quantum{ }¶
A group of keywords specifying quantum models, i.e. how the Schrödinger equation should be solved.
Groups located directly under quantum{ }
are:
- Code Example
quantum{ debuglevel = 1 allow_overlapping_regions = no #---------------- # Quantum regions #---------------- region{ name = "qr1" quantize_x{} quantize_y{} quantize_z{} no_density = yes x = [10.0, 20.0] y = [10.0, 20.0] z = [10.0, 20.0] # Boundary conditions #-------------------- boundary{ x = dirichlet y = dirichlet z = neumann classical_boundary_x = no classical_boundary_y = no classical_boundary_z = no num_classical_x = [1,1] num_classical_y = [1,1] num_classical_z = [1,1] } # Output definitions #------------------- output_wavefunctions{ max_num = 10 all_k_points = yes/no structured = no amplitudes = "S_X_Y_Z CB_HH_LH_SO" probabilities = "yes CB_HH_LH_SO" scale = 0.7 in_one_file = yes energy_shift = both include_energies_in_shifted_files = yes } output_subband_densities{ max_num = 10 in_one_file = yes } output_sparse_matrix{ type = all structured = no } output_rotated_inverse_mass_tensor{ boxes = yes structured = no } # Quantum models and solver definitions #-------------------------------------- Gamma{ num_ev = 10 # Eigensolvers (choose one) lapack{} arpack{} accuracy = 1e-6 iterations = 200 preconditioner = chebyshev cutoff = 0.3 abs_cutoff = 2.5 order_chebyshev = 20 # Dispersion #----------- dispersion{ path{ name = "100" point{ k = [1.0, 0.0, 0.0] k = [1.0, 1.0, 0.0] } spacing = 0.5 num_points = 10 } lines{ name = "lines" spacing = 0.5 k_max = 1.0 } full{ name = "3D" kxgrid{ line{ pos = -1 spacing = 0.02 } } kygrid{ line{ pos = -1 spacing = 0.02 } } kzgrid{ line{ pos = -1 spacing = 0.02 } } } superlattice{ name = "superlattice" num_points_x = 10 num_points_y = 15 num_points_z = 20 num_points = 20 } } } L{ ... (same as Gamma) } X{ ... (same as Gamma) } Delta{ ... (same as Gamma) } HH{ ... (same as Gamma) } LH{ ... (same as Gamma) } SO{ ... (same as Gamma) } kp_6band{ ... (same as Gamma) kp_parameters{ use_Luttinger_parameters = no approximate_kappa = no } lapack{} #arpack{} k_integration{ relative_size = 0.2 num_points = 5 num_subpoints = 2 max_symmetry = no force_k0_subspace = yes } } kp_8band{ num_electrons = 6 num_holes = 12 accuracy = 1e-8 iterations = 200 kp_parameters{ use_Luttinger_parameters = no from_6band_parameters = no approximate_kappa = no evaluate_S = no rescale_S_to = 1.0 } k_integration{ ... (same as kp_6band) } lapack{} #arpack_inv{} shift_window = 0 shift = 0.2 abs_shift = 2.5 linear_solver{ iterations = 500 abs_accuracy = 1e-9 rel_accuracy = 1e-9 use_cscg = no force_diagonal_preconditioner = no } #advanced settings for 8-band k.p quantum density shift_min_CB = 0.0 shift_max_VB = 0.0 tunneling = yes classify_kspace = 0 threshold_classification = 0.5 full_band_density = no } #Matrix elements definitions #--------------------------- interband_matrix_elements{ KP6_Gamma{} HH_Gamma{} # < HH_i | Gamma_j > LH_Gamma{} # < LH_i | Gamma_j > SO_Gamma{} # < SO_i | Gamma_j > HH_Delta{} # < HH_i | Delta_j > LH_Delta{} # < LH_i | Delta_j > SO_Delta{} # < SO_i | Delta_j > HH_X{} # < HH_i | X_j > LH_X{} # < LH_i | X_j > SO_X{} # < SO_i | X_j > HH_L{} # < HH_i | L_j > LH_L{} # < LH_i | L_j > SO_L{} # < SO_i | L_j > output_matrix_elements = yes output_transition_energies = yes/no # } intraband_matrix_elements{ direction = [1,1,0] Gamma{} Delta{} X{} L{} HH{} LH{} SO{} KP6{} KP8{} output_matrix_elements = yes/no output_transition_energies = yes/no output_oscillator_strengths = yes/no } dipole_moment_matrix_elements{ direction = [1,1,0] Gamma{} Delta{} X{} L{} HH{} LH{} SO{} KP6{} KP8{} output_matrix_elements = yes output_transition_energies = yes output_oscillator_strengths = yes } transition_energies{ Gamma{} KP6_Gamma{} HH_Gamma{} LH_Gamma{} SO_Gamma{} Delta{} HH_Delta{} LH_Delta{} SO_Delta{} X{} HH_X{} LH_X{} SO_X{} L{} HH_L{} LH_L{} SO_L{} HH{} LH{} SO{} KP6{} KP8{} } lifetimes{ phonon_energy = 0.036 Gamma{} HH{} LH{} } } # end: region{} #Many body effects #----------------- exchange_correlation{ type = lda initial_spin_pol = 1.0 output_spin_polarization{} output_exchange_correlation{} } }