Jul 2 – 6, 2018
Žofín Palace
Europe/Prague timezone

O4.407 Near-lossless positron injection into a dipole magnetic field

Jul 5, 2018, 6:15 PM
15m
Mánes Bar

Mánes Bar

Talk BSAP

Speaker

Eve Virginia Stenson

Description

See the full Abstract at http://ocs.ciemat.es/EPS2018ABS/pdf/O4.407.pdf Near-lossless positron injection into a dipole magnetic field E. V. Stenson1,2 , U. Hergenhahn1 , S. Nissl1,2 , J. Horn-Stanja1 , H. Saitoh1,3 , T. Sunn Pedersen1,4 , M. R. Stoneking5 , M. Singer2 , M. Dickmann2 , C. Hugenschmidt2 , J. R. Danielson6 , C. M. Surko6 1 Max Planck Institute for Plasma Physics, Garching & Greifswald, Germany 2 Technische Universität München, Garching, Germany 3 The University of Tokyo, Kashiwa, Japan 4 University of Greifswald, Greifswald, Germany 5 Lawrence University, Appleton, WI, U.S.A. 6 University of California, San Diego, La Jolla, CA, U.S.A. The nucleation and trapping of a small-Debye-length, electron-positron pair plasma in a toroidal device will enable laboratory studies of these systems, which are predicted to have novel properties significantly different from those of standard electron-ion plasmas — e.g., “re- markable stability” [1]. A key prerequisite is the development of a scheme that enables efficient injection of positrons from an external source, across flux surfaces, into the confinement region. Previously, the NEPOMUC (NEutron-induced POsitron source MUniCh) beam was injected with beam line 38% efficiency into the dipole field of a supported per- manent magnet and subsequently trapped [2]. Essen- tially lossless injection into the same device has now been demonstrated. This was accomplished by tailor- ExB plate ing positrons’ 3D guiding-center drift orbits via opti- mization of electrostatic potentials applied to various plates and wall segments, thereby producing localized particle transport via the E × B drift. Experimental re- magnet sults are in excellent agreement with numerical simu- lations (Fig. 1), enabling a comprehensive understand- ing of the process. This paves the way for upcoming experiments, in which dense pulses of positrons will be injected into the dipole field of a levitated coil. Figure 1: Simulated trajectories of a finite- References temperature positron bunch being loss- [1] P Helander. Phys. Rev. Lett., 113:135003, 2014. lessly drift-injected into a dipole trap. [2] H Saitoh, et al. New J. of Physics, 17(10):103038, 2015.

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