We present a scheme for laser cooling and magneto-optical trapping of the Group IV (a.k.a. Group 14 or tetrel) atoms silicon (Si), germanium (Ge), tin (Sn), and lead (Pb). These elements each possess a strong Type-II transition ( $J \rightarrow J' = J-1$ ) between the metastable $s^2p^2 \,^3P_1$ state and the excited $s^2ps'\, ^3P_0^o$ state at an accessible laser wavelength, making them amenable to laser cooling and trapping. We focus on the application of this scheme to Sn, which has several features that make it attractive for precision measurement applications. We perform numerical simulations of atomic beam slowing, capture into a magneto-optical trap (MOT), and subsequent sub-Doppler cooling and compression in a blue-detuned MOT of Sn atoms. We also discuss a realistic experimental setup for realizing a high phase-space density sample of Sn atoms.We present a scheme for laser cooling and magneto-optical trapping of the Group IV (a.k.a. Group 14 or tetrel) atoms silicon (Si), germanium (Ge), tin (Sn), and lead (Pb). These elements each possess a strong Type-II transition ($J \rightarrow J' = J-1$) between the metastable $s^2p^2 \,^3P_1$ state and the excited $s^2ps'\, ^3P_0^o$ state at an accessible laser wavelength, making them amenable to laser cooling and trapping. We focus on the application of this scheme to Sn, which has several features that make it attractive for precision measurement applications. We perform numerical simulations of atomic beam slowing, capture into a magneto-optical trap (MOT), and subsequent sub-Doppler cooling and compression in a blue-detuned MOT of Sn atoms. We also discuss a realistic experimental setup for realizing a high phase-space density sample of Sn atoms.

arXiv:2509.04635Physical Review AFeb 20, 20261 citation

Tuning and Locking a Diode Laser for a Magneto-Optical Trap

Rachel Livingston, Matthew Gift, J. H. Huckans +1 more

Bulletin of the American Physical SocietyOct 4, 20140 citations

A New Tool for Preparing Ultracold Atoms and Molecules

Xueping Long

Laser cooling and trapping has been essential to the study of ultracold atoms. Conventionally, continuous wave (CW) lasers have been used almost exclusively to transfer momentum to atoms, which is necessary for laser cooling and trapping. In this thesis, I will describe a technique to laser cool and trap atoms with optical frequency comb generated by a mode-locked (ML) laser, which is another type of laser that is better known as a metrology tool. \tWhile atomic magneto-optical trap (MOT), a spatially confined atomic sample created with laser cooling and trapping, has become the workhorse of ultracold atomic physics since its first demonstration a few decades ago, the first molecular MOT was only demonstrated a few years ago. The main reason for the low number of molecules in the trap is the low number of molecules that can be slowed to a laser trappable speed, which is due to their high likelihood of spontaneous emission into dark states. In this thesis I will also describe a mode-locked laser slowing technique that suppresses spontaneous emission.Laser cooling and trapping has been essential to the study of ultracold atoms. Conventionally, continuous wave (CW) lasers have been used almost exclusively to transfer momentum to atoms, which is necessary for laser cooling and trapping. In this thesis, I will describe a technique to laser cool and trap atoms with optical frequency comb generated by a mode-locked (ML) laser, which is another type of laser that is better known as a metrology tool. \tWhile atomic magneto-optical trap (MOT), a spatially confined atomic sample created with laser cooling and trapping, has become the workhorse of ultracold atomic physics since its first demonstration a few decades ago, the first molecular MOT was only demonstrated a few years ago. The main reason for the low number of molecules in the trap is the low number of molecules that can be slowed to a laser trappable speed, which is due to their high likelihood of spontaneous emission into dark states. In this thesis I will also describe a mode-locked laser slowing technique that suppresses spontaneous emission.

Jan 1, 20190 citations

Achieving a Stable Magneto-Optical Trap

Chasen S Himeda

Jan 1, 20180 citations

Frequency stabilization of a silicon magneto-optical trap repump laser

Jonathan Gilbert, Sam Ronald, S. A. Lee +1 more

Bulletin of the American Physical SocietyOct 18, 20130 citations

Magneto-Optical Trapping of 88 Sr atoms with 689 nm Laser

Qiang Wang, Bai-Ke Lin, Yang Chun Zhao +6 more

We report the experimental realization of strontium magneto-optical trap (MOT) operating on the intercombination transition 1 S 0 − 3 P 1 at 689 nm, namely red MOT. A 689 nm laser used for cooling and trapping is injection locked to a master laser, whose linewidth is narrowed to 150 Hz by locking to a high finesse optical reference cavity. 88 Sr atoms pre-cooled and trapped by the broad 1 S 0 − 1 P 1 transition at 461 nm are transferred to the red MOT with the help of a time sequence controller. The transfer ratio is about 20% and the red MOT's temperature is estimated to be less than 20 μK by the time-of-flight (TOF) image analysis.We report the experimental realization of strontium magneto-optical trap (MOT) operating on the intercombination transition 1 S 0 − 3 P 1 at 689 nm, namely red MOT. A 689 nm laser used for cooling and trapping is injection locked to a master laser, whose linewidth is narrowed to 150 Hz by locking to a high finesse optical reference cavity. 88 Sr atoms pre-cooled and trapped by the broad 1 S 0 − 1 P 1 transition at 461 nm are transferred to the red MOT with the help of a time sequence controller. The transfer ratio is about 20% and the red MOT's temperature is estimated to be less than 20 μK by the time-of-flight (TOF) image analysis.

Chinese Physics LettersMar 1, 201110 citations

J \rightarrow J' = J-1

) between the metastable

s^2p^2 \,^3P_1

state and the excited

s^2ps'\, ^3P_0^o

state at an accessible laser wavelength, making them amenable to laser cooling and trapping. We focus on the application of this scheme to Sn, which has several features that make it attractive for precision measurement applications. We perform numerical simulations of atomic beam slowing, capture into a magneto-optical trap (MOT), and subsequent sub-Doppler cooling and compression in a blue-detuned MOT of Sn atoms. We also discuss a realistic experimental setup for realizing a high phase-space density sample of Sn atoms.