ADVANCES IN NUCLEAR PHYSICS VOLUME 27 CONTRIBUTORS TO THIS VOLUME Stefan Scherer Institut für Kernphysik Johannes Gutenberg-Universität Mainz Mainz, Germany A Continuation…

Slide 1 The Collective Model Aard Keimpema Slide 2 Contents Vibrational modes of nuclei Deformed nuclei Rotational modes of nuclei Coupling between rotational and vibrational…

Slide 1 Planning for Electromagnetic Irradiation Studies of Silicon Strip Sensors at SLAC/SCIPP Viltaliy Fadeyev, Spencer Key *, Donish Khan *, Tom Markiewicz, Bruce Schumm…

Collective Model Collective Model Nuclei Z N Character j Qobs. Qsp. Qobs/Qsp 17O 8 9 doubly magic+1n 5/2 -2.6 -0.1 20 39K 19 20 doubly magic -1p 3/2 +5.5 +5 1.1 175Lu 71…

U.S. FCAL Efforts William Morse - BNL FCAL Munich October 17 2006 W.M. Morse U.S. Interests BNL – BeamCal, GamCal Yale – GamCal Colorado – SUSY studies Morse is the…

AUJOURD’ HUI…..et…. DEMAIN Keep contact with experimentalists, work together Beyond mean-field, but via Particle-Vibration Coupling 132Sn low-lying GDR strength Blue…

Planning for Electromagnetic Irradiation Studies of Silicon Strip Sensors at SLAC/SCIPP Viltaliy Fadeyev, Spencer Key*, Donish Khan*, Tom Markiewicz, Bruce Schumm** * Students…

The fission of a heavy fissile nucleus ( A, Z ) is the splitting of this nucleus into 2 fragments, called primary fragments A’1 and A’2. They are excited and de-excite…

Nuclear structure at finite temperature probed by the Giant Dipole Resonance G. Benzoni, O. Wieland, A. Bracco, N. Blasi, F. Camera, F. Crespi, S. Leoni, B. Million Dipartimento…