ISNAP Seminars - Abstracts 2007 Spring |
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Topic: Calculations with Finite-range forces in Neutron-rich Nuclei
Nicolas Schunck (Oak Ridge National Laboratory, University of Tennessee) / April 23, 2007
With the on-going development
of Radioactive Beam Facilities, proton- or neutron-rich
nuclei have come under more intense scrutiny. From a theoretical
point of view, these systems present a number of interesting
features. First of all they are characterized by a very
large isospin, whose influence on the density functional
is not very well-known. Moreover their Fermi level is quite
close to the continuum threshold, and residual interactions
such as pairing correlations can scatter particles into
it. The interplay of the nuclear system with the continuum
is therefore a crucial ingredient of all serious theoretical
approaches, and this has been the main argument to call
for the development of more appropriate techniques than
those used in stable nuclei. However, the description of
pairing correlations in such systems, e.g. in Skyrme HFB
approaches, has always been somewhat empirical. We therefore
developed a technique to extend the realm of HFB calculations
with finite-range forces like the Gogny force to weakly-bound
nuclei. In addition to include continuum effects, this technique
is amenable to go beyond the mean-field and to give a precise
measure of the true role of the continuum in ground-state
properties of atomic nuclei. I will describe this technique,
present some of the results we obtained and discuss critically
the extent of continuum effects in weakly-bound nuclei.
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Topic: Use of the 15N(p,a,g)12C Reaction for Nanoscale Studies of Cement Hydration
Jeffrey S. Schweitzer (University of Connecticut) / April 19, 2007
A better understanding of the mechanisms and kinetics of cement hydration during the induction period is critical to improved concrete technology. During the induction period a characteristic pattern of reaction layers develops at and just below the surface of the cement grain. To understand the processes that occur, it is necessary to study the time dependence of the reactions on a nanometer scale. The 15N(p,a,g)12C reaction is particularly well-suited to measure the distribution of hydrogen with depth with a spatial resolution of a few nanometers. Time-resolved measurement of the hydration profile is achieved by stopping the chemical reactions at specific times. The mechanism controlling the induction period of tricalcium silicate is a semi-permeable layer on the grain surface. The diffusion of the hydrogen cannot be represented by a simple Fickian profile, indicating that multiple diffusion and reaction processes are occurring. The hydration profiles for other common components of cement are significantly different. The effects of additives on the chemical reactions have also been studied.
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Topic: Molecular Picture in Heavy Ion Reactions at Low Energy
Alexis Diaz-Torres (Dept. of Nuclear Physics, Australian Nat'l University) / April 16, 2007
The molecular description of nuclear reactions is justified when the relative motion of the interacting nuclei is much slower than the motion of the nucleons in the volume of the system, which is expected to be valid at incident energies near and below the Coulomb barrier. As a consequence, the nucleons near the Fermi surface move in molecular orbitals when the colliding nuclei come into contact. The two-center shell model (TCSM) is a fundamental microscopic approach to describe this scenario. In my talk, I will introduce a new realistic TCSM based on Woods-Saxon potentials and discuss the impact of collective and single-particle molecular effects on fusion of light and heavy nuclear systems.
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Topic: ISAC, DRAGON and Exploding Stars
John D'Auria (Simon Fraser University, Canada) / April 2, 2007
Experimental nuclear science took a quantum leap forward with the advent of using energetic exotic radioactive beams for a wide variety of studies in nuclear astrophysics, fundamental symmetries, nuclear structure at the limits of stability and condensed matter physics. Probably the best facility in North America is the TRIUMF-ISAC facility (Canada). Based upon the ISOL approach, it produces the most intense RB in the world. A key application are measurements of rates of reactions occurring in exploding stars, involving radioactive reactants. Such studies require an intense RB, a low velocity accelerator, an appropriate recoil mass separator, and experienced personnel. This talk will review some of the history of RB production, but the main focus will be the experimental program using the DRAGON facility to measure key reaction rates involving species such as 21Na, 26gAl, 40Ca, and others.
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Topic: 24Mg(a,y)28Si Resonance Parameters at Low Alpha Energies
Elizabeth K. Strandberg (University of Notre Dame) / March 26, 2007
28Si is formed by successive alpha captures
on 12C during the AGB (asymptotic giant branch) stage of stellar burning.
The last reaction in this series, 24Mg(a,y)28Si, has not been examined
with sufficient sensitivity at alpha energies below 1.5 MeV. Several 28Si
states appear favorable for formation by this reaction in the alpha energy
range of 1.0 – 1.5 MeV, motivating a new study of this reaction at the
University of Notre Dame. To maximize experimental sensitivity, a high
efficiency coincidence detection system was developed. Several previously
unknown resonances were observed between 1.1 and 1.5 MeV, and an upper
limit for any lower energy resonances was obtained. Newly calculated resonance
parameters and reaction rates will be presented.
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Topic: Direct measurement of 4He(12C,16O)g cross section near stellar energy at KUTL
Kenshi Sagara (Kyushu University Tandem Laboratory, Fukuoka, Japan) / March 19, 2007
As is well known, 4He+12C→16O+g
reaction is very important in helium burning in stars, however, the reaction
rate at the stellar energy of Ecm = 0.3 MeV has been measured
yet in spite of many attempts in the world for about 40 years. Due
to resonances in 16O the cross section (S-factor) varies sharply
around 0.3 MeV. Hence we have to measure the cross section at energy
as low as possible, e.g., down to 0.7 MeV where the cross section is about
1 pbarn.
In Kyushu University tandem accelerator laboratory
(KUTL), direct measurement of 4He+12C→16O+g
reaction cross section is in progress. A 12C beam is
injected onto a 4He windowless target, and all the 16O
recoils in a charge state are separated from the 12C beam by
a recoil mass separator and are detected by a Si detector.
To measure the 4He+12C→16
O+g cross section down to 0.7MeV, we
need 1) to increase the beam intensity, target thickness and detection
efficiency, because 16O counts at 0.7 MeV are estimated as
about 5 counts/day at most, and 2) to thoroughly reduce backgrounds, because
the number of 16O recoils at 0.7 MeV is 10-18 smaller
than the number of 12C beam particles.
I will talk on several methods and instruments
at KUTL, such as a) a blow-in type windowless gas target and its cooling,
b) a new accel-decel strong-focus operation of the tandem accelerator,
c) a recoil mass separator, and d) a long-time chopper to reduce backgrounds
by 10-3.
Also our recent data on 4He(12C,16O)g
cross section at Ecm = 2.4 MeV will be shown.
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Topic: Study of Beta-delayed Neutron Decay Near the Neutron Drip Line
Chandana Sumithrarachchi (Michigan State University) / March 1, 2007
The rapid change in the location
of the neutron drip as one goes from carbon, to oxygen,
to fluorine isotopes is still not understood. Recently,
it has been suggested that the traditional single particle
shell structure changes significantly in approaching the
drip line. The study of nuclei in the region of the heaviest
oxygen and fluorine isotopes can provide important information
on the variation of nuclear shell structure leading to new
magic numbers. Very little spectroscopic information is
available on these neutron-rich nuclei. One way of exploring
information on them is to combine the traditional study
of the beta-delayed gamma-ray decay of exotic nuclei with
beta-delayed neutron spectroscopy. The first measurement
of beta-delayed neutrons and gamma-rays from the decays
of 22N and 23O has been performed at the NSCL (National
Superconducting Cyclotron Laboratory). The beta decay schemes
of 22N and 23O will be presented and compared to shell model
calculations.
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Topic: Structural Studies of the Most Exotic Nuclei: First Results from The Stopped RISING Project
Paddy Regan (University of Surrey, UK) / February 26, 2007
Projectile fragmentation reactions at relativistic
energies allow unpredecented experimental access to nuclei with the most
extreme values of proton-to-neutron ratio. The RISING (Rare Isotope Spectroscopic
Investigations at GSI) project couples the fragmentation production mechanism
with high-resolution gamma-ray spectroscopy for the study of internal
structure of nature's most exotic nuclear species. This talk will present
the first experimental results from the RISING gamma-ray array in its
'Stopped Beam'configuration, which is designed for studies of spectroscopy
of exotic nuclei following isomer and beta-delayed decay. I will specifically
present isomer-spectroscopy identifying new metastable states in nuclei
(i) along the N=Z line between the doubly magic systems 56Ni
and 100Sn and (ii) neutron-rich nuclei associated with proton
holes in the 132Sn and 208Pb doubly-magic closed
shells pertinent to the r-process path. These results reveal new physics
associated with T=1,0 proton-neutron pairing competition along the proton
drip line for N=Z nuclei and the persistence (or not) of the N=82 and
126 shell closures for large neutron excess.
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Topic: To chiral rotation and back again
S. Daniel Almehed (University of Notre Dame) / February 19, 2007
Several near degenerate rotational bands with
the same parity have been found in the A=135 and A=105 mass regions where
triaxiality of the nuclear shape appears. Some of these have been interpreted
as chiral rotational bands within the Tilted Axis Cranking (TAC) model.
Chiral rotation can appear in triaxial nuclei when proton and neutrons
align along different principal axes and the collective rotation occurs
along the third. These bands can some times be interpreted as a chiral
vibration, which is a vibration of the orientation of the principal axes
of the nucleus with respect to the angular momentum vector. Chiral vibration
can be studied with the RPA plus TAC formalism. I examine the limits of
chiral rotation as a function of particle number and angular momentum
in the A=135 region. The properties of the RPA phonons are discussed and
compared to experimental data.
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Topic: A Cluster Model of 6He and 6Li
Jeremy Armstrong (NSCL, Michigan State University) / January 29, 2007
Small nuclei provide an ideal testing ground
of few-body theories. 6He is particularly interesting in that
it shows an extended particle distribution similar to a halo nucleus,
is loosely bound, and is a Borromean system. We apply the Brink Formalism
in secondary quantization to study the structure of 6He. This
formalism allows for the proper treatment of Fermi statistics and correct
projection into eigenstates of angular momentum. The alpha plus dineutron
configuration and "cigar" (neutron, alpha, neutron chain) configuration
were studied to obtain binding energies, charge radii, matter radii, and
B(E2) for 6He. The same configurations were used to obtain
the same observables for 6Li. We were then able to calculate
the log ft value for the beta decay of 6He.
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Topic: Low-Energy Nuclear Astrophysics - the Fascinating Region of A=7
Michael Hass (Weizmann Institute of Science, Rehovot, Israel) / January 10, 2007
We discuss results of low-energy reactions that
play an important role in current nuclear astrophysics research and that
happen to concentrate around the region of A=7. The 7Be(p,gamma)8B
and the 3He(4He,gamma)7Be reactions are
crucial for understanding the solar-neutrino oscillations phenomenon and
the latter one plays a central role in the issue of cosmic 7Li
abundance and Big-Bang Nucleosynthesis. We also present results regarding
the host dependence of the half life of the electron-capture 7Be radio-nuclide
and future plans for reactions with radioactive beams.
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