AbstractThe density and geometry of p̄ and e+ plasmas in realistic trapping potentials are required if the rate of antihydrogen formation from them is to be understood. A new measurement technique determines these properties of trapped positron (e+) and antiproton (p̄) plasmas, the latter for the first time. The method does not require the common assumption of a spheroidal plasma geometry, which only pertains for a perfect electrostatic quadrupole trapping potential. Plasma densities, diameters, aspect ratios and angular momenta are deduced by comparing the number of particles that survive transmission through an aperture, to that obtained from self-consistent solutions of Poisson's equation. For p̄ the results differ substantially from the...
The ALPHA (Antihydrogen Laser Physics Apparatus) collaboration creates and performs precise measurem...
There are currently many uses of positrons as well as a strong potential for novel applications on t...
Control of the radial profile of trapped antiproton clouds is critical to trapping antihydrogen. We r...
The density and geometry of 0 and e(+) plasmas in realistic trapping potentials are required if the ...
The density and geometry of (p) over bar and e(+) plasmas in realistic trapping potentials are requi...
International audienceThe simultaneous control of the density and particle number of non-neutral pla...
Production of antihydrogen atoms by mixing antiprotons with a cold, confined, positron plasma depend...
Diagnostics of antiproton beams and nonneutral plasmas are described in this chapter. Parallel plate...
This dissertation focuses on three ideas useful to the nonneutral plasma experiment atUC Berkeley an...
The three-dimensional particle-in-cell (3-D PIC) simulation code WARP is used to study positron conf...
Abstract: We describe a multi-step “rotating wall” compression of a mixed cold antiproton–electron n...
The ALPHA (Antihydrogen Laser Physics Apparatus) collaboration creates and performs precise measurem...
There are currently many uses of positrons as well as a strong potential for novel applications on t...
Control of the radial profile of trapped antiproton clouds is critical to trapping antihydrogen. We r...
The density and geometry of 0 and e(+) plasmas in realistic trapping potentials are required if the ...
The density and geometry of (p) over bar and e(+) plasmas in realistic trapping potentials are requi...
International audienceThe simultaneous control of the density and particle number of non-neutral pla...
Production of antihydrogen atoms by mixing antiprotons with a cold, confined, positron plasma depend...
Diagnostics of antiproton beams and nonneutral plasmas are described in this chapter. Parallel plate...
This dissertation focuses on three ideas useful to the nonneutral plasma experiment atUC Berkeley an...
The three-dimensional particle-in-cell (3-D PIC) simulation code WARP is used to study positron conf...
Abstract: We describe a multi-step “rotating wall” compression of a mixed cold antiproton–electron n...
The ALPHA (Antihydrogen Laser Physics Apparatus) collaboration creates and performs precise measurem...
There are currently many uses of positrons as well as a strong potential for novel applications on t...
Control of the radial profile of trapped antiproton clouds is critical to trapping antihydrogen. We r...