par Dionisio, J.S. J.S.;Vieu, Ch;Schück, Carsten;Meunier, Robert;Ledu, D.;Lafoux, A.;Lagrange, J.M. J.M.;Pautrat, Michèle;Waast, Bernard;Phillips, W.R. W.R.;Varley, B.J. B.J.;Durell, J.L. J.L.;Dagnall, P.G. P.G.;Dorning, S.J. S.J.;Jones, M.A. M.A.;Smith, A.G. A.G.;Bacelar, Jose C S;Folger, Helmut;Vanhorenbeeck, Jean 
;Urban, Waldemar;Rzaca-Urban, Teresa
Référence Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment, 413, 1, page (59-73)
Publication Publié, 1998-08
;Urban, Waldemar;Rzaca-Urban, TeresaRéférence Nuclear instruments & methods in physics research. Section A, Accelerators, spectrometers, detectors and associated equipment, 413, 1, page (59-73)
Publication Publié, 1998-08
Article révisé par les pairs
| Résumé : | A few accelerated ion beam requirements for in-beam e-γ spectroscopy are briefly reviewed as well as several features of the MP Tandem accelerator of IPN-Orsay and the accelerated ion-beam transport devices leading to the experimental area of in-beam e-γ spectroscopy. In particular, the main capabilities of the ion-sources, the ion pulsing system, the ion stripping and stabilizing devices as well as the versatility of the ion beam transport system are discussed from the point of view of the different kinds of in-beam e-γ experiments performed in that area. © 1998 Elsevier Science B.V. All rights reserved. |
