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exotic nuclei structure and reaction noyaux exotiques ... - IPN - IN2P3

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width measurements.<br />

This relationship simply illustrates the fact that an<br />

atomic vacancy which has been created in the<br />

entrance channel phase of the collision in the <strong>reaction</strong><br />

partners — <strong>and</strong> transferred to the fused nucleus<br />

after electronic orbital arrangements — disappears<br />

either because it decays through X ray<br />

emission, characteristic of the formed element, or<br />

because a nuclear decay process has occurred,<br />

leading to a new element whose characteristic inner<br />

shell X-ray is different. These competing processes<br />

between nuclear <strong>and</strong> atomic decays will<br />

eventually continue along the decay chain. The<br />

experiment performed at Ganil in November 2009<br />

focused on the compared decay of 103 In <strong>and</strong> 109 In<br />

formed in the <strong>reaction</strong>s 76 Kr+ 27 Al <strong>and</strong> 82 Kr+ 27 Al at<br />

340 MeV.<br />

The second experiment entitled "Super-Heavy Element<br />

Fission Time Measurements Using Inner-<br />

Shell Ionization” is the first step of the SHE stability<br />

measurement program which extends our crystal<br />

blocking experiments. The lifetimes of K- <strong>and</strong> L-<br />

shell vacancies of such atoms, in the 10 -18 s <strong>and</strong><br />

10 -17 s range, respectively, should allow to measure<br />

fission times much longer than the nuclear formation<br />

time. In particular by choosing fissioning<br />

<strong>nuclei</strong> with atomic numbers near or at predicted<br />

closed shells for protons <strong>and</strong>/or neutrons, one<br />

should be able to probe the stability of super-heavy<br />

elements as the high fission barriers expected in<br />

the vicinity of shell closures should lead to fission<br />

times long enough for K <strong>and</strong> L X-ray emission from<br />

the compound nucleus. Moreover, X-ray observation<br />

from super-heavy compound <strong>nuclei</strong> gives access<br />

at the same time to their charge identification<br />

<strong>and</strong> to a quantitative estimate of their fission time,<br />

bringing thus valuable <strong>and</strong> complementary pieces<br />

of information to the crystal-blocking experiments<br />

performed at GANIL. In addition, this method allows<br />

the study of systems for which single crystal<br />

targets are not available.<br />

In a first step, this alternative method for fission<br />

time measurement, independent of any nuclear<br />

model has been applied in December 2009 to the<br />

Z=120 element formed in U induced <strong>reaction</strong>s on<br />

Ni targets. The confirmation of the existence of<br />

long lifetime ( > 10 -18 s) components for such heavy<br />

elements by two independent experimental methods<br />

is of crucial interest as within the present theoretical<br />

approaches it seems quite difficult to reconcile<br />

the very tiny measured residue cross sections<br />

<strong>and</strong> the rather high cross sections associated to<br />

compound <strong>nuclei</strong> surviving against fission longer<br />

than 10 -18 s. In addition , by studying the 238 U +<br />

58 Ni <strong>and</strong> 238 U + 64 Ni systems, the evolution of fission<br />

times with neutron numbers in the proximity of<br />

the neutron shell closure can also be studied, providing<br />

thus very sensitive tests of nuclear shell<br />

models.<br />

The experimental planning<br />

Successful tests have been realized in September<br />

2008, in order to check the background counting<br />

rates registered in the X-ray Germanium detectors<br />

at low energy <strong>and</strong> the feasibility of the lifetime<br />

measurement experiments based on the Atomic<br />

Clock technique. 2009 has been mainly dedicated<br />

to the realization <strong>and</strong> tests of the different parts of<br />

the experimental set-up: the sectorized ionization<br />

chambers constituting the first stage of the<br />

charged fragment telescopes built in Ganil have<br />

been tested in June. Then we tested the sensitivity<br />

of diamond monocristal detectors to radiation damage<br />

with 7.5 A MeV 129Xe beams, in order to<br />

check whether this type of detectors could be used<br />

to detect the elastically scattered projectiles in our<br />

experiments, to deduce the inner shell ionization<br />

probabilities. Finally it appeared that the pulseheight<br />

delivered by these diamond detectors was<br />

quite rapidly affected by the radiation damage,<br />

which led us to use alternatively the elastically<br />

scattered target <strong>nuclei</strong> in st<strong>and</strong>ard detectors located<br />

at large angles.<br />

Furthermore, all the mechanics needed to install<br />

the FluoX detection set up around the Vamos target<br />

have been designed <strong>and</strong> built this year: a set of<br />

supports for the Germanium detectors operated<br />

under vacuum, allowing precise displacements has<br />

been designed in <strong>IPN</strong>O whereas the <strong>reaction</strong><br />

chamber hosting the fragment detectors was<br />

drawn in Ganil. A few days of beam time have<br />

been used in September to check the whole setup,<br />

including the Vamos spectrometer <strong>and</strong> finally<br />

the two scheduled experiments have been successfully<br />

performed in the last months of 2009.<br />

The analysis of these two experiments just started<br />

in January 2010.<br />

References<br />

[1] Morjean M. et al «Fission time measurements: a new probe<br />

into super-heavy element stability», Physical Review Letters,<br />

101, 072701, 2008<br />

113

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