@@ -729,13 +730,14 @@ The volume can also be specified via the `center` and `size` arguments. The
default routine interpolates the Fourier-transformed fields at the center of each
voxel within the specified volume. Alternatively, the exact Fourier-transformed
fields evaluated at each corresponding Yee grid point is available by setting
-`yee_grid` to `True`. To reduce the memory-bandwidth burden of
-accumulating DFT fields, an integer `decimation_factor` >= 1 can be
-specified. DFT field values are updated every `decimation_factor`
-timesteps. Use this feature with care, as the decimated timeseries may be
-corrupted by [aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies.
-The choice of decimation factor should take into account the properties of all sources
-in the simulation as well as the frequency range of the DFT field monitor.
+`yee_grid` to `True`. To reduce the memory-bandwidth burden of accumulating
+DFT fields, an integer `decimation_factor` can be specified for updating the DFT
+fields at every `decimation_factor` timesteps. If `decimation_factor` is 0 (the default),
+this value is automatically determined from the
+[Nyquist rate](https://en.wikipedia.org/wiki/Nyquist_rate) of the bandwidth-limited
+sources and this DFT monitor. It can be turned off by setting it to 1. Use this feature
+with care, as the decimated timeseries may be corrupted by
+[aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies.
@@ -1097,7 +1099,7 @@ Given a bunch of [`FluxRegion`](#fluxregion) objects, you can tell Meep to accum
```python
def add_flux(self, *args, **kwargs):
-def add_flux(fcen, df, nfreq, freq, FluxRegions, decimation_factor=1):
+def add_flux(fcen, df, nfreq, freq, FluxRegions, decimation_factor=0):
```
@@ -1109,11 +1111,14 @@ field Fourier transforms for `nfreq` equally spaced frequencies covering the
frequency range `fcen-df/2` to `fcen+df/2` or an array/list `freq` for arbitrarily
spaced frequencies. Return a *flux object*, which you can pass to the functions
below to get the flux spectrum, etcetera. To reduce the memory-bandwidth burden of
-accumulating DFT fields, an integer `decimation_factor` >= 1 can be
-specified. DFT field values are updated every `decimation_factor`
-timesteps. Use this feature with care, as the decimated timeseries may be
-corrupted by [aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies.
-The choice of decimation factor should take into account the properties of all sources
+accumulating DFT fields, an integer `decimation_factor` can be specified for updating the DFT
+fields at every `decimation_factor` timesteps. If `decimation_factor` is 0 (the default),
+this value is automatically determined from the
+[Nyquist rate](https://en.wikipedia.org/wiki/Nyquist_rate) of the bandwidth-limited
+sources and this DFT monitor. It can be turned off by setting it to 1. Use this feature
+with care, as the decimated timeseries may be corrupted by
+[aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies. The choice
+of decimation factor should take into account the properties of all sources
in the simulation as well as the frequency range of the DFT field monitor.
@@ -1361,7 +1366,7 @@ Technically, MPB computes `ωₙ(k)` and then inverts it with Newton's method to
```python
def add_mode_monitor(self, *args, **kwargs):
-def add_mode_monitor(fcen, df, nfreq, freq, ModeRegions, decimation_factor=1):
+def add_mode_monitor(fcen, df, nfreq, freq, ModeRegions, decimation_factor=0):
```
@@ -1491,7 +1496,7 @@ The usage is similar to the flux spectra: you define a set of [`EnergyRegion`](#
```python
def add_energy(self, *args, **kwargs):
-def add_energy(fcen, df, nfreq, freq, EnergyRegions, decimation_factor=1):
+def add_energy(fcen, df, nfreq, freq, EnergyRegions, decimation_factor=0):
```
@@ -1503,12 +1508,13 @@ field Fourier transforms for `nfreq` equally spaced frequencies covering the
frequency range `fcen-df/2` to `fcen+df/2` or an array/list `freq` for arbitrarily
spaced frequencies. Return an *energy object*, which you can pass to the functions
below to get the energy spectrum, etcetera. To reduce the memory-bandwidth burden of
-accumulating DFT fields, an integer `decimation_factor` >= 1 can be
-specified. DFT field values are updated every `decimation_factor`
-timesteps. Use this feature with care, as the decimated timeseries may be
-corrupted by [aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies.
-The choice of decimation factor should take into account the properties of all sources
-in the simulation as well as the frequency range of the DFT field monitor.
+accumulating DFT fields, an integer `decimation_factor` can be specified for updating the DFT
+fields at every `decimation_factor` timesteps. If `decimation_factor` is 0 (the default),
+this value is automatically determined from the
+[Nyquist rate](https://en.wikipedia.org/wiki/Nyquist_rate) of the bandwidth-limited
+sources and this DFT monitor. It can be turned off by setting it to 1. Use this feature
+with care, as the decimated timeseries may be corrupted by
+[aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies.
@@ -1723,7 +1729,7 @@ The usage is similar to the [flux spectra](Python_Tutorials/Basics.md#transmitta
```python
def add_force(self, *args, **kwargs):
-def add_force(fcen, df, nfreq, freq, ForceRegions, decimation_factor=1):
+def add_force(fcen, df, nfreq, freq, ForceRegions, decimation_factor=0):
```
@@ -1735,12 +1741,13 @@ field Fourier transforms for `nfreq` equally spaced frequencies covering the
frequency range `fcen-df/2` to `fcen+df/2` or an array/list `freq` for arbitrarily
spaced frequencies. Return a `force`object, which you can pass to the functions
below to get the force spectrum, etcetera. To reduce the memory-bandwidth burden of
-accumulating DFT fields, an integer `decimation_factor` >= 1 can be
-specified. DFT field values are updated every `decimation_factor`
-timesteps. Use this feature with care, as the decimated timeseries may be
-corrupted by [aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies.
-The choice of decimation factor should take into account the properties of all sources
-in the simulation as well as the frequency range of the DFT field monitor.
+accumulating DFT fields, an integer `decimation_factor` can be specified for updating the DFT
+fields at every `decimation_factor` timesteps. If `decimation_factor` is 0 (the default),
+this value is automatically determined from the
+[Nyquist rate](https://en.wikipedia.org/wiki/Nyquist_rate) of the bandwidth-limited
+sources and this DFT monitor. It can be turned off by setting it to 1. Use this feature
+with care, as the decimated timeseries may be corrupted by
+[aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies.
@@ -2008,7 +2015,7 @@ There are three steps to using the near-to-far-field feature: first, define the
```python
def add_near2far(self, *args, **kwargs):
-def add_near2far(fcen, df, nfreq, freq, Near2FarRegions, nperiods=1, decimation_factor=1):
+def add_near2far(fcen, df, nfreq, freq, Near2FarRegions, nperiods=1, decimation_factor=0):
```
@@ -2020,12 +2027,13 @@ appropriate field Fourier transforms for `nfreq` equally spaced frequencies
covering the frequency range `fcen-df/2` to `fcen+df/2` or an array/list `freq`
for arbitrarily spaced frequencies. Return a `near2far` object, which you can pass
to the functions below to get the far fields. To reduce the memory-bandwidth burden of
-accumulating DFT fields, an integer `decimation_factor` >= 1 can be
-specified. DFT field values are updated every `decimation_factor`
-timesteps. Use this feature with care, as the decimated timeseries may be
-corrupted by [aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies.
-The choice of decimation factor should take into account the properties of all sources
-in the simulation as well as the frequency range of the DFT field monitor.
+accumulating DFT fields, an integer `decimation_factor` can be specified for updating the DFT
+fields at every `decimation_factor` timesteps. If `decimation_factor` is 0 (the default),
+this value is automatically determined from the
+[Nyquist rate](https://en.wikipedia.org/wiki/Nyquist_rate) of the bandwidth-limited
+sources and this DFT monitor. It can be turned off by setting it to 1. Use this feature
+with care, as the decimated timeseries may be corrupted by
+[aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies.
@@ -4266,8 +4274,7 @@ $\beta$ where $\beta=+\infty$ gives an unsmoothed, discontinuous interface. The
+\tanh(\beta\times(u-\eta)))/(\tanh(\beta\times\eta)+\tanh(\beta\times(1-\eta)))$ involving the parameters `beta`
($\beta$: bias or "smoothness" of the turn on) and `eta` ($\eta$: offset for erosion/dilation). The level set provides a general
approach for defining a *discontinuous* function from otherwise continuously varying (via the bilinear interpolation) grid values.
-The subpixel smoothing is based on an adaptive quadrature scheme with properties `subpixel_maxeval` and `subpixel_tol` which
-can be specified using the `Simulation` constructor.
+Subpixel smoothing is fast and accurate because it exploits an analytic formulation for level-set functions.
It is possible to overlap any number of different `MaterialGrid`s. This can be useful for defining grids which are symmetric
(e.g., mirror, rotation). One way to set this up is by overlapping a given `MaterialGrid` object with a symmetrized copy of
diff --git a/python/adjoint/objective.py b/python/adjoint/objective.py
index 802b5571a..e1d0159fb 100644
--- a/python/adjoint/objective.py
+++ b/python/adjoint/objective.py
@@ -121,7 +121,7 @@ def __init__(self,
mode,
forward=True,
kpoint_func=None,
- decimation_factor=1,
+ decimation_factor=0,
**kwargs):
super().__init__(sim)
self.volume = volume
@@ -206,7 +206,7 @@ def __call__(self):
class FourierFields(ObjectiveQuantity):
- def __init__(self, sim, volume, component, decimation_factor=1):
+ def __init__(self, sim, volume, component, decimation_factor=0):
super().__init__(sim)
self.volume = volume
self.component = component
@@ -306,7 +306,7 @@ def __call__(self):
class Near2FarFields(ObjectiveQuantity):
- def __init__(self, sim, Near2FarRegions, far_pts, decimation_factor=1):
+ def __init__(self, sim, Near2FarRegions, far_pts, decimation_factor=0):
super().__init__(sim)
self.Near2FarRegions = Near2FarRegions
self.far_pts = far_pts #list of far pts
diff --git a/python/adjoint/optimization_problem.py b/python/adjoint/optimization_problem.py
index 244103116..bb938cf45 100644
--- a/python/adjoint/optimization_problem.py
+++ b/python/adjoint/optimization_problem.py
@@ -72,7 +72,7 @@ def __init__(
decay_dt=50,
decay_fields=[mp.Ez],
decay_by=1e-6,
- decimation_factor=1,
+ decimation_factor=0,
minimum_run_time=0,
maximum_run_time=None,
):
diff --git a/python/adjoint/utils.py b/python/adjoint/utils.py
index 110a4c4c2..decbe9e11 100644
--- a/python/adjoint/utils.py
+++ b/python/adjoint/utils.py
@@ -69,6 +69,7 @@ def install_design_region_monitors(
frequencies,
where=design_region.volume,
yee_grid=True,
+ decimation_factor=0
) for design_region in design_regions
]
return design_region_monitors
diff --git a/python/geom.py b/python/geom.py
index 861b62d93..b061ad81e 100755
--- a/python/geom.py
+++ b/python/geom.py
@@ -547,7 +547,7 @@ def __init__(self,grid_size,medium1,medium2,weights=None,grid_type="U_DEFAULT",d
+\\tanh(\\beta\\times(u-\\eta)))/(\\tanh(\\beta\\times\\eta)+\\tanh(\\beta\\times(1-\\eta)))$ involving the parameters `beta`
($\\beta$: bias or "smoothness" of the turn on) and `eta` ($\\eta$: offset for erosion/dilation). The level set provides a general
approach for defining a *discontinuous* function from otherwise continuously varying (via the bilinear interpolation) grid values.
- Subpixel smoothing is fast and accurate because it exploits an analytic framework for level-set functions.
+ Subpixel smoothing is fast and accurate because it exploits an analytic formulation for level-set functions.
It is possible to overlap any number of different `MaterialGrid`s. This can be useful for defining grids which are symmetric
(e.g., mirror, rotation). One way to set this up is by overlapping a given `MaterialGrid` object with a symmetrized copy of
diff --git a/python/simulation.py b/python/simulation.py
index 62a8b54a4..34231ab6e 100644
--- a/python/simulation.py
+++ b/python/simulation.py
@@ -2413,7 +2413,7 @@ def _evaluate_dft_objects(self):
def add_dft_fields(self, *args, **kwargs):
"""
- `add_dft_fields(cs, fcen, df, nfreq, freq, where=None, center=None, size=None, yee_grid=False, decimation_factor=1)` ##sig
+ `add_dft_fields(cs, fcen, df, nfreq, freq, where=None, center=None, size=None, yee_grid=False, decimation_factor=0)` ##sig
Given a list of field components `cs`, compute the Fourier transform of these
fields for `nfreq` equally spaced frequencies covering the frequency range
@@ -2423,13 +2423,14 @@ def add_dft_fields(self, *args, **kwargs):
default routine interpolates the Fourier-transformed fields at the center of each
voxel within the specified volume. Alternatively, the exact Fourier-transformed
fields evaluated at each corresponding Yee grid point is available by setting
- `yee_grid` to `True`. To reduce the memory-bandwidth burden of
- accumulating DFT fields, an integer `decimation_factor` >= 1 can be
- specified. DFT field values are updated every `decimation_factor`
- timesteps. Use this feature with care, as the decimated timeseries may be
- corrupted by [aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies.
- The choice of decimation factor should take into account the properties of all sources
- in the simulation as well as the frequency range of the DFT field monitor.
+ `yee_grid` to `True`. To reduce the memory-bandwidth burden of accumulating
+ DFT fields, an integer `decimation_factor` can be specified for updating the DFT
+ fields at every `decimation_factor` timesteps. If `decimation_factor` is 0 (the default),
+ this value is automatically determined from the
+ [Nyquist rate](https://en.wikipedia.org/wiki/Nyquist_rate) of the bandwidth-limited
+ sources and this DFT monitor. It can be turned off by setting it to 1. Use this feature
+ with care, as the decimated timeseries may be corrupted by
+ [aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies.
"""
components = args[0]
args = fix_dft_args(args, 1)
@@ -2438,7 +2439,7 @@ def add_dft_fields(self, *args, **kwargs):
center = kwargs.get('center', None)
size = kwargs.get('size', None)
yee_grid = kwargs.get('yee_grid', False)
- decimation_factor = kwargs.get('decimation_factor', 1)
+ decimation_factor = kwargs.get('decimation_factor', 0)
center_v3 = Vector3(*center) if center is not None else None
size_v3 = Vector3(*size) if size is not None else None
use_centered_grid = not yee_grid
@@ -2487,7 +2488,7 @@ def get_dft_data(self, dft_chunk):
def add_near2far(self, *args, **kwargs):
"""
- `add_near2far(fcen, df, nfreq, freq, Near2FarRegions, nperiods=1, decimation_factor=1)` ##sig
+ `add_near2far(fcen, df, nfreq, freq, Near2FarRegions, nperiods=1, decimation_factor=0)` ##sig
Add a bunch of `Near2FarRegion`s to the current simulation (initializing the
fields if they have not yet been initialized), telling Meep to accumulate the
@@ -2495,18 +2496,19 @@ def add_near2far(self, *args, **kwargs):
covering the frequency range `fcen-df/2` to `fcen+df/2` or an array/list `freq`
for arbitrarily spaced frequencies. Return a `near2far` object, which you can pass
to the functions below to get the far fields. To reduce the memory-bandwidth burden of
- accumulating DFT fields, an integer `decimation_factor` >= 1 can be
- specified. DFT field values are updated every `decimation_factor`
- timesteps. Use this feature with care, as the decimated timeseries may be
- corrupted by [aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies.
- The choice of decimation factor should take into account the properties of all sources
- in the simulation as well as the frequency range of the DFT field monitor.
+ accumulating DFT fields, an integer `decimation_factor` can be specified for updating the DFT
+ fields at every `decimation_factor` timesteps. If `decimation_factor` is 0 (the default),
+ this value is automatically determined from the
+ [Nyquist rate](https://en.wikipedia.org/wiki/Nyquist_rate) of the bandwidth-limited
+ sources and this DFT monitor. It can be turned off by setting it to 1. Use this feature
+ with care, as the decimated timeseries may be corrupted by
+ [aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies.
"""
args = fix_dft_args(args, 0)
freq = args[0]
near2fars = args[1:]
nperiods = kwargs.get('nperiods', 1)
- decimation_factor = kwargs.get('decimation_factor', 1)
+ decimation_factor = kwargs.get('decimation_factor', 0)
n2f = DftNear2Far(self._add_near2far, [freq, nperiods, near2fars, decimation_factor])
self.dft_objects.append(n2f)
return n2f
@@ -2519,7 +2521,7 @@ def _add_near2far(self, freq, nperiods, near2fars, decimation_factor):
def add_energy(self, *args, **kwargs):
"""
- `add_energy(fcen, df, nfreq, freq, EnergyRegions, decimation_factor=1)` ##sig
+ `add_energy(fcen, df, nfreq, freq, EnergyRegions, decimation_factor=0)` ##sig
Add a bunch of `EnergyRegion`s to the current simulation (initializing the fields
if they have not yet been initialized), telling Meep to accumulate the appropriate
@@ -2527,17 +2529,18 @@ def add_energy(self, *args, **kwargs):
frequency range `fcen-df/2` to `fcen+df/2` or an array/list `freq` for arbitrarily
spaced frequencies. Return an *energy object*, which you can pass to the functions
below to get the energy spectrum, etcetera. To reduce the memory-bandwidth burden of
- accumulating DFT fields, an integer `decimation_factor` >= 1 can be
- specified. DFT field values are updated every `decimation_factor`
- timesteps. Use this feature with care, as the decimated timeseries may be
- corrupted by [aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies.
- The choice of decimation factor should take into account the properties of all sources
- in the simulation as well as the frequency range of the DFT field monitor.
+ accumulating DFT fields, an integer `decimation_factor` can be specified for updating the DFT
+ fields at every `decimation_factor` timesteps. If `decimation_factor` is 0 (the default),
+ this value is automatically determined from the
+ [Nyquist rate](https://en.wikipedia.org/wiki/Nyquist_rate) of the bandwidth-limited
+ sources and this DFT monitor. It can be turned off by setting it to 1. Use this feature
+ with care, as the decimated timeseries may be corrupted by
+ [aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies.
"""
args = fix_dft_args(args, 0)
freq = args[0]
energys = args[1:]
- decimation_factor = kwargs.get('decimation_factor', 1)
+ decimation_factor = kwargs.get('decimation_factor', 0)
en = DftEnergy(self._add_energy, [freq, energys, decimation_factor])
self.dft_objects.append(en)
return en
@@ -2740,7 +2743,7 @@ def load_minus_near2far_data(self, near2far, n2fdata):
def add_force(self, *args, **kwargs):
"""
- `add_force(fcen, df, nfreq, freq, ForceRegions, decimation_factor=1)` ##sig
+ `add_force(fcen, df, nfreq, freq, ForceRegions, decimation_factor=0)` ##sig
Add a bunch of `ForceRegion`s to the current simulation (initializing the fields
if they have not yet been initialized), telling Meep to accumulate the appropriate
@@ -2748,17 +2751,18 @@ def add_force(self, *args, **kwargs):
frequency range `fcen-df/2` to `fcen+df/2` or an array/list `freq` for arbitrarily
spaced frequencies. Return a `force`object, which you can pass to the functions
below to get the force spectrum, etcetera. To reduce the memory-bandwidth burden of
- accumulating DFT fields, an integer `decimation_factor` >= 1 can be
- specified. DFT field values are updated every `decimation_factor`
- timesteps. Use this feature with care, as the decimated timeseries may be
- corrupted by [aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies.
- The choice of decimation factor should take into account the properties of all sources
- in the simulation as well as the frequency range of the DFT field monitor.
+ accumulating DFT fields, an integer `decimation_factor` can be specified for updating the DFT
+ fields at every `decimation_factor` timesteps. If `decimation_factor` is 0 (the default),
+ this value is automatically determined from the
+ [Nyquist rate](https://en.wikipedia.org/wiki/Nyquist_rate) of the bandwidth-limited
+ sources and this DFT monitor. It can be turned off by setting it to 1. Use this feature
+ with care, as the decimated timeseries may be corrupted by
+ [aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies.
"""
args = fix_dft_args(args, 0)
freq = args[0]
forces = args[1:]
- decimation_factor = kwargs.get('decimation_factor', 1)
+ decimation_factor = kwargs.get('decimation_factor', 0)
force = DftForce(self._add_force, [freq, forces, decimation_factor])
self.dft_objects.append(force)
return force
@@ -2845,7 +2849,7 @@ def load_minus_force_data(self, force, fdata):
def add_flux(self, *args, **kwargs):
"""
- `add_flux(fcen, df, nfreq, freq, FluxRegions, decimation_factor=1)` ##sig
+ `add_flux(fcen, df, nfreq, freq, FluxRegions, decimation_factor=0)` ##sig
Add a bunch of `FluxRegion`s to the current simulation (initializing the fields if
they have not yet been initialized), telling Meep to accumulate the appropriate
@@ -2853,17 +2857,20 @@ def add_flux(self, *args, **kwargs):
frequency range `fcen-df/2` to `fcen+df/2` or an array/list `freq` for arbitrarily
spaced frequencies. Return a *flux object*, which you can pass to the functions
below to get the flux spectrum, etcetera. To reduce the memory-bandwidth burden of
- accumulating DFT fields, an integer `decimation_factor` >= 1 can be
- specified. DFT field values are updated every `decimation_factor`
- timesteps. Use this feature with care, as the decimated timeseries may be
- corrupted by [aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies.
- The choice of decimation factor should take into account the properties of all sources
+ accumulating DFT fields, an integer `decimation_factor` can be specified for updating the DFT
+ fields at every `decimation_factor` timesteps. If `decimation_factor` is 0 (the default),
+ this value is automatically determined from the
+ [Nyquist rate](https://en.wikipedia.org/wiki/Nyquist_rate) of the bandwidth-limited
+ sources and this DFT monitor. It can be turned off by setting it to 1. Use this feature
+ with care, as the decimated timeseries may be corrupted by
+ [aliasing](https://en.wikipedia.org/wiki/Aliasing) of high frequencies. The choice
+ of decimation factor should take into account the properties of all sources
in the simulation as well as the frequency range of the DFT field monitor.
"""
args = fix_dft_args(args, 0)
freq = args[0]
fluxes = args[1:]
- decimation_factor = kwargs.get('decimation_factor', 1)
+ decimation_factor = kwargs.get('decimation_factor', 0)
flux = DftFlux(self._add_flux, [freq, fluxes, decimation_factor])
self.dft_objects.append(flux)
return flux
@@ -2876,14 +2883,14 @@ def _add_flux(self, freq, fluxes, decimation_factor):
def add_mode_monitor(self, *args, **kwargs):
"""
- `add_mode_monitor(fcen, df, nfreq, freq, ModeRegions, decimation_factor=1)` ##sig
+ `add_mode_monitor(fcen, df, nfreq, freq, ModeRegions, decimation_factor=0)` ##sig
Similar to `add_flux`, but for use with `get_eigenmode_coefficients`.
"""
args = fix_dft_args(args, 0)
freq = args[0]
fluxes = args[1:]
- decimation_factor = kwargs.get('decimation_factor', 1)
+ decimation_factor = kwargs.get('decimation_factor', 0)
yee_grid = kwargs.get("yee_grid", False)
flux = DftFlux(self._add_mode_monitor, [freq, fluxes, yee_grid, decimation_factor])
self.dft_objects.append(flux)
diff --git a/python/tests/test_3rd_harm_1d.py b/python/tests/test_3rd_harm_1d.py
index f0bf9269f..87e9ee4e7 100644
--- a/python/tests/test_3rd_harm_1d.py
+++ b/python/tests/test_3rd_harm_1d.py
@@ -34,9 +34,9 @@ def setUp(self):
dimensions=dimensions)
fr = mp.FluxRegion(mp.Vector3(0, 0, (0.5 * self.sz) - self.dpml - 0.5))
- self.trans = self.sim.add_flux(0.5 * (fmin + fmax), fmax - fmin, nfreq, fr)
- self.trans1 = self.sim.add_flux(fcen, 0, 1, fr)
- self.trans3 = self.sim.add_flux(3 * fcen, 0, 1, fr)
+ self.trans = self.sim.add_flux(0.5 * (fmin + fmax), fmax - fmin, nfreq, fr, decimation_factor=1)
+ self.trans1 = self.sim.add_flux(fcen, 0, 1, fr, decimation_factor=1)
+ self.trans3 = self.sim.add_flux(3 * fcen, 0, 1, fr, decimation_factor=1)
def test_3rd_harm_1d(self):
diff --git a/python/tests/test_adjoint_jax.py b/python/tests/test_adjoint_jax.py
index 346946b13..0cc927b3f 100644
--- a/python/tests/test_adjoint_jax.py
+++ b/python/tests/test_adjoint_jax.py
@@ -117,7 +117,8 @@ def build_straight_wg_simulation(
simulation,
mp.Volume(center=center, size=monitor_size),
mode=1,
- forward=True) for center in monitor_centers
+ forward=True,
+ decimation_factor=1) for center in monitor_centers
]
return simulation, sources, monitors, design_regions, frequencies
diff --git a/python/tests/test_bend_flux.py b/python/tests/test_bend_flux.py
index 17dff7950..a21d7c71f 100644
--- a/python/tests/test_bend_flux.py
+++ b/python/tests/test_bend_flux.py
@@ -62,12 +62,13 @@ def init(self, no_bend=False, gdsii=False):
else:
fr = mp.FluxRegion(center=mp.Vector3(wvg_xcen, (sy / 2) - 1.5), size=mp.Vector3(w * 2, 0))
- self.trans = self.sim.add_flux(fcen, df, nfreq, fr)
+ self.trans = self.sim.add_flux(fcen, df, nfreq, fr, decimation_factor=1)
self.trans_decimated = self.sim.add_flux(fcen, df, nfreq, fr, decimation_factor=5)
refl_fr = mp.FluxRegion(center=mp.Vector3((-0.5 * sx) + 1.5, wvg_ycen),
size=mp.Vector3(0, w * 2))
- self.refl = self.sim.add_flux(np.linspace(fcen-0.5*df,fcen+0.5*df,nfreq), refl_fr)
+ self.refl = self.sim.add_flux(np.linspace(fcen-0.5*df,fcen+0.5*df,nfreq), refl_fr,
+ decimation_factor=1)
self.refl_decimated = self.sim.add_flux(np.linspace(fcen-0.5*df,fcen+0.5*df,nfreq), refl_fr,
decimation_factor=10)
diff --git a/python/tests/test_cavity_farfield.py b/python/tests/test_cavity_farfield.py
index 861831c94..93de61f01 100644
--- a/python/tests/test_cavity_farfield.py
+++ b/python/tests/test_cavity_farfield.py
@@ -56,7 +56,8 @@ def run_test(self, nfreqs):
size=mp.Vector3(0, d1),
weight=-1.0),
mp.Near2FarRegion(mp.Vector3(0.5 * sx - dpml, 0.5 * w + 0.5 * d1),
- size=mp.Vector3(0, d1))
+ size=mp.Vector3(0, d1)),
+ decimation_factor=1
)
sim.run(until=200)
d2 = 20
diff --git a/python/tests/test_chunks.py b/python/tests/test_chunks.py
index 886f57d4e..2af803b07 100644
--- a/python/tests/test_chunks.py
+++ b/python/tests/test_chunks.py
@@ -38,7 +38,7 @@ def test_chunks(self):
rgt = mp.FluxRegion(center=mp.Vector3(+0.5*sxy-dpml,0), size=mp.Vector3(0,sxy-2*dpml), weight=+1.0)
lft = mp.FluxRegion(center=mp.Vector3(-0.5*sxy+dpml,0), size=mp.Vector3(0,sxy-2*dpml), weight=-1.0)
- tot_flux = sim.add_flux(fcen, 0, 1, top, bot, rgt, lft)
+ tot_flux = sim.add_flux(fcen, 0, 1, top, bot, rgt, lft, decimation_factor=1)
sim.run(until_after_sources=mp.stop_when_fields_decayed(50, mp.Ez, mp.Vector3(), 1e-5))
@@ -61,7 +61,7 @@ def test_chunks(self):
sim.use_output_directory(self.temp_dir)
- tot_flux = sim.add_flux(fcen, 0, 1, top, bot, rgt, lft)
+ tot_flux = sim.add_flux(fcen, 0, 1, top, bot, rgt, lft, decimation_factor=1)
sim.load_minus_flux('tot_flux', tot_flux)
diff --git a/python/tests/test_dft_energy.py b/python/tests/test_dft_energy.py
index 856697a81..db43946ea 100644
--- a/python/tests/test_dft_energy.py
+++ b/python/tests/test_dft_energy.py
@@ -22,8 +22,10 @@ def test_dft_energy(self):
sim = mp.Simulation(resolution=resolution, cell_size=cell, geometry=geom,
boundary_layers=pml, sources=sources, symmetries=[mp.Mirror(direction=mp.Y)])
- flux = sim.add_flux(fsrc, 0, 1, mp.FluxRegion(center=mp.Vector3(3), size=mp.Vector3(y=5)))
- energy = sim.add_energy(fsrc, 0, 1, mp.EnergyRegion(center=mp.Vector3(3), size=mp.Vector3(y=5)))
+ flux = sim.add_flux(fsrc, 0, 1, mp.FluxRegion(center=mp.Vector3(3), size=mp.Vector3(y=5)),
+ decimation_factor=1)
+ energy = sim.add_energy(fsrc, 0, 1, mp.EnergyRegion(center=mp.Vector3(3), size=mp.Vector3(y=5)),
+ decimation_factor=1)
energy_decimated = sim.add_energy(fsrc, 0, 1,
mp.EnergyRegion(center=mp.Vector3(3), size=mp.Vector3(y=5)),
decimation_factor=10)
diff --git a/python/tests/test_dft_fields.py b/python/tests/test_dft_fields.py
index a66954abb..3b190adbe 100644
--- a/python/tests/test_dft_fields.py
+++ b/python/tests/test_dft_fields.py
@@ -102,7 +102,8 @@ def test_get_dft_array(self):
def test_decimated_dft_fields_are_almost_equal_to_undecimated_fields(self):
sim = self.init()
sim.init_sim()
- undecimated_field = sim.add_dft_fields([mp.Ez], self.fcen, 0, 1)
+ undecimated_field = sim.add_dft_fields([mp.Ez], self.fcen, 0, 1,
+ decimation_factor=1)
decimated_field = sim.add_dft_fields([mp.Ez],
self.fcen,
0,
diff --git a/python/tests/test_divide_mpi_processes.py b/python/tests/test_divide_mpi_processes.py
index ba7addf3c..574f0e834 100644
--- a/python/tests/test_divide_mpi_processes.py
+++ b/python/tests/test_divide_mpi_processes.py
@@ -1,5 +1,3 @@
-from __future__ import division
-
import unittest
import meep as mp
@@ -36,7 +34,8 @@ def test_divide_parallel_processes(self):
mp.FluxRegion(mp.Vector3(y=0.5*sxy), size=mp.Vector3(sxy)),
mp.FluxRegion(mp.Vector3(y=-0.5*sxy), size=mp.Vector3(sxy), weight=-1),
mp.FluxRegion(mp.Vector3(0.5*sxy), size=mp.Vector3(y=sxy)),
- mp.FluxRegion(mp.Vector3(-0.5*sxy), size=mp.Vector3(y=sxy), weight=-1))
+ mp.FluxRegion(mp.Vector3(-0.5*sxy), size=mp.Vector3(y=sxy), weight=-1),
+ decimation_factor=1)
self.sim.run(until_after_sources=30)
diff --git a/python/tests/test_force.py b/python/tests/test_force.py
index 136202d0d..a2588de45 100644
--- a/python/tests/test_force.py
+++ b/python/tests/test_force.py
@@ -20,7 +20,7 @@ def setUp(self):
sources=[sources])
fr = mp.ForceRegion(mp.Vector3(y=1.27), direction=mp.Y, size=mp.Vector3(4.38))
- self.myforce = self.sim.add_force(fcen, 0, 1, fr)
+ self.myforce = self.sim.add_force(fcen, 0, 1, fr, decimation_factor=1)
self.myforce_decimated = self.sim.add_force(fcen, 0, 1, fr, decimation_factor=10)
def test_force(self):
diff --git a/python/tests/test_geom.py b/python/tests/test_geom.py
index a0fe5325e..4b2f3a974 100644
--- a/python/tests/test_geom.py
+++ b/python/tests/test_geom.py
@@ -348,12 +348,12 @@ def check_warnings(sim, should_warn=True):
sim = mp.Simulation(cell_size=cell_size, resolution=resolution, sources=valid_sources[0],
extra_materials=[mat])
fregion = mp.FluxRegion(center=mp.Vector3(0, 1), size=mp.Vector3(2, 2), direction=mp.X)
- sim.add_flux(18, 6, 2, fregion)
+ sim.add_flux(18, 6, 2, fregion, decimation_factor=1)
check_warnings(sim)
# Invalid geometry material
sim = mp.Simulation(cell_size=cell_size, resolution=resolution, sources=valid_sources[0], geometry=geom)
- sim.add_flux(18, 6, 2, fregion)
+ sim.add_flux(18, 6, 2, fregion, decimation_factor=1)
check_warnings(sim)
def test_transform(self):
diff --git a/python/tests/test_holey_wvg_cavity.py b/python/tests/test_holey_wvg_cavity.py
index 5b486273f..a66998d28 100644
--- a/python/tests/test_holey_wvg_cavity.py
+++ b/python/tests/test_holey_wvg_cavity.py
@@ -134,7 +134,8 @@ def test_transmission_spectrum(self):
freg = mp.FluxRegion(center=mp.Vector3((0.5 * self.sx) - self.dpml - 0.5),
size=mp.Vector3(0, 2 * self.w))
- trans = self.sim.add_flux(self.fcen, self.df, self.nfreq, freg)
+ trans = self.sim.add_flux(self.fcen, self.df, self.nfreq, freg,
+ decimation_factor=1)
self.sim.run(
until_after_sources=mp.stop_when_fields_decayed(
diff --git a/python/tests/test_mode_decomposition.py b/python/tests/test_mode_decomposition.py
index b6abcd0e4..6c400cf56 100644
--- a/python/tests/test_mode_decomposition.py
+++ b/python/tests/test_mode_decomposition.py
@@ -116,7 +116,8 @@ def test_oblique_waveguide_backward_mode(self):
mode = sim.add_mode_monitor(fcen, 0, 1,
mp.FluxRegion(center=mp.Vector3(-0.5*sxy+dpml,0,0),
- size=mp.Vector3(0,sxy,0)))
+ size=mp.Vector3(0,sxy,0)),
+ decimation_factor=1)
mode_decimated = sim.add_mode_monitor(fcen, 0, 1,
mp.FluxRegion(center=mp.Vector3(-0.5*sxy+dpml,0,0),
size=mp.Vector3(0,sxy,0)),
diff --git a/python/tests/test_refl_angular.py b/python/tests/test_refl_angular.py
index 89acd03a4..209dd16eb 100644
--- a/python/tests/test_refl_angular.py
+++ b/python/tests/test_refl_angular.py
@@ -41,7 +41,7 @@ def test_refl_angular(self):
resolution=resolution)
refl_fr = mp.FluxRegion(center=mp.Vector3(z=-0.25 * sz))
- refl = sim.add_flux(fcen, df, nfreq, refl_fr)
+ refl = sim.add_flux(fcen, df, nfreq, refl_fr, decimation_factor=1)
sim.run(until_after_sources=mp.stop_when_fields_decayed(50, mp.Ex, mp.Vector3(z=-0.5 * sz + dpml), 1e-9))
@@ -59,7 +59,7 @@ def test_refl_angular(self):
dimensions=dimensions,
resolution=resolution)
- refl = sim.add_flux(fcen, df, nfreq, refl_fr)
+ refl = sim.add_flux(fcen, df, nfreq, refl_fr, decimation_factor=1)
sim.load_minus_flux_data(refl, empty_data)
sim.run(until_after_sources=mp.stop_when_fields_decayed(50, mp.Ex, mp.Vector3(z=-0.5 * sz + dpml), 1e-9))
diff --git a/python/tests/test_visualization.py b/python/tests/test_visualization.py
index 4400955e4..e2b9d2846 100644
--- a/python/tests/test_visualization.py
+++ b/python/tests/test_visualization.py
@@ -82,10 +82,10 @@ def setup_sim(zDim=0):
resolution = 10
sim = mp.Simulation(cell_size=cell,
- boundary_layers=pml_layers,
- geometry=geometry,
- sources=sources,
- resolution=resolution)
+ boundary_layers=pml_layers,
+ geometry=geometry,
+ sources=sources,
+ resolution=resolution)
# Line monitor
sim.add_flux(1,0,1,mp.FluxRegion(center=mp.Vector3(5,0,0),size=mp.Vector3(0,4,4), direction=mp.X))
diff --git a/src/dft.cpp b/src/dft.cpp
index cf5177caa..0ecf4825f 100644
--- a/src/dft.cpp
+++ b/src/dft.cpp
@@ -174,7 +174,26 @@ dft_chunk *fields::add_dft(component c, const volume &where, const double *freq,
dft_chunk_data data;
data.c = c;
data.vc = vc;
+
+ if (decimation_factor == 0) {
+ double tol = 1e-7;
+ double src_freq_max = 0;
+ for (src_time *s = sources; s; s = s->next) {
+ if (s->get_fwidth(tol) == 0)
+ decimation_factor = 1;
+ else
+ src_freq_max = std::max(src_freq_max, std::abs(s->frequency().real())+0.5*s->get_fwidth(tol));
+ }
+ double freq_max = 0;
+ for (size_t i = 0; i < Nfreq; ++i)
+ freq_max = std::max(freq_max, std::abs(freq[i]));
+ if ((freq_max > 0) && (src_freq_max > 0))
+ decimation_factor = std::max(1, int(std::floor(1/(dt*(freq_max + src_freq_max)))));
+ else
+ decimation_factor = 1;
+ }
data.decimation_factor = decimation_factor;
+
data.omega.resize(Nfreq);
for (size_t i = 0; i < Nfreq; ++i)
data.omega[i] = 2 * pi * freq[i];
diff --git a/src/meep.hpp b/src/meep.hpp
index aeb28211e..7dc9fdf93 100644
--- a/src/meep.hpp
+++ b/src/meep.hpp
@@ -973,6 +973,7 @@ class src_time {
return 1;
}
virtual std::complex
frequency() const { return 0.0; }
+ virtual double get_fwidth(double tol) const { return 0.0; }
virtual void set_frequency(std::complex f) { (void)f; }
private:
@@ -994,6 +995,7 @@ class gaussian_src_time : public src_time {
virtual src_time *clone() const { return new gaussian_src_time(*this); }
virtual bool is_equal(const src_time &t) const;
virtual std::complex frequency() const { return freq; }
+ virtual double get_fwidth(double tol) const;
virtual void set_frequency(std::complex f) { freq = real(f); }
std::complex fourier_transform(const double f);
@@ -1014,6 +1016,7 @@ class continuous_src_time : public src_time {
virtual src_time *clone() const { return new continuous_src_time(*this); }
virtual bool is_equal(const src_time &t) const;
virtual std::complex frequency() const { return freq; }
+ virtual double get_fwidth(double tol) const { return 0.0; };
virtual void set_frequency(std::complex f) { freq = f; }
private:
@@ -1046,6 +1049,7 @@ class custom_src_time : public src_time {
virtual src_time *clone() const { return new custom_src_time(*this); }
virtual bool is_equal(const src_time &t) const;
virtual std::complex frequency() const { return freq; }
+ virtual double get_fwidth(double tol) const { return 0.0; };
virtual void set_frequency(std::complex f) { freq = f; }
private:
@@ -1925,7 +1929,7 @@ class fields {
std::complex stored_weight = 1.0, dft_chunk *chunk_next = 0,
bool sqrt_dV_and_interp_weights = false,
std::complex extra_weight = 1.0, bool use_centered_grid = true,
- int vc = 0, int decimation_factor = 1) {
+ int vc = 0, int decimation_factor = 0) {
return add_dft(c, where, linspace(freq_min, freq_max, Nfreq), include_dV_and_interp_weights,
stored_weight, chunk_next, sqrt_dV_and_interp_weights, extra_weight,
use_centered_grid, vc, decimation_factor);
@@ -1935,13 +1939,13 @@ class fields {
std::complex stored_weight = 1.0, dft_chunk *chunk_next = 0,
bool sqrt_dV_and_interp_weights = false,
std::complex extra_weight = 1.0, bool use_centered_grid = true,
- int vc = 0, int decimation_factor = 1);
+ int vc = 0, int decimation_factor = 0);
dft_chunk *add_dft(component c, const volume &where, const std::vector& freq,
bool include_dV_and_interp_weights = true,
std::complex stored_weight = 1.0, dft_chunk *chunk_next = 0,
bool sqrt_dV_and_interp_weights = false,
std::complex extra_weight = 1.0, bool use_centered_grid = true,
- int vc = 0, int decimation_factor = 1) {
+ int vc = 0, int decimation_factor = 0) {
return add_dft(c, where, freq.data(), freq.size(), include_dV_and_interp_weights, stored_weight,
chunk_next, sqrt_dV_and_interp_weights, extra_weight, use_centered_grid, vc,
decimation_factor);
@@ -1962,34 +1966,34 @@ class fields {
void update_dfts();
dft_flux add_dft_flux(const volume_list *where, const double *freq, size_t Nfreq,
bool use_symmetry = true, bool centered_grid = true,
- int decimation_factor = 1);
+ int decimation_factor = 0);
dft_flux add_dft_flux(const volume_list *where, const std::vector &freq,
- int decimation_factor = 1, bool use_symmetry = true,
+ int decimation_factor = 0, bool use_symmetry = true,
bool centered_grid = true) {
return add_dft_flux(where, freq.data(), freq.size(), use_symmetry, centered_grid,
decimation_factor);
}
dft_flux add_dft_flux(const volume_list *where, double freq_min, double freq_max, int Nfreq,
bool use_symmetry = true, bool centered_grid = true,
- int decimation_factor = 1) {
+ int decimation_factor = 0) {
return add_dft_flux(where, linspace(freq_min, freq_max, Nfreq), use_symmetry, centered_grid,
decimation_factor);
}
dft_flux add_dft_flux(direction d, const volume &where, double freq_min, double freq_max,
int Nfreq, bool use_symmetry = true, bool centered_grid = true,
- int decimation_factor = 1) {
+ int decimation_factor = 0) {
return add_dft_flux(d, where, linspace(freq_min, freq_max, Nfreq), use_symmetry, centered_grid,
decimation_factor);
}
dft_flux add_dft_flux(direction d, const volume &where, const std::vector &freq,
bool use_symmetry = true, bool centered_grid = true,
- int decimation_factor = 1) {
+ int decimation_factor = 0) {
return add_dft_flux(d, where, freq.data(), freq.size(), use_symmetry, centered_grid,
decimation_factor);
}
dft_flux add_dft_flux(direction d, const volume &where, const double *freq, size_t Nfreq,
bool use_symmetry = true, bool centered_grid = true,
- int decimation_factor = 1);
+ int decimation_factor = 0);
dft_flux add_dft_flux_box(const volume &where, double freq_min, double freq_max, int Nfreq);
dft_flux add_dft_flux_box(const volume &where, const std::vector &freq);
dft_flux add_dft_flux_plane(const volume &where, double freq_min, double freq_max, int Nfreq);
@@ -1997,33 +2001,33 @@ class fields {
// a "mode monitor" is just a dft_flux with symmetry reduction turned off.
dft_flux add_mode_monitor(direction d, const volume &where, double freq_min, double freq_max,
- int Nfreq, bool centered_grid = true, int decimation_factor = 1) {
+ int Nfreq, bool centered_grid = true, int decimation_factor = 0) {
return add_mode_monitor(d, where, linspace(freq_min, freq_max, Nfreq), centered_grid,
decimation_factor);
}
dft_flux add_mode_monitor(direction d, const volume &where, const std::vector &freq,
- bool centered_grid = true, int decimation_factor = 1) {
+ bool centered_grid = true, int decimation_factor = 0) {
return add_mode_monitor(d, where, freq.data(), freq.size(), centered_grid,
decimation_factor);
}
dft_flux add_mode_monitor(direction d, const volume &where, const double *freq, size_t Nfreq,
- bool centered_grid = true, int decimation_factor = 1);
+ bool centered_grid = true, int decimation_factor = 0);
dft_fields add_dft_fields(component *components, int num_components, const volume where,
double freq_min, double freq_max, int Nfreq,
- bool use_centered_grid = true, int decimation_factor = 1) {
+ bool use_centered_grid = true, int decimation_factor = 0) {
return add_dft_fields(components, num_components, where, linspace(freq_min, freq_max, Nfreq),
use_centered_grid, decimation_factor);
}
dft_fields add_dft_fields(component *components, int num_components, const volume where,
const std::vector &freq, bool use_centered_grid = true,
- int decimation_factor = 1) {
+ int decimation_factor = 0) {
return add_dft_fields(components, num_components, where, freq.data(), freq.size(),
use_centered_grid, decimation_factor);
}
dft_fields add_dft_fields(component *components, int num_components, const volume where,
const double *freq, size_t Nfreq, bool use_centered_grid = true,
- int decimation_factor = 1);
+ int decimation_factor = 0);
/********************************************************/
/* process_dft_component is an intermediate-level */
@@ -2069,41 +2073,41 @@ class fields {
std::complex overlaps[2]);
dft_energy add_dft_energy(const volume_list *where, double freq_min, double freq_max, int Nfreq,
- int decimation_factor = 1) {
+ int decimation_factor = 0) {
return add_dft_energy(where, linspace(freq_min, freq_max, Nfreq), decimation_factor);
}
dft_energy add_dft_energy(const volume_list *where, const std::vector &freq,
- int decimation_factor = 1) {
+ int decimation_factor = 0) {
return add_dft_energy(where, freq.data(), freq.size(), decimation_factor);
}
dft_energy add_dft_energy(const volume_list *where, const double *freq, size_t Nfreq,
- int decimation_factor = 1);
+ int decimation_factor = 0);
// stress.cpp
dft_force add_dft_force(const volume_list *where, double freq_min, double freq_max, int Nfreq,
- int decimation_factor = 1) {
+ int decimation_factor = 0) {
return add_dft_force(where, linspace(freq_min, freq_max, Nfreq), decimation_factor);
}
dft_force add_dft_force(const volume_list *where, const std::vector &freq,
- int decimation_factor = 1) {
+ int decimation_factor = 0) {
return add_dft_force(where, freq.data(), freq.size(), decimation_factor);
}
dft_force add_dft_force(const volume_list *where, const double *freq, size_t Nfreq,
- int decimation_factor = 1);
+ int decimation_factor = 0);
// near2far.cpp
dft_near2far add_dft_near2far(const volume_list *where, double freq_min, double freq_max,
- int Nfreq, int decimation_factor = 1, int Nperiods = 1) {
+ int Nfreq, int decimation_factor = 0, int Nperiods = 1) {
return add_dft_near2far(where, linspace(freq_min, freq_max, Nfreq), decimation_factor,
Nperiods);
}
dft_near2far add_dft_near2far(const volume_list *where, const std::vector &freq,
- int decimation_factor = 1, int Nperiods = 1) {
+ int decimation_factor = 0, int Nperiods = 1) {
return add_dft_near2far(where, freq.data(), freq.size(), decimation_factor,
Nperiods);
}
dft_near2far add_dft_near2far(const volume_list *where, const double *freq, size_t Nfreq,
- int decimation_factor = 1, int Nperiods = 1);
+ int decimation_factor = 0, int Nperiods = 1);
// monitor.cpp
std::complex get_chi1inv(component, direction, const vec &loc, double frequency = 0,
bool parallel = true) const;
diff --git a/src/sources.cpp b/src/sources.cpp
index 65eda579c..3c814bd47 100644
--- a/src/sources.cpp
+++ b/src/sources.cpp
@@ -105,6 +105,13 @@ std::complex gaussian_src_time::fourier_transform(const double f) {
return width * polar(1.0, omega * peak_time) * exp(-0.5 * delta * delta);
}
+// bandwidth (in frequency units, not angular frequency) of the
+// continuous Fourier transform of the Gaussian source function
+// when it has decayed by a tolerance tol below its peak value
+double gaussian_src_time::get_fwidth(double tol) const {
+ return sqrt(-2.0 * log(tol)) / (width * pi);
+}
+
bool gaussian_src_time::is_equal(const src_time &t) const {
const gaussian_src_time *tp = dynamic_cast(&t);
if (tp)
diff --git a/tests/harmonics.cpp b/tests/harmonics.cpp
index 81a8eb9ec..2f318c035 100644
--- a/tests/harmonics.cpp
+++ b/tests/harmonics.cpp
@@ -45,9 +45,12 @@ void harmonics(double freq, double chi2, double chi3, double J, double &A2, doub
f.add_point_source(Ex, src, vec(-0.5 * sz + dpml), J);
vec fpt(0.5 * sz - dpml - 0.5);
- dft_flux d1 = f.add_dft_flux(Z, volume(fpt), freq, freq, 1);
- dft_flux d2 = f.add_dft_flux(Z, volume(fpt), 2 * freq, 2 * freq, 1);
- dft_flux d3 = f.add_dft_flux(Z, volume(fpt), 3 * freq, 3 * freq, 1);
+ dft_flux d1 = f.add_dft_flux(Z, volume(fpt), freq, freq, 1, true, true,
+ 1 /* decimation_factor */);
+ dft_flux d2 = f.add_dft_flux(Z, volume(fpt), 2 * freq, 2 * freq, 1, true, true,
+ 1 /* decimation_factor */);
+ dft_flux d3 = f.add_dft_flux(Z, volume(fpt), 3 * freq, 3 * freq, 1, true, true,
+ 1 /* decimation_factor */);
double emax = 0;