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- W2020778093 abstract "The fine-structure intervals of the $3^{2}P$ state of ${mathrm{Li}}^{6}$ and ${mathrm{Li}}^{7}$ and the $4^{2}P$ state of ${mathrm{Li}}^{7}$ have been measured by observing the level crossing signals from the ${{P}_{frac{3}{2}}}^{ensuremath{-}frac{3}{2}}$ and ${{P}_{frac{1}{2}}}^{frac{1}{2}}$ levels. Results for the magnetic fields at which the center of the crossing signals occur are the following, in terms of the proton NMR frequency in kHz for a mineral oil sample: $3^{2}P({mathrm{Li}}^{7})$, 3897.163(22); $3^{2}P({mathrm{Li}}^{6})$, 3896.89(20); $4^{2}P({mathrm{Li}}^{7})$, 1621.71(15). By using a theory of the Zeeman effect that includes estimates of the normal and specific mass effects and relativistic effects, we find the following values for the zero-field fine-structure intervals: $ensuremath{Delta}W({mathrm{Li}}^{7}ensuremath{-}3P)=2882.903(18)$ MHz; $ensuremath{Delta}W({mathrm{Li}}^{7}ensuremath{-}4P)=1199.65(11)$ MHz. The uncertainties are three times the standard error for the measurement." @default.
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- W2020778093 title "Fine Structure of the<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mn>3</mml:mn><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mprescripts /><mml:mrow /><mml:mrow><mml:mn>2</mml:mn></mml:mrow><mml:mrow /><mml:mrow /></mml:mmultiscripts></mml:mrow></mml:math>and<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mn>4</mml:mn><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi>P</mml:mi></mml:mrow><mml:mprescripts…" @default.
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- W2020778093 doi "https://doi.org/10.1103/physrev.187.66" @default.
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