Create Hofstadter_butterfly_of_graphene_ribbon.py
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"""
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This code is supported by the website: https://www.guanjihuan.com
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The newest version of this code is on the web page: https://www.guanjihuan.com/archives/12185
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"""
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import numpy as np
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from math import *
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import cmath
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import functools
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import guan
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def hamiltonian(B, k, N, M, t1): # graphene哈密顿量(N是条带的宽度参数)
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# 初始化为零矩阵
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h00 = np.zeros((4*N, 4*N), dtype=complex)
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h01 = np.zeros((4*N, 4*N), dtype=complex)
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# 原胞内的跃迁h00
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for i in range(N):
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h00[i*4+0, i*4+0] = M
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h00[i*4+1, i*4+1] = -M
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h00[i*4+2, i*4+2] = M
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h00[i*4+3, i*4+3] = -M
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# 最近邻
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h00[i*4+0, i*4+1] = t1*cmath.exp(-2*pi*1j*B*(3*i+1/4)*(np.sqrt(3)/2))
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h00[i*4+1, i*4+0] = np.conj(h00[i*4+0, i*4+1])
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h00[i*4+1, i*4+2] = t1
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h00[i*4+2, i*4+1] = np.conj(h00[i*4+1, i*4+2])
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h00[i*4+2, i*4+3] = t1*cmath.exp(2*pi*1j*B*(3*i+7/4)*(np.sqrt(3)/2))
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h00[i*4+3, i*4+2] = np.conj(h00[i*4+2, i*4+3])
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for i in range(N-1):
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# 最近邻
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h00[i*4+3, (i+1)*4+0] = t1
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h00[(i+1)*4+0, i*4+3] = t1
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# 原胞间的跃迁h01
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for i in range(N):
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# 最近邻
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h01[i*4+1, i*4+0] = t1*cmath.exp(-2*pi*1j*B*(3*i+1/4)*(np.sqrt(3)/2))
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h01[i*4+2, i*4+3] = t1*cmath.exp(-2*pi*1j*B*(3*i+7/4)*(np.sqrt(3)/2))
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matrix = h00 + h01*cmath.exp(1j*k) + h01.transpose().conj()*cmath.exp(-1j*k)
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return matrix
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def main():
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N = 30
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hamiltonian_function0 = functools.partial(hamiltonian, k=0, N=N, M=0, t1=1)
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B_array = np.linspace(0, 1/(3*np.sqrt(3)/2), 100)
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eigenvalue_array = guan.calculate_eigenvalue_with_one_parameter(B_array, hamiltonian_function0)
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BS_array = B_array*(3*np.sqrt(3)/2)
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guan.plot(BS_array, eigenvalue_array, xlabel='Flux (BS/phi_0)', ylabel='E', title='Ny=%i'%N, filename='a', show=1, save=0, type='k.', y_min=None, y_max=None, markersize=3)
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if __name__ == '__main__':
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main()
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