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 couplings to collective degrees of freedom of the target and projectile.
|23 Oct 2015||Daniel Santiago-Gonzalez, Louisiana State University/Argonne National Laboratory
An update on the HELIOS gas target and ionization chamber
|30 Oct 2015||DNP meeting,
|5 Nov 2015||Special Day: Thursday, 10 am
Rene Reifarth, Goethe Universitaet, Frankfurt
Radioactive isotopes - in stars and laboratories
Most of the time, stars gain their energy from fusion of the very light left-overs of the Big Bang into heavier elements over long periods of time.
The observation of radioactive isotopes in different regions of the Universe is an indicator of this ongoing nucleosynthesis. In addition, short-lived nuclei are often intermediate steps during the nucleosynthesis in stars.
|13 Nov 2015||Melina Avila Coronado, Physics Division, Argonne National Laboratory
Understanding stellar processes through nucler reactions
The understanding of stellar nucleosynthesis is one of the driving forces of nuclear astrophysics. Nuclear reactions provide an essential input for models of stellar evolution, energy generation in stars and stellar explosions. For instance, a large number of proton and α induced reactions such as (p,γ), (α,γ), (α,p) and (α,n) are known to play an important role in different astrophysical scenarios. In general, direct measurements are preferred. However, many of these reactions cannot be measured directly at relevant astrophysical energies because of their small cross section and it becomes crucial to have a reliable indirect technique to evaluate them. Extracting the Asymptotic Normalization Coefficients (ANCs) using sub-Coulomb transfer reactions can be used as an effective method to determine properties of near-threshold resonances, thus constraining key astrophysical reaction rates. In this talk, I will discuss different α induced reaction measurements using both direct and indirect techniques for nuclear astrophysics studies. Results on α-transfer reactions using the ANC technique at sub-Coulomb energies will be presented. In addition, I will also discuss results on direct measurements of (α,p) and (α,n) reactions using the active target system MUSIC.
|20 Nov 2015||Michael Carpenter, Physics Division, Argonne National Laboratory
The CAGRA Project
|27 Nov 2015||Thanksgiving,
|1 Dec 2015||Special Day: Tuesday, 10 am
Brian Bucher, LLNL
Understanding the creation of matter and the elements, one experiment at a time
How were the elements created? How even did the matter used to build the elements come about? These are a couple of fundamental questions that can be addressed by nuclear physics research. In this talk, I will present a few different projects aimed towards uncovering important clues to help answer these questions. One of these is centered around direct measurements of the 12C+12C fusion cross sections which have implications for a variety of astrophysical and nucleosynthesis scenarios. The others focus on nuclear structure in the mass region A=100-150, in particular how the evolution of single-particle structure relates to bulk nuclear properties such as ground-state shapes, isomerism, and masses. Especially intriguing about the nuclear structure in this mass region is the prospect for large octupole deformations which may provide additional candidates for atomic EDM searches. Our recent measurement indicates a significantly larger octupole deformation than those observed in the actinides with comparable quadrupole deformations. All of the projects discussed in this talk have either taken advantage of or can be further advanced by the many unique technical capabilities available at ATLAS.
|3 Dec 2015||Special Day: Thursday, 10 am
Farheen Naqvi, Michigan state University
Total Absorption Spectroscopy and its Applications
Total Absorption Spectroscopy (TAS) was used to extract the cross-sections of the proton capture reactions relevant to estimate the abundances of the light p-nuclei produced in the astrophysical p-process. On the neutron-rich side of the nuclear chart TAS was used to obtain the beta-decay strength distributions and to extract the neutron capture cross-sections which are one of the key components in predicting the path of astrophysical rapid neutron-capture process (r-process). The γ-summing technique was employed using the Summing NaI(Tl) detector (SuN) from the National Superconducting Cyclotron Laboratory. The experiment measuring the 72Ge(p,gamma)73As cross-section was performed at the University of Notre Dame using a 1.8 to 3.6 MeV proton beam. The results from this experiment will be reported in the first part of the talk. The second part will deal with the experiment aimed at measuring the beta-decay strength distribu- tions in neutron-rich Cu isotopes and extracting the neutron capture cross-sections of Ni isotopes. The experiment was performed at the National Superconducting Cyclotron Laboratory (NSCL) using the fragmentation of a 86Kr primary beam. The experimentally obtained total absorption spectra for the neutron-rich Cu isotopes will be presented and the implications of the extracted beta-feeding intensities will be discussed.
|8 Dec 2015||Special Day: Tuesday, 1:30 pm
Marina Petri, Technical University, Darmstadt
Interplay of experiment and theory in the quest to understand the nuclear force
Understanding the nature of the nuclear force that binds protons and neutrons into nuclei continues to be one of the main research frontiers of nuclear science. Key to this understanding is the productive interplay between experiment and theory. In this talk I will discuss how experiments on exotic nuclei have recently advanced our understanding of the nuclear many-body problem focusing on my work along these lines. On the theory frontier, a paradigm shift is currently taking place and theory is switching from phenomenology to a chiral-EFT description reflecting the symmetries of QCD. Testing and refining these new approaches require high-quality data on key experimental observables. I will present recent results and discuss further plans geared towards benchmarking such theories.
|10 Dec 2015||Special Day: Thursday, 10 am
Daniel Santiago-Gonzales, Luisiana State University
New experimental techniques for nuclear studies at ANL Recent advances in nuclear physics and astrophysics have been made possible by pushing the limits of experimental techniques. For example, studies on high-spin states, low-cross section reactions and neutron-rich/neutron-poor isotopes have taught us much about previously unknown aspects of the nuclear force.
In this talk, I will present two experimental techniques with great potential for unique studies of both nuclear structure and nuclear astrophysics at the ATLAS facility at ANL, namely 1) using isomer beams in order to probe otherwise inaccessible nuclear reactions and 2) using an active target with particle tracking to efficiently study low-cross section reactions.
The techniques discussed here take full advantage of the current and future capabilities of the ATLAS facility in order to answer some of the open questions in both nuclear structure and astrophysics in the coming years.
|11 Dec 2015||Christian Berner, Technical University Munich
"Characteristic X-ray Emission of Heavy Nuclei After Fusion"
|25 Dec 2015||Christmas,
|1 Jan 2016||New Year's Day,
|8 Jan 2016||Stefan Lalkovski,University of Surrey, UK
"FAst TIMing Array (FATIMA) in Argonne"
|15 Jan 2016||Herve Savajols, GANIL
"Status of the GANIL SPIRAL2 project"
|22 Jan 2016||Simone Bottoni, Physics Division, Argonne National Laboratory
"Nuclear structure studies around N=40 with heavy-ion transfer reactions"
|29 Jan 2016||The ATLAS RWP briefing will proceed the talk
Yogesh Gupta,University of Notre Dame
"Are there nuclear structure effects on Isoscalar Giant Monopole Resonance and Nuclear Incompressibility near A~90"
|5 Feb 2016||Rashi Talwar, Physics Division, Argonne National Laboratory
"Bubble Chamber : A novel technique for measuring thermonuclear rates at low energies"
|11 Feb 2016||Special Day: Thursday, 3:30 pm|
Keegan Kelly, University of North Carolina
"Investigation of the 22Ne(p,g)23Na Reaction Rate: The Globular Cluster Na-O Anticorrelation"
Globular clusters are thought to have been created early in the formation of the galaxy and contain snapshots of virtually all stages of stellar formation, making them excellent testing grounds for astrophysical models. However, the appearance of anomalous abundance patterns, such as the Na-O anticorrelation, in cluster stars of all stages of evolution indicate that these ancient stellar objects are more complicated than they seem. It has been suggested that the winds from asymptotic giant branch (AGB) stars massive enough to undergo hot bottom burning are a source of pollution in the globular cluster interstellar medium from which new stars formed, thereby contributing to these abundance anomalies. Unfortunately, the accuracy of the yield from AGB models is inhibited by reaction rate uncertainties in the 22Ne(p,g)23Na reaction rate, among others.
|18 Feb 2016||Special Day: Thursday, 3:30 pm
Stephanie Lyons, University of Notre Dame
"Low-Energy 20Ne(p,gamma)21Na Cross-section Study with the 5U-4 St. Ana Accelerator"
In stars whose temperature is greater than 0.05 GK, hydrogen burning can proceed via the NeNa cycle, which in important for the nucleosynthesis of Ne, Na, and Mg isotopes. The first reaction in this cycle is 20Ne(p,g)21Na, which also has the slowest proton capture reaction rate , thereby influencing the rest of the cycle and, potentially, abundances of the other nuclei that are synthesized in the cycle. The stellar reaction rate for 20Ne(p,g)21Na is dominated by direct capture and the high energy tail of a subthreshold resonance. The aim of this work is to understand the direct-capture component of this reaction. Using Notre Dame’s recently commissioned 5U-4 accelerator, the 20Ne(p,g)21Na cross-section has been measured relative to the 1169 keV resonance at low energies. The resonance strength of the 1169 keV resonance was also independently determined. Improvements to previous cross-section measurements will be discussed .
|26 Feb 2016||Daryl Hartley, United States Naval Academy
"A search for tetrahedral symmetry in 156Dy"
|4 Mar 2016||John Greene, Physics Division, Argonne National Laboratory
"Isotopic Carbon Targets"
|11 Mar 2016||Ben Kay and Clayton Dickerson, Physics Division, Argonne National Laboratory
"Discussion on beam imaging at ATLAS"
|18 Mar 2016||Bernhard Maass, Physics Division, Argonne National Laboratory
"Laser Spectroscopy and the Nuclear Charge Radius of 8B"
|25 Mar 2016||Gavin Lotay, University of Surrey, UK
|1 Apr 2016||NO DISCUSSION
|8 Apr 2016||Shea Mosby, Los Alamos National Laboratory
"Multi-Channel Probes to Understand Fission Dynamics"
|15 Apr 2016||"Daniel Doherty", "Univeristy of York, United Kingdom"
"Probing Nuclear Structure via Coulomb Excitation with Radioactive Beams at HIE-Isolde and ANL"
|22 Apr 2016||Dieter Ackermann, Grand Accélérateur National d’Ions Lourds - GANIL, 14076 Caen, France, and
GSI Helmholtzzentrum für Schwerionenforschung GmbH, 64846 Darmstadt, Germany
"SHN decay spectroscopy - recent studies at GSI/SHIP and perspectives for SPIRAL/S3"
In recent experiments at the velocity filter SHIP at GSI, Darmstadt, Germany, we extended our decay spectroscopy studies in the region of shell stabilized deformed superheavy nuclei around Z=108 and N=152-162. Among others we studied the decay properties of 258Db which has also consequences for the heaviest nucleus for which a K-isomer was observed, 270Ds and its decay products. These investigations will be discussed also in view of the SHN investigations, envisaged for the new separator/spectrometer set-up S3, presently being constructed at the new facility SPIRAL2 at GANIL, Caen, France.
|29 Apr 2016||Amel Korichi, CSNSM, IN2P3-CNRS, Orsay, France
"Status of the European Gamma Tracking Array: AGATA"
|6 May 2016||Stephen MacDonald, Physics Division, Argonne National Laboratory
|13 May 2016||TBD, TBD
|20 May 2016||TBD, TBD
|27 May 2016||TBD, TBD
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