Rydberg-positronium velocity and self-ionization studies in a 1T magnetic field and cryogenic environment
M. Antonello, Alexander S. Belov, G. Bonomi, R.S. Brusa, M. Caccia, A. Camper, R. Caravita, F. Castelli, D. Comparat, Giovanni Consolati, L. Di Noto, M. Doser, M. Fanì, R. Ferragut, J. Fesel, S. Gerber, A. Gligorova, L. T. Glöggler, F. Guatieri, S. Haider, A. Hinterberger, O. Khalidova, D. Krasnický, V. Lagomarsino, C. Malbrunot, S. Mariazzi, V. Matveev, Simon Müller, G. Nebbia, P. Nédélec, L. Nowak, Markus K. Oberthaler, E. Oswald, D. Pagano, L. Penasa, V. Petráček, F. Prelz, B. Rienäcker, O. Røhne, A. Rotondi, H. Sandaker, R. Santoro, G. Testera, I.C. Tietje, T. Wolz, Christian Zimmer, N. Zurlo
Abstract
We characterized the pulsed Rydberg-positronium production inside the Antimatter Experiment: Gravity, Interferometry, Spectroscopy ($\mathrm{AE}\overline{\text{g}}\mathrm{IS}$) apparatus in view of antihydrogen formation by means of a charge exchange reaction between cold antiprotons and slow Rydberg-positronium atoms. Velocity measurements on the positronium along two axes in a cryogenic environment ($\ensuremath{\approx}10\phantom{\rule{0.16em}{0ex}}\mathrm{K}$) and in $1\phantom{\rule{0.16em}{0ex}}\mathrm{T}$ magnetic field were performed. The velocimetry was done by microchannel-plate (MCP) imaging of a photoionized positronium previously excited to the $n=3$ state. One direction of velocity was measured via Doppler scan of this $n=3$ line, another direction perpendicular to the former by delaying the exciting laser pulses in a time-of-flight measurement. Self-ionization in the magnetic field due to the motional Stark effect was also quantified by using the same MCP-imaging technique for Rydberg positronium with an effective principal quantum number ${n}_{\mathrm{eff}}$ ranging between 14 and 22. We conclude with a discussion about the optimization of our experimental parameters for creating Rydberg positronium in preparation for an efficient pulsed production of antihydrogen.