Slow molecular beams from a cryogenic buffer gas source

We study the properties of a cryogenic buffer gas source that uses a low-temperature two-stage buffer gas cell to produce very slow beams of ytterbium monofluoride molecules. The molecules are produced by laser ablation inside the cell and extracted into a beam by a flow of cold helium. We measure the flux and velocity distribution of the beam as a function of ablation energy, helium flow rate, cell temperature, and the size of the gap between the first and second stages of the cell. We also compare the velocity distributions from one-stage and two-stage cells. The one-stage cell emits a beam with a speed of about <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mrow><a:mn>82</a:mn><a:mspace width="0.28em"/><a:mi mathvariant="normal">m</a:mi><a:mspace width="0.16em"/><a:msup><a:mrow><a:mi mathvariant="normal">s</a:mi></a:mrow><a:mrow><a:mo>−</a:mo><a:mn>1</a:mn></a:mrow></a:msup></a:mrow></a:math> and a translational temperature of 0.63 K. The slowest beams are obtained using the two-stage cell at the lowest achievable cell temperature of 1.8 K. This beam has a peak velocity of <f:math xmlns:f="http://www.w3.org/1998/Math/MathML"><f:mrow><f:mn>56</f:mn><f:mspace width="0.28em"/><f:mi mathvariant="normal">m</f:mi><f:mspace width="0.16em"/><f:msup><f:mrow><f:mi mathvariant="normal">s</f:mi></f:mrow><f:mrow><f:mo>−</f:mo><f:mn>1</f:mn></f:mrow></f:msup></f:mrow></f:math> and a flux of <k:math xmlns:k="http://www.w3.org/1998/Math/MathML"><k:mrow><k:mn>9</k:mn><k:mo>×</k:mo><k:msup><k:mn>10</k:mn><k:mn>9</k:mn></k:msup></k:mrow></k:math> ground-state molecules per steradian per pulse, with a substantial fraction at speeds below <l:math xmlns:l="http://www.w3.org/1998/Math/MathML"><l:mrow><l:mn>40</l:mn><l:mspace width="0.28em"/><l:mi mathvariant="normal">m</l:mi><l:mspace width="0.16em"/><l:msup><l:mrow><l:mi mathvariant="normal">s</l:mi></l:mrow><l:mrow><l:mo>−</l:mo><l:mn>1</l:mn></l:mrow></l:msup></l:mrow></l:math>. These slow molecules can be decelerated further by radiation pressure slowing and then captured in a magneto-optical trap. Published by the American Physical Society 2024

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Journal
Physical Review Research
Published
2024-12-03
DOI
https://doi.org/10.1103/physrevresearch.6.043232
Citations
5
Primary Topic
Cold Atom Physics and Bose-Einstein Condensates
Type
article
Field-Weighted Citation Impact
1.69

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article

Slow molecular beams from a cryogenic buffer gas source

Jongseok Lim, N. J. Fitch, Jorge Mellado Muñoz, S. Popa et al.
5 citations
Physical Review Research
Cold Atom Physics and Bose-Einstein Condensates
1.69
article

Slow molecular beams from a cryogenic buffer gas source

Jongseok Lim, N. J. Fitch, Jorge Mellado Muñoz, S. Popa, A. P. White, B. E. Sauer, M. R. Tarbutt
article en
5 citations

Abstract

We study the properties of a cryogenic buffer gas source that uses a low-temperature two-stage buffer gas cell to produce very slow beams of ytterbium monofluoride molecules. The molecules are produced by laser ablation inside the cell and extracted into a beam by a flow of cold helium. We measure the flux and velocity distribution of the beam as a function of ablation energy, helium flow rate, cell temperature, and the size of the gap between the first and second stages of the cell. We also compare the velocity distributions from one-stage and two-stage cells. The one-stage cell emits a beam with a speed of about <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mrow><a:mn>82</a:mn><a:mspace width="0.28em"/><a:mi mathvariant="normal">m</a:mi><a:mspace width="0.16em"/><a:msup><a:mrow><a:mi mathvariant="normal">s</a:mi></a:mrow><a:mrow><a:mo>−</a:mo><a:mn>1</a:mn></a:mrow></a:msup></a:mrow></a:math> and a translational temperature of 0.63 K. The slowest beams are obtained using the two-stage cell at the lowest achievable cell temperature of 1.8 K. This beam has a peak velocity of <f:math xmlns:f="http://www.w3.org/1998/Math/MathML"><f:mrow><f:mn>56</f:mn><f:mspace width="0.28em"/><f:mi mathvariant="normal">m</f:mi><f:mspace width="0.16em"/><f:msup><f:mrow><f:mi mathvariant="normal">s</f:mi></f:mrow><f:mrow><f:mo>−</f:mo><f:mn>1</f:mn></f:mrow></f:msup></f:mrow></f:math> and a flux of <k:math xmlns:k="http://www.w3.org/1998/Math/MathML"><k:mrow><k:mn>9</k:mn><k:mo>×</k:mo><k:msup><k:mn>10</k:mn><k:mn>9</k:mn></k:msup></k:mrow></k:math> ground-state molecules per steradian per pulse, with a substantial fraction at speeds below <l:math xmlns:l="http://www.w3.org/1998/Math/MathML"><l:mrow><l:mn>40</l:mn><l:mspace width="0.28em"/><l:mi mathvariant="normal">m</l:mi><l:mspace width="0.16em"/><l:msup><l:mrow><l:mi mathvariant="normal">s</l:mi></l:mrow><l:mrow><l:mo>−</l:mo><l:mn>1</l:mn></l:mrow></l:msup></l:mrow></l:math>. These slow molecules can be decelerated further by radiation pressure slowing and then captured in a magneto-optical trap. Published by the American Physical Society 2024

Physical Review ResearchVol. 6(4)
Imperial College London (GB)
Alfred P. Sloan Foundation, Gordon and Betty Moore Foundation, UK Research and Innovation, Engineering and Physical Sciences Research Council, Science and Technology Facilities Council
Affordable and clean energy
Openalex Percentile: Top 15%
Cold Atom Physics and Bose-Einstein Condensates
1.69
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