We present an experimental setup to laser cool and trap a large number of ytterbium atoms. Our design uses an oven with an array of micro-tubes for efficient collimation of the atomic beam, and we implement a magneto-optical trap of 174Yb on the 1S0 → 1P1 transition at 399 nm. Despite the absence of a Zeeman slower, we obtain a loading of 4 × 109 at./s. We trap up to N = 109 at., where light-assisted collisions become the dominant loss mechanism. We precisely characterize our atomic beam, the loading rate of the magneto-optical trap, and several loss mechanisms relevant for trapping a large number of atoms.We present an experimental setup to laser cool and trap a large number of ytterbium atoms. Our design uses an oven with an array of micro-tubes for efficient collimation of the atomic beam, and we implement a magneto-optical trap of 174Yb on the 1S0 → 1P1 transition at 399 nm. Despite the absence of a Zeeman slower, we obtain a loading of 4 × 109 at./s. We trap up to N = 109 at., where light-assisted collisions become the dominant loss mechanism. We precisely characterize our atomic beam, the loading rate of the magneto-optical trap, and several loss mechanisms relevant for trapping a large number of atoms.

arXiv:2308.00387Review of Scientific InstrumentsDec 1, 202312 citations

Multiply loaded magneto-optical trap

Christopher J. Myatt, Nathan R. Newbury, R. W. Ghrist +2 more

WORLD SCIENTIFIC eBooksJan 1, 20082 citations

Parameters involved in a magneto-optical trap

Alex Krüger, R. Zanon, Vanderlei Salvador Bagnato +1 more

Livro de ResumosJan 1, 20120 citations

High-flux two-dimensional magneto-optical-trap source for cold lithium atoms

T. G. Tiecke, S. D. Gensemer, A. Ludewig +1 more

We demonstrate a two-dimensional magneto-optical trap (2D MOT) as a beam source for cold $^{6}\text{L}\text{i}$ atoms. The source is side loaded from an oven operated at temperatures in the range $600\ensuremath{\lesssim}T\ensuremath{\lesssim}700\text{ }\text{K}$. The performance is analyzed by loading the atoms into a three-dimensional MOT located 220 mm downstream from the source. The maximum recapture rate of $\ensuremath{\sim}{10}^{9}\text{ }{\text{s}}^{\ensuremath{-}1}$ is obtained for $T\ensuremath{\approx}700\text{ }\text{K}$ and results in a total of up to ${10}^{10}$ trapped atoms. The recaptured fraction is estimated to be $30\ifmmode\pm\else\textpm\fi{}10%$ and limited by beam divergence. The most-probable velocity in the beam $({\ensuremath{\alpha}}_{z})$ is varied from 18 to 70 m/s by increasing the intensity of a push beam. The source is quite monochromatic with a full width at half maximum velocity spread of 11 m/s at ${\ensuremath{\alpha}}_{z}=36\text{ }\text{m}/\text{s}$, demonstrating that side loading completely eliminates beam contamination by hot vapor from the oven. We identify depletion of the low-velocity tail of the oven flux as the limiting loss mechanism. Our approach is suitable for other atomic species.We demonstrate a two-dimensional magneto-optical trap (2D MOT) as a beam source for cold $^{6}\text{L}\text{i}$ atoms. The source is side loaded from an oven operated at temperatures in the range $600\ensuremath{\lesssim}T\ensuremath{\lesssim}700\text{ }\text{K}$. The performance is analyzed by loading the atoms into a three-dimensional MOT located 220 mm downstream from the source. The maximum recapture rate of $\ensuremath{\sim}{10}^{9}\text{ }{\text{s}}^{\ensuremath{-}1}$ is obtained for $T\ensuremath{\approx}700\text{ }\text{K}$ and results in a total of up to ${10}^{10}$ trapped atoms. The recaptured fraction is estimated to be $30\ifmmode\pm\else\textpm\fi{}10%$ and limited by beam divergence. The most-probable velocity in the beam $({\ensuremath{\alpha}}_{z})$ is varied from 18 to 70 m/s by increasing the intensity of a push beam. The source is quite monochromatic with a full width at half maximum velocity spread of 11 m/s at ${\ensuremath{\alpha}}_{z}=36\text{ }\text{m}/\text{s}$, demonstrating that side loading completely eliminates beam contamination by hot vapor from the oven. We identify depletion of the low-velocity tail of the oven flux as the limiting loss mechanism. Our approach is suitable for other atomic species.

arXiv:0905.1063Physical Review AJul 20, 200988 citations

Efficient Loading of a Potassium Magneto-Optical Trap

Robert S. Williamson, Thad G Walker

APSMay 1, 19960 citations

Rapid axial loading of a grating MOT with a cold-atom beam

Rachel Cannon, Aidan S. Arnold, Paul F. Griffin +2 more

Laser-cooled atoms are increasingly being used to realise practical quantum devices, motivating the development of compact and robust atom sources. Grating magneto-optical traps (gMOTs) simplify the cold-atom source architecture but are typically vapour-loaded and provide limited atomic flux. Here we explore the loading of gMOTs from cold-atom beams. We numerically simulate loading to show that unbalanced diffracted beams deflect incoming atoms away from the trap centre, thereby strongly constraining radial loading. In contrast, axial loading injects atoms directly into the trapping volume and largely avoids these effects. We experimentally demonstrate rapid axial loading of a gMOT, achieving loading rates of $2.1 \times 10^9$ atoms~s $^{-1}$ using a moving optical molasses to transfer atoms from a 2D MOT into the gMOT. These results establish axial loading as a robust route to high-flux gMOT operation for portable cold-atom systems.Laser-cooled atoms are increasingly being used to realise practical quantum devices, motivating the development of compact and robust atom sources. Grating magneto-optical traps (gMOTs) simplify the cold-atom source architecture but are typically vapour-loaded and provide limited atomic flux. Here we explore the loading of gMOTs from cold-atom beams. We numerically simulate loading to show that unbalanced diffracted beams deflect incoming atoms away from the trap centre, thereby strongly constraining radial loading. In contrast, axial loading injects atoms directly into the trapping volume and largely avoids these effects. We experimentally demonstrate rapid axial loading of a gMOT, achieving loading rates of $2.1 \times 10^9$ atoms~s$^{-1}$ using a moving optical molasses to transfer atoms from a 2D MOT into the gMOT. These results establish axial loading as a robust route to high-flux gMOT operation for portable cold-atom systems.

arXiv:2603.29580Mar 31, 20260 citations

We demonstrate a two-dimensional magneto-optical trap (2D MOT) as a beam source for cold

^{6}\text{L}\text{i}

atoms. The source is side loaded from an oven operated at temperatures in the range $600\ensuremath{\lesssim}T\ensuremath{\lesssim}700\text{ }\text{K}$. The performance is analyzed by loading the atoms into a three-dimensional MOT located 220 mm downstream from the source. The maximum recapture rate of $\ensuremath{\sim}{10}^{9}\text{ }{\text{s}}^{\ensuremath{-}1}$ is obtained for $T\ensuremath{\approx}700\text{ }\text{K}$ and results in a total of up to

{10}^{10}

trapped atoms. The recaptured fraction is estimated to be $30\ifmmode\pm\else\textpm\fi{}10%$ and limited by beam divergence. The most-probable velocity in the beam $({\ensuremath{\alpha}}_{z})$ is varied from 18 to 70 m/s by increasing the intensity of a push beam. The source is quite monochromatic with a full width at half maximum velocity spread of 11 m/s at ${\ensuremath{\alpha}}_{z}=36\text{ }\text{m}/\text{s}$, demonstrating that side loading completely eliminates beam contamination by hot vapor from the oven. We identify depletion of the low-velocity tail of the oven flux as the limiting loss mechanism. Our approach is suitable for other atomic species.

2.1 \times 10^9

atoms~s

^{-1}

using a moving optical molasses to transfer atoms from a 2D MOT into the gMOT. These results establish axial loading as a robust route to high-flux gMOT operation for portable cold-atom systems.