1997
DOI: 10.1063/1.872284
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Antimatter plasmas and antihydrogen

Abstract: Measurement of the groundstate hyperfine structure of antihydrogen AIP Conf.Recent successes in confining antimatter in the form of positron and antiproton plasmas have created new scientific and technological opportunities. Plasma techniques have been the cornerstone of experimental work in this area, and this is likely to be true for the foreseeable future. Work by a number of groups on trapping antimatter plasmas is summarized, and an overview of the promises and challenges in this field is presented. Topic… Show more

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Cited by 126 publications
(100 citation statements)
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References 165 publications
(220 reference statements)
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“…Radial confinement is by an axial magnetic field [18,19]. Positrons from a conventional positron source are trapped by collisions with a buffer gas, usually nitrogen, in the high pressure region and accumulate and cool in the low pressure region.…”
Section: Positron Trappingmentioning
confidence: 99%
“…Radial confinement is by an axial magnetic field [18,19]. Positrons from a conventional positron source are trapped by collisions with a buffer gas, usually nitrogen, in the high pressure region and accumulate and cool in the low pressure region.…”
Section: Positron Trappingmentioning
confidence: 99%
“…Unneutralized plasmas are unique in that they can be trapped in a rotating near-thermal-equilibrium state by static electric and magnetic fields. Steady-state confinement of N 10 3 -10 9 electrons, ions, or antimatter particles [1,2] is routinely used in plasma experiments, atomic physics [3], and spectroscopy [4]. The thermal equilibrium characteristics become most evident with the formation of Coulomb crystals [5] when pure ion plasmas are cooled to the liquid and solid regimes at sub-Kelvin temperatures, but the higher temperature plasma regime studied here is also well described by near-equilibrium statistical mechanics [6].…”
mentioning
confidence: 99%
“…The experimental work follows previous discussions and simulations of trapping and sympathetic cooling of positrons via Coulomb collisions with cold 9 Be + ions [1,2]. Cold positron plasmas are useful as a source for cold beams of high brightness [3,4,5,6]. Many of the chapters in this volume, for example Chapter 12 by Greaves and Surko and Chapter 24 by Surko, discuss applications of cold positron beams.…”
Section: Introductionmentioning
confidence: 90%
“…They used a 3 mCi positron source and a tungsten positron moderator in the experiment. The positrons were cooled by thermalization with a cryogenic Penning trap which ensured a temperature of ∼4 K. Surko and coworkers [3,5,18,19,20], using a 90 mCi positron source, report the largest number of trapped positrons (∼ 3 × 10 8 ) with a trapping rate of 3×10 8 positrons in 8 minutes and a trapping efficiency greater than 25 % of the moderated positrons. The positrons were thermalized to room temperature since the trapping was achieved through collisions with a room-temperature buffer gas of N 2 .…”
Section: Introductionmentioning
confidence: 99%
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