Symmetrization¶
In this short tutorial, we introduce the use of the symmetrization feature in TBmodels. The theoretical background for this feature is described in this paper (arxiv version). The example we describe here is to symmetrize a model of diamond silicon. The initial model, and code for this example, can also be found in the TBmodels source on GitHub.
We start by loading the initial model:
In [1]: import tbmodels
The model is located in the examples directory of the TBmodels source. You will have to change the following part to point to your examples directory:
In [2]: import os
...: import pathlib
...: EXAMPLES_DIR = pathlib.Path('../examples')
...:
In [3]: model_nosym = tbmodels.io.load(
...: EXAMPLES_DIR / 'symmetrization' / 'nonsymmorphic_Si' / 'data' / 'model_nosym.hdf5'
...: )
...:
Setting up orbitals¶
The most difficult step in using the symmetrization feature is setting up the symmetry operations. These need to be in the format of the symmetry_representation module, which is also part of the Z2Pack ecosystem.
Starting with the 0.2 release, symmetry-representation contains some handy helper functions which allow us to construct the symmetry operations automatically by specifying the orbitals which constitute the tight-binding model. Thus, the first step to obtain the symmetry operations is to define the orbitals.
We can see that our initial model has two positions, which we store in the coords variable:
In [4]: model_nosym.pos
Out[4]:
array([[0.5 , 0.5 , 0.5 ],
[0.5 , 0.5 , 0.5 ],
[0.5 , 0.5 , 0.5 ],
[0.5 , 0.5 , 0.5 ],
[0.75, 0.75, 0.75],
[0.75, 0.75, 0.75],
[0.75, 0.75, 0.75],
[0.75, 0.75, 0.75],
[0.5 , 0.5 , 0.5 ],
[0.5 , 0.5 , 0.5 ],
[0.5 , 0.5 , 0.5 ],
[0.5 , 0.5 , 0.5 ],
[0.75, 0.75, 0.75],
[0.75, 0.75, 0.75],
[0.75, 0.75, 0.75],
[0.75, 0.75, 0.75]])
In [5]: coords = ((0.5, 0.5, 0.5), (0.75, 0.75, 0.75))
Since the initial model was calculated with Wannier90 and sp3 projections, we know that the orbitals are ordered as follows:
spin up
first coordinate \((0.5, 0.5, 0.5)\)
\(sp^3\) orbitals
second coordinate \((0.75, 0.75, 0.75)\)
\(sp^3\) orbitals
spin down
first coordinate \((0.5, 0.5, 0.5)\)
\(sp^3\) orbitals
second coordinate \((0.75, 0.75, 0.75)\)
\(sp^3\) orbitals
Consequently, we construct a list of symmetry_representation.Orbital orbitals in this order:
In [6]: import symmetry_representation as sr
In [7]: orbitals = []
In [8]: for spin in (sr.SPIN_UP, sr.SPIN_DOWN):
...: for pos in coords:
...: for fct in sr.WANNIER_ORBITALS['sp3']:
...: orbitals.append(sr.Orbital(
...: position=pos,
...: function_string=fct,
...: spin=spin
...: ))
...:
Here we used constants defined by symmetry_representation to specify the spin up / down components, and the \(sp^3\) orbitals in the order produced by Wannier90.
In [9]: sr.SPIN_UP, sr.SPIN_DOWN
Out[9]:
(Spin(total=Fraction(1, 2), z_component=Fraction(1, 2)),
Spin(total=Fraction(1, 2), z_component=Fraction(-1, 2)))
In [10]: sr.WANNIER_ORBITALS['sp3']
Out[10]: ['1 + x + y + z', '1 + x - y - z', '1 - x + y - z', '1 - x - y + z']
The function_string argument is a string which describes the orbital in terms of the cartesian coordinates x, y and z. The symmetry-representation code will use sympy to apply the symmetry operations to these functions and figure out which orbitals these are mapped to.
Creating symmetry operations¶
Having created the orbitals which describe our system, we can immediately generate the symmetry operation for time-reversal symmetry:
In [11]: time_reversal = sr.get_time_reversal(orbitals=orbitals, numeric=True)
Note that we use the numeric=True flag here. This keyword is used to switch between output using numpy arrays with numeric content, and sympy matrices with analytic content. Mixing these two formats is a bad idea, since basic operations between them don’t work as one might expect. For the use in TBmodels, we can always choose the numeric=True option.
Next, we use pymatgen to determine the space group symmetries of our crystal:
In [12]: from pymatgen.core import Structure
....: from pymatgen.symmetry.analyzer import SpacegroupAnalyzer
....:
In [13]: structure = Structure(
....: lattice=model_nosym.uc, species=['Si', 'Si'], coords=np.array(coords)
....: )
....:
In [14]: analyzer = SpacegroupAnalyzer(structure)
In [15]: sym_ops = analyzer.get_symmetry_operations(cartesian=False)
In [16]: sym_ops_cart = analyzer.get_symmetry_operations(cartesian=True)
Again, we can use a helper function from the symmetry-representation code to construct the symmetry operations automatically. Note that we need both the cartesian and the reduced symmetry operations:
In [17]: symmetries = []
In [18]: for sym, sym_cart in zip(sym_ops, sym_ops_cart):
....: symmetries.append(sr.SymmetryOperation.from_orbitals(
....: orbitals=orbitals,
....: real_space_operator=sr.RealSpaceOperator.from_pymatgen(sym),
....: rotation_matrix_cartesian=sym_cart.rotation_matrix,
....: numeric=True
....: ))
....:
Applying the symmetries¶
Finally, the simple task of applying the symmetries to the initial tight-binding model remains. We first apply the time-reversal symmetry.
In [19]: model_tr = model_nosym.symmetrize([time_reversal])
Note that, unlike the space group symmetries, the time-reversal symmetry does not constitute a full group. As a result, TBmodels will apply not only time-reversal \(\mathcal{T}\), but also \(\mathcal{T}^2 = -\mathbb{1}\), \(\mathcal{T}^3=-\mathcal{T}\), and the identity. For the space group, this extra effort is not needed since we already have the full group. This can be specified with the full_group=True flag:
In [20]: model_sym = model_tr.symmetrize(symmetries, full_group=True)
By comparing eigenvalues, we can see for example that the symmetrized model is two-fold degenerate at the \(\Gamma\) point, while the initial model is not:
In [21]: model_nosym.eigenval((0, 0, 0))
Out[21]:
array([-5.74263139, -5.74262186, 6.21206569, 6.21207289, 6.25909606,
6.25910078, 6.25910527, 6.25910906, 8.80451686, 8.80452023,
8.83906923, 8.83907362, 8.83907975, 8.83908456, 9.56537577,
9.56538949])
In [22]: model_sym.eigenval((0, 0, 0))
Out[22]:
array([-5.74262663, -5.74262663, 6.2129382 , 6.2129382 , 6.25823388,
6.25823388, 6.25910279, 6.25910279, 8.80515697, 8.80515697,
8.83843836, 8.83843836, 8.83907679, 8.83907679, 9.56538262,
9.56538263])