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@PHDTHESIS{Xu:201580,
author = {Xu, Xiaodong},
othercontributors = {Scheidenberger, Christoph},
title = {{O}bservation and investigation of the new proton-unbound
nuclei $^{30}${A}r and $^{29}${C}l with in-flight decay
spectroscopy},
school = {Justus-Liebig-Universität Gießen},
type = {Dr.},
reportid = {GSI-2017-00682},
pages = {134 p.},
year = {2016},
note = {Justus-Liebig-Universität Gießen, Diss., 2016},
abstract = {Two-proton (2p) radioactivity is an exotic nuclear decay
mode resulting in the simultaneous emission of two protons.
The ground-state 2p radioactivity was discovered in the
decay of 45Fe in 2002. Later, this novel decay mode was also
found in the decays of 48Ni, 54Zn, and 19Mg. <br>In order to
study a promising 2p radioactivity candidate 30Ar, an
experiment was performed at the Fragment Separator of GSI in
Darmstadt (Germany). The in-flight decay technique, which is
based on the tracking of the in-flight decay products by
using the silicon strip detectors, was employed. Several
calibration and alignment procedures were performed to
achieve the best-possible accuracy of position and angle
measurements. In order to determine the angular and
half-life resolutions as well as the detection efficiency,
the decays of the previously-known 2p emitter 19Mg were
remeasured. The 2p radioactivity of 19Mg ground state and
sequential emission of protons from several known excited
states in 19Mg were confirmed. The deduced 2p decay energies
are consistent with previous data. The evidence on a new
excited state in 19Mg at $8.9^(+0.8)_(-0.7)$ MeV above the
2p threshold was found. It was tentatively suggested that
this new 19Mg state decays by sequential emission of protons
via two unknown 18Na resonances at $2.5^(+0.7)_(-0.3)$ MeV
and $4.0^(+1.5)_(-0.6)$ MeV above the 1p threshold,
respectively.Two previously-unknown proton-unbound nuclei
30Ar and 29Cl were identified by measuring the trajectories
of their in-flight decay products 28S+p+p and 28S+p,
respectively. The analysis of 28S-proton angular
correlations provided information on the decay energies and
structure of the observed states in 30Ar and 29Cl. The
assigned ground state and first excited state of 29Cl were
found at $1.8^(+0.1)_(-0.1)$ MeV and $2.3^(+0.1)_(-0.1)$ MeV
above the one-proton threshold, respectively. The ground
state of 30Ar was found to be $2.45^(+0.05)_(-0.10)$ MeV
above the 2p emission threshold. Due to a strong
Thomas-Ehrman shift, the lowest states in 30Ar and 29Cl
point to a violation of isobaric mirror symmetry in the
structure of these unbound nuclei. Detailed theoretical
calculations of the correlations between 2p decay products
followed by the Monte Carlo simulations of the detector
response to the 2p decay were performed in order to
investigate the decay mechanism of the 30Ar ground state.
Its decay is located in a transition region between
simultaneous 2p decay and sequential emission of protons.
Such an interplay between the true three-body and the
sequential two-body decay mechanisms is the first-time
observation in a nuclear ground state. The theoretical
investigations of the transition dynamics demonstrated a
surprisingly strong sensitivity of the decay correlation
patterns to the 2p decay energy of the 30Ar ground state and
the one-proton decay energy as well as the one-proton decay
width of the 29Cl ground state. The first hint on so-called
fine structure in the decay of 30Ar*(2+) was obtained by
detecting two decay branches into both ground state and
first excited state of 28S. The comparison of the
experimental 28S-proton angular correlations with those
resulting from the Monte Carlo simulations of the detector
response illustrates that other observed 30Ar excited states
decay by sequential emission of protons via intermediate
resonances in 29Cl. The decay schemes of the observed states
in 30Ar and 29Cl were constructed.},
cin = {FRS / SuperFRS-EC@FAIR},
cid = {I:(DE-Ds200)FRS-20110310OR124 /
I:(DE-Ds200)Coll-FAIR-SuperFRS-EC},
pnm = {612 - Cosmic Matter in the Laboratory (POF3-612) /
SUC-GSI-Giessen - Strategic university cooperation GSI-U
Gießen (SUC-GSI-GI) / HGF-IVF-VH-GS-201 - HGS-HIRe :
(HGF-IVF-VH-GS-201)},
pid = {G:(DE-HGF)POF3-612 / G:(DE-Ds200)SUC-GSI-GI /
G:(DE-Ds200)HGF-IVF-VH-GS-201},
typ = {PUB:(DE-HGF)11},
urn = {urn:nbn:de:hebis:26-opus-122036},
url = {https://repository.gsi.de/record/201580},
}