quantax.symmetry.Translation#

class quantax.symmetry.Translation#

Bases: Symmetry

Translation symmetry.

__init__(vectors: Sequence[int] | NDArray[integer], sector: int | Sequence[int] = 0)#

Translation symmetry.

Parameters:

vectors – The translation vectors, in the unit of lattice basis vectors.
sector – The symmetry sector.

property vectors: ndarray#: The translation vectors.

get_sublattice_coord() → ndarray#: Get the coordinate of lattice sites in the sublattice.

property Nmodes: int#: The length of a configuration array, i.e. the number of local modes per sample. This is Nsites for spins or spinless fermions and 2 * Nsites for spinful fermions.

property Nparticles: int | tuple[int, int] | None#

The number of particles.

None: No particle conservation.
int: Conservation of total particle number.
Tuple[int, int]: Conservation of spin-up and spin-down particle numbers.

property Nsites: int#: The number of sites.

property Z2_inversion: int#

The Z2 inversion symmetry. It represents the spin flip in spin-1/2 systems, and the particle-hole symmetry in fermionic systems. The meaning of each number is

1: Eigenvalue 1 after Z2 inversion
0: No Z2 inversion symmetry
-1: Eigenvalue -1 after Z2 inversion

property basis#: The QuSpin basis corresponding to the symmetry.

basis_make() → None#: Make the QuSpin basis stored in the symmetry.

property character: Array#: Characters \(\chi\) of all group elements.

property double_occ: bool#: Whether the system allows double occupancy.

get_symm_spins(spins: Array) → Array#

Get all symmetrized bases \(s'=Ts\) generated by the symmetry permutations.

Parameters:: spins – Input spin or fermion configuration \(s\).

Note

This function is jittable.

property is_fermion: bool#: Whether the system is made of fermions.

property is_spinful: bool#: Whether the system is spinful.

property nsymm: int#: Number of elements in the symmetry group.

property particle_type: PARTICLE_TYPE#: The type of particle in the system. See PARTICLE_TYPE.

Symmetrize the wavefunction as

\[\psi^{\mathrm{symm}}(s) = \frac{d}{|G|} \sum_g \mathrm{sign}(s, g) \chi_g \psi(T_g s),\]

where \(d\) is the dimension of the group representation, \(|G|\) is the number of elements in the symmetry group, and \(\mathrm{sign}(s, g)\) is the additional sign generated by the symmetry depending on the input Fock state (only for fermionic systems).

Parameters:

psi – Wavefunctions \(\psi(T_i s)\).
spins – Input spin or fermion configuration \(s\). This is only necessary in fermionic systems, where additional minus signs \(\mathrm{sign}(s, g)\) can be generated by the symmetry.

Returns:

The symmetrized wave function

Note

This function is jittable.