Measurement of the tune-out wavelength for $^{133}$Cs at $880$ nm (2110.00043v1)
Abstract: We perform a measurement of the tune-out wavelength, $\lambda_{0}$, between the $D_{1}$, $62S_{1/2}\rightarrow62P_{1/2}$, and $D_{2}$, $62S_{1/2}\rightarrow62P_{3/2}$, transitions for ${133}$Cs in the ground hyperfine state $(F=3, m_{F}=+3)$. At $\lambda_{0}$, the frequency-dependent scalar polarizability is zero leading to a zero scalar ac Stark shift. We measure the polarizability as a function of wavelength using Kapitza-Dirac scattering of a ${133}$Cs Bose-Einstein condensate in a one-dimensional optical lattice, and determine the tune-out wavelength to be $\lambda_{0}=880.21790(40){\textrm{stat}}(8){\textrm{sys}}$ nm. From this measurement we determine the ratio of reduced matrix elements to be $\left|\left<{6P_{3/2}| d|6S_{1/2}}\right>\right|{2}\left|\left<{6P_{1/2}| d|6S_{1/2}}\right>\right|{2}=1.9808(2)$. This represents an improvement of a factor of 10 over previous results derived from excited-state lifetime measurements. We use the present measurement as a benchmark test of high-precision theory.
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