Create local_Chern_marker_of_half_BHZ_model.py

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guanjihuan 2024-08-19 08:02:07 +08:00
parent d636bd256c
commit 6b3baa95c4

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import numpy as np
import guan
# 计算投影算符
def compute_projection_operator(Ny, Nx):
H0, H1, H2 = guan.get_onsite_and_hopping_terms_of_half_bhz_model_for_spin_down(A=0.3645/5, B=-0.686/25, C=0, D=-0.512/25, M=-0.01, a=1)
hamiltonian = guan.hamiltonian_of_finite_size_system_along_two_directions_for_square_lattice(N1=Ny, N2=Nx, on_site=H0, hopping_1=H1, hopping_2=H2, period_1=0, period_2=0)
P = np.zeros((2*Ny*Nx, 2*Ny*Nx), dtype=complex)
eigenvalue, eigenvector = np.linalg.eigh(hamiltonian)
occupied = 0
for i0 in eigenvalue:
if i0 <= 0:
occupied += 1
for i0 in range(occupied):
P += np.outer(eigenvector[:, i0], eigenvector[:, i0].conj())
return P
# 计算local Chern marker
def compute_local_chern_marker(Ny, Nx, P):
C_local = np.zeros((Ny, Nx), dtype=complex)
x_array = np.zeros((2*Ny*Nx))
y_array = np.zeros((2*Ny*Nx))
for iy in range(Ny):
for ix in range(Nx):
x_array[2*Nx*iy + 2*ix + 0] = ix
x_array[2*Nx*iy + 2*ix + 1] = ix
y_array[2*Nx*iy + 2*ix + 0] = iy
y_array[2*Nx*iy + 2*ix + 1] = iy
x_matrix = np.diag(x_array)
y_matrix = np.diag(y_array)
PxP = P @ x_matrix @ P
PyP = P @ y_matrix @ P
commutator = PxP @ PyP - PyP @ PxP
for iy in range(Ny):
for ix in range(Nx):
C_local[iy, ix] = -2 * np.pi * 1j * (commutator[2*Nx*iy+ 2*ix + 0, 2*Nx*iy+ 2*ix + 0] + commutator[2*Nx*iy+ 2*ix + 1, 2*Nx*iy+ 2*ix + 1])
# # 或者用这个
# temp = 4 * np.pi * np.imag(P @ x_matrix @ P @ y_matrix @ P)
# for iy in range(Ny):
# for ix in range(Nx):
# C_local[iy, ix] = temp[2*Nx*iy + 2*ix + 0, 2*Nx*iy + 2*ix + 0] + temp[2*Nx*iy + 2*ix + 1, 2*Nx*iy + 2*ix + 1]
return C_local.real
Nx=30
Ny=30
P = compute_projection_operator(Ny, Nx)
C_local = compute_local_chern_marker(Ny, Nx, P)
guan.plot_pcolor(range(Nx), range(Ny), C_local, cmap='RdBu')