Proposal # |
PI Name |
Title |
Days |
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993-3 |
C. Wu |
Rotational alignment of j15/2 neutron orbitals in the Np isotopes |
(5) |
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1046-2 |
R. Weinstein |
Continuing Optimization of Pinning Centers: Entanglement and
Area Density |
2 |
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1113-4 |
D. Hartley |
Competition Between the Wobbling Mode and Particle-Hole
Excitations: Search for TSD Bands in 167Ta |
5 |
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1159-3 |
D. Seweryniak |
Core excitations and single-neutron states in 101Sn |
10 |
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1163-2 |
T. Ahn |
Evolution of the one-phonon mixed-symmetry 2+ state in the
spherical-to-axially-deformed shape phase transition in Sm isotopes from
inverse-kinematics Coulomb excitation |
3 |
|
1179X-2 |
N. R. Patel |
Experiments to further the understanding of the triple-alpha
process in hot astrophysical scenarios |
8 |
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1184-2 |
J. Clark |
Mass measurements around 92Pd relevant for the rp-process and the new vp-process |
7 |
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1185-2 |
S. Tandel |
K isomers and collective states in Cf isotopes |
5 |
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1186X-2 |
P. Collon |
New ion source techniques to reduce 39K and improve sensitivity for measuring 39Ar - a
continuation of 39Ar AMS at ATLAS |
5 |
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1190-2 |
M. Notani |
Spin determination of levels critical to (p, gamma) capture,
studied via (d,t) reactions: 27Si(d,t)26Si |
3 |
|
1194 |
S. Tabor |
Structure of N=Z=47, 94Ag, and its exotic decay modes |
10 |
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1195X |
D. G. Sarantites |
Improvements of HERCULES and Design Tests for SuperHERCULES |
2 |
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1197 |
A.G. Smith |
Lifetime measurements of excited states in fission fragments |
17 |
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1198X |
J. C. Lighthall |
Commissioning of the HELIOS spectrometer |
4 |
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1199X |
J. C. Lighthall |
Commissioning of the HELIOS beam line |
6 |
|
1200 |
G. Montagnoli |
The 60Ni+100Mo fusion excitation function at far sub-barrier energies |
5 |
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1202 |
G. Dracoulis |
Long-lived isomers and K-forbiddenness in well-deformed and
transitional, neutron-rich nuclei |
3 |
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1203 |
D. Jenkins |
Two photon emission from the 0_2+ state in 98Mo |
2 |
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1205X |
M. Paul |
Half-life and (gamma, n) production of p-process nuclide 146Sm |
4 |
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1207 |
R. Segel |
Electroweak interaction tests using trapped Li-8 ions |
4 |
|
1209 |
R.C. Pardo |
Test of the new ATLAS radioactive beam sweeper |
2 |
|
1210 |
T. Lauritsen |
Entry distribution measurement: Probing rotational damping in 194Hg |
5 |
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1211X |
C.J. Lister |
Precision measurements of electromagnetic matrix elements as a
test of AB-Initio calculations in light nuclei: The A=10 systems |
4 |
|
1212 |
H.Y. Lee |
Determination of reaction rates for 18F(a,p)21Ne at T<0.3 GK |
(5) |
|
1213 |
A. Hayes |
Direct measuremnet of the GSB->K=16+ isomer band matrix
elements in 178Hf |
5 |
|
1215 |
C.L. Jiang |
A measurement of 12C + 12C at energies of astrophysical interest |
2 |
|
1216 |
Z. Liu |
Study of the spin-gap isomers in 96,97Cd |
(3) |
|
1217 |
D. Seweryniak |
Proton-neutron interactions in 100In |
(5) |
|
1220 |
F.G. Kondev |
Properties of excited states in 75,77Ge and 75,77Se nuclei |
4 |
|
1222X |
S. Zhu |
Production of neutron-rich isotopes in reactions at beam
energies well above the Coulomb barrier |
3 |
|
1223 |
T.L. Khoo |
High-K isomer and 1-quasiparticle energies in 255Lr: testing
theories of superheavy nuclei |
7 |
|
1226 |
J. Clark |
Precise mass measurement of doubly-magic 56Ni with the Canadian penning trap mass spectrometer |
(4) |
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Total Beam Days |
120+(22) |
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Please Note: |
Because of the
pressure on ATLAS beam time, the PAC ranked the approved experiments in two
categories. Priority I experiments are
those that must be run at all costs. Priority II experiments are those that
should be granted beam time (indicated in parenthesis) if at all possible.
Priority I experiments are approved for the present cycle of experiments, but
can be run during the next PAC cycle as well if scheduling conflicts occur.
Priority II experiments that cannot be scheduled during the present cycle
will have to be resubmitted at the next PAC meeting. It is our intention to
try as hard as possible to schedule a full experimental program and to
accommodate as many, if not all, of
the priority II experiments. |
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Shown in red is a
Gammasphere source experiment which does not require ATLAS beam time. |
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