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  • Amsler, C; Antonello, M; Belov, A; Bonomi, G; Brusa, R S; Caccia, M; Camper, A; Caravita, R; Castelli, F; Cerchiari, G; Comparat, D; Consolati, G; Demetrio, A; L Di Noto; Doser, M; Fanì, M; Gerber, S; Gligorova, A; Guatieri, F; Hackstock, P; Haider, S; Hinterberger, A; Holmestad, H; Kellerbauer, A; Khalidova, O; Krasnicky, D; Lagomarsino, V; Lansonneur, P; Lebrun, P; Malbrunot, C; Mariazzi, S; Matveev, V; Muller, S R; Nebbia, G; Nedelec, P; Oberthaler, M; Pagano, D; Penasa, L; Petracek, V; Prelz, F; Prevedelli, M; Rienaecker, B; Robert, J; Rohne, O M; Rotondi, A; Sandaker, H; Santoro, R; Smestad, L; Sorrentino, F; Testera, G; Tietje, I C; Widmann, E; Yzombard, P; Zimmer, C; Zurlo, N; The AEgIS collaboration

    arXiv.org, 04/2019
    Paper

    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.