Proposal # |
PI Name |
Title |
Days |
1183-2 |
A. A. Hecht |
Towards 100Sn: measuring the masses of the light tin isotopes |
4 |
1206-2 |
B. S. N. Singh |
Quantifying oblate collectivity in the N = Z nucleus 68Se |
4 |
1219-2 |
A. Lopez-Martens |
Superdeformed ridge properties in 192Hg: probing the new phenomena of ergodic bands and
motional narrowing |
7 |
1228X |
W. Loveland |
The Synthesis of Superheavy Nuclei Using Damped Collisions--A
Test |
1 |
1230 |
X. Wang |
Lifetimes of the TSD candidate bands in 157,158Er at ultra-high spin |
12 |
1231 |
W. Walters |
What happened to the isomers in 72,74Ni? collectivity vs. seniority |
5 |
1233 |
U. Garg |
Search for Chiral Bands in 133Ce: Testing the Theoretical Predictions and Affirming
Chiral Behavior in the A~130 Region |
3 |
1234 |
T. Grahn |
RDDS lifetime measurements of yrast states in 184,186,188Hg |
5 |
1235 |
W. Kwok |
Thermodynamic and Vortex Pinning Studies of the Newly Discovered
Doped Oxypnictide Superconductor La(FxO2-x)FeAs |
1 |
1237 |
N. Pietralla |
Inverse-kinematics two-step Coulomb excitation of two-phonon
mixed-symmetry states of 94Mo and 96Ru -- part I |
2 |
1238 |
C.L. Jiang |
Measurement of sub-barrier fusion of 27Al + 45Sc |
5 |
1239 |
D. Rudolph |
Particle and Gamma-Ray Coincidence Spectroscopy of 57Cu |
8 |
1242 |
J. M. Figueira |
The Structure of 30S above the 29P(p,g) Threshold |
5 |
1244 |
K. E. Rehm |
Bypassing the Triple-a Process via the 9C(a,p)12N reaction |
5 |
1245 |
F.G. Kondev |
Electron capture delayed fission of 180Tl: testing theoretical predictions for fission barriers
in nuclei far from the line of beta stability |
7 |
1247 |
G. Savard |
Mass measurements around 92Pd relevant for the rp-process, the new nup-process and
the puzzle surrounding the two-proton decay of the high-spin isomer in 94Ag |
7 |
1248 |
C. J. Lister |
Precision measurements of electromagnetic matrix elements as a
test of ab-inito calculations |
6 |
1249X |
J. C. Lighthall |
In-flight beam commissioning of the HELIOS spectrometer |
6 |
1250 |
L. Riedinger |
Solving
the mystery of "missing E2" transitions at N = 90: tetrahedral
symmetry in rare-earth nuclei? |
3 |
1252 |
P. Fallon |
Identification
of low lying 2p2h states in N=20 nuclei |
6 |
1253 |
S. Tandel |
Collective oblate rotation at high spins in neutron-rich W
isotopes |
(6) |
1254 |
E. A. McCutchan |
Feasibility of (18O, 2n)224Th, (18O, 3n)223Th spectroscopy with Gammasphere and HERCULES |
2 |
1257 |
C. M. Deibel |
Measurement of the 30S(a,p)33Cl Rate in X-Ray Bursts |
5 |
1258 |
J. Hamilton |
Study of the fission process and identification of levels in 158Nd, 162Sm and 166Gd |
16 |
1259 |
C. Wrede |
Precise mass measurements of 32Cl and 31S |
(5) |
1260 |
J.F.Smith |
Non-Yrast spectroscopy on high spin states of reflection
assymetric 222Th |
(7) |
1262 |
S. Zhu |
Condensation of Rotational-aligned octupole phonons in 230Th? |
5 |
|
|
Total Beam Days |
114+(18) |
|
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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