Yb171_P05_HighN

class rydstate.species.ytterbium.yb171_eigen_channel_model_data.Yb171_P05_HighN(mqdt)[source]
Parameters:

mqdt (MQDT)

species = 'Yb171'

The species for which the MQDT model is defined.

name = 'P F=1/2, nu > 5.9'

The name of the atomic species.

f_tot = 0.5

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 = (5.9, 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', 'fit for nu > 28, but extrapolates nicely down for nu > 5.9)')

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=1, s_tot=0.0, l_tot=1, j_tot=1.0, f_tot=0.5, n_c=6), AngularKetLS(i_c=0.5, s_c=0.5, l_c=0, s_r=0.5, l_r=1, s_tot=1.0, l_tot=1, j_tot=1.0, f_tot=0.5, 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=0.5, 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=0.5, 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=0.5, 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=0.5, parity=-1, n_c=Unknown, label=4f13 5d 6snl d), AngularKetLS(i_c=0.5, s_c=0.5, l_c=0, s_r=0.5, l_r=1, s_tot=1.0, l_tot=1, j_tot=0.0, f_tot=0.5, 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=0.5, parity=-1, n_c=Unknown, label=4f13 5d 6snl e)]

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=1, j_c=0.5, f_c=1.0, j_r=1.5, f_tot=0.5, n_c=6), AngularKetFJ(i_c=0.5, s_c=0.5, l_c=0, s_r=0.5, l_r=1, j_c=0.5, f_c=1.0, j_r=0.5, f_tot=0.5, 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=0.5, 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=0.5, 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=0.5, 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=0.5, parity=-1, n_c=Unknown, label=4f13 5d 6snl d), AngularKetFJ(i_c=0.5, s_c=0.5, l_c=0, s_r=0.5, l_r=1, j_c=0.5, f_c=0.0, j_r=0.5, f_tot=0.5, 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=0.5, parity=-1, n_c=Unknown, label=4f13 5d 6snl e)]

List of outer channels in the MQDT model.

eigen_quantum_defects = [[3.922094502, 2.12370136], [3.981191543, -4.54209175], [4.229094016, 0], [4.206073107, 0], [4.193527627, 0], [4.181165673, 0], [3.953185132, 0.0277444042], [4.198448494, 0]]

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, [-0.102285383, 153.521338, -15393.2283]), (1, 6, [0.00168607392]), (0, 2, [-0.0719467433]), (0, 3, [-0.0673315968]), (0, 4, [-0.0221077377]), (0, 5, [-0.107638329]), (1, 2, [0.0416653549]), (1, 3, [0.0590660991]), (1, 4, [0.0861585559]), (1, 5, [0.0566417469]), (6, 7, [0.163113423])]

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.