We present tabulated data for several families of static electric and magnetic multipole susceptibilities for hydrogenic atoms with nuclear charge numbers from the range $1\leq Z\leq137$. Atomic nuclei are assumed to be point-like and spinless. The susceptibilities considered include the multipole electric polarizabilities $\alpha_{\mathrm{E}L\to\mathrm{E}L}$ and magnetizabilities (magnetic susceptibilities) $\chi_{\mathrm{M}L\to\mathrm{M}L}$ with $1\leq L\leq4$ (i.e., the dipole, quadrupole, octupole and hexadecapole ones), the electric-to-magnetic cross-susceptibilities $\alpha_{\mathrm{E}L\to\mathrm{M}(L−1)}$ with $2\leq L\leq5$ and $\alpha_{\mathrm{E}L\to\mathrm{M}(L+1)}$ with $1\leq L\leq4$, the magnetic-to-electric cross-susceptibilities $\chi_{\mathrm{M}L\to\mathrm{E}(L−1)}$ with $2\leq L\leq5$ and $\chi_{\mathrm{M}L\to\mathrm{E}(L+1)}$ with $1\leq L\leq4$ (it holds that $\chi_{\mathrm{M}L\to\mathrm{E}(L∓1)}=\alpha_{\mathrm{E}(L∓1)\to\mathrm{M}L}), and the electric-to-toroidal-magnetic cross-susceptibilities $\alpha_{\mathrm{E}L\to\mathrm{T}L}$ with $1\leq L\leq4$. Numerical values are computed from general exact analytical formulas, derived by us elsewhere within the framework of the Dirac relativistic quantum mechanics, and involving generalized hypergeometric functions ${}_{3}F_{2}$ of the unit argument.
Authors
Additional information
- DOI
- Digital Object Identifier link open in new tab 10.1016/j.adt.2016.02.002
- Category
- Publikacja w czasopiśmie
- Type
- artykuł w czasopiśmie wyróżnionym w JCR
- Language
- angielski
- Publication year
- 2016
