Abstract
All buffer-gas positron traps in use today rely on N2 as the primary trapping gas due to its conveniently placed electronic excitation cross-section. The energy loss per excitation in this process is 8.5 eV, which is sufficient to capture positrons from low-energy moderated beams into a Penning-trap configuration of electric and magnetic fields. However, the energy range over which this cross-section is accessible overlaps with that for positronium (Ps) formation, resulting in inevitable losses and setting an intrinsic upper limit on the overall trapping efficiency of ∼25%. In this paper we present a numerical simulation of a device that uses CF4 as the primary trapping gas, exploiting vibrational excitation as the main inelastic capture process. The threshold for such excitations is far below that for Ps formation and hence, in principle, a CF4 trap can be highly efficient; our simulations indicate that it may be possible to achieve trapping efficiencies as high as 90%. We also report the results of an attempt to re-purpose an existing two-stage N2-based buffer-gas positron trap. Operating the device using CF4 proved unsuccessful, which we attribute to back scattering and expansion of the positron beam following interactions with the CF4 gas, and an unfavourably broad longitudinal beam energy spread arising from the magnetic field differential between the source and trap regions. The observed performance was broadly consistent with subsequent simulations that included parameters specific to the test system, and we outline the modifications that would be required to realise efficient positron trapping with CF4. However, additional losses appear to be present which require further investigation through both simulation and experiment.
Highlights
Since production of the first slow positron beams in the 1970s [1] significant technological improvements have occurred [2, 3]
Operating the device using CF4 proved unsuccessful, which we attribute to back scattering and expansion of the positron beam following interactions with the CF4 gas, and an unfavourably broad longitudinal beam energy spread arising from the magnetic field differential between the source and trap regions
This means that the interplay between the positron scattering dynamics and the device geometry is controlled artificially, and the implementation of any real representation of simulated device parameters would have to take into account the true differential pumping requirements
Summary
This content has been downloaded from IOPscience. 49 215001 (http://iopscience.iop.org/0953-4075/49/21/215001) View the table of contents for this issue, or go to the journal homepage for more. You may be interested in: Ultra-low energy antihydrogen M H Holzscheiter and M Charlton Methods and progress in studying inelastic interactions between positrons and atoms R D DuBois Experimental studies of positrons scattering in gases M Charlton A trap-based positron beamline for the study of materials J P Sullivan, J Roberts, R W Weed et al Positron cooling by vibrational and rotational excitation of molecular gases M R Natisin, J R Danielson and C M Surko Positron extraction to an electromagnetic field free region D A Cooke, G Barandun, S Vergani et al Progress, Challenges and Perspectives in Positron Physics: Report on the XIIth International Positron Workshop G F Gribakin, H Knudsen and C M Surko. Journal of Physics B: Atomic, Molecular and Optical Physics doi:10.1088/0953-4075/49/21/215001. Received 8 July 2016, revised 30 August 2016 Accepted for publication 13 September 2016 Published 10 October 2016
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