Yb171_F35_HighN
- class rydstate.species.ytterbium.yb171_eigen_channel_model_data.Yb171_F35_HighN(mqdt)[source]
- Parameters:
mqdt (MQDT)
- species = 'Yb171'
The species for which the MQDT model is defined.
- name = 'F F=7/2, nu > 20'
The name of the atomic species.
- f_tot = 3.5
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 = (20.0, 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 = [AngularKetLS(i_c=0.5, s_c=0.5, l_c=0, s_r=0.5, l_r=3, s_tot=0.0, l_tot=3, j_tot=3.0, f_tot=3.5, n_c=6), AngularKetLS(i_c=0.5, s_c=0.5, l_c=0, s_r=0.5, l_r=3, s_tot=1.0, l_tot=3, j_tot=3.0, f_tot=3.5, n_c=6), AngularKetFJ(i_c=0.5, s_c=0.5, l_c=Unknown, s_r=0.5, l_r=Unknown, j_c=Unknown, f_c=Unknown, j_r=Unknown, f_tot=3.5, parity=-1, n_c=Unknown, label=4f13 5d 6snl a), AngularKetFJ(i_c=0.5, s_c=0.5, l_c=Unknown, s_r=0.5, l_r=Unknown, j_c=Unknown, f_c=Unknown, j_r=Unknown, f_tot=3.5, parity=-1, n_c=Unknown, label=4f13 5d 6snl b), AngularKetFJ(i_c=0.5, s_c=0.5, l_c=Unknown, s_r=0.5, l_r=Unknown, j_c=Unknown, f_c=Unknown, j_r=Unknown, f_tot=3.5, parity=-1, n_c=Unknown, label=4f13 5d 6snl c), AngularKetFJ(i_c=0.5, s_c=0.5, l_c=Unknown, s_r=0.5, l_r=Unknown, j_c=Unknown, f_c=Unknown, j_r=Unknown, f_tot=3.5, parity=-1, n_c=Unknown, label=4f13 5d 6snl d), AngularKetFJ(i_c=0.5, s_c=0.5, l_c=Unknown, s_r=0.5, l_r=Unknown, j_c=Unknown, f_c=Unknown, j_r=Unknown, f_tot=3.5, parity=-1, n_c=Unknown, label=4f13 5d 6snl e), AngularKetLS(i_c=0.5, s_c=0.5, l_c=0, s_r=0.5, l_r=3, s_tot=1.0, l_tot=3, j_tot=4.0, f_tot=3.5, 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=3, j_c=0.5, f_c=1.0, j_r=3.5, f_tot=3.5, n_c=6), AngularKetFJ(i_c=0.5, s_c=0.5, l_c=0, s_r=0.5, l_r=3, j_c=0.5, f_c=1.0, j_r=2.5, f_tot=3.5, n_c=6), AngularKetFJ(i_c=0.5, s_c=0.5, l_c=Unknown, s_r=0.5, l_r=Unknown, j_c=Unknown, f_c=Unknown, j_r=Unknown, f_tot=3.5, parity=-1, n_c=Unknown, label=4f13 5d 6snl a), AngularKetFJ(i_c=0.5, s_c=0.5, l_c=Unknown, s_r=0.5, l_r=Unknown, j_c=Unknown, f_c=Unknown, j_r=Unknown, f_tot=3.5, parity=-1, n_c=Unknown, label=4f13 5d 6snl b), AngularKetFJ(i_c=0.5, s_c=0.5, l_c=Unknown, s_r=0.5, l_r=Unknown, j_c=Unknown, f_c=Unknown, j_r=Unknown, f_tot=3.5, parity=-1, n_c=Unknown, label=4f13 5d 6snl c), AngularKetFJ(i_c=0.5, s_c=0.5, l_c=Unknown, s_r=0.5, l_r=Unknown, j_c=Unknown, f_c=Unknown, j_r=Unknown, f_tot=3.5, parity=-1, n_c=Unknown, label=4f13 5d 6snl d), AngularKetFJ(i_c=0.5, s_c=0.5, l_c=Unknown, s_r=0.5, l_r=Unknown, j_c=Unknown, f_c=Unknown, j_r=Unknown, f_tot=3.5, parity=-1, n_c=Unknown, label=4f13 5d 6snl e), AngularKetFJ(i_c=0.5, s_c=0.5, l_c=0, s_r=0.5, l_r=3, j_c=0.5, f_c=0.0, j_r=3.5, f_tot=3.5, n_c=6)]
List of outer channels in the MQDT model.
- eigen_quantum_defects = [[0.277086649, -13.290196, 0], [0.0719837014, -0.754736076, 0], [4.251457795, 0, 0], [4.227434828, 0, 0], [4.175780645, 0, 0], [4.196547521, 0, 0], [4.21440857, 0, 0], [0.0834193873, -1.11453386, -1545.71844]]
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, [-0.0209955122, 0.251041249]), (0, 2, [-0.0585753224]), (0, 3, [-0.0750574327]), (0, 4, [0.122671919]), (0, 5, [-0.0401036164]), (0, 6, [0.0654271994]), (1, 2, [-0.0683007974]), (1, 3, [0.035415976]), (1, 4, [-0.0327625807]), (1, 5, [-0.050225071]), (1, 6, [0.0455759316])]
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.