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6257254579
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add fdfd.poynting_e_cross_h()
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2019-10-27 12:41:08 -07:00 |
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88123342be
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note that venv is optional
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2019-10-10 00:01:57 -07:00 |
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9709a0a415
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make subheading smaller
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2019-10-09 00:11:27 -07:00 |
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cde8537f14
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add see-also links
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2019-10-09 00:10:46 -07:00 |
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ca7bc71788
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add git to necessary programs
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2019-10-09 00:03:31 -07:00 |
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2ba75a4189
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branch name changes to
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2019-10-09 00:00:24 -07:00 |
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c6e463209f
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Update repo location
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2019-10-08 23:59:22 -07:00 |
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6c032fbdc3
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Note temporary source location
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2019-10-08 23:59:03 -07:00 |
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74e212f560
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examples require gridlock
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2019-10-08 23:56:49 -07:00 |
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7f22f83c68
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Update README with install instructions
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2019-10-08 23:56:33 -07:00 |
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6850fe532f
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poynting calculation comparison
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2019-09-27 20:48:03 -07:00 |
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6333dbd110
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add missing __init__.py's
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2019-09-27 20:47:22 -07:00 |
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0ad289e5ac
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Switch to file-based version number
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2019-09-27 20:44:31 -07:00 |
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487bdd61ec
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Fixup poynting operators for new approach
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2019-09-27 20:43:32 -07:00 |
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a1a7aa5511
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Alternate approach to poynting matrices
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2019-09-14 19:59:08 +02:00 |
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9cd2dd131b
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Move version into setup.py and read it back with pkg_resources
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2019-09-12 12:21:09 +02:00 |
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c92656bed8
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Compactify args
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2019-09-05 22:53:43 +02:00 |
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10e275611d
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Use overlap_e
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2019-09-05 22:42:39 +02:00 |
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2289c6d116
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dx_prop should be a scalar?
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2019-09-05 22:42:20 +02:00 |
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bedec489aa
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Don't pre-conjugate e_overlap
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2019-09-05 22:41:34 +02:00 |
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f04c0daf28
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solve_waveguide_mode_2d -> vsolve_*
- return (e_xy. wavenumber)
- vectorized inputs since we returned a vectorized output
- exy -> e_xy
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2019-09-05 22:41:06 +02:00 |
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b5ad284966
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dx_prop -> prop_phase
propagation direction wavenumber might be different from
operator-derived (2D) wavenumber due to numerical dispersion, so lump it
in with dx_prop
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2019-09-05 22:35:23 +02:00 |
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8eac9df76e
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in progress
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2019-08-30 22:03:54 -07:00 |
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a4c2239ad9
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formatting
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2019-08-27 00:40:59 -07:00 |
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e99019b37f
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v -> e_xy for cylindrical mode result
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2019-08-27 00:40:49 -07:00 |
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f4bac9598d
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Remove unused waveguide_mode functions
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2019-08-26 01:18:44 -07:00 |
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d2d4220313
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update example code
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2019-08-26 01:12:36 -07:00 |
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337cee8018
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Add epsilon arg to compute_overlap_e
currently unused but useful for reusing solve_wgmode arguments
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2019-08-26 01:10:54 -07:00 |
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5f96474497
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Use e_boundary_source for compute_source
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2019-08-26 01:03:13 -07:00 |
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7b56aa363f
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Use non-vectorized fields for waveguide_mode functions
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2019-08-26 01:02:54 -07:00 |
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3887a8804f
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fix phase in expand_wgmode
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2019-08-26 00:28:19 -07:00 |
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d6a34b280e
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Simplify compute_source and fix propagation direction
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2019-08-26 00:28:06 -07:00 |
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1860d754cd
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Fix shifts applied to E and H fields
Only some components need shifting
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2019-08-26 00:27:32 -07:00 |
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7006b5e6e4
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Flip propagation direction by flipping H
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2019-08-26 00:27:05 -07:00 |
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c306bb1f46
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Correct for numerical dispersion at 3d solve_waveguide_mode level
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2019-08-26 00:26:54 -07:00 |
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af8efd00eb
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Add E-field versions of waveguide mode operators, rename v->e_xy or h_xy, and add ability to specify mode margin in solve_waveguide_mode_2d
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2019-08-26 00:25:36 -07:00 |
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41bec05d4e
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Remove unwanted return
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2019-08-26 00:24:17 -07:00 |
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2787908640
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Add E variants of waveguide equations
rename 2d vector from v to e_xy or h_xy
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2019-08-26 00:21:39 -07:00 |
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054ac994d5
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Don't perform dx_prop wavenumber correction in waveguide_mode_2d
It's technically a correction for discretization in the third direction
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2019-08-26 00:17:52 -07:00 |
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0503e9d6ef
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Fix shift_with_mirror() for C-ordered arrays
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2019-08-26 00:16:45 -07:00 |
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b466ed02ea
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Add e_boundary_source
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2019-08-26 00:16:27 -07:00 |
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ccdb423ba2
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add e_tfsf_source
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2019-08-26 00:15:34 -07:00 |
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aade81c21e
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alternate src formulation
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2019-08-07 02:27:04 -07:00 |
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07c94617fe
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Operator-based soruce
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2019-08-07 01:01:55 -07:00 |
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1a04bab361
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Fixup slices
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2019-08-07 01:01:35 -07:00 |
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2c91ea249f
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Fix wgmode expansion
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2019-08-07 01:00:57 -07:00 |
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3429120993
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d_prop -> dx_prop
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2019-08-07 01:00:21 -07:00 |
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938c4c9a35
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move to 3xnnn arrays
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2019-08-05 01:09:52 -07:00 |
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5951f2bdb1
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various fixes and improvements
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2019-08-05 00:20:06 -07:00 |
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94ff3f7853
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further fdfd_tools->meanas updates
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2019-08-04 14:13:51 -07:00 |
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