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								2022.11.06_band_folding/band_folding.py
									
									
									
									
									
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								2022.11.06_band_folding/band_folding.py
									
									
									
									
									
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| """ | ||||
| This code is supported by the website: https://www.guanjihuan.com | ||||
| The newest version of this code is on the web page: https://www.guanjihuan.com/archives/27656 | ||||
| """ | ||||
|  | ||||
| import guan | ||||
| import numpy as np | ||||
|  | ||||
| # one dimensional chain model | ||||
| unit_cell = 0 | ||||
| hopping = 1 | ||||
| hamiltonian_function = guan.one_dimensional_fourier_transform_with_k(unit_cell, hopping) | ||||
| k_array = np.linspace(-np.pi, np.pi, 100) | ||||
| eigenvalue_array = guan.calculate_eigenvalue_with_one_parameter(k_array, hamiltonian_function) | ||||
| guan.plot(k_array, eigenvalue_array, xlabel='k', ylabel='E', style='k', title='one dimensional chain model') | ||||
|  | ||||
| # n times band folding | ||||
| max_n = 10 | ||||
| for n in np.arange(2, max_n+1): | ||||
|     unit_cell = np.zeros((n, n)) | ||||
|     for i0 in range(int(n)): | ||||
|         for j0 in range(int(n)): | ||||
|             if abs(i0-j0)==1: | ||||
|                 unit_cell[i0, j0] = 1 | ||||
|     hopping = np.zeros((n, n)) | ||||
|     hopping[0, n-1] = 1 | ||||
|     hamiltonian_function = guan.one_dimensional_fourier_transform_with_k(unit_cell, hopping) | ||||
|     k_array = np.linspace(-np.pi, np.pi, 100) | ||||
|     eigenvalue_array = guan.calculate_eigenvalue_with_one_parameter(k_array, hamiltonian_function) | ||||
|     guan.plot(k_array, eigenvalue_array, xlabel='k', ylabel='E', style='k', title='%i times band folding'%n) | ||||
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