A. Linek

most citedAbsolute frequency measurement of the

6 s^{2}^{1} S_{0} \to 6 s 6 p^{3} P_{1}

F = 3/2 \to F^{'} = 5/2

^{201}

Hg transition with background-free saturation spectroscopy

5 citations · 5 across the 3 of their papers we have counts for

collaborators

3 papers

physics.atom-ph2026

Optical Dipole Trap for Hg Atoms

I. Nandi, A. Sahu, M. Veis +3

We report the first realization of an optical dipole trap (ODT) for ultracold mercury atoms, overcoming the challenge posed by the exceptionally low polarizability of Hg and the re…

physics.atom-ph2026

Isotopic effect on collisional widths and shifts of Hg clock transition induced by cold Rb atoms

Renu Bala, Adam Linek, Marcin Witkowski +4

We study the isotopic dependence of collisional widths and shifts of the Hg clock transition $^{1}$ S $_{0}$ - $^{3}$ P $_{0}$ perturbed by the Rb atoms in the temperature range from 1 nK to 1 K…

physics.atom-ph2022★ 5 cited

Absolute frequency measurement of the $6 s^{2}^{1} S_{0} \to 6 s 6 p^{3} P_{1}$ $F = 3/2 \to F^{'} = 5/2$ $^{201}$ Hg transition with background-free saturation spectroscopy

Adam Linek, Piotr Morzyński, Marcin Witkowski

We report the development of a method for eliminating background-induced systematic shifts affecting precise measurements of saturation absorption signals. With this technique, we…

Optical Dipole Trap for Hg Atoms

Isotopic effect on collisional widths and shifts of Hg clock transition induced by cold Rb atoms

Absolute frequency measurement of the 6s2 1S0​→6s6p 3P1​ F=3/2→F′=5/2 201Hg transition with background-free saturation spectroscopy

Absolute frequency measurement of the $6 s^{2}^{1} S_{0} \to 6 s 6 p^{3} P_{1}$ $F = 3/2 \to F^{'} = 5/2$ $^{201}$ Hg transition with background-free saturation spectroscopy