From: Rydberg energies and transition probabilities of Li I for np–ms (m ≤ 5) transitions
Level | Energy | Lifetime (ns) | ||||
---|---|---|---|---|---|---|
cm−1 | This work | Experimental value and method | Theoretical value and method | |||
2p | 14,904 | 27.400 | 27.102 | Photoassociation [18] | 27.2 | Central field approximation [6] |
27.29 | Laser excited atoms [15] | 27.24 | Realistic potentials [17] | |||
27.22 (0.2) | Delayed coincidence technique [20] | 27.32 | Coulomb approximation [8] | |||
26.99 (0.16) | Photoassociation in a magneto-optical trap [21] | 27.12 | CI-Hylleraas method [25] | |||
27.11 (6) | Beam-gas-laser spectroscopy [22] | 27.13 | ||||
27.9 (1) | Time resolved detection [23] | |||||
26.9 (8) | Pulsed dye laser excitation [24] | |||||
26.1 (1.0) | Beam foil excitation [14] | |||||
3s | 27,206.1 | 30.1736 | 29.72 (17) | Beam-gas-laser spectroscopy [22] | 30.46 | |
30 | Central field approximation [6] | |||||
30.02 | Realistic potentials [14] | |||||
30.32 | Coulomb approximation [8] | |||||
3p | 30,925.4 | 215.578 | 203 (8) | Level-crossing spectroscopy [28] | 209 | Central field approximation [6] |
182 (6) | Level crossing spectroscopy [28] | 212 | Realistic potentials [17] | |||
216.4 | Coulomb approximation [8] | |||||
4p | 36,469.6 | 416.997 | 364 | Central field approximation [6] | ||
383.9 | Realistic potentials [17] | |||||
402.6 | Coulomb approximation [8] |