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Extra info for 4th International Workshop on Nuclear Fission and Fission-Product Spectroscopy, Cadarache, France, May 13-16 2009
Org/about/rights_permissions FIGURE 5. Atomic number Z versus charge-state q (left), and versus neutron number N (right) for the whole fission-fragment production in this experiment. The limits of observed isotopes are shown for reference in the right panel. The measurement of fission fragments in inverse kinematics using the VAMOS spectrometer allowed, for the first time in a single experiment, the complete characterization of the whole distribution of fission fragments along with the fissioning system.
Fragment-Z identification in VAMOS. Left panel: dE-E correlation. The dashed lines correspond to the analytical description of dE-E correlation for each Z. Right panel: Z projection along the analytical lines. The shape of the distribution is due to the addition of different sets of data not yet normalized. to cover the most of the momentum and charge-state distributions, different values of the central magnetic rigidity were used during the experiment. 360 Tm of magnetic rigidity. The detection area in VAMOS consisted of two Drift Chambers (DC) to measure particle positions and angles, a Secondary-electron Detector (SeD) to measure the time of flight, an Ionization Chamber (IC) to measure energy loss, and a wall of twenty-one Silicon detectors to measure the residual energy of the particle (see  for more details on the detectors).
The segmentation of the detectors allows the measurement of the recoil angle with ^ 1 deg of geometrical uncertainty; depending on the reaction, this is translated in ^ 2 MeV of excitation-energy resolution, in both the recoil and the fissioning system. Figure 2 shows the dE-E correlation with the identification of the different recoil species. Recoil identification resulted in the detection of C, B, Be, Li and He. Despite the isotopic identification of the target-like recoil is not achieved, the most probable channels may be estimatedfi-omthe Qgg values .