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guanjihuan 2022-11-06 22:10:55 +08:00
parent 49e3efd12c
commit 92b1824a1d
3 changed files with 7 additions and 7 deletions
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6
academic_codes/2020.09.30_bandstructure_of_graphene_on_high_symmetric_axes/bandstructure_of_graphene_on_high_symmetric_axes.py
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@ -10,9 +10,9 @@ import cmath # 要处理复数情况，用到cmath.exp()
def hamiltonian(k1, k2, M=0, t1=1, a=1/sqrt(3)): # Haldane哈密顿量(a为原子间距，不赋值的话默认为1/sqrt(3)） def hamiltonian(k1, k2, M=0, t1=1, a=1/sqrt(3)): # Haldane哈密顿量(a为原子间距，不赋值的话默认为1/sqrt(3)）
h0 = np.zeros((2, 2))*(1+0j) h0 = np.zeros((2, 2), dtype=complex)
h1 = np.zeros((2, 2))*(1+0j) h1 = np.zeros((2, 2), dtype=complex)
h2 = np.zeros((2, 2))*(1+0j) h2 = np.zeros((2, 2), dtype=complex)
# 质量项(mass term), 用于打开带隙 # 质量项(mass term), 用于打开带隙
h0[0, 0] = M h0[0, 0] = M

6
academic_codes/2021.01.10_Berry_curvature_distribution_of_graphene_under_broken_inversion_symmery/Berry_curvature_distribution_of_graphene_under_broken_inversion_symmery.py
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@ -11,7 +11,7 @@ import time
def hamiltonian(k1, k2, t1=2.82, a=1/sqrt(3)): # 石墨烯哈密顿量（a为原子间距，不赋值的话默认为1/sqrt(3)） def hamiltonian(k1, k2, t1=2.82, a=1/sqrt(3)): # 石墨烯哈密顿量（a为原子间距，不赋值的话默认为1/sqrt(3)）
h = np.zeros((2, 2))*(1+0j) h = np.zeros((2, 2), dtype=complex)
h[0, 0] = 0.28/2 h[0, 0] = 0.28/2
h[1, 1] = -0.28/2 h[1, 1] = -0.28/2
h[1, 0] = t1*(cmath.exp(1j*k2*a)+cmath.exp(1j*sqrt(3)/2*k1*a-1j/2*k2*a)+cmath.exp(-1j*sqrt(3)/2*k1*a-1j/2*k2*a)) h[1, 0] = t1*(cmath.exp(1j*k2*a)+cmath.exp(1j*sqrt(3)/2*k1*a-1j/2*k2*a)+cmath.exp(-1j*sqrt(3)/2*k1*a-1j/2*k2*a))
@ -69,9 +69,9 @@ def main():
j0 += 1 j0 += 1
if band==0: if band==0:
plot_3d_surface(kx_array/pi, ky_array/pi, F_all, xlabel='kx', ylabel='ky', zlabel='Berry curvature', title='Valence Band', rcount=300, ccount=300) plot_3d_surface(kx_array/pi, ky_array/pi, F_all, xlabel='k_x (pi)', ylabel='k_y (pi)', zlabel='Berry curvature', title='Valence Band', rcount=300, ccount=300)
else: else:
plot_3d_surface(kx_array/pi, ky_array/pi, F_all, xlabel='kx', ylabel='ky', zlabel='Berry curvature', title='Conductance Band', rcount=300, ccount=300) plot_3d_surface(kx_array/pi, ky_array/pi, F_all, xlabel='k_x (pi)', ylabel='k_y (pi)', zlabel='Berry curvature', title='Conductance Band', rcount=300, ccount=300)
# import guan # import guan
# if band==0: # if band==0:
# guan.plot_3d_surface(kx_array/pi, ky_array/pi, F_all, xlabel='kx', ylabel='ky', zlabel='Berry curvature', title='Valence Band', rcount=300, ccount=300) # guan.plot_3d_surface(kx_array/pi, ky_array/pi, F_all, xlabel='kx', ylabel='ky', zlabel='Berry curvature', title='Valence Band', rcount=300, ccount=300)

2
academic_codes/2021.01.10_Berry_curvature_distribution_of_graphene_under_broken_inversion_symmery/Berry_curvature_distribution_with_ky=0.py
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@ -11,7 +11,7 @@ import time
def hamiltonian(k1, k2, t1=2.82, a=1/sqrt(3)): # 石墨烯哈密顿量（a为原子间距，不赋值的话默认为1/sqrt(3)） def hamiltonian(k1, k2, t1=2.82, a=1/sqrt(3)): # 石墨烯哈密顿量（a为原子间距，不赋值的话默认为1/sqrt(3)）
h = np.zeros((2, 2))*(1+0j) h = np.zeros((2, 2), dtype=complex)
h[0, 0] = 0.28/2 h[0, 0] = 0.28/2
h[1, 1] = -0.28/2 h[1, 1] = -0.28/2
h[1, 0] = t1*(cmath.exp(1j*k2*a)+cmath.exp(1j*sqrt(3)/2*k1*a-1j/2*k2*a)+cmath.exp(-1j*sqrt(3)/2*k1*a-1j/2*k2*a)) h[1, 0] = t1*(cmath.exp(1j*k2*a)+cmath.exp(1j*sqrt(3)/2*k1*a-1j/2*k2*a)+cmath.exp(-1j*sqrt(3)/2*k1*a-1j/2*k2*a))