Author(s)
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Banerjee, D ; Biraben, F ; Brook-Roberge, D ; Charlton, M ; Cladé, P ; Comini, P ; Crivelli, P ; Dalkarov, O ; Debu, P ; Douillet, A ; Dufour, G ; Dupré, P ; Eriksson, S ; Froelich, P ; Grandemange, P ; Guellati, S ; Guérout, R ; Heinrich, J-M ; Hervieux, P-A ; Hilico, L ; Husson, A ; Indelicato, P ; Jonsell, S ; Karr, J-P ; Khabarova, K ; Kolachevsky, N ; Kuroda, N ; Lambrecht, A ; Leite, A M M ; Liszkay, L ; Lotrus, P ; Lunney, D ; Madsen, N ; Manfredi, G ; Mansoulié, B ; Matsuda, Y ; Mohri, A ; Mortensen, T ; Nagashima, Y ; Nesvizhevsky, V ; Nez, F ; Pérez, P ; Regenfus, C ; Rey, J-M ; Reymond, J-M ; Roussé, J-Y ; Reynaud, S ; Rubbia, A ; Sacquin, Y ; Schmidt-Kaler, F ; Sillitoe, N ; Staszczak, M ; Szabo-Foster, C I ; Torii, H ; Vallage, B ; Valdes, M ; van der Werf, D P ; Voronin, A ; Walz, J ; Wolf, S ; Wronka, S ; Yamazaki, Y |
Abstract
| The GBAR experiment will use one of the low energy antiproton beam lines from the ELENA ring that is being prepared and scheduled to start operating in 2017. The apparatus is broadly divided into four sections: antiproton deceleration and focussing, positron production and accumulation, antihydrogen cooling and preparation, and detection. In the following, we give updates on the different parts and the status of preparation for installation in the AD hall, referring to the previous report that was submitted in April of 2014 |