import numpy as np
import logging
import copy
from typing import Iterable, Literal
from types import EllipsisType
logger = logging.getLogger(__name__)
__all__ = ["Lattice"]
def _parse_kpts(kpts, dim):
"""
Parse special string cases for 1D and ensure array shape (n_nodes, dim).
"""
if isinstance(kpts, str) and dim == 1:
presets = {
"full": [[0.0], [0.5], [1.0]],
"fullc": [[-0.5], [0.0], [0.5]],
"half": [[0.0], [0.5]],
}
return np.array(presets[kpts], float)
arr = np.array(kpts, float)
if arr.ndim == 1 and dim == 1:
arr = arr[:, None]
return arr
[docs]
class Lattice:
r"""Store lattice and orbital information.
The :class:`Lattice` class encapsulates the real-space lattice vectors, orbital
positions, and periodicity information for tight-binding models. It provides methods
to access and manipulate lattice properties, such as retrieving lattice vectors,
orbital positions, and cutting finite pieces from periodic lattices. Internally,
it also computes the reciprocal lattice vectors based on the specified periodic directions.
.. versionadded:: 2.0.0
Parameters
----------
lat_vecs : array_like
Array of shape ``(dim_r, dim_r)`` containing the real-space lattice vectors as rows
in Cartesian coordinates.
orb_vecs : array_like, int
Array of shape ``(norb, dim_r)`` containing the orbital positions as rows
in reduced coordinates (fractions of the lattice vectors). If ``orb_vecs``
is an integer, it specifies the number of orbitals at the origin.
periodic_dirs : array_like of int or {'all'} or Ellipsis, optional
Real-space lattice directions that treated as periodic. The indices
refer to the ``lat_vecs`` array, e.g. ``[0]`` would indicate that the first
lattice vector is periodic. Use ``...`` or ``"all"`` to indicate that all directions
are periodic. If an empty list (default) or None, all directions are considered
finite (open boundary conditions).
Notes
-----
- The dimension of the real-space lattice, ``dim_r``, is inferred from the shape of ``lat_vecs``.
- The dimension of the k-space, ``dim_k``, is inferred from the number of entries in ``periodic_dirs``.
- The lattice vectors must form a right-handed system with non-zero volume.
- Orbital positions are given in reduced coordinates, i.e., fractions of the lattice vectors.
- Works for 0D, 1D, 2D, and 3D lattices. For 0D, use empty arrays for ``lat_vecs`` and an
integer for ``orb_vecs``.
"""
def __init__(
self,
lat_vecs: np.ndarray,
orb_vecs: np.ndarray,
periodic_dirs: Iterable[int] | Literal["all"] | EllipsisType = [],
):
self._periodic_dirs = [] # temporary placeholder for lat_vecs setter
self.lat_vecs = lat_vecs
if periodic_dirs in ("all", Ellipsis):
periodic_dirs = list(range(self.dim_r))
elif periodic_dirs is None:
logger.info("All lattice directions are considered open (non-periodic).")
periodic_dirs = []
elif isinstance(periodic_dirs, (list, tuple, np.ndarray)):
periodic_dirs = list(periodic_dirs)
else:
raise TypeError(
"periodic_dirs must be a list of integers, 'all', or Ellipsis."
)
self.periodic_dirs = periodic_dirs # set only after lat_vecs are set
self.orb_vecs = orb_vecs
self._nsuper = [1 for _ in range(self.dim_r)] # default supercell sizes
def __eq__(self, value):
if not isinstance(value, Lattice):
return False
return (
np.allclose(self.lat_vecs, value.lat_vecs)
and np.allclose(self.orb_vecs, value.orb_vecs)
and self.periodic_dirs == value.periodic_dirs
)
def _set_orb_vecs(self, orb_vecs):
if isinstance(orb_vecs, int):
if orb_vecs < 0:
raise ValueError("Number of orbitals must be positive.")
orb_vecs = np.zeros((orb_vecs, self.dim_r), dtype=float)
elif isinstance(orb_vecs, (list, np.ndarray)):
orb_vecs = np.array(orb_vecs, dtype=float)
if orb_vecs.ndim != 2 or orb_vecs.shape[1] != self.dim_r:
raise ValueError(
"Wrong orb array dimensions. Must have shape (norb, dim_r)."
)
else:
raise TypeError("Orbital vectors must be an integer, list, or numpy array.")
if orb_vecs.shape[1] != self.dim_r:
raise ValueError(
"Orbital vectors have wrong shape. Must have shape (norb, dim_r)."
)
self._orb_vectors = orb_vecs
if hasattr(self, "_lat_vectors"):
self._orb_vecs_cart = orb_vecs @ self._lat_vectors
def _set_lat_vecs(self, lat_vecs):
if isinstance(lat_vecs, (list, np.ndarray)):
lat_vecs = np.array(lat_vecs, dtype=float)
else:
raise TypeError("Lattice vectors must be a list or numpy array.")
if lat_vecs.shape[0] == 0:
lat_vecs = np.identity(0, dtype=float)
if lat_vecs.shape[1] != lat_vecs.shape[0]:
raise ValueError(
"Wrong lat array dimensions. Must have shape (dim_r, dim_r)."
)
if lat_vecs.shape[0] > 3:
raise ValueError("Argument dim_r must be from 0 to 3.")
if lat_vecs.shape[0] > 0:
det_lat = np.linalg.det(lat_vecs)
if det_lat < 0:
raise ValueError("Lattice vectors need to form right handed system.")
elif det_lat < 1e-10:
raise ValueError("Volume of unit cell is zero.")
self._lat_vectors = lat_vecs
# Cell volume
if self.dim_r == 0:
self._cell_vol = 0.0
else:
vol = np.sqrt(np.linalg.det(lat_vecs @ lat_vecs.T))
self._cell_vol = vol
# Reciprocal lattice
self._recip_lat = self._get_recip_lat() if self.dim_k > 0 else None
if self.dim_k == 0:
self._recip_vol = 0.0
else:
self._recip_vol = np.sqrt(
np.linalg.det(self._recip_lat @ self._recip_lat.T)
)
if hasattr(self, "_orb_vectors"):
# reframe fractional orbital positions into new lattice
self.orb_vecs = self.orb_vecs @ np.linalg.inv(lat_vecs)
@property
def periodic_dirs(self) -> list[int]:
"""List of periodic directions."""
return self._periodic_dirs
@property
def orb_vecs(self) -> np.ndarray:
"""Orbital vectors in reduced coordinates with shape ``(norb, dim_r)``."""
return self._orb_vectors.copy()
@property
def lat_vecs(self) -> np.ndarray:
"""Lattice vectors in Cartesian coordinates with shape ``(dim_r, dim_r)``."""
return self._lat_vectors.copy()
@lat_vecs.setter
def lat_vecs(self, new_lat_vecs: np.ndarray):
self._set_lat_vecs(new_lat_vecs)
@orb_vecs.setter
def orb_vecs(self, new_orb_vecs: np.ndarray):
self._set_orb_vecs(new_orb_vecs)
@periodic_dirs.setter
def periodic_dirs(self, new_per: list[int]):
if not isinstance(new_per, (list, tuple, np.ndarray)):
raise TypeError("periodic_dirs must be a list of integers.")
new_per = list(new_per)
if not hasattr(self, "_lat_vectors"):
raise AttributeError(
"Lattice vectors must be defined before setting periodic_dirs."
)
dim_r = self._lat_vectors.shape[0]
validated: list[int] = []
seen = set()
for idx in new_per:
if not isinstance(idx, (int, np.integer)):
raise TypeError("periodic_dirs entries must be integers.")
val = int(idx)
if val < 0 or val >= dim_r:
raise ValueError(
f"Periodic direction {val} is out of bounds for lattice dimension {dim_r}."
)
if val in seen:
raise ValueError("periodic_dirs entries must be unique.")
seen.add(val)
validated.append(val)
self._periodic_dirs = validated
# Update reciprocal lattice since periodic directions may have changed
if self.dim_k == 0:
self._recip_lat = None
self._recip_vol = 0.0
else:
self._recip_lat = self._get_recip_lat()
self._recip_vol = np.sqrt(
np.linalg.det(self._recip_lat @ self._recip_lat.T)
)
# Read-only properties inferred from mutable attributes
@property
def nsuper(self) -> list[int]:
"""List of supercell sizes along each real-space lattice vector."""
return self._nsuper.copy()
@property
def dim_r(self) -> int:
"""The dimensionality of real space."""
return self._lat_vectors.shape[0]
@property
def dim_k(self) -> int:
"""The dimensionality of reciprocal space (periodic directions)."""
return len(self._periodic_dirs)
@property
def norb(self) -> int:
"""The number of orbitals in the lattice."""
return self.orb_vecs.shape[0]
@property
def recip_lat_vecs(self) -> np.ndarray:
"""Reciprocal lattice vectors in Cartesian coordinates with shape ``(dim_k, dim_r)``."""
if self._recip_lat is None:
raise ValueError(
"Reciprocal lattice vectors are not defined for zero-dimensional k-space."
)
return self._recip_lat.copy()
@property
def recip_volume(self) -> float:
"""Volume of the reciprocal unit cell in Cartesian coordinates."""
return self._recip_vol
@property
def cell_volume(self) -> float:
"""Volume of the real-space unit cell in Cartesian coordinates."""
return self._cell_vol
def __str__(self) -> str:
return self.info(show=False)
def _report_list(self) -> list:
output = []
header = (
"----------------------------------------\n"
" Lattice structure report \n"
"----------------------------------------"
)
output.append(header)
output.append(f"r-space dimension = {self.dim_r}")
output.append(f"k-space dimension = {self.dim_k}")
output.append(f"periodic directions = {self.periodic_dirs}")
output.append(f"number of orbitals = {self.norb}")
formatter = {
"float_kind": lambda x: f"{0:6.3f}" if abs(x) < 1e-10 else f"{x:6.3f}"
}
output.append("\nLattice vectors (Cartesian):")
for i, vec in enumerate(self.lat_vecs):
output.append(
f" # {i} ===> {np.array2string(vec, formatter=formatter, separator=', ')}"
)
output.append(
f"Volume of unit cell (Cartesian) = {self.cell_volume:5.3f} [A^d]\n"
)
if self.dim_k > 0:
output.append("Reciprocal lattice vectors (Cartesian):")
for i, vec in enumerate(self.recip_lat_vecs):
output.append(
f" # {i} ===> {np.array2string(vec, formatter=formatter, separator=', ')}"
)
output.append(
f"Volume of reciprocal unit cell = {self.recip_volume:5.3f} [A^-d]\n"
)
output.append("Orbital vectors (Cartesian):")
for i, orb in enumerate(self._orb_vecs_cart):
output.append(
f" # {i} ===> {np.array2string(orb, formatter=formatter, separator=', ')}"
)
output.append("")
output.append("Orbital vectors (fractional):")
for i, orb in enumerate(self.orb_vecs):
output.append(
f" # {i} ===> {np.array2string(orb, formatter=formatter, separator=', ')}"
)
output.append("----------------------------------------")
return output
[docs]
def info(self, show: bool = True) -> str:
"""Generate a report of the lattice properties.
Parameters
----------
show : bool, optional
If True, prints the report to standard output (default).
If False, only returns the report string.
Returns
-------
str
The report string.
"""
output = self._report_list()
if show:
print("\n".join(output))
else:
return "\n".join(output)
[docs]
def get_orb_vecs(self, cartesian=False):
"""Return orbital positions.
Parameters
----------
cartesian : bool, optional
If True, returns orbital positions in Cartesian coordinates.
If False, returns reduced coordinates (default).
Returns
-------
np.ndarray
Array of orbital positions, shape (norb, dim_r).
"""
if cartesian:
return self._orb_vecs_cart.copy()
else:
return self.orb_vecs
[docs]
def get_lat_vecs(self):
"""Return lattice vectors in Cartesian coordinates.
Returns
-------
np.ndarray
Lattice vectors, shape ``(dim_r, dim_r)``.
"""
return self.lat_vecs
[docs]
def get_recip_lat_vecs(self):
"""Return reciprocal lattice vectors in Cartesian coordinates.
Returns
-------
np.ndarray
Reciprocal lattice vectors, shape ``(dim_k, dim_r)``.
Raises
------
ValueError
If the k-space dimension ``dim_k`` is zero (no periodic directions).
"""
return self.recip_lat_vecs
def _get_recip_lat(self):
r"""Reciprocal lattice vectors in inverse Cartesian coordinates.
Returns
-------
np.ndarray
Array of shape (dim_k, dim_r): rows are the reciprocal vectors :math:`\mathbf{b}_i`
in :math:`\mathbb{R}^{\texttt{dim_r}}`
satisfying :math:`\mathbf{a}_i \cdot \mathbf{b}_j = 2\pi \delta_{ij}`,
where :math:`\mathbf{a}_i` are the periodic real-space lattice vectors that
define k-space.
Notes
-----
- Works for ``dim_k <= dim_r``. When ``dim_k < dim_r``, returns the minimum-norm solution.
- Requires the periodic real-space vectors (rows of A_sub) to be linearly independent.
"""
if self.dim_k == 0:
logger.warning(
"Reciprocal lattice vectors are not defined for zero-dimensional k-space."
)
return None
# Select the real-space lattice vectors that generate k-space.
# Prefer an explicit list (e.g. self.per holds indices of periodic directions).
# Fallback: take the first dim_k lattice vectors.
lat = np.asarray(
self.lat_vecs, dtype=float
) # shape (dim_r, dim_r) in Cartesian coords
per = np.asarray(self.periodic_dirs, dtype=int)
if per.size != self.dim_k:
raise ValueError(
f"'per' must list exactly dim_k={self.dim_k} periodic directions."
)
A_sub = lat[per, :] # (dim_k, dim_r)
# Fast path: square case -> inverse transpose
if self.dim_k == self.dim_r:
# rows of B satisfy A_sub @ B.T = 2π I → B = 2π (A_sub^{-1})^T
try:
B = (2.0 * np.pi) * np.linalg.inv(A_sub).T
except np.linalg.LinAlgError:
raise ValueError(
"Real-space lattice vectors are linearly dependent (singular)."
)
else:
# Rectangular case (dim_k < dim_r): minimum-norm solution
# Check independence via Cholesky of Gram matrix (SPD iff independent)
G = A_sub @ A_sub.T # (dim_k, dim_k)
try:
# Cholesky proves PD and is faster than matrix_rank/SVD
np.linalg.cholesky(G)
except np.linalg.LinAlgError:
raise ValueError(
"Periodic real-space vectors are not linearly independent; "
"cannot construct reciprocal lattice for k-subspace."
)
# Solve G X = A_sub -> A_sub @ B.T = 2pi I, with X = G^{-1} A_sub
X = np.linalg.solve(G, A_sub) # (dim_k, dim_r)
# Rows b_i satisfy A_sub @ B^T = 2pi I_{dim_k}
B = (2.0 * np.pi) * X
return B
[docs]
def cut_piece(self, num_cells, periodic_dir) -> "Lattice":
r"""Cut a (d-1)-dimensional piece out of a d-dimensional Lattice.
Constructs a (d-1)-dimensional Lattice out of a
d-dimensional one by repeating the unit cell a given number of
times along one of the periodic lattice vectors. The lattice
vector along which the cut is made is no longer considered periodic,
but otherwise remains unchanged. Orbitals are added in the new unit cells
by translating the original orbitals by integer multiples of the lattice vectors.
Parameters
----------
num : int
How many times to repeat the unit cell.
fin_dir : int
Index of the real space lattice vector along
which you no longer wish to maintain periodicity.
Returns
-------
fin_lat : Lattice
Object of type :class:`pythtb.Lattice` representing a cutout
lattice.
See Also
--------
:ref:`cubic-slab-hwf-nb` : For an example
:ref:`three-site-thouless-nb` : For an example
Notes
-----
- Orbitals in `fin_lat` are numbered so that the `i`-th orbital of the `n`-th unit
cell has index ``i + norb * n`` (here `norb` is the number of orbitals in the original model).
- The real-space lattice vectors of the returned model are the same as those of
the original model; only the dimensionality of reciprocal space
is reduced.
"""
if self.dim_k == 0:
raise Exception("Lattice is already finite")
if not isinstance(num_cells, int):
raise TypeError("Parameter `num_cells` is not an integer")
if num_cells < 1:
raise ValueError("Argument num_cells must be positive!")
new_per = copy.deepcopy(self.periodic_dirs)
if periodic_dir not in new_per:
raise Exception("Can not make model finite along this direction!")
# remove index which is no longer periodic
new_per.remove(periodic_dir)
# generate orbitals of a finite model
fin_orb = []
for i in range(num_cells): # go over all cells in finite direction
for j in range(self.norb): # go over all orbitals in one cell
orb_tmp = np.copy(self.orb_vecs[j, :])
# change coordinate along finite direction
orb_tmp[periodic_dir] += float(i)
fin_orb.append(orb_tmp)
fin_orb = np.array(fin_orb)
fin_lat = Lattice(self.lat_vecs, fin_orb, periodic_dirs=new_per)
fin_lat._nsuper = copy.deepcopy(self.nsuper)
fin_lat._nsuper[periodic_dir] = num_cells
return fin_lat
[docs]
def add_orb(self, orb_pos):
r"""Add an orbital to the lattice.
Parameters
----------
orb_pos : array_like
Position of the new orbital in reduced coordinates (fractions of the lattice vectors).
Must be of length ``dim_r``.
Returns
-------
None
Notes
-----
- The new orbital is added at the end of the list of orbitals.
- The number of orbitals ``norb`` is updated accordingly.
"""
if isinstance(orb_pos, (float, int)):
orb_pos = np.array([orb_pos], float)
elif isinstance(orb_pos, list):
orb_pos = np.array(orb_pos, float)
elif not isinstance(orb_pos, np.ndarray):
raise TypeError(f"Expected array_like or float, got {type(orb_pos)}")
if orb_pos.ndim != 1 or orb_pos.shape[0] != self.dim_r:
raise ValueError(f"Orbital position must be of length {self.dim_r}.")
self.orb_vecs = np.vstack([self.orb_vecs, orb_pos])
[docs]
def remove_orb(self, to_remove):
r"""Remove an orbital from the lattice.
Parameters
----------
to_remove : array-like or int
List of orbital indices to be removed, or index of single orbital to be removed
Returns
-------
None
Notes
-----
- The number of orbitals ``norb`` is updated accordingly.
- Raises an error if the index is out of bounds.
"""
if isinstance(to_remove, int):
indices = [to_remove]
elif isinstance(to_remove, (list, np.ndarray)):
indices = list(to_remove)
else:
raise TypeError("to_remove must be an integer or a list of integers.")
for index in indices:
if not isinstance(index, int):
raise TypeError("All indices in to_remove must be integers.")
if index < 0 or index >= self.norb:
raise ValueError("Index out of bounds.")
# check that all indices are unique
if len(indices) != len(set(indices)):
raise ValueError("All indices in to_remove must be unique.")
# put the orbitals to be removed in descending order
orb_index = sorted(indices, reverse=True)
# remove indices one by one
for i, orb_ind in enumerate(orb_index):
# adjust variables
self.orb_vecs = np.delete(self.orb_vecs, orb_ind, 0)
[docs]
def change_nonperiodic_vector(self, fin_dir: int, new_lat_vec=None):
r"""Change non-periodic lattice vector.
Returns :class:`Lattice` in which one of the non-periodic "lattice vectors"
is changed. Non-periodic lattice vectors are those that are not listed as periodic
with the `periodic_dirs` parameter. The returned object has modified reduced coordinates
of orbitals, consistent with the new choice of lattice vector. Therefore, the actual
(Cartesian) coordinates of orbitals in original and new :class:`Lattice`
are the same.
Parameters
----------
fin_dir : int
Index of non-periodic lattice vector to change.
new_lat_vec : array_like, optional
The new non-periodic lattice vector. If None (default), the new
non-periodic lattice vector is constructed to be orthogonal to all periodic
vectors and to have the same length as the original non-periodic vector.
See Also
--------
periodic_dirs : Property listing periodic directions.
:ref:`boron-nitride-nb` : For an example.
"""
if not isinstance(fin_dir, int):
raise TypeError("Argument fin_dir must be an integer")
if fin_dir in self.periodic_dirs:
raise ValueError(f"Selected direction {fin_dir} is not nonperiodic")
if new_lat_vec is None:
# construct new nonperiodic lattice vector
per_temp = np.zeros_like(self.lat_vecs)
for direc in self.periodic_dirs:
per_temp[direc] = self.lat_vecs[direc]
# find projection coefficients onto space of periodic vectors
coeffs = np.linalg.lstsq(per_temp.T, self.lat_vecs[fin_dir], rcond=None)[0]
projec = np.dot(self.lat_vecs.T, coeffs)
# subtract off to get new nonperiodic vector
np_lattice_vec = self.lat_vecs[fin_dir] - projec
if np.linalg.norm(np_lattice_vec) < 1e-10:
raise ValueError("""New nonperiodic vector has zero length!?""")
# normalize new nonperiodic vector to have same length as original
np_lattice_vec /= np.linalg.norm(np_lattice_vec)
np_lattice_vec *= np.linalg.norm(self.lat_vecs[fin_dir])
# check that new nonperiodic vector is perpendicular to all periodic vectors
for i in self.periodic_dirs:
if np.abs(np.dot(self.lat_vecs[i], np_lattice_vec)) > 1e-6:
raise ValueError(
"""This shouldn't happen. New nonperiodic vector
is not perpendicular to periodic vectors!?"""
)
else:
# new_latt_vec is passed as argument
np_lattice_vec = np.array(new_lat_vec)
# check shape
if np_lattice_vec.shape != (self.dim_r,):
raise ValueError("Non-periodic vector has wrong shape.")
if np.linalg.norm(np_lattice_vec) < 1e-10:
raise ValueError("New non-periodic vector has zero length.")
og_orb_cart = copy.deepcopy(self._orb_vecs_cart)
# Define new set of lattice vectors
new_lat = copy.deepcopy(self.lat_vecs)
new_lat[fin_dir] = np_lattice_vec
# Update reduced orb vecs
new_orb = []
for orb_cart in og_orb_cart:
# convert to reduced coordinates
new_orb.append(np.linalg.solve(new_lat.T, orb_cart))
# update lattice vectors and orbitals
self.lat_vecs = np.array(new_lat, dtype=float)
self.orb_vecs = np.array(new_orb, dtype=float)
logger.info(
f"Updated lattice vectors to {new_lat} and orbitals to {new_orb} after changing nonperiodic vector."
)
# Are cartesian coordinates of orbitals the same in two cases?
for idx, orb_cart in enumerate(og_orb_cart):
cart_old = orb_cart
cart_new = self._orb_vecs_cart[idx]
if np.max(np.abs(cart_old - cart_new)) > 1e-6:
raise ValueError(
"""This shouldn't happen. New choice of nonperiodic vector
somehow changed Cartesian coordinates of orbitals."""
)
def _prepare_supercell_geometry(self, sc_red_lat):
"""Validate and build geometric data for a super-cell transformation."""
if self.dim_r == 0:
raise ValueError(
"Must have at least one periodic direction to make a super-cell"
)
use_sc_red_lat = np.asarray(sc_red_lat)
if use_sc_red_lat.shape != (self.dim_r, self.dim_r):
raise ValueError("Dimension of sc_red_lat array must be dim_r*dim_r")
if not np.issubdtype(use_sc_red_lat.dtype, np.integer):
raise TypeError("sc_red_lat array elements must be integers")
use_sc_red_lat = use_sc_red_lat.astype(int, copy=False)
per_mask = np.isin(np.arange(self.dim_r), self.periodic_dirs)
diag = np.diag(use_sc_red_lat)
if np.any(~per_mask & (diag != 1)):
raise ValueError(
"Diagonal elements of sc_red_lat for non-periodic directions must equal 1."
)
off_mask = ~(per_mask[:, None] & per_mask[None, :])
off_diag = use_sc_red_lat - np.diag(diag)
if np.any(off_mask & (off_diag != 0)):
raise ValueError(
"Off-diagonal elements of sc_red_lat for non-periodic directions must equal 0."
)
vol = float(np.linalg.det(use_sc_red_lat))
if abs(vol) < 1e-6:
raise ValueError("Super-cell lattice vectors volume too close to zero.")
if vol < 0:
raise ValueError(
"Super-cell lattice vectors volume is negative. Must form right-handed system."
)
red_transform = np.linalg.inv(use_sc_red_lat.astype(float))
max_R = int(np.max(np.abs(use_sc_red_lat))) * self.dim_r
candidate_axis = np.arange(-max_R, max_R + 1, dtype=int)
if self.dim_r == 1:
candidates = candidate_axis[:, None]
else:
grids = np.meshgrid(*([candidate_axis] * self.dim_r), indexing="ij")
candidates = np.stack(grids, axis=-1).reshape(-1, self.dim_r)
reduced = candidates @ red_transform
eps_shift = np.sqrt(2) * 1e-8
inside = np.all((-eps_shift < reduced) & (reduced <= 1 - eps_shift), axis=1)
sc_vec = candidates[inside]
expected = int(round(abs(vol)))
if sc_vec.shape[0] != expected:
raise Exception(
"Super-cell generation failed! Wrong number of super-cell vectors found."
)
sc_cart_lat = use_sc_red_lat @ self.lat_vecs
orb_grid = sc_vec[:, None, :] + self.orb_vecs[None, :, :]
sc_orb = (
(orb_grid.reshape(-1, self.dim_r) @ red_transform)
if orb_grid.size
else np.zeros((0, self.dim_r), dtype=float)
)
return {
"lat_vecs": sc_cart_lat,
"orb_vecs": sc_orb,
"translations": sc_vec,
"red_transform": red_transform,
"sc_red_lat": use_sc_red_lat,
}
[docs]
def make_supercell(
self,
sc_red_lat,
return_sc_vectors: bool = False,
to_home: bool = True,
to_home_warning: bool = True,
):
r"""Make lattice a super-cell.
.. versionchanged:: 2.0.0
Parameter `to_home_supress_warning` has been renamed to `to_home_warning`.
Note: this change inverts the meaning of the boolean parameter.
Constructs a :class:`pythtb.TBModel` representing a super-cell
of the current object. This function can be used together with :func:`cut_piece`
in order to create slabs with arbitrary surfaces.
By default all orbitals will be shifted to the home cell after
unit cell has been created. That way all orbitals will have
reduced coordinates between 0 and 1. If you wish to avoid this
behavior, you need to set, *to_home* argument to *False*.
"""
geom = self._prepare_supercell_geometry(sc_red_lat)
self.lat_vecs = geom["lat_vecs"]
self.orb_vecs = geom["orb_vecs"]
self._nsuper = list(np.diag(geom["sc_red_lat"]))
if to_home:
self._shift_orb_to_home(to_home_warning=to_home_warning)
if return_sc_vectors:
return geom["translations"].copy()
def _shift_orb_to_home(self, to_home_warning: bool = True):
r"""Shifts orbital coordinates (along periodic directions) to the home
unit cell.
After this function is called reduced coordinates
(along periodic directions) of orbitals will be between 0 and
1.
Version of pythtb 1.7.2 (and earlier) was shifting orbitals to
home along even nonperiodic directions. In the later versions
of the code (this present version, and future versions) we
don't allow this anymore, as this feature might produce
counterintuitive results. Shifting orbitals along nonperiodic
directions changes physical nature of the tight-binding model.
This behavior might be especially non-intuitive for
tight-binding models that came from the *cut_piece* function.
Parameters
----------
to_home_warning: bool, optional
Default value is ``True``. If ``True`` prints warning messages
about orbitals being outside the home cell (reduced coordinate larger
than 1 or smaller than 0 along non-periodic direction).
Note that setting this parameter to *True* or *False* has no effect on
resulting coordinates of the model.
"""
orb_vecs_new = copy.deepcopy(self.orb_vecs)
# go over all orbitals
for i in range(self.norb):
# find displacement vector needed to bring back to home cell
disp_vec = np.zeros(self.dim_r, dtype=int)
for k in range(self.dim_r):
shift = np.floor(self.orb_vecs[i, k]).astype(int)
# shift only in periodic directions
if k in self.periodic_dirs:
disp_vec[k] = shift
elif (
k not in self.periodic_dirs and shift != 0 and to_home_warning
): # check for shift in non-periodic directions
logger.warning(
f"Orbital {i} has reduced coordinate {self.orb_vecs[i, k]:.3f} "
f"along non-periodic direction {k}, which is outside the home cell."
)
orb_vecs_new[i] -= disp_vec
self.orb_vecs = orb_vecs_new
[docs]
def nn_bonds(self, n_shell: int, report: bool = False):
r"""Enumerate nearest-neighbor shells of the lattice.
The lattice's orbitals are treated as points in real space (Cartesian
coordinates). We form all displacement vectors connecting each orbital
to every other orbital translated by integer lattice vectors and group
them into ``n_shell`` distinct radial shells.
Parameters
----------
n_shell : int
Number of shells to return (starting from the shortest non-zero
displacement).
report : bool, optional
If True, print a human-readable table of the shells and their
degeneracies. Default is ``False``.
Returns
-------
list of dict
List of length ``n_shell``. Each entry is a dictionary with keys:
``radius``
Shell radius in Cartesian units (float).
``coordination_number``
Dict mapping each orbital index to the number of neighbors it
has in this shell (int). For a single-orbital model this is
simply ``{0: Z}`` where ``Z`` is the coordination number (e.g.
``{0: 6}`` for the NN shell of a simple cubic lattice). For
multi-orbital models each entry gives the per-site count
independently, which may differ between inequivalent sites.
``bonds``
List of bonds in this shell. Each bond is a dictionary with:
- ``i`` (int): index of the orbital in the home unit cell.
- ``j`` (int): index of the neighboring orbital.
- ``lattice_vector`` (tuple of int): lattice translation ``R``
such that the neighbor sits at orbital ``j`` in unit cell
``R``. Pass directly to :meth:`set_hop`.
- ``displacement`` (list of float): Cartesian vector
:math:`\Delta\mathbf{r}` from orbital ``i`` to orbital
``j + R``.
Only one of each conjugate pair ``(i, j, R)`` / ``(j, i, -R)``
is included; :meth:`set_hop` adds the conjugate automatically.
Raises
------
ValueError
If ``n_shell`` is not a positive integer, or if the lattice has no
orbitals or zero real-space dimension.
"""
if not isinstance(n_shell, int) or n_shell < 1:
raise ValueError("Invalid n_shell: must be an integer > 1.")
n_shell = int(n_shell)
if self.norb == 0:
raise ValueError("No orbitals in the lattice.")
if self.dim_r == 0:
raise ValueError("Lattice dimension is zero.")
lat_vecs = self.lat_vecs
dim_r = self.dim_r
orb_cart = self._orb_vecs_cart
norb = self.norb
# Enumerate candidate neighbors up to a reasonable window of lattice shifts
# R in Z^{dim_r} with components in [-n_shell, n_shell]
from itertools import product as _product
d2_list = [] # squared distances
dr_list = [] # Cartesian displacement vectors delta_r
idx_list = [] # integer meta: [i, j, [R]]
periodic_dirs = set(self.periodic_dirs)
shift_ranges = [
range(-n_shell - 1, n_shell + 2) if k in periodic_dirs else (0,)
for k in range(dim_r)
]
shifts = np.array(list(_product(*shift_ranges)), dtype=int)
for i in range(norb):
ri = orb_cart[i] # Cartesian position of orbital i
for R in shifts:
T_R = R @ lat_vecs # (dim_r,) Cartesian translation vector
for j in range(norb):
if i == j and not np.any(R):
# Skip self-pair with zero shift
continue
rj = orb_cart[j] + T_R # Cartesian position of orbital j
dr = rj - ri # delta_r (Cartesian)
d2 = float(dr @ dr) # squared distance
d2_list.append(d2)
dr_list.append(dr)
idx_list.append(np.concatenate(([i, j], R)))
if not d2_list:
return [] # No neighbors (e.g., single-orbital 0D model)
# Convert to arrays
dr_arr = np.vstack(dr_list) # (N, dim_r)
idx_arr = np.vstack(idx_list).astype(int) # (N, 2+dim_r)
d2_arr = np.asarray(d2_list)
# Numerical stability: round squared norms to cluster nearly-equal distances
d2_rounded = np.round(d2_arr, 12)
# Sort by distance
order = np.argsort(d2_rounded)
d2_sorted = d2_rounded[order]
dr_sorted = dr_arr[order]
idx_sorted = idx_arr[order]
# First n_shell unique radii
unique_d2 = []
for val in d2_sorted:
if not unique_d2 or val > unique_d2[-1]:
unique_d2.append(val)
if len(unique_d2) == n_shell:
break
# If fewer unique shells exist, truncate gracefully
n_take = min(n_shell, len(unique_d2))
unique_d2 = unique_d2[:n_take]
# Build one shell dict per unique radius
shells = []
for d2_target in unique_d2:
mask_s = d2_sorted == d2_target
dr_s = dr_sorted[mask_s]
idx_s = idx_sorted[mask_s]
radius = float(np.sqrt(d2_target))
# Collect canonical (non-redundant) bonds for this shell.
# For each pair (i→j+R) we skip its conjugate (j→i-R) to avoid
# double-counting. The conjugate is always added by set_hop automatically.
seen = set()
bonds = []
for k in range(idx_s.shape[0]):
i = int(idx_s[k, 0])
j = int(idx_s[k, 1])
R = tuple(int(x) for x in idx_s[k, 2:])
conj_key = (j, i, tuple(-x for x in R))
if conj_key in seen:
continue
key = (i, j, R)
if key not in seen:
seen.add(key)
bonds.append(
{
"i": i,
"j": j,
"lattice_vector": R,
"displacement": dr_s[k].tolist(),
}
)
# Count neighbors seen by each orbital (both directions included).
coordination_number = {
i: int(np.sum(idx_s[:, 0] == i)) for i in range(norb)
}
shells.append(
{
"radius": radius,
"coordination_number": coordination_number,
"bonds": bonds,
}
)
if report:
lines = ["nn-shell report", "═" * 60]
lines.append(f"dim_r: {dim_r} norb: {norb} shells: {len(shells)}")
for s, shell in enumerate(shells, start=1):
n = len(shell["bonds"])
cn = shell["coordination_number"]
cn_str = ", ".join(f"orb {i}: {c}" for i, c in cn.items())
lines.append(
f"shell {s:>2}: radius={shell['radius']:.8g} bonds={n} coordination=({cn_str})"
)
for bond in shell["bonds"][:6]:
R_str = str(bond["lattice_vector"])
dr_str = np.array2string(
np.array(bond["displacement"]),
precision=6,
floatmode="maxprec_equal",
suppress_small=True,
)
lines.append(
f" i={bond['i']} -> j={bond['j']}, R={R_str}, Δr={dr_str}"
)
if len(shell["bonds"]) > 6:
lines.append(f" ... (+{len(shell['bonds']) - 6} more)")
print("\n".join(lines))
return shells
[docs]
def nn_k_shell(self, nks: tuple, n_shell: int, report: bool = False):
r"""Generates shells of k-points around the :math:`\Gamma` point.
.. versionadded:: 2.0.0
Returns array of vectors connecting the origin to nearest
neighboring k-points in the mesh. The functions works only
for full k-meshes, i.e., when the number of k-points is specified
along all periodic directions.
Parameters
----------
nks : tuple of int
Number of k-points along each periodic direction. Length must be `dim_k`.
n_shell : int
Number of nearest neighbor shells to include.
report : bool
If True, prints a summary of the k-shell.
Returns
-------
k_shell : list[np.ndarray[float]]
List of :math:`\mathbf{b}` vectors in inverse units of lattice vectors
connecting nearest neighbor k-mesh points. Length is `n_shell`.
idx_shell : list[np.ndarray[int]]
Each entry is an array of integer shifts that takes a k-point
index in the mesh to its nearest neighbors.
Length is `n_shell`.
"""
if not isinstance(nks, (list, tuple, np.ndarray)):
raise TypeError("nks must be a sequence of ints with length dim_k.")
nks = np.asarray(nks, dtype=int)
if nks.ndim != 1 or nks.size != self.dim_k:
raise ValueError(f"nks must have length dim_k={self.dim_k}.")
if np.any(nks <= 0):
raise ValueError("All mesh sizes in nks must be positive.")
if not isinstance(n_shell, int) or n_shell < 1:
raise ValueError("n_shell must be a positive integer.")
if self.dim_k == 0:
raise ValueError("k-shells are not defined when dim_k == 0.")
# Reciprocal primitive vectors for periodic dirs: rows (dim_k) embed in R^{dim_r}
B = self.recip_lat_vecs
def shift_to_dk_cart(s):
# s: (dim_k, ), delta_k = sum (s_mu /nks_mu) b_mu
coeffs = s / nks.astype(float) # (dim_k,)
return coeffs @ B # (dim_r,)
shells = []
idx_shell = []
seen_radii = []
tol = 1e-12
rmax = 1
while len(shells) < n_shell:
# enumerate integer shifts in the hypercube [-rmax, rmax]^dim_k excluding zero
from itertools import product
ranges = [range(-rmax, rmax + 1) for _ in range(self.dim_k)]
cand_shifts = np.array(
[s for s in product(*ranges) if any(si != 0 for si in s)], dtype=int
)
if cand_shifts.size == 0:
rmax += 1
continue
dk_cart = np.array(
[shift_to_dk_cart(s) for s in cand_shifts]
) # (Ncand, dim_r)
dists = np.linalg.norm(dk_cart, axis=1)
order = np.argsort(dists)
cand_shifts = cand_shifts[order]
dk_cart = dk_cart[order]
dists = dists[order]
i = 0
while i < len(dists) and len(shells) < n_shell:
r0 = dists[i]
# skip if this radius already captured
if any(abs(r0 - rr) <= tol * max(1.0, rr) for rr in seen_radii):
j = i + 1
while j < len(dists) and abs(dists[j] - r0) <= tol * max(1.0, r0):
j += 1
i = j
continue
# collect current shell
j = i + 1
while j < len(dists) and abs(dists[j] - r0) <= tol * max(1.0, r0):
j += 1
shells.append(dk_cart[i:j].copy())
idx_shell.append(cand_shifts[i:j].copy())
seen_radii.append(r0)
i = j
rmax += 1
if report:
print("k-shell summary:")
for s, (vecs, shifts, rrep) in enumerate(
zip(shells, idx_shell, seen_radii)
):
print(f" shell {s}: M_s={len(vecs)}, |Δk|≈{rrep:.6e} (first)")
return shells, idx_shell
[docs]
def k_shell_weights(
self,
nks: tuple,
n_shell: int = 1,
return_shell: bool = True,
report: bool = False,
):
r"""Generates the finite difference weights on a k-shell.
This function uses the k-shells generated by :func:`nn_k_shell`
to compute the weights for finite difference approximations of
:math:`\nabla_{\mathbf{k}}` on a Monkhorst-Pack k-mesh. To linear
order, the following expression must be satisfied
.. math::
\sum_{s}^{N_{\rm sh}} w_s \sum_{i}^{M_s} b_{\alpha}^{i,s}
b_{\beta}^{i,s} = \delta_{\alpha,\beta}
where :math:`N_{\rm sh} \equiv` ``n_shell`` is the number of shells
defining the order of nearest neighbors, :math:`M_s` is the number of
k-points in the :math:`s`-th shell, and :math:`b_{\alpha}^{i,s}` is the
:math:`\alpha`-th Cartesian component of :math:`i`-th vector
connecting k-points to their nearest neighbors in the
:math:`s`-th shell.
Parameters
----------
n_shell : int
The number of shells to consider.
report : bool
Whether to print a report of the k-shells.
Returns
-------
w : np.ndarray
The finite difference weights.
k_shell : list[np.ndarray[float]], optional
List of :math:`\mathbf{b}` vectors in inverse units of lattice vectors
connecting nearest neighbor k-mesh points. Length is `n_shell`.
idx_shell : list[np.ndarray[int]], optional
Each entry is an array of integer shifts that takes a k-point
index in the mesh to its nearest neighbors.
Length is `n_shell`.
"""
from itertools import combinations_with_replacement as comb
k_shell, idx_shell = self.nn_k_shell(nks, n_shell=n_shell, report=report)
dim_k = self.dim_k
cart_idx = list(comb(range(dim_k), 2))
n_comb = len(cart_idx)
A = np.zeros((n_comb, n_shell))
q = np.zeros((n_comb))
for j, (alpha, beta) in enumerate(cart_idx):
if alpha == beta:
q[j] = 1
for s in range(n_shell):
b_star = k_shell[s]
for i in range(b_star.shape[0]):
b = b_star[i]
A[j, s] += b[alpha] * b[beta]
U, D, Vt = np.linalg.svd(A, full_matrices=False)
w = (Vt.T @ np.linalg.inv(np.diag(D)) @ U.T) @ q
if return_shell:
return w, k_shell, idx_shell
return w
[docs]
def k_path(self, k_nodes, nk: int, report: bool = False):
r"""Interpolates a path in reciprocal space.
Interpolates a path in reciprocal space between specified
k-points. In 2D or 3D the k-path can consist of several
straight segments connecting high-symmetry points ("nodes").
The interpolated path is constructed so that the k-points
are (nearly) equidistant in Cartesian k-space.
Parameters
----------
k_nodes : array-like, str
Array of k-vectors in reduced units, between
which the interpolated path will be constructed.
In 1D k-space, value may be a string:
- `"full"`: Implies ``[0.0, 0.5, 1.0]`` (full BZ)
- `"fullc"`: Implies ``[-0.5, 0.0, 0.5]`` (full BZ, centered)
- `"half"`: Implies ``[ 0.0, 0.5]`` (half BZ)
nk : int
Total number of k-points along the path.
report : bool, optional
Optional parameter specifying whether printout
is desired (default is False).
Returns
-------
k_vec : np.ndarray
Array of (nearly) equidistant interpolated k-points. Shape is ``(nk, dim_k)``.
k_dist : np.ndarray
Array giving accumulated k-distance to each
k-point in the path. This array is useful when plotting
bands along the path. The distances between the points
can be used to ensure that the plot accurately reflects
the k-space geometry. Shape is ``(nk,)``.
.. versionchanged:: 2.0.0
The returned ``k_dist`` now includes the factors of :math:`2\pi`.
See notes for further details.
k_node : np.ndarray
Array giving accumulated k-distance to each
node on the path in Cartesian coordinates. This array can
be used to reference the nodes on the 1D ``k_dist`` array,
e.g., when plotting high-symmetry points. Shape is ``(n_nodes,)``.
Notes
-----
- The distance between the points is calculated in the Cartesian frame,
however coordinates themselves are given in dimensionless reduced coordinates!
This is done so that this array can be directly passed to function
:func:`pythtb.TBModel.solve_ham`.
- Unlike array ``k_vec``, ``k_dist`` has dimensions! Units are defined
so that for a one-dimensional crystal with lattice constant equal to
for example :math:`10` the length of the Brillouin zone would equal
:math:`2\pi/10`.
Examples
--------
Construct a path connecting four nodal points in k-space
Path will contain 401 k-points, roughly equally spaced
>>> path = [[0.0, 0.0], [0.0, 0.5], [0.5, 0.5], [0.0, 0.0]]
>>> (k_vec, k_dist, k_node) = my_model.k_path(path,401)
Solve for eigenvalues on that path and plot the band structure
>>> import matplotlib.pyplot as plt
>>> evals = tb.solve_ham(k_vec)
>>> for n in range(evals.shape[1]):
... plt.plot(k_dist, evals[:, n], 'b-')
>>> for node_dist in k_node:
... plt.axvline(x=node_dist, color='k', linestyle='--')
>>> plt.xlabel('k')
>>> plt.ylabel('Energy (eV)')
>>> plt.show()
"""
# Parse kpts and validate
k_list = _parse_kpts(k_nodes, self.dim_k)
if k_list.shape[1] != self.dim_k:
raise ValueError(
f"Dimension mismatch: kpts shape {k_list.shape}, model dim {self.dim_k}"
)
if nk < len(k_list):
raise ValueError("nk must be >= number of nodes in kpts")
# Extract periodic lattice and compute k-space metric
lat_per = self.lat_vecs[self.periodic_dirs]
B = self.recip_lat_vecs
k_metric = B @ B.T
# Compute segment vectors and lengths in Cartesian metric
diffs = k_list[1:] - k_list[:-1]
seg_lengths = np.sqrt(np.einsum("ij,ij->i", diffs @ k_metric, diffs))
# Accumulated node distances
k_node = np.concatenate(([0.0], np.cumsum(seg_lengths)))
# Determine indices in the final array corresponding to each node
node_index = np.rint(k_node / k_node[-1] * (nk - 1)).astype(int)
# Initialize output arrays
k_vec = np.empty((nk, self.dim_k))
k_dist = np.empty(nk)
# Interpolate each segment
for i, (start, end) in enumerate(zip(node_index[:-1], node_index[1:])):
length = end - start
t = np.linspace(0, 1, length + 1)
k_vec[start : end + 1] = k_list[i] + np.outer(t, diffs[i])
k_dist[start : end + 1] = k_node[i] + t * seg_lengths[i]
# Trim any round-off overshoot
k_vec = k_vec[:nk]
k_dist = k_dist[:nk]
if report:
print("----- k_path report -----")
np.set_printoptions(precision=5)
print("Real-space lattice vectors:\n", lat_per)
print("K-space metric tensor:\n", k_metric)
print("Nodes (reduced coords):\n", k_list)
if lat_per.shape[0] == lat_per.shape[1]:
gvecs = np.linalg.inv(lat_per).T
print("Reciprocal-space vectors:\n", gvecs)
print("Nodes (Cartesian coords):\n", k_list @ gvecs)
print("Segments:")
for n in range(1, len(k_node)):
length = k_node[n] - k_node[n - 1]
print(
f" Node {n - 1} {k_list[n - 1]} to Node {n} {k_list[n]}: "
f"distance = {length:.5f}"
)
print("Node distances (cumulative):", k_node)
print("Node indices in path:", node_index)
print("-------------------------")
return k_vec, k_dist, k_node
[docs]
def get_kpath_distance(
self, kpts, k_nodes=None, labels=None, cartesian=False, tol=1e-8
):
"""Transform k-points to k-distance along a path.
Parameters
----------
kpts : array_like
Array of k-points in reduced coordinates.
k_nodes : array_like, optional
Array of special k-point nodes along the path.
labels : list of str, optional
Labels corresponding to the k_nodes.
tol : float, optional
Tolerance for matching k-points, by default 1e-8
Returns
-------
k_dist : array
Cumulative k-point distances along the path.
node_dist : array, optional
Distances of the special k-point nodes.
node_indices : dict, optional
Indices of the special k-point nodes.
label_indices : dict, optional
Mapping from labels to k-point nodes.
"""
B = self.recip_lat_vecs
if cartesian:
kpts = kpts @ np.linalg.inv(B).T
# cumulative distances between points
_, k_dist, _ = self.k_path(kpts, nk=kpts.shape[0], report=False)
# k_dist = kpath_distance(kpts, b1=B[0], b2=B[1], b3=B[2])
if k_nodes is not None:
node_indices = {}
for i, node in enumerate(k_nodes):
mask = np.all(np.isclose(kpts, node, atol=tol), axis=1)
idx = np.where(mask)[0]
if len(idx) > 0:
node_indices[f"{str(node)}"] = list(idx)
else:
node_indices[f"{str(node)}"] = None
# flatten all values into a single list
all_indices = [idx for indices in node_indices.values() for idx in indices]
# sort them
all_indices_sorted = np.sort(all_indices)
# now you can index into k_dist
node_dist = k_dist[all_indices_sorted]
if labels is not None:
label_indices = {}
for i, node in enumerate(k_nodes):
label_indices[labels[i]] = node
return k_dist, node_dist, node_indices, label_indices
else:
return k_dist, node_dist, node_indices
else:
return k_dist
[docs]
def visualize(
self,
proj_plane=None,
n_cells=1,
):
r"""Visualizes the lattice geometry.
This function creates a 2D plot of your tight-binding model,
showing the unit-cell origin, lattice vectors (with arrowheads),
and orbitals.
Parameters
----------
proj_plane : list of int, optional
List of two integers specifying the directions to project onto.
For example, in a 3D model, ``proj_plane=[0, 2]`` would project
onto the x-z plane. If not provided, the function will attempt
to automatically select a suitable projection plane based on
the model's dimensionality.
n_cells : int, optional
Number of unit cells to display along each lattice vector.
Default is 1.
Returns
-------
fig : matplotlib.figure.Figure
ax : matplotlib.axes.Axes
Notes
-----
- This function is intended for visualizing two dimensional lattices.
For three-dimensional visualizations, consider using
the :func:`visualize_3d` method.
"""
from pythtb.visualization import plot_lattice
return plot_lattice(self, n_cells=n_cells, proj_plane=proj_plane)
[docs]
def visualize_3d(
self,
n_cells=1,
site_colors=None,
site_names=None,
show_lattice_info=True,
):
r"""Visualize a 3D tight-binding model using ``Plotly``.
This function creates an interactive 3D plot of your tight-binding model,
showing the unit-cell origin, lattice vectors (with arrowheads), orbitals,
hopping lines, and (optionally) an eigenstate overlay with marker sizes
proportional to amplitude and colors reflecting the phase.
Parameters
----------
n_cells: int, optional
Number of unit cells to display along each lattice vector.
Default is 1.
site_colors: list of str, optional
List of colors for each orbital site (e.g. ``["red", "blue", "green"]``).
Must abide by Plotly color specifications. If not provided, default colors will be used.
site_names: list of str, optional
List of names for each orbital site (e.g. ``["A", "B", "C"]``).
If provided, these names will be displayed next to the corresponding orbitals.
show_lattice_info: bool, optional
Whether to display lattice information (lattice vectors, orbital positions).
Returns
-------
plotly.graph_objs.Figure
"""
from pythtb.visualization import plot_lattice_3d
return plot_lattice_3d(
self,
n_cells=n_cells,
show_lattice_info=show_lattice_info,
site_colors=site_colors,
site_names=site_names,
)
