Bulletin of the American Physical Society
66th Annual Meeting of the APS Division of Plasma Physics
Monday–Friday, October 7–11, 2024; Atlanta, Georgia
Session NP12: Poster Session V:
Fundamental Plasma Physics III: waves, self-organization
Fundamental Plasma Physics IV: turbulence, reconnection, non-neutral/antimatter
High Field Tokamaks
Mirrors
9:30 AM - 12:30 PM
Wednesday, October 9, 2024
Hyatt Regency
Room: Grand Hall West
Abstract: NP12.00083 : Magnetically confined positrons forming positronium*
Presenter:
Jens Von Der Linden
(Max Planck Institute for Plasma Physics)
Authors:
Jens Von Der Linden
(Max Planck Institute for Plasma Physics)
Adam Deller
(Max Planck Institute of Plasma Physics)
Stefan Nissl
(Max Planck Institute for Plasma Physics)
Haruhiko Saitoh
(University of Tokyo)
Hiroyuki Higaki
(University of Hiroshima)
Koji Michishio
(National Institute of Advanced Industrial Science and Technology (AIST))
Eve V Stenson
(Max Planck Institute for Plasma Physics)
Collaboration:
APEX
Recent experiments pinpoint charge exchange as dominant loss channel for magnetically confined positrons above threshold energies. A bunch of 10⁵ positrons is accumulated, cooled (=300meV), and E×B drift-injected (=7eV) into the dipole field of a permanent magnet trap. Once injected, the positrons are trapped through electrostatic reflection off the biased magnet. After one elastic collision (~4ms), their pitch angles are scattered and they are magnetically confined. A 21-BGO detector array situated 1cm from the confinement volume detects ~10,000 gammas per shot. The time evolution of the 511keV peak-to-valley ratio identifies Positronium (Ps) formation through charge exchange of the positrons with impurities in the ~5·10-6 Pa vacuum as dominant loss mechanism during the first ~500ms of confinement. An increase in the positron kinetic energy, achieved by reducing the electrostatic bias, leads to an increase in charge exchange and associated triple coincidence detection. Inelastic collisions cool the positrons, enabling diagnosis through a ramp of the magnet bias to negative voltages pulling them into the loss cone. Once the positron population above the Ps-formation energy threshold is depleted, transport to the wall through elastic collisions becomes the dominant loss mechanism.
*We gratefully acknowledge the support of the Advanced Beam Measurement Group at the National Institute of Advanced Industrial Science and Technology (AIST) in Japan.The APEX collaboration receives/has received support from IPP/MPG; the European Research Council (ERC) under the European Union's Horizon 2020 research and innovation programme; the Helmholtz Association; the Deutsche Forschungsgemeinschaft (DFG); the Alexander von Humboldt Foundation, the UC San Diego Foundation; the United States Department of Energy, the Japan Society for the Promotion of Science (JSPS); and the National Institute for Fusion Science (NIFS).
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