0.0.88

PyPI/setup.cfg

@@ -1,7 +1,7 @@
 [metadata]
 # replace with your username:
 name = guan
-version = 0.0.87
+version = 0.0.88
 author = guanjihuan
 author_email = guanjihuan@163.com
 description = An open source python package

PyPI/src/guan/__init__.py

@@ -115,7 +115,11 @@ hopping = guan.get_hopping_term_of_graphene_ribbon_along_zigzag_direction(N, eta
 
 hamiltonian = guan.hamiltonian_of_finite_size_system_along_two_directions_for_graphene(N1, N2, period_1=0, period_2=0)
 
-H0, H1, H2 = get_onsite_and_hopping_terms_of_BHZ_model(A=0.3645/5, B=-0.686/25, C=0, D=-0.512/25, M=-0.01, a=1)
+H0, H1, H2 = guan.get_onsite_and_hopping_terms_of_BHZ_model(A=0.3645/5, B=-0.686/25, C=0, D=-0.512/25, M=-0.01, a=1)
+
+H0, H1, H2 = guan.get_onsite_and_hopping_terms_of_half_BHZ_model_for_spin_up(A=0.3645/5, B=-0.686/25, C=0, D=-0.512/25, M=-0.01, a=1)
+
+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)
 
 
 
@@ -141,6 +145,8 @@ hamiltonian = guan.hamiltonian_of_haldane_model_in_quasi_one_dimension(k, N=10,
 
 hamiltonian = guan.hamiltonian_of_one_QAH_model(k1, k2, t1=1, t2=1, t3=0.5, m=-1)
 
+hamiltonian = guan.hamiltonian_of_BHZ_model(kx, ky, A=0.3645/5, B=-0.686/25, C=0, D=-0.512/25, M=-0.01)
+
 hamiltonian = guan.hamiltonian_of_half_BHZ_model_for_spin_up(kx, ky, A=0.3645/5, B=-0.686/25, C=0, D=-0.512/25, M=-0.01)
 
 hamiltonian = guan.hamiltonian_of_half_BHZ_model_for_spin_down(kx, ky, A=0.3645/5, B=-0.686/25, C=0, D=-0.512/25, M=-0.01)
@@ -682,6 +688,50 @@ def get_onsite_and_hopping_terms_of_BHZ_model(A=0.3645/5, B=-0.686/25, C=0, D=-0
     H2[3, 2] = -1j*V_sp
     return H0, H1, H2
 
+def get_onsite_and_hopping_terms_of_half_BHZ_model_for_spin_up(A=0.3645/5, B=-0.686/25, C=0, D=-0.512/25, M=-0.01, a=1):
+    E_s = C+M-4*(D+B)/(a**2)
+    E_p = C-M-4*(D-B)/(a**2)
+    V_ss = (D+B)/(a**2)
+    V_pp = (D-B)/(a**2)
+    V_sp = -1j*A/(2*a)
+    H0 = np.zeros((2, 2), dtype=complex)
+    H1 = np.zeros((2, 2), dtype=complex)
+    H2 = np.zeros((2, 2), dtype=complex)
+    H0[0, 0] = E_s
+    H0[1, 1] = E_p
+    H1[0, 0] = V_ss
+    H1[1, 1] = V_pp
+    H1[0, 1] = V_sp
+    H1[1, 0] = -np.conj(V_sp)
+    H2[0, 0] = V_ss
+    H2[1, 1] = V_pp
+    H2[0, 1] = 1j*V_sp
+    H2[1, 0] = 1j*np.conj(V_sp)
+    return H0, H1, H2
+
+def 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):
+    E_s = C+M-4*(D+B)/(a**2)
+    E_p = C-M-4*(D-B)/(a**2)
+    V_ss = (D+B)/(a**2)
+    V_pp = (D-B)/(a**2)
+    V_sp = -1j*A/(2*a)
+    H0 = np.zeros((2, 2), dtype=complex)
+    H1 = np.zeros((2, 2), dtype=complex)
+    H2 = np.zeros((2, 2), dtype=complex)
+    H0[0, 0] = E_s
+    H0[1, 1] = E_p
+    H1[0, 0] = V_ss
+    H1[1, 1] = V_pp
+    H1[0, 1] = np.conj(V_sp)
+    H1[1, 0] = -V_sp
+    H2[0, 0] = V_ss
+    H2[1, 1] = V_pp
+    H2[0, 1] = -1j*np.conj(V_sp)
+    H2[1, 0] = -1j*V_sp
+    return H0, H1, H2
+
+
+
 
 
 
@@ -817,6 +867,21 @@ def hamiltonian_of_one_QAH_model(k1, k2, t1=1, t2=1, t3=0.5, m=-1):
     hamiltonian[1, 1] = -(m+2*t3*math.sin(k1)+2*t3*math.sin(k2)+2*t2*math.cos(k1+k2))
     return hamiltonian
 
+def hamiltonian_of_BHZ_model(kx, ky, A=0.3645/5, B=-0.686/25, C=0, D=-0.512/25, M=-0.01):
+    hamiltonian = np.zeros((4, 4), dtype=complex)
+    varepsilon = C-2*D*(2-math.cos(kx)-math.cos(ky))
+    d3 = -2*B*(2-(M/2/B)-math.cos(kx)-math.cos(ky))
+    d1_d2 = A*(math.sin(kx)+1j*math.sin(ky))
+    hamiltonian[0, 0] = varepsilon+d3
+    hamiltonian[1, 1] = varepsilon-d3
+    hamiltonian[0, 1] = np.conj(d1_d2)
+    hamiltonian[1, 0] = d1_d2
+    hamiltonian[2, 2] = varepsilon+d3
+    hamiltonian[3, 3] = varepsilon-d3
+    hamiltonian[2, 3] = -d1_d2 
+    hamiltonian[3, 2] = -np.conj(d1_d2)
+    return hamiltonian
+
 def hamiltonian_of_half_BHZ_model_for_spin_up(kx, ky, A=0.3645/5, B=-0.686/25, C=0, D=-0.512/25, M=-0.01):
     hamiltonian = np.zeros((2, 2), dtype=complex)
     varepsilon = C-2*D*(2-math.cos(kx)-math.cos(ky))