Fast Fourier Transform (FFT) which allows, in a single step, to determine the field at the far field.
Rayleigh-Sommerfeld (RS) [Appl. Opt., 45(6) 1102–1110, (2006)] RS allows, in a single step, to propagate to a near or far observation plane, which allows fast computations. The fields and the masks must be defined in a plane.
Plane Wave Decomposition (PWD) [Opt. Comm. 281 4219-4233 (2008)] PWD allows to propagate to a near or far observation plane. It presents a complexity of O(n) in the two-dimensional and O(n2) in the three-dimensional case. It is computed according to the split-step propagation scheme.
Beam propagation method (BPM) [Appl. Opt. 24, 3390-3998 (1978)] which allows to analyze the propation of light in volumetric elements, such as spheres, cylinders and other complex forms, provided that the spatial variations in the refractive index are small. It allows graded index structures. It presents a complexity of O(n) in the two-dimensional and O(n2) in the three-dimensional case. It is computed according to the split-step propagation scheme.
Wave Propagation Method (WPM). [Appl. Opt. 32, 4984 (1993)] WPM was introduced in order to overcome the major limitations of the beam propagation method (BPM). With the WPM, the range of application can be extended from the simulation of waveguides to simulation of other optical elements like lenses, prisms and gratings. WPM can accurately simulate scalar light propagation in inhomogeneous media at high numerical apertures, and provides valid results for propagation angles up to 85° and that it is not limited to small index variations in the axis of propagation. Fast implementation with discrete number of refractive indexes is also implemented.
Chirped Z-Transform (CZT). [Light: Science and Applications, 9(1), (2020)] CZT allows, in a single step, to propagate to a near or far observation plane. It present advantages with respecto to RS algorithm, since the region of interest and the sampling numbers can be arbitrarily chosen, endowing the proposed method with superior flexibility. CZT algorithm allows to have a XY mask and compute in XY, Z, XZ, XYZ schemes, simply defining the output arrays.

Other features

When possible, multiprocessing is implemented for a faster computation.
The fields, masks, and sources can be stored in files.
Also drawings can be easily obtained, for intensity, phase, fields, etc.
In some modules, videos can be generated for a better analysis of optical fields.
Intensity, MTF and other parameters are obtained from the optical fields.
Fields can be added simply with the + signe, and interference is produced. Masks can be multiplied, added and substracted in order to make complex structures
Resampling fields in order to analyze only areas of interest.
Save and load data for future analysis.
Rayleigh-Sommerfeld implementation is performed in multiprocessing for fast computation.
Polychromatic and extended source problems can also be analyzed using multiprocessing.

.. image:: readme6.png :width: 600

Vector propagation

Sources

Vector sources as implemented in vector_sources_XY module.

The can present any spatial distribution of the electric field, and can be defined in the XY plane.

In addition, the polarization state is defined by the Jones vector, which can be constant (linear, circular, elliptical) or spatially varying, such as (azimuthal, radial, spiral, etc.).

constant_polarization.
azimuthal_wave, azimuthal_inverse_wave.
radial_wave, radial_inverse_wave.
local_polarized_vector_wave, local_polarized_vector_wave_radial, local_polarized_vector_wave_hybrid.
spiral_polarized_wave.

Masks

Vector masks are defined in the vector_masks_XY module by Jones matrices.

For example, a scalar mask is transformed to a vector mask by applying a Jones matrix to the scalar mask (scalar_to_vector_mask).

There are also predefined vector masks for standard polarizers (linear, quarter-wave, half-wave). Arbitrary Jones matrices can be defined for any mask using from_pypol method.

Binary scalar masks can also be transformed to vector masks using two Jones matrices (complementary_masks).

Also, arbitrary vector masks can be defined by defining the Jones matrix for each index level. This can be used for defining Spatial Light Modulators (SLM).

Here, we implement new classes where the E_x, E_y, and E_z fields are generated and propagated using Rayleigh-Sommerfeld and Chirped z-transform algorithms. Also, simple and complex polarizing masks can be created.

Intensity of vector field

.. image:: readme4.png :width: 700

Polarization: Stokes parameters

.. image:: readme5.png :width: 700

Propagation algorithms

The main algorithms for Vector propagation are:

Vector Fast Fourier Tranform (VFFT), which allows to determine the (Ex, Ey, Ez) fields at the far field.
Vector Rayleigh-Sommerfeld (VRS). The VRS method [Laser Phys. Lett. 10(6) 065004 (2013)] allows to propagate (Ex,Ey,Ez) fields offering the advantage of significant reduction in computation, from flat diffractive elements (Thin Element Approximation) with full control of polarization. It addresses simultaneously both longitudinal polarization. This approach offers the advantage of significant reduction in computation.
Vector Chirp Z-Transform (VCZT). [Light: Science and Applications, 9(1), (2020)]. CZT is also implemented in vector fields.
Fast Polarized Wave Propagation Method (FP_WPM) [Opt Express. 30(22) 40161-40173 (2022)] Wave Propagation Method for vector fields. It is an efficient method for vector wave optical simulations of microoptics. The FPWPM is capable of handling comparably large simulation volumes while maintaining quick runtime. By considering polarization in simulations, the FPWPM facilitates the analysis of optical elements which employ this property of electromagnetic waves as a feature in their optical design, e.g., diffractive elements, gratings, or optics with high angle of incidence like high numerical aperture lenses.

Other features

Vector fields can be converted to py-pol objects for further analysis.

Conventions

In this module we assume that the optical field is defined as:

.. math:: u(x,y,z)=A e^{i(\vec{k} . \vec{r}-\omega t)},

where A is the amplitude, k is the wave vector, r is the position vector, :math:\omega is the angular frequency, and t is the time.

For the vector case, the field is defined as:

.. math:: \vec{E}(x,y,z)=\left[\begin{array}{c} E_{x}(x,y)\ E_{y}(x,y)\ E_{z}(x,y) \end{array}\right]e^{i(\vec{k} . \vec{r}-\omega t)},

where :math:E_x, :math:E_y and :math:E_z are the components of the electric field.

The spatial units are defined in micrometers: :math:\mu m = 1.

Authors

Luis Miguel Sanchez Brea optbrea@ucm.es

Universidad Complutense de Madrid_ Faculty of Physical Sciences_ Department of Optics_ Applied Optics Complutense Group_ Plaza de las ciencias 1 ES-28040 Madrid (Spain)

.. image:: logoUCM.png :width: 125 :align: right

Collaborators

Ángela Soria Garcia
Jesús del Hoyo Muñoz
Francisco Jose Torcal-Milla

Citing

There is a paper about Diffractio <https://doi.org/10.1117/12.3021879>_.

If you are using Diffractio in your scientific research, please help our scientific visibility by citing our work.

Luis Miguel Sanchez-Brea, Angela Soria-Garcia, Joaquin Andres-Porras, Veronica Pastor-Villarrubia, Mahmoud H. Elshorbagy, Jesus del Hoyo Muñoz, Francisco Jose Torcal-Milla, and Javier Alda "Diffractio: an open-source library for diffraction and interference calculations", Proc. SPIE 12997, Optics and Photonics for Advanced Dimensional Metrology III, 129971B (18 June 2024); https://doi.org/10.1117/12.3021879

BibTex:

.. code::

@inproceedings{10.1117/12.3021879, author = {Luis Miguel Sanchez-Brea and Angela Soria-Garcia and Joaquin Andres-Porras and Veronica Pastor-Villarrubia and Mahmoud H. Elshorbagy and Jesus del Hoyo Mu{~n}oz and Francisco Jose Torcal-Milla and Javier Alda}, title = {{Diffractio: an open-source library for diffraction and interference calculations}}, volume = {12997}, booktitle = {Optics and Photonics for Advanced Dimensional Metrology III}, editor = {Peter J. de Groot and Felipe Guzman and Pascal Picart}, organization = {International Society for Optics and Photonics}, publisher = {SPIE}, pages = {129971B}, keywords = {Design of micro-optical devices, Diffractive optical elements, Propagation algorithms, Scalar propagation, Vector propagation}, year = {2024}, doi = {10.1117/12.3021879}, URL = {https://doi.org/10.1117/12.3021879} }

CFF:

There is a cff file (CITATION.cff) at top of the project.

Credits

This package was created with Cookiecutter_ and the audreyr/cookiecutter-pypackage_ project template.

.. _Cookiecutter: https://github.com/audreyr/cookiecutter .. _audreyr/cookiecutter-pypackage: https://github.com/audreyr/cookiecutter-pypackage .. _Universidad Complutense de Madrid: https://www.ucm.es/ .. _Faculty of Physical Sciences: https://fisicas.ucm.es/ .. _Department of Optics: https://www.ucm.es/doptica .. _Applied Optics Complutense Group: https://www.ucm.es/aocg

Keywords

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Install

diffractio

================================================ Python Diffraction-Interference module

Features

Scalar propagation

Sources

Masks

Propagation algorithms

Other features

Vector propagation

Sources

Masks

Propagation algorithms

Other features

Conventions

Authors

Citing

Credits

Keywords

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