Metadata-Version: 2.1
Name: chi1chi2
Version: 0.9.5
Summary: set of scripts for calculating linear and nonlinear optical properties of organic crystals
Home-page: https://bitbucket.org/tomeks86/chi1chi2
Author: Tomasz Seidler
Author-email: tomasz.z.seidler@gmail.com
License: MIT License
Platform: UNKNOWN
Classifier: Development Status :: 3 - Alpha
Classifier: Environment :: Console
Classifier: Intended Audience :: Science/Research
Classifier: License :: OSI Approved :: MIT License
Classifier: Natural Language :: English
Classifier: Operating System :: POSIX :: Linux
Classifier: Programming Language :: Python :: 3 :: Only
Classifier: Programming Language :: Fortran
Classifier: Topic :: Scientific/Engineering :: Physics
Classifier: Topic :: Scientific/Engineering :: Chemistry
Description-Content-Type: text/markdown
Requires-Dist: numpy (==1.21.5)
Requires-Dist: PyCifRW (==4.4.3)

# *chi1chi2* program

The aim of the program is to calculate linear (refractive indices) 
and nonlinear (*chi(2)* for second harmonic generation) 
optical properties of organic crystals.

[TOC]

---

## Installation

Make sure you have installed:
 - gfortran
 - python 3.6

Installation:
 - pip install chi1chi2
 - for the fortran programs a Makefile is provided with the repository:
   *make* command builds the programs in the build/ directory

#Description

The whole program constitutes a set of scripts that need to be executed in order.

There are four main steps:

1. Input preparation (optionally - geometry optimization)
2. Optical properties of molecular sub-units calculations
3. Calculations of bulk properties
4. Analysis of the results

The purpose of this file is to lead the user through all these steps.


Step *1* - Input preparation
____________________________

A) from Cif (easy path)

use *chi.from_cif* to get geometry for further optimization with *e.g.* crystal09/14/..

B) from fractional coordinates

use *chi.from_fra* script (see: examples/mna_cif.fra, examples/mna_cif2.fra to see the convention)
(remember to adjust the symmetry operations!)

C) manually

see examples for the convention


Step *1a* after geometry optimization
_____________________________________

D) use *chi.from_crystal* script to adjust the coordinates and charges after *crystal* geometry optimization

E) run *chi.input_preparator* script to get input files for:

- *charge_generator* program (example usage: *charge_generator < chg1.inp*)
- Lorentz tensor with *lorentz* program (example usage: *lorentz < lorentz.inp > L.dat*)


Step *2* - property calculation
_______________________________

Use sets of charges, geometries and follow your favorite property calculation procedure.
Additional shell scripts could be provided in later releases.

Step *3* - core calculations
____________________________

Use the script *chi.main* to get the `chi(1)` and `chi(2)` tensor components in the so called a'bc* reference frame.

Q-LFT calculations enabled! (since 0.1.1)

Step *4* - result analysis
__________________________

Use the script *chi.analyze* with output file generated in step 3

- Refractive indices analysis (since 0.1.3)
- Magnitude of the `chi(2)` tensor components in the direction of the optical indicatrix (since 0.1.3)


Helpers
-------

Helper scripts are available to use around molecular calculations:
 - *read_g09.py* for reading the molecular properties after the QC calculations
 - *scale_props.py* for scaling the static properties with use of the reference calculations
 - *calc_pol.py* for calculation of distributed polarizabilities using AIMALL output of finite field calculations

Note: the scripts minimize depencencies on the project library so that they could
be used as standalone scripts on an external machine

Preparations for distributed polarizabilities calculations
----------------------------------------------------------

Two variants are possible:
 - with only one external field magnitude (0.003 a.u.)

  The input files for AIMALL have to be preparated in the following convention:

  1 /no field/; 2 /0.003, 0, 0/; 3 /0, 0.003, 0/; 4 /0, 0, 0.003/;

  5 /-0.003, 0, 0/; 6 /0, -0.003, 0/; 7 /0, 0, -0.003/

 - with two external field magnitudes (0.003 a.u. and 0.006 a.u.)
   (using Romberg numerical differentiation procedure)

  The input files for AIMALL should follow the convention:

  1 /no field/; 2 /0.003, 0, 0/; 3 /0, 0.003, 0/; 4 /0, 0, 0.003/;

  5 /-0.003, 0, 0/; 6 /0, -0.003, 0/; 7 /0, 0, -0.003/

  8 /0.006, 0, 0/; 9 /0, 0.006, 0/; 10 /0, 0, 0.006/;

  11 /-0.006, 0, 0/; 12 /0, -0.006, 0/; 13 /0, 0, -0.006/

Examples
--------

See the examples/examples.pdf to follow the steps used in the integration tests.
The files used for the tests are located in the tests/integration directory:

- *input* as a starting point
- *expected* as a reference

Example gaussian09 input file for calculations could be found in examples/mna.com

Version history
---------------

- 0.1.0 - first release (31.01.2019)
- 0.1.1 - Q-LFT calculations support added (05.02.2019)
- 0.1.2 - a minor README fix on the PyPI (06.02.2019)
- 0.2.0 - analysis of the core calculations - reporting in tables (09.03.2019)
- 0.2.1 - property scaling helper (27.03.2019)
- 0.3.0 - atomic polarizability scaling approach change (03.03.2020)
- 0.4.0 - distributed polarizability calculation script & format change (10.03.2020)
- 0.4.1 - correction of molecules placement in the unit cell (23.03.2020)
- 0.5.0 - from_crystal old input backing up strategy change (04.04.2020)
- 0.5.1 - HYDROGEN_TOLERANCE environment variable could be used to modify default maximum hydrogen distance (1.15A)
- 0.6.1 - input preparation and main calculations allow for arbitrary redefinition 
of molecule-ionic composition of the unit cell (31.08.2020)
- 0.7.0 - fix for calculation of properties in non-orthogonal systems (15.02.2021)
- 0.8.0 - added script for calculation of d_effective for selected solid angles (21.02.2021)
- 0.9.0 - openbabel dependency removed (30.12.2021)
- 0.9.5 - automatic release pipeline (7.01.2022)

