Probing Nuclear Interactions Through Isotope Shift Spectroscopy of Mercury (2510.18514v1)
Abstract: We present precision isotope shift spectroscopy of the $\mathrm{6s{2}}\, {}{1}\mathrm{S}_{0}{\rightarrow\,}\mathrm{6s\, 6p}\, {}{3}\mathrm{P}_{1}$ intercombination line and the $\mathrm{6s\,6p}\, {}{3}\mathrm{P}_{1}{\rightarrow\,}\mathrm{6s\,6d}\, {}{3}\mathrm{D}_{J}$ ($J=1,2$) transitions in neutral mercury, performed on the five naturally abundant even isotopes, including the low-abundant isotope ${}{196}\mathrm{Hg}$. Using laser-cooled atoms in a magneto-optical trap, we achieve uncertainties down to $20\,\mathrm{kHz}$, resolving the isotope shift to a fractional uncertainty of ${\sim}\,2{\,\times\,}10{-6}$. A King plot analysis comparing our ${}{1}\mathrm{S}{0}{\rightarrow}{}{3}\mathrm{P}{1}$ data to previous results on the $\mathrm{6s\,6p}\,{}{3}\mathrm{P}{2}{\rightarrow\,}\mathrm{6s\,7s}\,{}{3}\mathrm{S}{1}$ line reveals a nonlinearity with $4.9\,\sigma$ significance at this $\mathrm{kHz}$-level resolution -- substantially larger than the $\mathrm{Hz}$-level nonlinearities recently reported in $\mathrm{Yb}$ and $\mathrm{Ca}$. Our generalized King plot nonlinear decomposition analysis discusses potential contributions from quadratic ($\propto \delta\langle r{2}\rangle{2}$) and higher order field shifts ($\propto \delta\langle r{4}\rangle$) also induced by nuclear deformation. These measurements yield new insights into the structure of the $\mathrm{Hg}$ nucleus and provide benchmarks for nuclear-structure models. They further establish mercury as a potential platform to search for hypothetical Yukawa-type boson-mediated forces coupling electrons to neutrons.
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