From f77d69dfb8eb356aaedd1e1b54ad7c313e7e6dab Mon Sep 17 00:00:00 2001 From: guanjihuan Date: Fri, 1 Apr 2022 16:40:05 +0800 Subject: [PATCH] update --- .../02_Fourier_transform_and_calculate_band_structures.py | 2 +- Tutorial/04_some_models_in_the_reciprocal_space.py | 4 ++-- Tutorial/05_calculate_density_of_states.py | 2 +- Tutorial/06_calculate_conductance_and_scattering_matrix.py | 2 +- 4 files changed, 5 insertions(+), 5 deletions(-) diff --git a/Tutorial/02_Fourier_transform_and_calculate_band_structures.py b/Tutorial/02_Fourier_transform_and_calculate_band_structures.py index 9d8b677..b4a212c 100644 --- a/Tutorial/02_Fourier_transform_and_calculate_band_structures.py +++ b/Tutorial/02_Fourier_transform_and_calculate_band_structures.py @@ -4,4 +4,4 @@ import numpy as np k_array = np.linspace(-np.pi, np.pi, 100) hamiltonian_function = guan.one_dimensional_fourier_transform_with_k(unit_cell=0, hopping=1) # one dimensional chain eigenvalue_array = guan.calculate_eigenvalue_with_one_parameter(k_array, hamiltonian_function) -guan.plot(k_array, eigenvalue_array, xlabel='k', ylabel='E', type='-k') \ No newline at end of file +guan.plot(k_array, eigenvalue_array, xlabel='k', ylabel='E', style='-k') \ No newline at end of file diff --git a/Tutorial/04_some_models_in_the_reciprocal_space.py b/Tutorial/04_some_models_in_the_reciprocal_space.py index c30ef36..567a0ef 100644 --- a/Tutorial/04_some_models_in_the_reciprocal_space.py +++ b/Tutorial/04_some_models_in_the_reciprocal_space.py @@ -3,6 +3,6 @@ import numpy as np k_array = np.linspace(-np.pi, np.pi, 100) eigenvalue_array = guan.calculate_eigenvalue_with_one_parameter(k_array, guan.hamiltonian_of_square_lattice_in_quasi_one_dimension) -guan.plot(k_array, eigenvalue_array, xlabel='k', ylabel='E', type='-k') +guan.plot(k_array, eigenvalue_array, xlabel='k', ylabel='E', style='-k') eigenvalue_array = guan.calculate_eigenvalue_with_one_parameter(k_array, guan.hamiltonian_of_graphene_with_zigzag_in_quasi_one_dimension) -guan.plot(k_array, eigenvalue_array, xlabel='k', ylabel='E', type='-k') \ No newline at end of file +guan.plot(k_array, eigenvalue_array, xlabel='k', ylabel='E', style='-k') \ No newline at end of file diff --git a/Tutorial/05_calculate_density_of_states.py b/Tutorial/05_calculate_density_of_states.py index 4b0a820..73b0106 100644 --- a/Tutorial/05_calculate_density_of_states.py +++ b/Tutorial/05_calculate_density_of_states.py @@ -4,7 +4,7 @@ import numpy as np hamiltonian = guan.hamiltonian_of_finite_size_system_along_two_directions_for_square_lattice(2,2) fermi_energy_array = np.linspace(-4, 4, 400) total_dos_array = guan.total_density_of_states_with_fermi_energy_array(fermi_energy_array, hamiltonian, broadening=0.1) -guan.plot(fermi_energy_array, total_dos_array, xlabel='E', ylabel='Total DOS', type='-') +guan.plot(fermi_energy_array, total_dos_array, xlabel='E', ylabel='Total DOS', style='-') fermi_energy = 0 N1 = 3 diff --git a/Tutorial/06_calculate_conductance_and_scattering_matrix.py b/Tutorial/06_calculate_conductance_and_scattering_matrix.py index 5f50d13..a935bd7 100644 --- a/Tutorial/06_calculate_conductance_and_scattering_matrix.py +++ b/Tutorial/06_calculate_conductance_and_scattering_matrix.py @@ -5,7 +5,7 @@ fermi_energy_array = np.linspace(-4, 4, 400) h00 = guan.hamiltonian_of_finite_size_system_along_one_direction(4) h01 = np.identity(4) conductance_array = guan.calculate_conductance_with_fermi_energy_array(fermi_energy_array, h00, h01) -guan.plot(fermi_energy_array, conductance_array, xlabel='E', ylabel='Conductance', type='-') +guan.plot(fermi_energy_array, conductance_array, xlabel='E', ylabel='Conductance', style='-') fermi_energy = 0 guan.print_or_write_scattering_matrix(fermi_energy, h00, h01) \ No newline at end of file