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1.3.1

-----------------------------------

**2021-11-20**

- ``Survey.select`` removes now empty source-receiver-frequency pairs. If you
want the old behaviour set ``remove_empty=False``.

- Maintenance: Added a cron to GHA; 20th of every month at 14:14.

1.3.0

--------------------------------

**2021-10-27**

- ``electrodes``:

- New source ``TxMagneticPoint`` (requires ``discretize``; mainly used as
adjoint source for magnetic receivers; does not work in the presence of
magnetic permeabilities in the vicinity of the source).
- Both receivers (``Rx{Electric;Magnetic}Point``) can now produce their
proper adjoint (thanks to sgkang!).

- Changes in Simulation and parallel execution.

- Parallel computation is not sharing the simulation any longer.
- Parallel computation can new be done both file-based or all in memory.
The new possibility for file-based computation should make it possible
to compute responses for any amount of source-frequency pairs. See
parameter ``file_dir`` in the Simulation class (or corresponding parameter
in the CLI parameter file).
- ``get_model`` and ``get_hfield`` are now done on the fly, they are not
stored in a dict; ``simulation._dict_model`` and
``simulation._dict_hfield`` do not exist any longer.
- New methods ``jvec`` (sensitivity times a vector) and ``jtvec``
(sensitivity transpose times a vector). These methods are currently
experimental; documentation and examples are lacking behind.

- Various small things:

- Models and Fields return itself (not a copy) when the grid provided to
``interpolate_to_grid`` is the same as the current one.

1.2.1

----------------------------------

**2021-08-22**

- ``io``: Adjustment so that hdf5 tracks the order of dicts.

- ``simulations``:

- Adjust printing: correct simulation results for adjusted solver printing
levels; **default solver verbosity is new 1**; ``log`` can now be
overwritten in ``solver_opts`` (mainly for debugging).

- Functions moved out of ``simulations``: ``expand_grid_model`` moved to
``models`` and ``estimate_gridding_options`` to ``meshes``. The
availability of these functions through ``simulations`` will be removed in
v1.4.0.

- ``optimize``: the module is deprecated and will be removed in v1.4.0. The two
functions ``optimize.{misfit;gradient}`` are embedded directly in
``Simulation.{misfit;gradient}``.

1.2.0

--------------------

**2021-07-27**

- CLI:

- New parameters ``save`` and ``load`` to save and load an entire simulation.
In the parameter file, they are under ``[files]``; on the command line,
they are available as ``--save`` and ``--load``; they are followed by the
filename including its path and suffix. (In turn, the parameter
``store_simulation`` was removed.)

- ``simulations.Simulation``:

- Warns if the gradient is called, but ``receiver_interpolation`` is not
``'linear'``.
- Slightly changed the added noise in ``compute(observed=True)``: It uses new
the ``survey.add_noise`` attribute. There is new a flag to set if noise
should be added or not (``add_noise``), and if the amplitudes should be
chopped or not (``min_amplitude``). Also note that the added noise is new
white noise with constant amplitude and random phase.

- ``surveys``:

- New function ``random_noise``, which can be used to create random noise in
different ways. The default noise is white noise, hence constant amplitude
with random phase. (This is different to before, where random Gaussian
noise was added separately to the real and imaginary part.) For the random
noise it requires new at least NumPy 1.17.0.

- New attribute ``Survey.add_noise``, which uses under the hood above
function.

- A ``Survey`` can new be instantiated without receivers by setting
``receivers`` to ``None``. This is useful if one is only interested in
forward modelling the entire fields. In this case, the related data object
and the noise floor and relative error have no meaning. Also, in
conjunction with a Simulation, the misfit and the gradient will be zero.

- Various:

- All emg3d-warnings (not solver warnings) are now set to ``'always'``, and
corresponding print statements were removed.
- Simplified (unified) ``_edge_curl_factor`` (private fct).

1.1.0

-------------------------------------------

**2021-06-30**

This release contains, besides the usual small bugfixes, typos, and small
improvements, an important fix for ``optimize.gradient``. Keep in mind that
while the forward modelling is regarded as stable, the ``optimize`` module is
still work in progress.

The fixes with regard to ``optimize.gradient`` ensure that the gradient is
indeed using the proper adjoint to back-propagate the field. This is currently
*only* given for electric receivers, not yet for magnetic receivers. These
improvement happened mainly thanks to the help of Seogi (sgkang).

The changes in more detail:

- ``fields``:

- ``get_receiver`` has a new keyword ``method``, which can be ``'cubic'`` or
``'linear'``; default is the former, which is the same behaviour as before.
However, if you want to compute the gradient, you should set it to
``'linear'`` in your Simulation parameters. Otherwise the adjoint-state
gradient will not exactly be the adjoint state.
- ``get_source_field`` returns new the real-valued, frequency-independent
source vector if ``frequency=None``.
- ``get_source_field`` uses the adjoint of trilinear interpolation for point
sources (new). For dipoles and wires it the source is distributed onto the
cells as fraction of the source length (as before).

- ``electrodes``: Re-introduced the point source as ``TxElectricPoint``.

- ``simulations.Simulation``:

- New keyword ``receiver_interpolation``, which corresponds to the ``method``
in ``get_receiver`` (see above). Cubic is more precise. However, if you are
interested in the gradient, you need to choose linear interpolation at the
moment, as the point source is the adjoint of linear interpolation. To be
the proper adjoint for the gradient the receiver has to be interpolated
linearly too.
- If ``gridding`` is ``'same'`` or ``'input'``, it checks now if the provided
grid is a sensible grid for emg3d; if not, it throws a warning.

- ``meshes``: New function ``check_grid`` to verify if a given grid is good for
emg3d.

- ``optimize.gradient``: Changed order when going from computational grid to
inversion grid. Changing the grids at the field stage (cubic interpolation)
seems to be better than changing at the cell-averaged stage::

New: field_comp -> field_inv -> cells_inv
Old: field_comp -> cells_comp -> cells_inv

- ``cli``: Uses now by default linear receiver interpolation if the
``gradient`` is wanted (new), otherwise it uses cubic interpolation (as
before). The new keyword ``receiver_interpolation`` of the simulation can be
set in the parameter file, which overwrites the described default behaviour.

1.0.0

-------------------

**2021-05-28**

Here it is, three months of hard labour lead to v1.0.0!

There are _many_ changes, and they are listed below for each module.

*Your existing code will break, and I apologize for it. Please do not hesitate
to get in touch if you have troubles updating your code.*

**API**: With version 1.0 the API becomes stable and you can expect that your
code will work fine for the duration of ``emg3d v1.x``.

- Removed all deprecated features.
- Reduced top namespace to principal functions; ``get_receiver`` is not in the
top namespace any longer. It is advised to use directly the field method:
``field.get_receiver``.
- Moved emsig.github.io to emsig.xyz and emsig.readthedocs.io to
emg3d.emsig.xyz.
- Changed principal repo branch from ``master`` to ``main``.


Detailed changes by module
''''''''''''''''''''''''''


**CLI**

- Because frequencies are now dicts as well in a Survey they have to be named
by their key instead of their value when selecting data in the parameter
file.
- Entire configuration is now added to the log file.


**Core**

- ``restrict_weights``: New signature.


**Electrodes**

- New module containing all sources and receivers. Currently implemented are
``TxElectricDipole``, ``TxMagneticDipole``, ``TxElectricWire``,
``RxElectricPoint``, and ``RxMagneticPoint``.
- New class ``TxElectricWire`` for an arbitrary electric wire.
- Receivers can be defined in absolute coordinates, or in coordinates relative
to source position if they move with the source. Latter makes only sense
within a Survey/Simulation.
- ``dip`` is new called ``elevation`` to make it clear that it is the angle
positive upwards (anticlockwise from the horizontal plane).
- Bugfix of the loop area for a magnetic dipole (the area was previously wrong
except for dipoles of length of 1).
- Zero source strength does no longer mean "normalized", it means zero
strength (hence no source).
- Besides the sources and receivers it contains utilities how to move
electrodes in the coordinate system (e.g., ``rotation``).


**Fields**

- ``fields.Field``:

- Is *not* a subclassed ndarray any longer; with all its advantages and
disadvantages. E.g., operations on ``Field`` are not possible any longer
and have to be carried out on ``Field.field``. However, it should be easier
to maintain and expand in the future.
- New signature.
- Knows new its ``grid``. As a consequence, all functions that required
previously the ``grid`` and the ``field`` require new only the ``field``;
e.g., ``emg3d.fields.get_receiver``.
- Has no property ``ensure_pec`` any longer, it is ensured directly in
``solver.prolongation``.
- Has new the methods ``interpolate_to_grid`` and ``get_receiver``.

- Renamed parameters in all functions:

- ``src`` to ``source``;
- ``freq`` to ``frequency``;
- ``rec`` to ``receiver``.

- Removed functions and classes:

- ``SourceField``; it is just a regular ``Field`` now;
- ``get_receiver`` (the name still exists, but it is now what was before
``fields.get_receiver_response``).

- Renamed functions and classes (both do not take a ``grid`` any longer):

- ``get_h_field`` to ``get_magnetic_field``;
- ``fields.get_receiver_response`` to ``fields.get_receiver``.


**I/O**

- ``Model``, ``Field``, ``Survey``, and ``Simulation`` instances saved with an
older version of emg3d will not be able to de-serialize with version 1.0. You
have to update those files, see this gist:
https://gist.github.com/prisae/8345c3798e35f1c73efef617ac495538


**Maps**

- Changed function and class names:

- ``_Map`` to ``BaseMap``;
- ``grid2grid`` to ``interpolate`` (new signature);
- ``edges2cellaverages`` to ``interp_edges_to_vol_averages`` (new signature);
- ``volume_average`` to ``interp_volume_average`` (new signature);
- ``interp3d`` to ``interp_spline_3d`` (new signature).

- ``maps.interpolate``:

- Can now be used to interpolate values living on a grid to another grid or
to points defined either by a tuple or by an ndarray.
- The implemented interpolation methods are 'nearest' (new), 'linear',
'cubic', and 'volume'. Volume averaging ('volume') only works for
grid-to-grid interpolations, not for grid-to-points interpolations.
- Does not accept entire fields any longer. Entire fields can be mapped with
their own ``field.interpolate_to_grid`` method.

- Maps cannot be (de-)serialized any longer (``{to;from_dict}``); simply store
its name, which can be provided to ``models.Model``.

- Function ``rotation`` should be used for anything involving angles to use
the defined coordinate system consistently.


**Meshes**

- Changed function and class names:

- ``_TensorMesh`` to ``BaseMesh``;
- ``min_cell_width`` to ``cell_width``.
- ``get_origin_widths`` to ``origin_and_widths`` (has new finer loops to fine
grid sizes than before).

- ``meshes.BaseMesh``:

- Reduced to the attributes ``origin``, ``h``, ``shape_{cells;nodes}``,
``n_{cells;edges;faces}``, ``n_{edges;faces}_{x;y;z}``,
``{nodes;cell_centers}_{x;y;z}``, ``shape_{edges;faces}_{x;y;z}``, and
``cell_volumes``. These are the only required attributes for ``emg3d``.

- ``meshes.construct_mesh``: ``domain``, ``vector``, ``distance``,
``stretching``, ``min_width_limits``, and ``min_width_pps`` can now also
be provided as a dict containing the three keys ``'{x;y;z}'``.

- ``meshes.skin_depth`` takes new ``mu_r`` instead of ``mu``.

- ``good_mg_cell_nr``: ``max_prime`` is new ``max_lowest``, as it could also
be, e.g., 9, which is not a prime.


**Models**

- ``models.Model``:

- Knows new its ``grid``. As a consequence, all the functions that used to
require the ``grid`` and the ``model`` require new only the ``model``;
e.g., ``emg3d.solver.solve`` or ``emg3d.fields.get_magnetic_field``.

- If ``property_y`` or ``property_z`` are not set they return now ``None``,
not ``property_x``.

- If a float is provided for a property it is new expanded to the shape of
the model, and not kept as a float.

- Has to be initiated with all desired properties; it cannot be changed
afterwards. E.g., if it was initiated without electric permittivity, it
cannot be added afterwards. However, it can be initiated with dummy values
and adjusted later.

- Renamed ``interpolate2grid`` to ``interpolate_to_grid``.

- ``models.VolumeModel``: Does not take a ``grid`` any longer.


**Simulations**

- ``Simulation``:

- Works new for electric and magnetic dipole sources as well as electric wire
sources; electric and magnetic point receivers.
- Works now as well for surveys that contain receivers which are positioned
relatively to the source.
- New signature: no ``grid`` any longer, ``name`` is new an optional keyword
parameter, new optional keyword parameter ``info``.
- Method ``get_sfield`` is removed.

- ``expand_grid_model`` and ``estimate_gridding_opts`` have new signatures and
do not take a ``grid`` any longer.


**Solver**

- ``solver.solve``:

- New signature: no ``grid`` any longer; ``efield`` and ``cycle`` are moved
to keyword arguments.

- The defaults for ``sslsolver``, ``semicoarsening``, and ``linerelaxation``
is new ``True`` (before it was ``False``). This is not necessarily the
fastest setting, but generally the most robust setting.

- New keyword parameter ``plain``, which is by default ``False``. If it is
set to ``True`` it uses plain multigrid, hence ``sslsolver=False``,
``semicoarsening=False``, and ``linerelaxation=False``, unless these
parameters were set to anything different than ``True``.

- Some verbosity levels changed (for consistency reasons throughout emg3d).
The new levels are [old levels in brackets]:

- -1: Nothing [0]
- 0: Warnings [1]
- 1: One-liner at the end [2]
- 2: One-liner (dynamically updated) [-1]
- 3: Runtime and information about the method [same]
- 4: Additional information for each MG-cycle [same]
- 5: Everything (slower due to additional error computations) [same]

Level three updates now dynamically, just as level 2.

- ``solve_source()``: New function, a shortcut for ``solve()``. It takes a
``source`` and a ``frequency`` instead of a ``sfield``, gets the ``sfield``
internally, and forwards everything to ``solver.solve``.

- ``multigrid``, ``krylov``, ``smoothing``, ``restriction``, ``prolongation``,
``residual``, ``RegularGridProlongator``: New signature, mainly not taking a
``grid`` any longer.


**Surveys**

- ``Survey``:

- ``frequencies`` is new a dict just like ``sources`` and ``receivers``.
- ``sources`` and ``receivers`` must be tuples or dicts; lists are no longer
permitted. For this, the module ``surveys`` has new convenience functions
``txrx_coordinates_to_dict`` and ``txrx_lists_to_dict``.
- Has no attribute ``observed`` any longer; access it just like any other
data through ``Survey.data.observed``.
- ``rec_coords`` and ``src_coords`` attributes changed to the methods
``receiver_coordinates`` and ``source_coordinates``.
``receiver_coordinates`` takes an optional source key.
For relatively located receivers, it returns by default all positions of
this receiver for all source position. If a source-key is provided it only
returns the receiver position for this source. This does not affect
absolutely positioned receivers.
- Has no attribute ``rec_types`` any longer.
- ``name`` is new optional.
- New optional keywords ``date`` and ``info``.
- ``noise_floor`` and ``relative_error`` are new stored as data array if they
are not floats.
- The keyword ``fixed`` has been dropped. To simulate fixed surveys define
the receivers with a relative offset to the source, instead of absolute
coordinates.
- ``data`` can be a dict containing many data set.
- Automatic key names start now with 1 and have a hyphen between the prefix
and the number; they also contain the abbreviated electrode name. E.g.,
``Tx0`` becomes ``TxED-1`` or ``TxMD-1`` or ``TxEW-1``. Similar, ``Rx9``
becomes ``RxEP-10`` or ``RxMp-10``, and ``f0`` becomes ``f-1``.
- ``Survey.size`` is now the total number, ``Survey.count`` is the count of
the data that actually has non-NaN values.
- Now completely functional for receivers which are positioned relatively to
the source.

- New functions ``txrx_coordinates_to_dict`` and ``txrx_lists_to_dict`` to
collocate many sources or receivers into dicts (also
``frequencies_to_dict``).

- ``Dipole``: Replaced by the new source and receiver classes in the new module
``electrodes``.

**Time**

- Moved ``Fourier`` from ``emg3d.utils`` to its own module ``emg3d.time``.

- Renamed parameters:

- ``freq_req`` to ``freq_required``;
- ``freq_calc`` to ``freq_compute``;
- ``freq_calc_i`` to ``ifreq_compute``;
- ``freq_inp`` to ``input_freq``;
- ``freq_extrapolate_i`` to ``ifreq_extrapolate``;
- ``freq_interpolate_i`` to ``ifreq_interpolate``;


**Utils**

- Renamed ``Time`` to ``Timer``.
- Moved ``Fourier`` to its own module ``emg3d.time.Fourier``.
- ``_process_map`` new avoids ``concurrent.futures`` if ``max_workers<2``.



0.x-Series
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