Velocity-selected production of 2 S 3 metastable positronium

Claude Amsler, M. Antonello,A. S. Belov,Germano Bonomi, R. S. Brusa,Massimo Caccia, A. Camper,Ruggero Caravita,Fabrizio Castelli,Giovanni Cerchiari,Daniel Comparat,Giovanni Consolati, A. Demetrio,L. Di Noto,Michael Doser, M. Fanì,Sebastian Gerber, Angela Gligorova, F. Guatieri, P. Hackstock, S. Haider, A. Hinterberger, H. Holmestad,Alban Kellerbauer, O. Khalidova, D. Krasnický, V. Lagomarsino, P. Lansonneur, Ph. Lebrun,Chloé Malbrunot,Sebastiano Mariazzi,V. Matveev, S. Müller, G. Nebbia,Patrick Nedelec, M. Oberthaler,Davide Pagano,Luca Penasa, V. Petráček, F. Prelz,Marco Prevedelli, B. Rienaecker, J. Robert,Ole Røhne,Alberto Rotondi,Heidi Sandaker,Romualdo Santoro,Lillian Smestad, Felice Sorrentino,G. Testera, I. C. Tietje, E. Widmann, P. Yzombard, C. Zimmer,Nicola Zurlo

Physical Review A(2019)

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摘要
Positronium in the $2^3S$ metastable state exhibits a low electrical polarizability and a long lifetime (1140 ns) making it a promising candidate for interferometry experiments with a neutral matter-antimatter system. In the present work, $2^3S$ positronium is produced - in absence of electric field - via spontaneous radiative decay from the $3^3P$ level populated with a 205nm UV laser pulse. Thanks to the short temporal length of the pulse, 1.5 ns full-width at half maximum, different velocity populations of a positronium cloud emitted from a nanochannelled positron/positronium converter were selected by delaying the excitation pulse with respect to the production instant. $ 2^3S $ positronium atoms with velocity tuned between $ 7 \cdot 10^4 $ m/s and $ 10 \cdot 10^4 $ m/s were thus produced. Depending on the selected velocity, a $2^3S$ production effciency ranging from $\sim 0.8 \%$ to $\sim 1.7%$, with respect to the total amount of emitted positronium, was obtained. The observed results give a branching ratio for the $3^3P$-$2^3S$ spontaneous decay of $(9.7 \pm 2.7) \% $. The present velocity selection technique could allow to produce an almost monochromatic beam of $\sim 1 \cdot 10^3 $ $2^3S$ atoms with a velocity spread $ < 10^4 $ m/s and an angular divergence of $\sim$ 50 mrad.
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