Heavy Ion Discussion Group
Conference Room R-150, Building 203, Argonne National Laboratory
Fridays at 3:30 PM
|24 Aug 2015||Special Day: Monday
Sean Kuvin, Florida State University,
"Measurement of the 17F (d, n)18Ne reaction using RESONEUT"
The 17F(p, γ)18Ne reaction of astrophysical importance has been studied using the
surrogate reaction 17F(d, n)18Ne in inverse kinematics. The usefulness of this type of
approach has been demonstrated in previous experiments at the RESOLUT facility.
In this work we have developed a compact neutron detector array, RESONEUT, which
is specialized for (d, n) reactions in inverse kinematics. The threshold and efficiency
properties of the neutron detectors were characterized using the 12C(d, n)13N reaction.
Spectroscopy of the 18Ne nucleus was accomplished using two methods. The first was by
neutron time of flight spectroscopy and the second was by kinematic reconstruction of the
unbound compound nucleus by detecting the emitted proton and heavy ion. We compared
our results with those obtained from 17F+p elastic scattering measurements and from the
direct 17F(p, γ) measurement conducted at Oak Ridge[2,3]. Our results provide additional
confirmation that the state at ~600 keV is the 3+ state. No other resonances directly
above the proton threshold were detected. However, using NaI(T1) detectors detecting
gammas in coincidence with the neutrons in RESONEUT, we have placed upper limits on
the possibility of having a low-lying proton resonance with a significant Γγ > Γp branching
|27 Aug 2015||Special Day: Thursday
Ran Hong, University of Washington,
High-Precision Measurement of the β-ν Correlation in the 6He Decay
High-precision measurements of β-decays are sensitive probes of new physics beyond the Standard Model (SM). Particularly, the β-ν correlation of Gamow-Teller decays is sensitive to the exotic tensor type weak current which is predicted by the leptoquark model and some super symmetric models. A new experiment that measures the β-ν correlation coefficient αβν of the 6He decay is being developed at the Center of Experimental Nuclear Physics and Astrophysics (CENPA), University of Washington. In this experiment, the 6He atoms are laser-trapped while both the
β-particle and the recoil ion are detected.
The αβν is extracted by fitting the time-of-flight (TOF) spectrum of the recoil ions. The ultimate goal of this experiment is a 0.1% determination of αβν and the short-term goal is to determine αβν at or lower than 1% and pave the way to the 0.1% level measurement.
|31 Aug 2015||Special Day: Monday
Kenneth Whitmore, Michigan State University,
New Experimental Probes of the Halo Nucleus 19C
Halo nuclei occur at the limits of stability, where a low binding energy allows valence nucleons to tunnel beyond the nuclear core to form a diffuse nuclear cloud. Several experimental probes have been used to identify and characterize halo nuclei, including interaction cross section measurements, momentum distributions following knockout reactions, and Coulomb dissociation reactions. In particular, an enhanced electric dipole (E1) response at low energy has become a unique signature of halo nuclei. Despite numerous investigations into the E1 response, there is very little information on the magnetic dipole (M1) response of halo nuclei.
|3 Sep 2015||Special Day: Thursday
Michael Jones, Michigan State University,
Two-neutron Sequential Decay of 24O
|17 Sep 2015||Special Day: Thursday
Kalle Auranen, University of Jyvaskyla,
Spectroscopy of 199,201At
The excited states of 199At and 201At were studied using fusion evaporation reactions, a gas-filled recoil separator and various tagging methods.
The level scheme of 201At was extended a lot including a cascade of magnetic dipole transitions, that is suggested to form a shears band.
In addition, a 29/2+ [T1/2 = 3.39(9) ms] isomeric state was observed. The 29/2+ state is suggested to originate
from the π(h9/2)X|200Po; 11- > configuration, and it depopulates through 269-keV E2 and 339-keV E3 transitions.
In both nuclei 199,201At we have observed also the isomeric 1/2+ [T1/2 = 273(9), 45(3) ms, respectively] intruder state,
that is suggested to originate from the π(s1/2)-1 configuration. The 1/2+ state decays through 103-keV and 269-keV E3 transitions
in 199,201At, respectively.
In both nuclei the 1/2+ state is fed from 3/2+ and 5/2+ states, which are suggested to originate from the
π(d3/2)-1 and π(d5/2)-1 configurations, respectively.
|25 Sep 2015||S&T review,
|2 Oct 2015||Torben Lauritsen,Physics Division, Argonne National Laboratory
|9 Oct 2015||Andrei Andreyev, University of York, UK/JAEA, Tokai, Japan
on behalf of Leuven-Gatchina-ISOLDE-Mainz-Manchester-York and Windmill-ISOLTRAP-RILIS collaboration
Shape coexistence and charge radii in the long chains of gold, mercury and astatine isotopes studied by in-source laser spectroscopy at RILIS-ISOLDE
The competition between spherical and deformed configurations gives rise to shape coexistence in the neutron-deficient isotopes around Z~82 and N~104  while on the neutron-rich side, effects due to octupole deformation in the vicinity of N~133 could be expected . In order to determine to which extent the ground and isomeric states of these nuclides are affected by these phenomena, an extensive campaign of investigation of changes in the mean-square charge radii and electromagnetic moments is being conducted by our collaboration at the mass-separator ISOLDE (CERN). The measurements rely on the high sensitivity provided by the in-source laser spectroscopy technique [3, 4].
|15 Oct 2015||Special Day: Thursday
Sandrine Courtin,IPHC, CNRS/IN2P3, and Universite de Strasbourg, France
Low energy heavy-ion fusion reactions : tunneling through multidimentional barriers
Fusion-evaporation is the dominant reaction mechanism in medium-mass heavy-ion collisions around the Coulomb barrier. At these energies and at moderate sub-barrier energies, enhancement of the fusion cross-sections was observed whereas hindrance of the fusion cross- section has been identified in many systems at deep sub-barrier energies. Fusion cross-sections around the Coulomb barrier have been discussed extensively to be driven by couplings of the relative motion of the colliding nuclei to their low energy surface vibrations and/or stable deformations. The corresponding coupled-channel calculations and the distributions of barriers have revealed to be a powerful tool to better understand the role of
|23 Oct 2015||Calem Hoffman, Physics Division, Argonne National Laboratory
|30 Oct 2015||DNP meeting,
|6 Nov 2015||TBD,
|13 Nov 2015||TBD,
|20 Nov 2015||TBD,
|27 Nov 2015||Thanksgiving,
|4 Dec 2015||TBD,
|11 Dec 2015||TBD,
|18 Dec 2015||TBD,
|25 Dec 2015||Christmas,
|1 Jan 2016||New Year's Day,
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