r != 'y' -%}
+        {%- set se, sh = '-', '+' -%}
+    {%- else -%}
+        {%- set se, sh = '+', '-' -%}
+    {%- endif -%}
+
+int pml_{{r ~ p}}_thickness = {{pml['thickness']}};
+
+    {%- if p == 'n' %}
+
+if ( {{r}} < pml_{{r ~ p}}_thickness ) {
+    const size_t ir = {{r}};                          // index into pml parameters
+
+    {%- elif p == 'p' %}
+
+if ( s{{r}} > {{r}} && {{r}} >= s{{r}} - pml_{{r ~ p}}_thickness ) {
+    const size_t ir = (s{{r}} - 1) - {{r}};                     // index into pml parameters
+
+    {%- endif %}
+    const size_t ip = {{v}} + {{u}} * s{{v}} + ir * s{{v}} * s{{u}};  // linear index into Psi
+    dH{{v ~ r}} *= p{{r}}2e{{p}}[ir];
+    dH{{u ~ r}} *= p{{r}}2e{{p}}[ir];
+    {{psi ~ u}}[ip] = p{{r}}0e{{p}}[ir] * {{psi ~ u}}[ip] + p{{r}}1e{{p}}[ir] * dH{{v ~ r}};
+    {{psi ~ v}}[ip] = p{{r}}0e{{p}}[ir] * {{psi ~ v}}[ip] + p{{r}}1e{{p}}[ir] * dH{{u ~ r}};
+    pE{{u}}i {{se}}= {{psi ~ u}}[ip];
+    pE{{v}}i {{sh}}= {{psi ~ v}}[ip];
+}
+{%- endfor %}
+
+/*
+ *  Update E
+ */
+Ex[i] += dt / epsx[i] * (dHzy - dHyz + pExi);
+Ey[i] += dt / epsy[i] * (dHxz - dHzx + pEyi);
+Ez[i] += dt / epsz[i] * (dHyx - dHxy + pEzi);

opencl_fdtd/kernels/update_h.cl

@@ -1,36 +1,58 @@
 /*
  *  Update H-field, including any PMLs.
  *   Also precalculate values for poynting vector if necessary.
- *  
+ *
  *  Template parameters:
  *   common_header: Rendered contents of common.cl
- *   pmls: [('x', 'n'), ('z', 'p'),...] list of pml axes and polarities
- *   pml_thickness: Number of cells (integer)
- *   do_poynting: Whether to precalculate poynting vector components (boolean)  
+ *   pmls: [{'axis': 'x', 'polarity': 'n', 'thickness': 8}, ...] list of pml dicts containing
+ *      axes, polarities, and thicknesses.
+ *   do_poynting: Whether to precalculate poynting vector components (boolean)
+ *   uniform_dx: If grid is uniform, uniform_dx should be the grid spacing.
+ *      Otherwise, uniform_dx should be False and [inv_de{xyz}] arrays must be supplied as
+ *      OpenCL args.
  *
  *  OpenCL args:
- *   E, H, dt, [p{01}h{np}, Psi_{xyz}{np}_H], [oS]
+ *   E, H, dt, [inv_de{xyz}], [p{xyz}{01}h{np}, Psi_{xyz}{np}_H], [oS]
  */
 
 {{common_header}}
 
 ////////////////////////////////////////////////////////////////////////////
 
-{% if pmls -%}
-const int pml_thickness = {{pml_thickness}};
-{%- endif %}
-
 /*
  *  Precalculate derivatives
  */
-ftype dExy = Ex[i + py] - Ex[i];
-ftype dExz = Ex[i + pz] - Ex[i];
+{%- if uniform_dx %}
+ftype inv_dx = 1.0 / {{uniform_dx}};
+ftype inv_dy = 1.0 / {{uniform_dx}};
+ftype inv_dz = 1.0 / {{uniform_dx}};
+{%- else %}
+ftype inv_dx = inv_dex[x];
+ftype inv_dy = inv_dey[y];
+ftype inv_dz = inv_dez[z];
+{%- endif %}
 
-ftype dEyx = Ey[i + px] - Ey[i];
-ftype dEyz = Ey[i + pz] - Ey[i];
 
-ftype dEzx = Ez[i + px] - Ez[i];
-ftype dEzy = Ez[i + py] - Ez[i];
+ftype dExy = (Ex[i + py] - Ex[i]) * inv_dy;
+ftype dExz = (Ex[i + pz] - Ex[i]) * inv_dz;
+
+ftype dEyx = (Ey[i + px] - Ey[i]) * inv_dx;
+ftype dEyz = (Ey[i + pz] - Ey[i]) * inv_dz;
+
+ftype dEzx = (Ez[i + px] - Ez[i]) * inv_dx;
+ftype dEzy = (Ez[i + py] - Ez[i]) * inv_dy;
+
+
+{% for bloch in bloch_boundaries -%}
+    {%- set r = bloch['axis'] -%}
+    {%- set u, v = ['x', 'y', 'z'] | reject('equalto', r) -%}
+if ({{r}} == s{{r}} - 1) {
+    ftype bloch_re = {{bloch['real']}};
+    ftype bloch_im = {{bloch['imag']}};
+    dE{{u ~ r}} = bloch_re * dE{{u ~ r}} + bloch_im * (F{{u}}[i + p{{u}}] - F{{u}}[i]);
+    dE{{v ~ r}} = bloch_re * dE{{v ~ r}} + bloch_im * (F{{v}}[i + p{{v}}] - F{{v}}[i]);
+}
+{% endfor -%}
 
 {%- if do_poynting %}
 
@@ -49,6 +71,8 @@ ftype aEzy = Ez[i + py] + Ez[i];
 {%- endif %}
 
 
+
+
 /*
  *  PML Update
  */
@@ -57,29 +81,35 @@ ftype pHxi = 0;
 ftype pHyi = 0;
 ftype pHzi = 0;
 
-{%- for r, p in pmls -%}
+{% for pml in pmls -%}
+    {%- set r = pml['axis'] -%}
+    {%- set p = pml['polarity'] -%}
     {%- set u, v = ['x', 'y', 'z'] | reject('equalto', r) -%}
     {%- set psi = 'Psi_' ~ r ~ p ~ '_H' -%}
     {%- if r != 'y' -%}
         {%- set se, sh = '-', '+' -%}
     {%- else -%}
         {%- set se, sh = '+', '-' -%}
-    {%- endif -%}
+    {%- endif %}
+
+int pml_{{r ~ p}}_thickness = {{pml['thickness']}};
 
     {%- if p == 'n' %}
 
-if ( {{r}} < pml_thickness ) {
+if ( {{r}} < pml_{{r ~ p}}_thickness ) {
     const size_t ir = {{r}};                          // index into pml parameters
 
     {%- elif p == 'p' %}
 
-if ( s{{r}} > {{r}} && {{r}} >= s{{r}} - pml_thickness ) {
+if ( s{{r}} > {{r}} && {{r}} >= s{{r}} - pml_{{r ~ p}}_thickness ) {
     const size_t ir = (s{{r}} - 1) - {{r}};                     // index into pml parameters
 
     {%- endif %}
     const size_t ip = {{v}} + {{u}} * s{{v}} + ir * s{{v}} * s{{u}};  // linear index into Psi
-    {{psi ~ u}}[ip] = p0h{{p}}[ir] * {{psi ~ u}}[ip] + p1h{{p}}[ir] * dE{{v ~ r}};
-    {{psi ~ v}}[ip] = p0h{{p}}[ir] * {{psi ~ v}}[ip] + p1h{{p}}[ir] * dE{{u ~ r}};
+    dE{{v ~ r}} *= p{{r}}2h{{p}}[ir];
+    dE{{u ~ r}} *= p{{r}}2h{{p}}[ir];
+    {{psi ~ u}}[ip] = p{{r}}0h{{p}}[ir] * {{psi ~ u}}[ip] + p{{r}}1h{{p}}[ir] * dE{{v ~ r}};
+    {{psi ~ v}}[ip] = p{{r}}0h{{p}}[ir] * {{psi ~ v}}[ip] + p{{r}}1h{{p}}[ir] * dE{{u ~ r}};
     pH{{u}}i {{sh}}= {{psi ~ u}}[ip];
     pH{{v}}i {{se}}= {{psi ~ v}}[ip];
 }
@@ -96,9 +126,9 @@ ftype Hz_old = Hz[i];
 {%- endif %}
 
 // H update equations
-Hx[i] -= dt * (dEzy - dEyz + pHxi);
-Hy[i] -= dt * (dExz - dEzx + pHyi);
-Hz[i] -= dt * (dEyx - dExy + pHzi);
+Hx[i] -= dt * (dEzy - dEyz - pHxi);
+Hy[i] -= dt * (dExz - dEzx - pHyi);
+Hz[i] -= dt * (dEyx - dExy - pHzi);
 
 {% if do_poynting -%}
 // Average H across timesteps

opencl_fdtd/kernels/update_j.cl

@@ -0,0 +1,32 @@
+/*
+ *  Update E-field from J field
+ *
+ *  Template parameters:
+ *   common_header: Rendered contents of common.cl
+ *
+ *  OpenCL args:
+ *   E, Jr, Ji, c, s, xmin, xmax, ymin, ymax, zmin, zmax
+ */
+
+{{common_header}}
+
+////////////////////////////////////////////////////////////////////////////
+
+__global ftype *Jrx = Jr + XX;
+__global ftype *Jry = Jr + YY;
+__global ftype *Jrz = Jr + ZZ;
+__global ftype *Jix = Ji + XX;
+__global ftype *Jiy = Ji + YY;
+__global ftype *Jiz = Ji + ZZ;
+
+
+if (x < xmin || y < ymin || z < zmin) {
+   PYOPENCL_ELWISE_CONTINUE;
+}
+if (x >= xmax || y >= ymax || z >= zmax) {
+   PYOPENCL_ELWISE_CONTINUE;
+}
+
+Ex[i] += c * Jrx[i] + s * Jix[i];
+Ey[i] += c * Jry[i] + s * Jiy[i];
+Ez[i] += c * Jrz[i] + s * Jiz[i];

opencl_fdtd/kernels/update_s.cl

@@ -1,11 +1,11 @@
 /*
  *  Update E-field, including any PMLs.
- *  
+ *
  *  Template parameters:
  *   common_header: Rendered contents of common.cl
  *   pmls: [('x', 'n'), ('z', 'p'),...] list of pml axes and polarities
  *   pml_thickness: Number of cells (integer)
- *   
+ *
  *  OpenCL args:
  *   E, H, dt, S, oS
  */
@@ -17,12 +17,12 @@
 
 /*
  * Calculate S from oS (pre-calculated components)
- */ 
+ */
 __global ftype *Sx = S + XX;
 __global ftype *Sy = S + YY;
 __global ftype *Sz = S + ZZ;
 
-// Use unscaled S components from H locations 
+// Use unscaled S components from H locations
 __global ftype *oSxy = oS + 0 * field_size;
 __global ftype *oSyz = oS + 1 * field_size;
 __global ftype *oSzx = oS + 2 * field_size;

opencl_fdtd/simulation.py

@@ -0,0 +1,376 @@
+"""
+Class for constructing and holding the basic FDTD operations and fields
+"""
+
+from typing import List, Dict, Callable
+from collections import OrderedDict
+import numpy
+import jinja2
+import warnings
+
+import pyopencl
+import pyopencl.array
+from pyopencl.elementwise import ElementwiseKernel
+
+from fdfd_tools import vec
+
+
+__author__ = 'Jan Petykiewicz'
+
+
+# Create jinja2 env on module load
+jinja_env = jinja2.Environment(loader=jinja2.PackageLoader(__name__, 'kernels'))
+
+
+class Simulation(object):
+    """
+    Constructs and holds the basic FDTD operations and related fields
+
+    After constructing this object, call the (update_E, update_H, update_S) members
+     to perform FDTD updates on the stored (E, H, S) fields:
+
+        pmls = [{'axis': a, 'polarity': p} for a in 'xyz' for p in 'np']
+        sim = Simulation(grid.grids, do_poynting=True, pmls=pmls)
+        with open('sources.c', 'w') as f:
+            f.write('{}'.format(sim.sources))
+
+        for t in range(max_t):
+            sim.update_E([]).wait()
+
+            # Find the linear index for the center point, for Ey
+            ind = numpy.ravel_multi_index(tuple(grid.shape//2), dims=grid.shape, order='C') + \
+                    numpy.prod(grid.shape) * 1
+            # Perturb the field (i.e., add a soft current source)
+            sim.E[ind] += numpy.sin(omega * t * sim.dt)
+            event = sim.update_H([])
+            if sim.update_S:
+                event = sim.update_S([event])
+            event.wait()
+
+            with lzma.open('saved_simulation', 'wb') as f:
+                dill.dump(fdfd_tools.unvec(sim.E.get(), grid.shape), f)
+
+    Code in the form
+        event2 = sim.update_H([event0, event1])
+     indicates that the update_H operation should be prepared immediately, but wait for
+     event0 and event1 to occur (i.e. previous operations to finish) before starting execution.
+     event2 can then be used to prepare further operations to be run after update_H.
+    """
+    E = None            # type: pyopencl.array.Array
+    H = None            # type: pyopencl.array.Array
+    S = None            # type: pyopencl.array.Array
+    eps = None          # type: pyopencl.array.Array
+    dt = None           # type: float
+    inv_dxes = None     # type: List[pyopencl.array.Array]
+
+    arg_type = None     # type: numpy.float32 or numpy.float64
+
+    context = None      # type: pyopencl.Context
+    queue = None        # type: pyopencl.CommandQueue
+
+    update_E = None     # type: Callable[[List[pyopencl.Event]], pyopencl.Event]
+    update_H = None     # type: Callable[[List[pyopencl.Event]], pyopencl.Event]
+    update_S = None     # type: Callable[[List[pyopencl.Event]], pyopencl.Event]
+    update_J = None     # type: Callable[[List[pyopencl.Event]], pyopencl.Event]
+    sources = None      # type: Dict[str, str]
+
+    def __init__(self,
+                 epsilon: List[numpy.ndarray],
+                 pmls: List[Dict[str, int or float]],
+                 bloch_boundaries: List[Dict[str, int or float]] = (),
+                 dxes: List[List[numpy.ndarray]] or float = None,
+                 dt: float = None,
+                 initial_fields: Dict[str, List[numpy.ndarray]] = None,
+                 context: pyopencl.Context = None,
+                 queue: pyopencl.CommandQueue = None,
+                 float_type: numpy.float32 or numpy.float64 = numpy.float32,
+                 do_poynting: bool = True,
+                 do_fieldsrc: bool = False):
+        """
+        Initialize the simulation.
+
+        :param epsilon: List containing [eps_r,xx, eps_r,yy, eps_r,zz], where each element is a Yee-shifted ndarray
+                spanning the simulation domain. Relative epsilon is used.
+        :param pmls: List of dicts with keys:
+            'axis': One of 'x', 'y', 'z'.
+            'direction': One of 'n', 'p'.
+            'thickness': Number of layers, default 8.
+            'epsilon_eff': Effective epsilon to match to. Default 1.0.
+            'mu_eff': Effective mu to match to. Default 1.0.
+            'ln_R_per_layer': Desired (ln(R) / thickness) value. Default -1.6.
+            'm': Polynomial grading exponent. Default 3.5.
+            'ma': Exponent for alpha. Default 1.
+        :param bloch_boundaries: List of dicts with keys:
+            'axis': One of 'x', 'y', 'z'.
+            'real': Real part of bloch phase factor (i.e. real(exp(i * phase)))
+            'imag': Imaginary part of bloch phase factor (i.e. imag(exp(i * phase)))
+        :param dt: Time step. Default is min(dxes) * .99/sqrt(3).
+        :param initial_fields: Dict with optional keys ('E', 'H', 'F', 'G') containing initial values for the
+            specified fields (default is 0 everywhere). Fields have same format as epsilon.
+        :param context: pyOpenCL context. If not given, pyopencl.create_some_context(False) is called.
+        :param queue: pyOpenCL command queue. If not given, pyopencl.CommandQueue(context) is called.
+        :param float_type: numpy.float32 or numpy.float64. Default numpy.float32.
+        :param do_poynting: If true, enables calculation of the poynting vector, S.
+                Poynting vector calculation adds the following computational burdens:
+                    * During update_H, ~6 extra additions/cell are performed in order to spatially
+                        average E and temporally average H. These quantities are multiplied
+                        (6 multiplications/cell) and then stored (6 writes/cell, cache-friendly).
+                    * update_S performs a discrete cross product using the precalculated products
+                        from update_H. This is not nice to the cache and similar to e.g. update_E
+                        in complexity.
+                    * GPU memory requirements are approximately doubled, since S and the intermediate
+                        products must be stored.
+        """
+        if initial_fields is None:
+            initial_fields = {}
+
+        self.shape = epsilon[0].shape
+        self.arg_type = float_type
+        self.sources = {}
+        self._create_context(context, queue)
+        self._create_eps(epsilon)
+
+        if dxes is None:
+            dxes = 1.0
+
+        if isinstance(dxes, (float, int)):
+            uniform_dx = dxes
+            min_dx = dxes
+        else:
+            uniform_dx = False
+            self.inv_dxes = [self._create_field(1 / dxn) for dxn in dxes[0] + dxes[1]]
+            min_dx = min(min(dxn) for dxn in dxes[0] + dxes[1])
+
+        max_dt = min_dx * .99 / numpy.sqrt(3)
+
+        if dt is None:
+            self.dt = max_dt
+        elif dt > max_dt:
+            warnings.warn('Warning: unstable dt: {}'.format(dt))
+        elif dt <= 0:
+            raise Exception('Invalid dt: {}'.format(dt))
+        else:
+            self.dt = dt
+
+        self.E = self._create_field(initial_fields.get('E', None))
+        self.H = self._create_field(initial_fields.get('H', None))
+        if bloch_boundaries:
+            self.F = self._create_field(initial_fields.get('F', None))
+            self.G = self._create_field(initial_fields.get('G', None))
+
+        for pml in pmls:
+            pml.setdefault('thickness', 8)
+            pml.setdefault('epsilon_eff', 1.0)
+            pml.setdefault('mu_eff', 1.0)
+            pml.setdefault('ln_R_per_layer', -1.6)
+            pml.setdefault('m', 3.5)
+            pml.setdefault('cfs_alpha', 0)
+            pml.setdefault('ma', 1)
+
+        ctype = type_to_C(self.arg_type)
+
+        def ptr(arg: str) -> str:
+            return ctype + ' *' + arg
+
+        base_fields = OrderedDict()
+        base_fields[ptr('E')] = self.E
+        base_fields[ptr('H')] = self.H
+        base_fields[ctype + ' dt'] = self.dt
+        if uniform_dx == False:
+            inv_dx_names = ['inv_d' + eh + r for eh in 'eh' for r in 'xyz']
+            for name, field in zip(inv_dx_names, self.inv_dxes):
+                base_fields[ptr(name)] = field
+
+        eps_field = OrderedDict()
+        eps_field[ptr('eps')] = self.eps
+
+        if bloch_boundaries:
+            base_fields[ptr('F')] = self.F
+            base_fields[ptr('G')] = self.G
+
+            bloch_fields = OrderedDict()
+            bloch_fields[ptr('E')] = self.F
+            bloch_fields[ptr('H')] = self.G
+            bloch_fields[ctype + ' dt'] = self.dt
+            bloch_fields[ptr('F')] = self.E
+            bloch_fields[ptr('G')] = self.H
+
+        common_source = jinja_env.get_template('common.cl').render(
+                ftype=ctype,
+                shape=self.shape,
+                )
+        jinja_args = {
+                'common_header': common_source,
+                'pmls': pmls,
+                'do_poynting': do_poynting,
+                'bloch': bloch_boundaries,
+                'uniform_dx': uniform_dx,
+                }
+        E_source = jinja_env.get_template('update_e.cl').render(**jinja_args)
+        H_source = jinja_env.get_template('update_h.cl').render(**jinja_args)
+        self.sources['E'] = E_source
+        self.sources['H'] = H_source
+
+        if bloch_boundaries:
+            bloch_args = jinja_args.copy()
+            bloch_args['do_poynting'] = False
+            bloch_args['bloch'] = [{'axis': b['axis'],
+                                    'real': b['imag'],
+                                    'imag': b['real']}
+                                   for b in bloch_boundaries]
+            F_source = jinja_env.get_template('update_e.cl').render(**bloch_args)
+            G_source = jinja_env.get_template('update_h.cl').render(**bloch_args)
+            self.sources['F'] = F_source
+            self.sources['G'] = G_source
+
+
+        S_fields = OrderedDict()
+        if do_poynting:
+            S_source = jinja_env.get_template('update_s.cl').render(**jinja_args)
+            self.sources['S'] = S_source
+
+            self.oS = pyopencl.array.zeros(self.queue, self.E.shape + (2,), dtype=self.arg_type)
+            self.S = pyopencl.array.zeros_like(self.E)
+            S_fields[ptr('oS')] = self.oS
+            S_fields[ptr('S')] = self.S
+
+        J_fields = OrderedDict()
+        if do_fieldsrc:
+            J_source = jinja_env.get_template('update_j.cl').render(**jinja_args)
+            self.sources['J'] = J_source
+
+            self.Ji = pyopencl.array.zeros_like(self.E)
+            self.Jr = pyopencl.array.zeros_like(self.E)
+            J_fields[ptr('Jr')] = self.Jr
+            J_fields[ptr('Ji')] = self.Ji
+
+
+        '''
+        PML
+        '''
+        pml_e_fields, pml_h_fields = self._create_pmls(pmls)
+        if bloch_boundaries:
+            pml_f_fields, pml_g_fields = self._create_pmls(pmls)
+
+        '''
+        Create operations
+        '''
+        self.update_E = self._create_operation(E_source, (base_fields, eps_field, pml_e_fields))
+        self.update_H = self._create_operation(H_source, (base_fields, pml_h_fields, S_fields))
+        if do_poynting:
+            self.update_S = self._create_operation(S_source, (base_fields, S_fields))
+        if bloch_boundaries:
+            self.update_F = self._create_operation(F_source, (bloch_fields, eps_field, pml_f_fields))
+            self.update_G = self._create_operation(G_source, (bloch_fields, pml_g_fields))
+        if do_fieldsrc:
+            args = OrderedDict()
+            [args.update(d) for d in (base_fields, J_fields)]
+            var_args = [ctype + ' ' + v for v in 'cs'] + ['uint ' + r + m for r in 'xyz' for m in ('min', 'max')]
+            update = ElementwiseKernel(self.context, operation=J_source,
+                                       arguments=', '.join(list(args.keys()) + var_args))
+            self.update_J = lambda e, *a: update(*args.values(), *a, wait_for=e)
+
+
+    def _create_pmls(self, pmls):
+        ctype = type_to_C(self.arg_type)
+        def ptr(arg: str) -> str:
+            return ctype + ' *' + arg
+
+        pml_e_fields = OrderedDict()
+        pml_h_fields = OrderedDict()
+        for pml in pmls:
+            a = 'xyz'.find(pml['axis'])
+
+            sigma_max = -pml['ln_R_per_layer'] / 2 * (pml['m'] + 1)
+            kappa_max = numpy.sqrt(pml['mu_eff'] * pml['epsilon_eff'])
+            alpha_max = pml['cfs_alpha']
+
+            def par(x):
+                scaling = (x / pml['thickness']) ** pml['m']
+                sigma = scaling * sigma_max
+                kappa = 1 + scaling * (kappa_max - 1)
+                alpha = ((1 - x / pml['thickness']) ** pml['ma']) * alpha_max
+                p0 = numpy.exp(-(sigma / kappa + alpha) * self.dt)
+                p1 = sigma / (sigma + kappa * alpha) * (p0 - 1)
+                p2 = 1 / kappa
+                return p0, p1, p2
+
+            xe, xh = (numpy.arange(1, pml['thickness'] + 1, dtype=self.arg_type)[::-1] for _ in range(2))
+            if pml['polarity'] == 'p':
+                xe -= 0.5
+            elif pml['polarity'] == 'n':
+                xh -= 0.5
+
+            pml_p_names = [['p' + pml['axis'] + i + eh + pml['polarity'] for i in '012'] for eh in 'eh']
+            for name_e, name_h, pe, ph in zip(pml_p_names[0], pml_p_names[1], par(xe), par(xh)):
+                pml_e_fields[ptr(name_e)] = pyopencl.array.to_device(self.queue, pe)
+                pml_h_fields[ptr(name_h)] = pyopencl.array.to_device(self.queue, ph)
+
+            uv = 'xyz'.replace(pml['axis'], '')
+            psi_base = 'Psi_' + pml['axis'] + pml['polarity'] + '_'
+            psi_names = [[psi_base + eh + c for c in uv] for eh in 'EH']
+
+            psi_shape = list(self.shape)
+            psi_shape[a] = pml['thickness']
+
+            for ne, nh in zip(*psi_names):
+                pml_e_fields[ptr(ne)] = pyopencl.array.zeros(self.queue, tuple(psi_shape), dtype=self.arg_type)
+                pml_h_fields[ptr(nh)] = pyopencl.array.zeros(self.queue, tuple(psi_shape), dtype=self.arg_type)
+        return pml_e_fields, pml_h_fields
+
+    def _create_operation(self, source, args_fields):
+        args = OrderedDict()
+        [args.update(d) for d in args_fields]
+        update = ElementwiseKernel(self.context, operation=source,
+                                   arguments=', '.join(args.keys()))
+        return lambda e: update(*args.values(), wait_for=e)
+
+    def _create_context(self, context: pyopencl.Context = None,
+                        queue: pyopencl.CommandQueue = None):
+        if context is None:
+            self.context = pyopencl.create_some_context()
+        else:
+            self.context = context
+
+        if queue is None:
+            self.queue = pyopencl.CommandQueue(self.context)
+        else:
+            self.queue = queue
+
+    def _create_eps(self, epsilon: List[numpy.ndarray]):
+        if len(epsilon) != 3:
+            raise Exception('Epsilon must be a list with length of 3')
+        if not all((e.shape == epsilon[0].shape for e in epsilon[1:])):
+            raise Exception('All epsilon grids must have the same shape. Shapes are {}', [e.shape for e in epsilon])
+        if not epsilon[0].shape == self.shape:
+            raise Exception('Epsilon shape mismatch. Expected {}, got {}'.format(self.shape, epsilon[0].shape))
+        self.eps = pyopencl.array.to_device(self.queue, vec(epsilon).astype(self.arg_type))
+
+    def _create_field(self, initial_value: List[numpy.ndarray] = None):
+        if initial_value is None:
+            return pyopencl.array.zeros_like(self.eps)
+        else:
+            if len(initial_value) != 3:
+                Exception('Initial field value must be a list of length 3')
+            if not all((f.shape == self.shape for f in initial_value)):
+                Exception('Initial field list elements must have same shape as epsilon elements')
+            return pyopencl.array.to_device(self.queue, vec(initial_value).astype(self.arg_type))
+
+
+def type_to_C(float_type) -> str:
+    """
+    Returns a string corresponding to the C equivalent of a numpy type.
+    Only works for float16, float32, float64.
+
+    :param float_type: e.g. numpy.float32
+    :return: string containing the corresponding C type (eg. 'double')
+    """
+    if float_type == numpy.float16:
+        arg_type = 'half'
+    elif float_type == numpy.float32:
+        arg_type = 'float'
+    elif float_type == numpy.float64:
+        arg_type = 'double'
+    else:
+        raise Exception('Unsupported type')
+    return arg_type

requirements.txt

@@ -2,7 +2,7 @@ numpy
 h5py
 pyopencl
 jinja2
--e git+https://mpxd.net/gogs/jan/float_raster.git@release#egg=float_raster
--e git+https://mpxd.net/gogs/jan/gridlock.git@release#egg=gridlock
--e git+https://mpxd.net/gogs/jan/masque.git@release#egg=masque
--e git+https://mpxd.net/gogs/jan/fdfd_tools.git@master#egg=fdfd_tools
+-e git+https://mpxd.net/code/jan/float_raster.git@release#egg=float_raster
+-e git+https://mpxd.net/code/jan/gridlock.git@release#egg=gridlock
+-e git+https://mpxd.net/code/jan/masque.git@release#egg=masque
+-e git+https://mpxd.net/code/jan/fdfd_tools.git@master#egg=fdfd_tools

setup.py

@@ -0,0 +1,30 @@
+#!/usr/bin/env python3
+
+from setuptools import setup, find_packages
+import opencl_fdtd
+
+with open('README.md', 'r') as f:
+    long_description = f.read()
+
+setup(name='opencl_fdtd',
+      version=opencl_fdtd.version,
+      description='OpenCL FDTD solver',
+      long_description=long_description,
+      long_description_content_type='text/markdown',
+      author='Jan Petykiewicz',
+      author_email='anewusername@gmail.com',
+      url='https://mpxd.net/code/jan/opencl_fdtd',
+      packages=find_packages(),
+      package_data={
+          'opencl_fdfd': ['kernels/*']
+      },
+      install_requires=[
+            'numpy',
+            'pyopencl',
+            'jinja2',
+            'fdfd_tools>=0.3',
+      ],
+      extras_require={
+      },
+      )
+