Quadratic Stark Shift in the Ground State of Indium: a Measurement of the Tensor Polarizability.

Marshall A. Weissberger

Published Apr 1, 1976• 0 citations

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Quadratic Stark Shift in the Ground State of Indium: a Measurement of the Tensor Polarizability.

Marshall A. Weissberger

Published Apr 1, 1976• 0 citations

OpenAlex

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We have constructed an atom interferometer with interfering beams that are physically isolated by a metal foil. By applying an interaction to one of the two interfering beams, we can measure ground-state energy shifts with a spectroscopic precision of 6.6\ifmmode\times\else\texttimes\fi{}${10}^{\mathrm{\ensuremath{-}}14}$ eV/\ensuremath{\surd}min , or 16 Hz/\ensuremath{\surd}min . Applying an electric field to one beam of the interferometer, we have measured the phase shift induced from the quadratic Stark effect. By analyzing these phase shifts, we have determined the ground-state polarizability of sodium, with much improved accuracy, to be 24.11(6 ${)}_{\mathrm{statistical}}$ (6 ${)}_{\mathrm{systematic}}$ \ifmmode\times\else\texttimes\fi{}${10}^{\mathrm{\ensuremath{-}}24}$ ${\mathrm{cm}}^{3}$ .We have constructed an atom interferometer with interfering beams that are physically isolated by a metal foil. By applying an interaction to one of the two interfering beams, we can measure ground-state energy shifts with a spectroscopic precision of 6.6\ifmmode\times\else\texttimes\fi{}${10}^{\mathrm{\ensuremath{-}}14}$ eV/\ensuremath{\surd}min , or 16 Hz/\ensuremath{\surd}min . Applying an electric field to one beam of the interferometer, we have measured the phase shift induced from the quadratic Stark effect. By analyzing these phase shifts, we have determined the ground-state polarizability of sodium, with much improved accuracy, to be 24.11(6${)}_{\mathrm{statistical}}$(6${)}_{\mathrm{systematic}}$\ifmmode\times\else\texttimes\fi{}${10}^{\mathrm{\ensuremath{-}}24}$ ${\mathrm{cm}}^{3}$.

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Two-photon Doppler-free spectroscopy has been used to measure Stark shifts of n ${\mathrm{}}^{2}$ D Rydberg states of $^{85}\mathrm{Rb}$ (for n=13--55). Scalar and tensor polarizabilities were determined and found to depend on ( ${n}^{\mathrm{*}}$ ${)}^{6}$ and ( ${n}^{\mathrm{*}}$ ${)}^{7}$ , in agreement with theory. The resulting polarizabilities were used to obtain estimates of radial integrals for D-P transitions.Two-photon Doppler-free spectroscopy has been used to measure Stark shifts of n ${\mathrm{}}^{2}$D Rydberg states of $^{85}\mathrm{Rb}$ (for n=13--55). Scalar and tensor polarizabilities were determined and found to depend on (${n}^{\mathrm{*}}$${)}^{6}$ and (${n}^{\mathrm{*}}$${)}^{7}$, in agreement with theory. The resulting polarizabilities were used to obtain estimates of radial integrals for D-P transitions.

Physical Review AMar 1, 198634 citations

A Precise Measurement of the Stark Shift in the 5

P_{1/2}\to

S_{1/2}

410nm Transition in Indium

Precise measurement of the scalar polarizability of

^{115}

In in an indium atomic beam

{)}_{\mathrm{statistical}}

{)}_{\mathrm{systematic}}

\ifmmode\times\else\texttimes\fi{}${10}^{\mathrm{\ensuremath{-}}24}$

{\mathrm{cm}}^{3}

Two-photon Doppler-free spectroscopy has been used to measure Stark shifts of n

{\mathrm{}}^{2}

D Rydberg states of

^{85}\mathrm{Rb}

(for n=13--55). Scalar and tensor polarizabilities were determined and found to depend on (

{n}^{\mathrm{*}}

{)}^{6}

and (

{n}^{\mathrm{*}}

{)}^{7}

, in agreement with theory. The resulting polarizabilities were used to obtain estimates of radial integrals for D-P transitions.