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Extra resources for Comparison, Evaluation of Fission-Yield Nuclear Data (IAEA TECDOC-1168)
For fission in inverse kinematics the fissile nuclides are projected at high (relativistic) energies on a still-standing target of varying composition. A transfer of excitation energy occurs to the fissile ions when they pass through the target and they subsequently undergo fission — in flight. g. 100 GeV). In consequence, the kinetic energy of the fission fragments is much higher and the fission fragments form a beam of a small divergence and therefore may be analysed in a fragment separator and by time of flight instrumentation quite effectively.
The HeidelbergDarmstadt crystal-ball-spectrometer as a 4p-neutron detector", High Resolution Spectroscopy of Fission Fragments, Neutrons, and g-Rays (Proc. Int. ), Rep. FZR 93-08 (1993) 81-93. , Low-energy fission studies of neutron-deficient projectile fragments of 238U; Phys. Lett. B 325 (1994) 313–316. , Low-energy fission investigated in reactions of 750 AMeV 238 U-ions with Pb and Be targets, Z. Phys. A 355 (1996) 191–201. , Reaction and fission cross sections of 750 AMeV 238U-ions on Pb, Cu and Al-targets, Z.
45]. 48]. 50] and by subtracting it from the initial kinetic energy as determined by the mass separator Lohengrin. These arrangements have the disadvantage of using only a small part (a few mm) of the total length of the exit slit of Lohengrin (of 70 cm). 51] allows the use of up to 40 cm of the exit slit and, this way, offers a considerable increase in sensitivity allowing measurements in regions of low yield as will be discussed. The big ionization chamber has a split anode that allows a simultaneous measurement of the energy loss DE in a first part of the chamber and the remaining energy ER in the second part of the chamber.