The API documentation can be found here.
The sisl toolbox provides a simple API for manipulating, constructing and creating tight-binding matrices
in a standard and uniform way.
Secondly, it provides easy interfaces for creating and calculating band-structures of
simple tight-binding models as well as interfacing to more advanced DFT utilities.
sisl may also be used together with the ASE environment.
sisl provides an interface to TBtrans and enables the calculation of transport using the non-equilibrium Green function method and easily allows calculation of tight-binding systems of millions of atoms.
Installing sisl using PyPi or Conda is the easiest:
pip install sisl
pip install sisl[analysis] # also installs tqdm and xarray
# or
conda install -c conda-forge sisl
If performing a manual installation, these packages are required:
- A C- and fortran-compiler
- six
- numpy (1.10 or later)
- scipy
- netCDF4
- setuptools
- pyparsing
- matplotlib, encouraged optional dependency
- tqdm, encouraged optional dependency
- xarray, optional dependency
You are encouraged to also install matplotlib and tqdm for plotting utilities and
progress-bar support.
Subsequently manual installation may be done using this command:
python setup.py install --prefix=<prefix>
If trying to install without root access, you may be required to use this command:
python setup.py install --user --prefix=<prefix>
After installation it may be a good idea to check that the tests shipped with sisl pass.
To do this the pytest package is necessary. Then run
pytest --pyargs sisl
which will run the shipped sisl test-suite.
If used to produce scientific contributions, please use this DOI for citation. It is recommend to specify the version of sisl in combination of this citation:
@misc{zerothi_sisl,
author = {Papior, Nick R.},
title = {sisl: v<fill-version>},
doi = {10.5281/zenodo.597181},
url = {https://doi.org/10.5281/zenodo.597181}
}
sisl contains a utility to easily convert geometries from existing files
to other formats. After installation the executable sgeom is available which
enables the conversion between all formats accessible as Sile objects.
To convert a SIESTA FDF file to xyz and an XV file one does
sgeom siesta.fdf geom.xyz geom.XV
Try sgeom -h for additional features such as repeating the structure.
sisl contains a class for manipulating geometries in a consistent and easy way. Without using any other feature this enables you to easily create and manipulate structures in a consistent manner.
For instance to create a huge graphene flake
sq3h = 3.**.5 * 0.5
sc = SuperCell(np.array([[1.5, sq3h, 0.],
[1.5,-sq3h, 0.],
[ 0., 0., 10.]],np.float64) * 1.42,
nsc=[3,3,1])
gr = Geometry(np.array([[ 0., 0., 0.],
[ 1., 0., 0.]],np.float64) * 1.42,
atom=Atom(Z=6, R=1.42), sc=sc)
huge = gr.tile(100, axis=0).tile(100, axis=1)
Which results in a 20,000 atom big graphene flake.
Several basic geometries are intrinsically available
from sisl.geom import *
# Graphene basic unit-cell
g = graphene()
# SC crystal structure
g = sc(<lattice constant>, <Atom>)
# BCC crystal structure
g = bcc(<lattice constant>, <Atom>)
# FCC crystal structure
g = fcc(<lattice constant>, <Atom>)
# HCP crystal structure
g = hcp(<lattice constant>, <Atom>)
The Graphene, BCC, FCC and HCP structures can be created in
an orthogonal unit-cell by adding the flag orthogonal=True in the call:
g = graphene(orthogonal=True)
sisl employs a variety of IO interfaces for managing different physical quantities. A large variety of files describing the geometry (atomic positions and species) are the main part of the IO routines.
All text files can also be read from their gzipped file formats with transparency.
All file formats in sisl are called a Sile (sisl file). This small difference prohibits name clashes with other implementations.
To read geometries from content you may do
import sisl
geom = sisl.Geometry.read('file.xyz')
which will read the geometry in file.xyz and return a Geometry object.
If you want to read several different objects from a single file you should
use the specific get_sile routine to retrieve the Sile object:
import sisl
fxyz = sisl.get_sile('file.xyz')
which returns an xyzSile file object that enables reading the geometry in
file.xyz. Subsequently you may read the geometry and obtain a geometry object
using
geom = fxyz.read_geometry()
The above two methods are equivalent.
Even though these are hard coded you can easily extend your own file format
sisl.add_sile(<file ending>, <SileObject>)
for instance the xyzSile is hooked using:
sisl.add_sile('xyz', xyzSile, case=False)
which means that sisl.get_sile understands files *.xyz and *.XYZ files as
an xyzSile object. You can put whatever file-endings here and classes to retain API
compatibility. See the sisl.io package for more information. Note that a call to
add_sile with an already existing file ending results in overwriting the initial
meaning of that file object.
NOTE: if you know the file is in xyz file format but the ending is erroneous, you can force the xyzSile by instantiating using that class
sisl.io.xyzSile(<filename>)
which disregards the ending check.
To create a tight-binding model you extend a geometry to a Hamiltonian class which
contains the required sparse pattern.
To create the nearest neighbour tight-binding model for graphene you simply do
# Create nearest-neighbour tight-binding
# graphene lattice constant 1.42
R = ( 0.1 , 1.5 )
# Ensure that graphene has supercell connections
gr.sc.set_nsc([3, 3, 1])
tb = Hamiltonian(gr)
for ia in tb.geom:
idx_a = tb.close(ia, R=R)
tb[ia,idx_a[0]] = 0. # on-site
tb[ia,idx_a[1]] = -2.7 # nearest neighbour
at this point you have the tight-binding model for graphene and you can easily create the Hamiltonian using this construct:
Hk = tb.Hk(k=[0., 0.5, 0])
which returns the Hamiltonian in the scipy.sparse.csr_matrix
format. To calculate the dispersion you diagonalize and plot the eigenvalues
import matplotlib.pyplot as plt
klist = ... # dispersion curve
eigs = np.empty([len(klist), tb.no])
for ik, k in enumerate(klist):
eigs[ik,:] = tb.eigh(k, eigvals_only=True)
# Or equivalently:
# Hk = tb.Hk(k)
# eigs[ik,:] = sli.eigh(Hk.todense(), eigvals_only=True)
for i in range(tb.no):
plt.plot(eigs[:,i])
Very large tight-binding models are notoriously slow to create, however, sisl implements a much faster method to loop over huge geometries
for ias, idxs in tb.geom.iter_block(iR = 10):
for ia in ias:
idx_a = tb.geom.close(ia, R, idx = idxs)
tb[ia,idx_a[0]] = 0.
tb[ia,idx_a[1]] = -2.7
which accomplishes the same thing, but at much faster execution. iR should be a
number such that tb.geom.close(<any index>,R = tb.geom.maxR() * iR) is approximately
1,000 atoms.
The above example is for the default orthogonal Hamiltonian. However, sisl is not limited to orthogonal basis functions. To construct the same example using explicit overlap matrix the following procedure is necessary:
# Create nearest-neighbour tight-binding
# graphene lattice constant 1.42
R = ( 0.1 , 1.5 )
tb = Hamiltonian(gr, orthogonal=False)
for ia in tb.geom:
idx_a = tb.close(ia, R)
tb.H[ia,idx_a[0]] = 0.
tb.S[ia,idx_a[0]] = 1.
tb.H[ia,idx_a[1]] = -2.7
tb.S[ia,idx_a[1]] = 0. # still orthogonal (fake overlap matrix)
Hk = tb.Hk(k=[0., 0.5, 0])
Sk = tb.Sk(k=[0., 0.5, 0])
eigs = sli.eigh(Hk.todense(), Sk.todense(), eigvals_only=True)
I would advice any users to contribute as much feedback and/or PRs to further maintain and expand this library.
Please do not hesitate to contribute!
If you find any bugs please form a bug report/issue.
If you have a fix please consider adding a pull request.
The sisl license is LGPL, please see the LICENSE file.