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0.0.107 period

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guanjihuan 2022-07-13 06:53:27 +08:00
parent 35f2d18463
commit cf5a6f1031
3 changed files with 21 additions and 8 deletions
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6
API_Reference.py
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@ -103,7 +103,7 @@ hamiltonian = guan.hamiltonian_of_simple_chain(k)
hamiltonian = guan.hamiltonian_of_square_lattice(k1, k2) hamiltonian = guan.hamiltonian_of_square_lattice(k1, k2)
hamiltonian = guan.hamiltonian_of_square_lattice_in_quasi_one_dimension(k, N=10) hamiltonian = guan.hamiltonian_of_square_lattice_in_quasi_one_dimension(k, N=10, period=0)
hamiltonian = guan.hamiltonian_of_cubic_lattice(k1, k2, k3) hamiltonian = guan.hamiltonian_of_cubic_lattice(k1, k2, k3)
@ -111,11 +111,11 @@ hamiltonian = guan.hamiltonian_of_ssh_model(k, v=0.6, w=1)
hamiltonian = guan.hamiltonian_of_graphene(k1, k2, M=0, t=1, a=1/math.sqrt(3)) hamiltonian = guan.hamiltonian_of_graphene(k1, k2, M=0, t=1, a=1/math.sqrt(3))
hamiltonian = guan.hamiltonian_of_graphene_with_zigzag_in_quasi_one_dimension(k, N=10, M=0, t=1) hamiltonian = guan.hamiltonian_of_graphene_with_zigzag_in_quasi_one_dimension(k, N=10, M=0, t=1, period=0)
hamiltonian = guan.hamiltonian_of_haldane_model(k1, k2, M=2/3, t1=1, t2=1/3, phi=math.pi/4, a=1/math.sqrt(3)) hamiltonian = guan.hamiltonian_of_haldane_model(k1, k2, M=2/3, t1=1, t2=1/3, phi=math.pi/4, a=1/math.sqrt(3))
hamiltonian = guan.hamiltonian_of_haldane_model_in_quasi_one_dimension(k, N=10, M=2/3, t1=1, t2=1/3, phi=math.pi/4) hamiltonian = guan.hamiltonian_of_haldane_model_in_quasi_one_dimension(k, N=10, M=2/3, t1=1, t2=1/3, phi=math.pi/4, period=0)
hamiltonian = guan.hamiltonian_of_one_QAH_model(k1, k2, t1=1, t2=1, t3=0.5, m=-1) hamiltonian = guan.hamiltonian_of_one_QAH_model(k1, k2, t1=1, t2=1, t3=0.5, m=-1)

2
PyPI/setup.cfg
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@ -1,7 +1,7 @@
[metadata] [metadata]
# replace with your username: # replace with your username:
name = guan name = guan
version = 0.0.106 version = 0.0.107
author = guanjihuan author = guanjihuan
author_email = guanjihuan@163.com author_email = guanjihuan@163.com
description = An open source python package description = An open source python package

21
PyPI/src/guan/__init__.py
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@ -2,7 +2,7 @@
# With this package, you can calculate band structures, density of states, quantum transport and topological invariant of tight-binding models by invoking the functions you need. Other frequently used functions are also integrated in this package, such as file reading/writing, figure plotting, data processing. # With this package, you can calculate band structures, density of states, quantum transport and topological invariant of tight-binding models by invoking the functions you need. Other frequently used functions are also integrated in this package, such as file reading/writing, figure plotting, data processing.
# The current version is guan-0.0.106, updated on July 12, 2022. # The current version is guan-0.0.107, updated on July 13, 2022.
# Installation: pip install --upgrade guan # Installation: pip install --upgrade guan
@ -442,12 +442,15 @@ def hamiltonian_of_square_lattice(k1, k2):
hamiltonian = guan.two_dimensional_fourier_transform_for_square_lattice(k1, k2, unit_cell=0, hopping_1=1, hopping_2=1) hamiltonian = guan.two_dimensional_fourier_transform_for_square_lattice(k1, k2, unit_cell=0, hopping_1=1, hopping_2=1)
return hamiltonian return hamiltonian
def hamiltonian_of_square_lattice_in_quasi_one_dimension(k, N=10): def hamiltonian_of_square_lattice_in_quasi_one_dimension(k, N=10, period=0):
h00 = np.zeros((N, N), dtype=complex) # hopping in a unit cell h00 = np.zeros((N, N), dtype=complex) # hopping in a unit cell
h01 = np.zeros((N, N), dtype=complex) # hopping between unit cells h01 = np.zeros((N, N), dtype=complex) # hopping between unit cells
for i in range(N-1): for i in range(N-1):
h00[i, i+1] = 1 h00[i, i+1] = 1
h00[i+1, i] = 1 h00[i+1, i] = 1
if period == 1:
h00[N-1, 0] = 1
h00[0, N-1] = 1
for i in range(N): for i in range(N):
h01[i, i] = 1 h01[i, i] = 1
hamiltonian = guan.one_dimensional_fourier_transform(k, unit_cell=h00, hopping=h01) hamiltonian = guan.one_dimensional_fourier_transform(k, unit_cell=h00, hopping=h01)
@ -473,7 +476,7 @@ def hamiltonian_of_graphene(k1, k2, M=0, t=1, a=1/math.sqrt(3)):
hamiltonian = h0 + h1 hamiltonian = h0 + h1
return hamiltonian return hamiltonian
def hamiltonian_of_graphene_with_zigzag_in_quasi_one_dimension(k, N=10, M=0, t=1): def hamiltonian_of_graphene_with_zigzag_in_quasi_one_dimension(k, N=10, M=0, t=1, period=0):
h00 = np.zeros((4*N, 4*N), dtype=complex) # hopping in a unit cell h00 = np.zeros((4*N, 4*N), dtype=complex) # hopping in a unit cell
h01 = np.zeros((4*N, 4*N), dtype=complex) # hopping between unit cells h01 = np.zeros((4*N, 4*N), dtype=complex) # hopping between unit cells
for i in range(N): for i in range(N):
@ -490,6 +493,9 @@ def hamiltonian_of_graphene_with_zigzag_in_quasi_one_dimension(k, N=10, M=0, t=1
for i in range(N-1): for i in range(N-1):
h00[i*4+3, (i+1)*4+0] = t h00[i*4+3, (i+1)*4+0] = t
h00[(i+1)*4+0, i*4+3] = t h00[(i+1)*4+0, i*4+3] = t
if period == 1:
h00[(N-1)*4+3, 0] = t
h00[0, (N-1)*4+3] = t
for i in range(N): for i in range(N):
h01[i*4+1, i*4+0] = t h01[i*4+1, i*4+0] = t
h01[i*4+2, i*4+3] = t h01[i*4+2, i*4+3] = t
@ -509,7 +515,7 @@ def hamiltonian_of_haldane_model(k1, k2, M=2/3, t1=1, t2=1/3, phi=math.pi/4, a=1
hamiltonian = h0 + h1 + h2 + h2.transpose().conj() hamiltonian = h0 + h1 + h2 + h2.transpose().conj()
return hamiltonian return hamiltonian
def hamiltonian_of_haldane_model_in_quasi_one_dimension(k, N=10, M=2/3, t1=1, t2=1/3, phi=math.pi/4): def hamiltonian_of_haldane_model_in_quasi_one_dimension(k, N=10, M=2/3, t1=1, t2=1/3, phi=math.pi/4, period=0):
h00 = np.zeros((4*N, 4*N), dtype=complex) # hopping in a unit cell h00 = np.zeros((4*N, 4*N), dtype=complex) # hopping in a unit cell
h01 = np.zeros((4*N, 4*N), dtype=complex) # hopping between unit cells h01 = np.zeros((4*N, 4*N), dtype=complex) # hopping between unit cells
for i in range(N): for i in range(N):
@ -534,6 +540,13 @@ def hamiltonian_of_haldane_model_in_quasi_one_dimension(k, N=10, M=2/3, t1=1, t2
h00[(i+1)*4+0, i*4+2] = h00[i*4+2, (i+1)*4+0].conj() h00[(i+1)*4+0, i*4+2] = h00[i*4+2, (i+1)*4+0].conj()
h00[i*4+3, (i+1)*4+1] = t2*cmath.exp(1j*phi) h00[i*4+3, (i+1)*4+1] = t2*cmath.exp(1j*phi)
h00[(i+1)*4+1, i*4+3] = h00[i*4+3, (i+1)*4+1].conj() h00[(i+1)*4+1, i*4+3] = h00[i*4+3, (i+1)*4+1].conj()
if period == 1:
h00[(N-1)*4+3, 0] = t1
h00[0, (N-1)*4+3] = t1
h00[(N-1)*4+2, 0] = t2*cmath.exp(1j*phi)
h00[0, (N-1)*4+2] = h00[(N-1)*4+2, 0].conj()
h00[(N-1)*4+3, 1] = t2*cmath.exp(1j*phi)
h00[1, (N-1)*4+3] = h00[(N-1)*4+3, 1].conj()
for i in range(N): for i in range(N):
h01[i*4+1, i*4+0] = t1 h01[i*4+1, i*4+0] = t1
h01[i*4+2, i*4+3] = t1 h01[i*4+2, i*4+3] = t1