We demonstrate, for the first time, a hollow-conical atomic beam from a standard low-velocity intense source. Experimental results and numerical simulations indicate that the hollow-conical feature is caused by the converging-diverging extraction process. The degree of hollowness can be reduced by using a weaker push beam and extending the length of transverse cooling. Analytical models are proposed to quantitatively describe the hollowness of the atomic beam. This study can find applications where a compact and solid atomic beam is needed, such as coupling cold atoms into matter waveguides or continuous cold atomic beam interferometers.
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http://dx.doi.org/10.1364/OE.507048 | DOI Listing |
Small Methods
December 2024
Faculty of Materials Science and Engineering, Kunming University of Science and Technology, No. 68 Wenchang Road, Kunming, 650093, China.
Controllably modulating the structure of transition-metal chalcogenides (TMCs) from 2D to 1D and tuning their electronic properties has drawn particular attention currently due to their remarkable properties and potential applications. In this work, by precisely controlling the chemical concentration of Te atoms, the transformation from the 2D honeycomb AgTe monolayer to high-quality and well-defined 1D AgTe nanowires on the Ag(111) substrate has been successfully achieved. The combination of scanning tunneling microscopy measurements and first-principles calculations has confirmed that the mechanism underlying the entire dimensional transformation lies in the directional movement of Ag atoms in the 2D AgTe monolayer regulated by the concentration of Te atoms.
View Article and Find Full Text PDFRev Sci Instrum
December 2024
J-PARC Center, Japan Atomic Energy Agency, 2-4, Shirakata, Tokai-mura, Ibaraki, Japan.
A gas-sheet beam profile monitor enabling non-destructive two-dimensional profile measurements of a high-intensity beam by capturing an image of a beam-induced fluorescence was developed. For quantitative profile measurements, the monitor's response function comprising, e.g.
View Article and Find Full Text PDFAppl Radiat Isot
December 2024
Facility for Rare Isotope Beams, Michigan State University, 640 South Shaw Lane, East Lansing, 48824, MI, USA; Department of Chemistry, Michigan State University, 640 South Shaw Lane, East Lansing, 48824, MI, USA. Electronic address:
For the generation of beams with the offline ion source at the Facility for Rare Isotope Beams (FRIB), suitable source samples are required. Arsenic-73 is a frequently requested user beam due to its significance in nuclear structure studies and astrophysics. In this work, we outline the process of preparing a As source sample, containing (5.
View Article and Find Full Text PDFAppl Radiat Isot
December 2024
Institute of Nuclear Techniques of Budapest University of Technology and Economics, Műegyetem Rkp 9, 1111, Budapest, Hungary.
This study presents a compact accelerator-driven neutron source design with a thermal neutron port and an epithermal neutron port for Boron Neutron Capture Therapy (BNCT), based on 10 mA 2.5 MeV protons bombarding on a 100 μm thick disc-shaped Li target with a diameter of 10 cm. The moderator consists of 2 parts, the epithermal neutron moderator and the thermal neutron moderator.
View Article and Find Full Text PDFPhys Rev Lett
December 2024
Department of Physics and Astronomy, University College London, Gower Street, London WC1E 6BT, United Kingdom.
We have measured the spin polarization of a slow positron beam via state-selective depopulation of 2^{3}S_{1} positronium atoms, generated by passing the beam through a gas cell. Our method employs circularly polarized microwave radiation to drive 2^{3}S_{1}→2^{3}P_{1} transitions, for which either Δm_{J}=+1 or Δm_{J}=-1, and relies on the fact that asymmetries between the two cases yield the underlying positron beam polarization. Using this technique we show that the polarization of a positron beam derived from a solid neon moderator may be increased from 30% to 90% by increasing the moderator thickness, with an associated reduction in beam intensity of 60%.
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