Answers are grounded in this paper and cite their sources.
The E-H-gradient balance technique has been used to measure the static electric dipole polarizabilities of the alkali-metal atoms and the tensor polarizabilities of the ³P₂ metastable noble-gas atoms. All of the measurements are normalized to the scalar polarizability of ³S₁ metastable helium, a value which has been accurately calculated. The scalar polarizabilities of the alkali atoms, in units of 10^-24 cm³, are for lithium, 24.3 ±{} 0.5; sodium, 23.6 ±{} 0.5; potassium, 43.4 ±{} 0.9; rubidium, 47.3 ±{} 0.9; cesium, 59.6 ±{} 1.2. For the ³P₂ metastable noble-gas atoms we measure the zz components of the polarizability tensors for mJ=1 and 2, which completely determines the polarizability tensors for all mJ. For αzz(mJ) we find, in units of 10^-24 cm³, for neon, 28.4 ±{} 0.6 (mJ=1) and 26.7 ±{} 0.5 (mJ=2); argon, 49.5 ±{} 1.0 (mJ=1) and 44.7 ±{} 0.9 (mJ=2); krypton, 52.7 ±{} 1.0 (mJ=1) and 46.8 ±{} 0.9 (mJ=2); xenon, 66.6 ±{} 1.3 (mJ=1) and 57.4 ±{} 1.1 (mJ=2). The rare-gas results, while more precise, are in good agreement with earlier work. The alkali-metal results are in excellent agreement with recent theory and the experiment of Hall and Zorn.
No takes yet. Share an insight, caveat, or question.
Molof et al. (1974) studied this question.
Synapse has enriched 5 related papers. Consider them for comparative context: