3/26/2021
-
New
get_epsilon_grid
function for evaluating ε on user-specified grid with arbitrary resolution (#1522). -
Support for user-specified chunk layouts for manual control over load-balancing (#1528).
-
MaterialGrid
design_parameters
is renamed toweights
andU_SUM
is renamed toU_MEAN
(#1512). -
Performance improvement in chunk division (#1499).
-
Various bugfixes (#1487, #1515, #1519, #1521, #1527), additional documentation, and tests.
1/8/2021
- Fix accidental breakage of the adjoint routines (#1464).
1/4/2021
-
get_array_slice
now does continuous interpolation as the slice position is moved (#1456). -
New
contour
option for contour-plotting inplot2D
(#1437). -
Adjoint optimization of
near2far
transformations (#1417). -
get_array_metadata
is now consistent between array slices and DFT slices (#1456), no longer leaks memory (#1447), and returns numpy arrays rather than tuples (#1458). -
Bugfixes in adjoint-optimization filters (#1427).
10/20/2020
- Bugfix in adjoint code (#1403).
10/6/2020
-
New API for specifying planewave diffraction orders for eigenmode sources and coefficients (#1316).
-
More accurate gradients in adjoint code (#1285).
-
Simpler Python API for outputting ε or μ at a given frequency (#1374).
-
--with-libctl-dir
option ofconfigure
now accepts simply the installationprefix
in addition toprefix/share/libctl
(#1286). -
Less verbose mode-solver output from MPB (#1302, #1388), and new
meep.verbosity
option in Python (#1349). -
Bug fix for single-point DFT monitor (#1333).
7/8/2020
-
Minimum-lengthscale filters for adjoint optimization (#1205).
-
Python API documentation in docstrings (#1240).
-
MaterialGrid
material type in Python to interpolate an array of material values as the "material" of an object, especially for topology optimization (#1242). -
merge_subgroup_data
Python function for coordinating parallel computations (#1192). -
Eigenmode sources now ensure that the source has the same frequency as the mode (#1218).
-
Performance improvements to eigenmode sources (#1233, #1244, #1257).
4/17/2020
-
New adjoint solver for density-based topology optimization, including filtering, automatic differentiation, and other frequencies (#1167).
-
DFT functions now allow you to pass an arbitrary array of frequencies, instead of being limited to equally spaced frequencies (#1154 and #1156).
-
Experimental shift-and-invert frequency-domain eigensolver (#1158).
-
Renamed
omega
parameter tofrequency
at some places in the Python API, for consistency (#1171), anddft_fields
object now takesfcen
anddf
instead offreq_min
andfreq_max
in Python. -
Support for SWIG 4.0 (#1159), and various other minor fixes.
2/25/2020
- Avoid writing to source directory in remaining tests (#1132).
2/19/2020
-
Optional parameter
omega
foroutput-epsilon
and similar functions, allowing the complex ε and μ at a given frequency to be outputted (#1112, following #919). -
near2far
computation now supports cylindrical coordinates (#1090). -
Experimental support for slanted prisms (requires libctl 4.5) via
sidewall_angle
parameter to prism objects (#1129). -
New
yee_grid=False
optional argument toadd_dft_fields
; by passingTrue
one can compute the fields on the original Yee grid (#1095). -
New function
meep::make_output_directory()
to make a temporary directory (inTMPDIR
or similar) andmeep::delete_directory(path)
to perform recursive deletion (likerm -rf
). These are now used in tests to avoid writing to the source directory (#1121, #1122 and #1126). -
Jupyter notebooks now show a graphical progress bar during simulations (#1078).
-
kz-2d
option in Scheme, mirroring Pythonkz_2d
(#1062). -
Various bugfixes, documentation supplements, and other minor improvements.
11/12/19
-
Faster 2d simulations with nonzero
kz
via thekz_2d
option (#1047). -
New Meep
verbosity
option supersedingquiet
andverbose
flags (#994). -
Output now only shows ≤ 10 geometric objects by default (#1002).
-
Performance improvements for
split_chunks_evenly=False
.
7/29/19
-
Experimental support for gyrotropic media including magneto-optical effects (#863).
-
Mode decomposition for oblique waveguides (#940, #945) and dispersive materials (#919).
-
Accept tuples in place of Vector3 arguments (#960).
-
Capture C++ error messages in Python notebooks (#953).
-
Automatically abort simulation if the fields blow up (#922).
-
Various small bugfixes and documentation improvements.
6/5/19
-
New Python functions for simple visualization of the simulation domain (#872).
-
Capture Meep and MPB output in Python notebooks (#891, #894)
-
Add optional
meep.quiet()
parameter to the Python interface (#876). -
Python evaluation of materials ε(ω) and μ(ω) (#862).
-
Experimental multithreading support for near2far calculation (#868) and other speedups (#869).
-
Add
stop_after_walltime
andstop_on_interrupt
in Python (#860). -
GDSII file introspection (#817).
-
Various small bugfixes and documentation improvements.
4/17/19
-
Adjoint solver to compute sensitivity of solution to material perturbations (#795).
-
Experimental
do_averaging
feature for user-defined material functions (#771, #791). -
Periodic boundaries support in
near2far
vianperiods
option (#769, #789). -
Eigenmode sources are normalized to unit power (#728).
-
Fix interpolation of DFT slice output (#787).
-
Bug fix in
run-k-points
(#779). -
Eigenmode sources for negative angles (#752).
-
Various other minor bugfixes, build fixes, documentation improvements, tutorials, etcetera.
2/13/19
-
libctl 4.2 is required
-
Add
--without-scheme
flag to./configure
(#705) -
Improve error messages in Python interface (#699)
-
Allow
kguess
to specify MPB lattice vector for launching oblique waveguide modes (#675) -
Allow user materials when checking for conductivity (#689)
-
Add
split_chunks_evenly
flag toSimulation
constructor. Setting toFalse
will improve parallel simulation performance by dividing chunks based on work instead of size (#681) -
Added
Simulation.visualize_chunks()
to visualize the chunk layout (#671) -
Improved stability of lorentzian susceptibility (#666)
-
Get array metadata for
get_array
andget_dft_array
(#655) -
Add ability to get a source slice as a numpy array (#652)
-
Fixed performance issues in ModeSolver.find_k (#644)
-
Add
force_all_components
flag toSimulation
constructor (#631) -
libmeepgeom was merged into libmeep (#630)
-
Expose
run_k_point
to access more Harminv data (#626) -
Various other bug fixes, documentation improvements, etc.
11/16/18
-
Add
transform
method tomeep.Medium
(#603). -
Read epsilon input from a numpy array when passed to a
Simulation
asdefault_material
(#593). -
Support
geometry_center
in Python (#599). -
Add Python
Ldos
class (#581). -
Compute Fourier-transformed fields (e.g. fluxes) in
solve_cw
(#570). -
Enable builds without MPB (#558).
-
Add birefringent materials to materials library (#559).
-
Print dominant planewave in
get_eigenmode
(#531). -
Python API for GDSII regions (#518)
-
Multilevel atom susceptibilities for Python and Scheme (#500).
-
Fix bug in
get_eigenmode_coefficients
for 2d cell with non-zero kz (#602). -
Fix sync of eigenmode calculation when no mode is found (#596).
-
Fix memory leak in
get_dft_array
(#577). -
Use same MPB phase on all processes, fixing bug with eigenmodes and multiprocessing (#578).
-
Fix memory leaks in
get_eigenmode
(#558). -
Various other bug fixes, documentation improvements, etc.
9/7/2018
-
Python interface to import GDSII files (#392).
-
New binary grating tutorial (#376).
-
Get source amplitude from HDF5 file (#388).
-
get_eigenmode_coefficients now returns group velocity and kpoints (#396).
-
New tutorial for visualizing 3d structures (#416).
-
Mode decomposition feature supports symmetries (#417).
-
Support for Guile >= 2.0.12 (#419). Merged upstream to SWIG repo (#1288).
-
Python get_eigenmode function and EigenmodeData class (#422)
-
Symmetry support in dft arrays (#427).
-
Python 3.7 support (#456).
-
get-eigenmode-coefficients added to Scheme API (#477).
-
materials_library.py now part of Python package (e.g., from meep.materials import Al) (#479).
-
materials-library.scm automatically available in Meep scripts (#483).
-
Structure dump/load feature now supports dispersive materials (#454).
-
Various bug fixes, documentation improvements, etc.
6/7/2018
-
Python interface to MPB (#191 etc.).
-
Mode decomposition: given a DFT flux plane, decompose the fields at each frequency into the power in each mode of a waveguide or similar (#192, #248, etc.).
-
DFT slices: output Fourier-transformed fields in any given region of space (#259).
-
New
prism
geometric-object type for polygonal prisms (#341, #345) for upcoming GDSII import (#357). Libctl 4.1.0 is required. -
Structure dump/load feature to rapidly load in a geometry from a previous calculation (#261, #266).
-
Susceptibilities are now supported in user-defined materials in Python (#203, #305).
-
64-bit support for extremely large computations (#193).
-
Various bug fixes, documentation improvements, etc.
2/1/2018
- Allow
meep
Python module to be imported without settingPYTHONPATH
(#189).
1/26/2018
- Build fix for Python due to missing file (#184).
1/19/2018
- Minor packaging fixes.
1/18/2018
-
Full-featured Python interface.
-
Migrated documentation to github/markdown/readthedocs (#55).
-
New feature to get slice as array in C++ and Python APIs (#96, #105).
-
libmeepgeom
library to allow C++ users to access geometric-object API (#56). -
Removed overly conservative stability check for Lorentzian susceptibilities (#150).
-
Corrected small error in frequency interval for
dft-ldos
(#40). -
Bug fixes in near-to-farfield spectra (#21), eigenmode source (#20), and LDOS (#40).
31 March 2015.
-
New near-to-far-field functionality: given a bounding surface, automatically computes the Fourier-transformed field in any desired grid of "far-field" points arbitrarily far away.
-
Compatibility with Harminv 1.4 (fixes issue #13: ppc64 portability).
-
Fix compilation with latest C++ standard (e.g. on OS X 10.9).
-
Bug fix in CW solver convergence test; thanks to Wu Chuanren and @FilipDominec for the bug report.
-
Build fix for Fedora 21 (thanks to Dean Brettle) (issue #14).
2 April 2014.
-
Added new absorber type, as an alternative to PML, which simply provides a scalar conductivity gradient for cases where PML fails.
-
Fixed bug which sometimes prevented dispersive materials from being used in PML regions.
-
Some fixes to BLAS/LAPACK linking.
-
Bug fixes in LDOS computation.
-
Work around gcc bug #54498, which caused a spurious PML test failure with gcc 4.7 and 4.7.1; thanks to Brahmanand Jogai and Thorsten Alteholz for the bug reports.
20 July 2012.
-
Fixed to work with Guile version 2.x (older versions still work); requires libctl 3.2 or later.
-
Added
epsilon-input-file
feature to read a scalar dielectric function from an HDF5 file (similar to MPB). -
Support for anisotropic dispersive materials (tensor sigma parameter).
-
Support for Drude dispersion model. New syntax is
make drude-susceptibility
,make lorentzian-susceptibility
, etc. (oldmake polarizability
is still supported for backwards compatibility). -
Support for "thermal" dispersive materials which include noise term in the polarization.
-
Added
dft-ldos
feature for efficient LDOS-spectrum computation. -
Documented stress-tensor (force) spectrum computation feature.
-
Added
mean-stretch
property of PML (defaults to 1), to support real coordinate stretching for damping evanescent modes. -
Support for eigenmode-source feature using upcoming MPB release.
-
Various small bugfixes.
31 August 2009.
-
Added
make check
test (in 2D_convergence) for newspecial-kz?
feature (for computing out-of-plane modes in 2d more efficiently). -
Fix typo preventing Casimir calculations from running for periodic problems.
24 August 2009.
- Fixed release bug preventing Casimir calculation from running.
20 August 2009.
-
Meep's PML is now a true PML for arbitrary anisotropic, dispersive, and conducting media. (Now uses a slightly unconventional reformulation of PML described at ab-initio.mit.edu/meep/pml-meep.pdf)
-
Fixed bug which caused anisotropic non-diagonal mu to be unstable.
-
Fix compilation failure with gcc 4.4 due to missing cstdio header (thanks to Linran Fan and Bin Shao for the bug reports).
-
C++ interface: volume was renamed to grid_volume and geometric_volume was renamed to volume, to better reflect their respective roles.
-
Added
accurate-fields-near-cylorigin?
option to have more accurate fields near the r=0 origin for large m in cylindrical coordinates, at the expense of requiring a smaller Courant factor. (Default isfalse
, corresponding to behavior in older Meep versions.) -
In 2d computational cells, added much more efficient support for exp(ikz) z-dependence, enabled by new
special-kz?
input variable (default isfalse
since it only works in 2d and is a little subtle for real fields). -
Includes preliminary new features to aid in computation of optical forces (both classical and quantum Casimir forces); further documentation pending more testing.
-
Removed obsolete
doc
directory (all documentation is on the website these days). -
Small performance improvements in Lorentzian dispersion handling.
-
Fix configure script failure when cross-compiling.
-
Fix compilation failure with MPICH.
5 June 2009.
- Allow
GUILE_CONFIG
environment variable to override location ofguile-config
program inconfigure
script; this is useful when cross-compiling.
2 June 2009.
-
Correct superficial
make check
failure on 32-bit x86 machines with gcc 4.3.x, due to slight impact on floating-point rounding by automatic SSE/SSE2 vectorization; thanks to Silviu Popescu for the bug report. -
Correct superficial
make check
failure when compiling under icc.
Meep 1.0.1
28 May 2009.
-
Enable correct operation and passed test suite when
MEEP_SINGLE
(single-precision) mode is enabled in meep.hpp; thanks to Seyoon Kim for the bug reports. -
Use new automake features to have less-verbose build output by default (you can build in verbose mode by
make V=1
), and running all test programs then reporting which ones failed instead of stopping at the first failure. -
Fix superficial failure in 2D_convergence test under gcc 3.4.6; thanks to Alex Prengel for the bug report.
-
Fix failure in flux test under gcc 4.3.1 in some cases; thanks to Alex Prengel for the bug report.
-
Fix compilation problem with gcc 4.4, correcting Debian bug #505002.
28 April 2009.
-
New timestepping scheme for off-diagonal anisotropic epsilon and mu, based on technique by Werner and Cary [ J. Comp. Phys. 226, 1085 (2007) ], that improves FDTD stability when anisotropy is present (such as when subpixel averaging is used on isotropic media).
-
Scheme user interface now supports user-specified anisotropic (real-symmetric) epsilon and mu (via epsilon-diag, epsilon-offdiag, mu-diag, and mu-offdiag parameters, similar to MPB). Accurate subpixel averaging of anisotropic media based on the method by Kottke, Farjadpour, & Johnson [ Phys. Rev. E. 77, 036611 (2008) ].
-
Anisotropic dispersive materials are now supported, although currently the dispersive part of the epsilon/mu tensor must be diagonal, via the new sigma-diag parameter of polarizability. (The corresponding C++ interface has also removed delta_epsilon.)
-
The delta-epsilon parameter of polarizability has been removed; you should use sigma instead.
-
New
fields::integrate2
function (and corresponding Scheme functionintegrate2-field-function
) to perform integrations involving two simulations with the same computational cell (e.g. field-overlap calculations for coupled-mode theory). -
In the Scheme interface, subpixel averaging is not used for user-specified material-function types; you only get subpixel averaging for the standard shapes (blocks, cylinders, etcetera).
-
Haskell code-generation is no longer used, and hsrc directory is removed. Bitrotted and undocumented (hence unused) saturable-absorber feature has been removed, along with energy-saturation parameter of polarizability.
-
Some bug-fixes to test programs that made them overly sensitive to roundoff errors and possibly fail depending on the compiler. (New
fields::round_time
and meep-round-time functions to round times to single-precision, useful for robust time comparisons.)
17 March 2009.
-
Bug fix in cylindrical code, which caused it to blow up in some circumstances for nonzero m.
-
Bug fix: non-integrated sources with conductivity are now second-order accurate, thanks to Alejandro Rodriguez.
-
Bug fix in writing strings with parallel HDF5, thanks to Zheng Li for the bug report.
-
Check that PML parameters are sensible (e.g. that total PML thickness is no greater than cell thickness) to avoid common mistakes.
-
New extra-materials input variable, so that you no longer have to use "dummy objects" to specify the existence of some materials when using material-function types.
24 July 2008.
- Fixed circular dependency in Makefile, which caused problems with some versions of make; thanks to Kaoru Narita for the bug report.
21 July 2008.
- Fixed incompatibility with Guile 1.6.x or earlier; thanks to the bug report by Andreas Unger.
20 July 2008.
-
Improved handling of nested synchronized-magnetic calls.
-
Bug fix: parallel builds (
make -j
) should now work. -
Bug fix: pkg-config file was incorrectly installed for MPI version; thanks to Majid Sodagar for the bug report.
19 July 2008.
-
Support for user-specified permeability (mu). Renamed
dielectric
tomedium
in libctl interface, newmu
property and new output-bfield and output-mu functions, and newPermeability
andBx
etc. field types. -
Support for user-specified electric and/or magnetic conductivities. These are especially useful to add a desired dissipation loss (an imaginary part of epsilon/mu) in a narrow bandwidth, without messing around with Lorentzian dispersive materials.
-
Add predefined perfect-magnetic-conductor (mu = -infinity) material, along with perfect-electric-conductor (eps = -infinity).
-
Added synchronized-magnetic step function to allow step functions to run with the electric and magnetic fields synchronized in time to second-order accuracy.
-
New PML implementation (UPML instead of split-field), should have lower reflection in many cases.
-
User-specified PML profile and asymptotic reflection.
-
Internally, all timestepping code is now handwritten (and much shorter) rather than old verbose Haskell-generated code; this should make it easier to add new features.
-
Add support for non-integrated current sources, if the is-integrated? property of the current is set to false; this is now the default, to make handling of E and H sources more similar and intuitive.
-
Work with HDF5 1.8 (which previously would not compile unless you manually set a preprocessor flag, due to API changes).
-
Check for ctl.h in /usr/include/ctl/ctl.h (default in Fedora), and check for libctl in /usr/share/libctl3 (default in Debian & Ubuntu).
-
Bug fix: fixed relative phase of E and H sources (which were off from one another by half a timestep); thanks to M. Megens for bug report.
-
Bug fix: make sure h5 filenames have unique timestep for cases where dt is very small or very large.
13 Nov. 2007.
-
Bug fix in flux_in_box, which accidentally returned the flux multiplied by the number of processors, instead of the flux.
-
Bug fix in epsilon averaging for structures including metals (
epsilon < 0
), fixing an instability. -
Bug fix in output-png when running in parallel (removing race condition).
-
Fixed bug that disabled subpixel averaging for dimensions=1 (thanks to Mischa Megens for the bug report).
-
Fixed bug that caused output-tot-pwr to stop Meep with an error message; thanks to Vyacheslav Sokolov for the bug report.
-
Make
at-every
step functions less susceptible to rounding errors; thanks to L. Le Guyader for the bug report. -
Fixed bug in dispersive media that wasted memory on parallel machines (the polarization memory was not parallelized); thanks to J. L. Silva for the bug report.
-
Bug fix in output-png+h5, thanks to a report by Chad Husko.
-
Fixed several deadlocks that could occur when the parallel Meep is used with a serial HDF5 library (we continue to recommend using the parallel HDF5 library with parallel Meep, however). Thanks in part to Lingling Tang for his bug report.
-
For maintainer-mode, improved detection of Haskell package names; thanks to Liang Huo for the bug report.
21 Aug. 2006.
-
eps-averaging?
is now turned on by default (in libctl interface), using much-improved algorithm by Ardavan Farjadpour. This greatly improves accuracy, and also allows continuous tuning of geometric parameters. (See our upcoming paper in Optics Lett., with a preprint linked on the web site.) New input variables subpixel-tol and subpixel-maxeval to control the accuracy of the subpixel averaging. -
Support for chi2 (Pockels) as well as chi3 (Kerr) nonlinearities.
-
Symmetries no longer require the cell size to be an even number of pixels. Previously, Meep exited with an error in this case, whereas now it simply adds an extra pixel to the cell size as needed.
-
New with-prefix step function to allow you to use a different filename-prefix for selected outputs.
-
New feature for output-png: built-in shell variable $EPS that refers to the last-output epsilon .h5 file, which you can use to easily add dielectric contours/overlays to the field output image.
-
Added output-png+h5 function that outputs both .png and .h5 files.
-
New functions flux-in-box, electric-energy-in-box, magnetic-energy-in-box, and field-energy-in-box (convenience wrappers around C++ functions).
-
Bug fix in Kerr nonlinearity - chi3 was accidentally scaled by epsilon^4 factor.
-
Bug fix: if you specified three or more symmetries, at most two symmetries were used (ignoring the rest).
-
Bug fix in rotate2 symmetry, which wasn't working correctly.
-
Bug fix in add-flux for multiple flux regions, thanks to K. Choi.
-
Bug fix in harminv where it wouldn't allow you to call harminv more than once for the same run loop; thanks to Aristos Karalis.
-
Bug fix in save-flux/load-flux that prevented it from working properly without output directories, thanks to Karl Koch.
-
Fixed abort that sometimes occurred due to rounding when the source was the same width as the cell (thanks to G. J. Parker).
-
Fixed minor build problems on Cygwin, SGI, and other systems, thanks to Christopher Kang, Robyn Landers, Florencio Garcia, and others.
1 Apr. 2006.
- Initial public release.