“…The entire catcher foil stack can be rotated at various frequencies of up to 80Hz. In order to apply the highest beam intensities of up to 1012 particles per second presently available at the UNILAC, the target was also rotating during bombardment using the wheel system described in [25]. The metallic, selfsupporting targets, typically 40 x 20 mm 2 in area and 3 to 5 mg/cm 2 thick, were positioned at the periphery of a rotating disk in sixteen window positions.…”
The production of fermium isotopes was attempted by complete fusion of different targets and projectiles spanning a wide range of effective entrance channel fissilities below and above the predicted threshold value Xef fthr~(l'/-v... For the most asymmetric systems where fusion is expected to occur without dynamical hindrance we investigate to what extent the expected amount of sub-barrier fusion contributes to the production of fermium evaporation residues. For increasingly symmetric systems the experimental fusion barriers are found to exceed the fusion barriers predicted by the proximity formalism. The barrier heights are discussed in the framework of both the extra-push model and the surface friction model.
“…The entire catcher foil stack can be rotated at various frequencies of up to 80Hz. In order to apply the highest beam intensities of up to 1012 particles per second presently available at the UNILAC, the target was also rotating during bombardment using the wheel system described in [25]. The metallic, selfsupporting targets, typically 40 x 20 mm 2 in area and 3 to 5 mg/cm 2 thick, were positioned at the periphery of a rotating disk in sixteen window positions.…”
The production of fermium isotopes was attempted by complete fusion of different targets and projectiles spanning a wide range of effective entrance channel fissilities below and above the predicted threshold value Xef fthr~(l'/-v... For the most asymmetric systems where fusion is expected to occur without dynamical hindrance we investigate to what extent the expected amount of sub-barrier fusion contributes to the production of fermium evaporation residues. For increasingly symmetric systems the experimental fusion barriers are found to exceed the fusion barriers predicted by the proximity formalism. The barrier heights are discussed in the framework of both the extra-push model and the surface friction model.
“…The thicknesses of the 2~ targets were (470-530) gg/cm 2. The melting point of Bi is 544 K. To withstand the high beam currents, the targets were covered with (20)(21)(22)(23)(24)(25)(26)(27)(28)(29)(30) ~tg/cm 2 carbon films for radiative cooling and mounted on a rotating wheel [11]. The wheel that supported 9 targets was synchronized with the UNILAC beam pulsing, which has a repetition rate of 50 cps and a duty factor of 25 %.…”
An experiment to synthesize element 109 is presented. Decay patterns characteristic of complete fusion products were searched for in an irradiation of 2~ targets with SaFe projectiles at specific incident energies of 4.95, 5.05, and 5.15 MeV/u. A total dose of 7 X 1017 particles was obtained. The experimental method involves in-flight separation of forward peaked reaction products with a static-field velocity filter, their passage through a time-of-flight device and their final implantation into position sensitive solid state detectors to measure their kinetic energy, approximate mass and their time and position of incidence. The subsequent decay of the narrowly localised reaction products by cascades of alpha particles and/or spontaneous fission is also registered in terms of the energies and times of all the emitted particles. One outstanding decay sequence that started with the emission of two alpha particles within subsequent time intervals of 5 ms and 22 ms and ended with spontaneous fission after 13 s was found at 5.15 MeV/u. The first alpha particle had a kinetic energy of (11.10_+0.04) MeV. A detailed analysis of all the alternative interpretations of this observation, such as a purely random correlation of signals, the decay of a product from a transfer reaction or of any of the various energetically possible evaporation residues, shows that the isotope with mass 266 of element 109, i.e. the one neutron evaporation channel after complete fusion, is the statistically most significant assignment. The outlook for new element synthesis is also briefly discussed.
“…The current has been measured by a Faraday cup. To withstand high beam intensities, the targets are covered with carbon films of 0.03mg/cm 2 to improve radiative cooling [6] and are mounted on a rotating target wheel [7]. The UNILAC beam provides a macro-pulse structure with beam bursts of 5 ms duration followed by intervals of 15 ms.…”
Section: Methodsmentioning
confidence: 99%
“…The halflive evaluated by the maximum likelihood method ( +_1.7) is 2.9 1.2 s. Four decays were observed at (7,889 _+25)keV, two of them correlated as daughter decays with times distances of 6s and 17s, respectively. The daughter decays fit to 243Es, which has a decay energy of (7,890_+ 20) keV and an average lifetime of 30s [19].…”
The evaporation residues produced in heavy ion fusion reactions between 4~ and z~ Z~ and 2~ respectively, were investigated. They were separated in-flight using a velocity filter (SHIP) and identified after implantation into an array of position sensitive surface barrier detectors by measuring their decay characteristics.Three new e-emitting isotopes were found: 247Md, 243Fm, and 239Cf. Z~TMd was identified by correlation to its known daughter decay 243Es, and 243Fm and 239Cf were observed as correlated decays. Moreover, all previously known deexcitation channels, characterized by spontaneous fission or by ~ decay, could be observed for the first time in one experimental setup. Our results for formation cross sections and decay characteristics are in agreement with known data.
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