A. Camper*, S. Alfaro Campos, M. Auzins, M. Berghold, B. Bergmann, P. Burian,
R.S. Brusa, R. Caravita, F. Castelli, G. Cerchiari, R. Ciuryło, A. Chehaimi, G. Consolati, M. Doser, K. Eliaszuk, R. Ferguson, M. Germann, A. Giszczak, L.T. Glöggler, Ł. Graczykowski, M. Grosbart, F. Guatieri, N. Gusakova, F.P. Gustafsson, S. Haider, S. Huck, C. Hugenschmidt, M. Janik, T. Januszek, G. Kasprowicz, K. Kempny, G. Khatri, Ł. Kłosowski, G. Kornakov, V. Krumins, L. Lappo, A. Linek, S. Mariazzi, P. Moskal, M. Münster, P. Pandey, D. Pecak, L. Penasa, V. Petracek, M. Piwinski, S. Pospišil, F. Prelz, S.A. Rangwala, T. Rauschendorfer, B.S. Rawat, B. Rienacker, V. Rodin, O. Røhne, H. Sandaker, S. Sharma, P. Smolyanskiy, T. Sowiński, D. Tefelski, M. Volponi, C.P. Welsch, M. Zawada, J. Zielinski, N. Zurlo on behalf of the AEgIS Collaborationet al. (click to show)
Abstract
The experimental demonstration of positronium laser cooling with stationary broadband laser pulses with negative detuning is briefly described. Considerations on the limits of the current experiment and possible future developments follow. In particular, the benefit of positron remoderation, use of a magnetic field, positronium polarization, pulse shaping, coherent laser cooling and deceleration are shortly discussed.