import matplotlib.pyplot as plt from matplotlib import rc filename = 'unit_cell_1-02_two_reg' write_solver_input(filename +'.msh',dimension = 2, bc_type = 'Bloch', \ parameter = [], eq = 'EM', sol_type = 'Stationary',analysis_param \ = ['y', 'y', 15, 15, 21, 21, 5], bc_filename = filename +'_guide.bc') simu = Simulation() simu.read_solver_input(filename +'.msh') simu.domain.read_mesh_file(filename +'.msh',simu) inter = Interpreter(vectorial = True) eq = inter.build_EM_bloch_eq(simu) my_solver = Solver() k_coords, energy = my_solver.solve_bloch_Brillouin(simu, eq) fig = plt.figure() ax = fig.add_subplot(111) plt.title("Dispersion relations for Square lattice") k_div = k_coords.shape[0]/3 from numpy import sqrt, around print max(energy[:,-1]) for i in range(energy.shape[1]): energy[:,i] = sqrt(around(energy[:,i],10)) ax.plot(energy[:,i]) l = plt.axvline(x=k_div) l = plt.axvline(x=k_div*2+1) l = plt.axvline(x= k_coords.shape[0]) plt.ylim(0, max(energy[:,-1]))