Yb171_G45_HighN
- class rydstate.species.ytterbium.yb171_eigen_channel_model_data.Yb171_G45_HighN(mqdt)[source]
- Parameters:
mqdt (MQDT)
- species = 'Yb171'
The species for which the MQDT model is defined.
- name = 'G F=9/2, nu > 25'
The name of the atomic species.
- f_tot = 4.5
Total angular momentum f_tot of the Rydberg state.
- parity = 1
Parity (-1 or +1) of the Rydberg state, i.e. (-1)^(l_c + l_r) of its channels.
- nu_range = (25.0, inf)
Range of effective principal quantum numbers nu for which the MQDT model is valid.
- reference = 'R. Kuroda et al., Phys. Rev. A 112, 042817 (2025), https://doi.org/10.1103/mzsv-rckx'
Reference for the MQDT model, e.g., a publication doi where the model is described.
- inner_channels = [AngularKetJJ(i_c=0.5, s_c=0.5, l_c=0, s_r=0.5, l_r=4, j_c=0.5, j_r=4.5, j_tot=4.0, f_tot=4.5, n_c=6), AngularKetJJ(i_c=0.5, s_c=0.5, l_c=0, s_r=0.5, l_r=4, j_c=0.5, j_r=3.5, j_tot=4.0, f_tot=4.5, n_c=6), AngularKetJJ(i_c=0.5, s_c=0.5, l_c=0, s_r=0.5, l_r=4, j_c=0.5, j_r=4.5, j_tot=5.0, f_tot=4.5, n_c=6)]
List of inner channels in the MQDT model.
- outer_channels = [AngularKetFJ(i_c=0.5, s_c=0.5, l_c=0, s_r=0.5, l_r=4, j_c=0.5, f_c=1.0, j_r=4.5, f_tot=4.5, n_c=6), AngularKetFJ(i_c=0.5, s_c=0.5, l_c=0, s_r=0.5, l_r=4, j_c=0.5, f_c=1.0, j_r=3.5, f_tot=4.5, n_c=6), AngularKetFJ(i_c=0.5, s_c=0.5, l_c=0, s_r=0.5, l_r=4, j_c=0.5, f_c=0.0, j_r=4.5, f_tot=4.5, n_c=6)]
List of outer channels in the MQDT model.
- eigen_quantum_defects = [[0.02628545, -0.13182564], [0.02548145, -0.12028462], [0.02536571, -0.18507079]]
List of eigen quantum defects for the close-coupling channels. Each entry is a list of polynomial coefficients; a constant is a single element list.
- mixing_angles = [(0, 1, [-0.089123698])]
List of mixing angles between close-coupling channels. Each entry is a tuple (i_idx, j_idx, coefficients) where i_idx and j_idx are the indices of the involved channels and coefficients is the list of expansion coefficients for the energy dependence of the angle (a constant angle is a single element list). The energy dependence is expanded in the nui of the first channel of the model, see
calc_frame_transformation_inner_closecoupling(). The default None means no mixing between the close-coupling channels.