Diode-laser hyperfine-structure spectroscopy of 1 3 8 , 1 3 9 La
Diode-laser hyperfine-structure spectroscopy of 1 3 8 , 1 3 9 La
复制标题
1 3 8 , 1 3 9 La 的二极管激光超精细结构光谱
DOI：
10.1103/physreva.63.064501
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发表时间：
2001
影响因子：
2.9
通讯作者：
H. Katsuragawa
中科院分区：
文献类型：
--
作者：
W. Jin;Toshiaki Endo;H. Uematsu;T. Minowa;H. Katsuragawa
With a beam of unenriched lanthanum, the hyperfine structure (hfs) of ${}^{138,139}\mathrm{La}$ has been measured for the transition from the ${5d6s}^{2}{}^{2}{D}_{3/2}$ ground state to the $5d6s6p{}^{4}{F}_{5/2}$ level at 675.304 nm by means of atomic-beam diode-laser spectroscopy. Magnetic-dipole (A) and electric-quadrupole $(B)\mathrm{hfs}$ constants of the 0.090% abundant ${}^{138}\mathrm{La},$ as well as those of ${}^{139}\mathrm{La},$ have been determined for the ${5d6s}^{2}{}^{2}{D}_{3/2}$ and $5d6s6p{}^{4}{F}_{5/2}$ levels; this serves as a measurement of hyperfine structure constants A and B for ${}^{138}\mathrm{La}.$ The isotope shift between ${}^{139}\mathrm{La}$ and ${}^{138}\mathrm{La}$ has been obtained for the 675.304-nm transition and change in mean-square nuclear charge radii $\ensuremath{\delta}〈{r}^{2}〉$ derived.
With a beam of unenriched lanthanum, the hyperfine structure (hfs) of ${}^{138,139}\mathrm{La}$ has been measured for the transition from the ${5d6s}^{2}{}^{2}{D}_{3/2}$ ground state to the $5d6s6p{}^{4}{F}_{5/2}$ level at 675.304 nm by means of atomic-beam diode-laser spectroscopy. Magnetic-dipole (A) and electric-quadrupole $(B)\mathrm{hfs}$ constants of the 0.090% abundant ${}^{138}\mathrm{La},$ as well as those of ${}^{139}\mathrm{La},$ have been determined for the ${5d6s}^{2}{}^{2}{D}_{3/2}$ and $5d6s6p{}^{4}{F}_{5/2}$ levels; this serves as a measurement of hyperfine structure constants A and B for ${}^{138}\mathrm{La}.$ The isotope shift between ${}^{139}\mathrm{La}$ and ${}^{138}\mathrm{La}$ has been obtained for the 675.304-nm transition and change in mean-square nuclear charge radii $\ensuremath{\delta}〈{r}^{2}〉$ derived.