triqs.lattice.super_lattice.TBSuperLattice
- class triqs.lattice.super_lattice.TBSuperLattice(tb_lattice, super_lattice_units, cluster_sites=None, remove_internal_hoppings=False)[source]
Builds a superlattice on top of a base TBLattice.
- Parameters:
tb_lattice (TBLattice instance) – The base tight binding lattice.
super_lattice_units (ndarray (2D)) – The unit vectors of the superlattice in the
tb_lattice
(integer) coordinates.cluster_sites – Coordinates of the cluster in tb_lattice coordinates. If
None
, an automatic computation of cluster positions is made as follows: it takes all points whose coordinates in the basis of the superlattice are in [0, 1[^dimension.remove_internal_hoppings (bool) – If
true
, the hopping terms are removed inside the cluster. Useful to add Hartree Fock terms at the boundary of a cluster, e.g.
Methods
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Given a point on the tb_lattice in lattice coordinates, returns its coordinates (R, alpha) in the Superlattice |
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Given a point in the supercell R, site (number) alpha, it computes its position on the tb_lattice in lattice coordinates |
Generate the position of the cluster site in the tb_lattice coordinates. |
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Signature : (k_cvt K) -> nda::array<double, 1> Evaluate the dispersion relation for a momentum vector k in units of the reciprocal lattice vectors |
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Input: a function r-> f(r) on the tb_lattice given as a dictionnary Output: the function R-> F(R) folded on the superlattice. |
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Signature : (k_cvt K) -> matrix<dcomplex> Evaluate the fourier transform for a momentum vector k in units of the reciprocal lattice vectors |
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Return a mesh on the Brillouin zone with a given discretization |
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Return a mesh on the Bravais lattice with a given periodicity |
Signature : (r_t x) -> r_t Transform into real coordinates. |
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nsite and n_orbital must start at 0 |
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Inverse of pack_index_site_orbital |
Attributes
Number of orbitals in the unit cell |
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Number of dimensions of the lattice |
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The list of orbital names |
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The list of orbital positions |
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Number of dimensions of the lattice |