Publications by Year: 2004

2004
Stolz A, Estrade A, Davies AD, Ginter TN, Hosmer PT, Kwan E, Liddick SN, Mantica PF, Mertzimekis TJ, Montes FA, et al. Radioactive ion beams in the region of $^{100}$Sn and $^{78}$Ni at the NSCL. Nucl. Phys. A. 2004;746:–.Abstract
The regions around the doubly magic nuclei 100Sn and 78Ni are of great interest from a nuclear structure standpoint. These nuclei also play a key role in the astrophysical rp- and r-processes, respectively. Recently, nuclei in these regions were studied at the Coupled Cyclotron Facility at the National Superconducting Cyclotron Laboratory (NSCL) at Michigan State University. © 2004 Elsevier B.V. All rights reserved.
Stolz A, Estrade A, Davies AD, Ginter TN, Hosmer PT, Kwan E, Liddick SN, Mantica PF, Mertzimekis TJ, Montes FA, et al. Radioactive ion beams in the region of $^{100}Sn and $^{78}Ni at the NSCL. In: Proceedings of the Sixth International Conference on Radioactive Nuclear Beams (RNB6). Vol. 746. ; 2004. pp. 54–60.Abstract
The regions around the doubly magic nuclei 100Sn and 78Ni are of great interest from a nuclear structure standpoint. These nuclei also play a key role in the astrophysical rp- and r-processes, respectively. Recently, nuclei in these regions were studied at the Coupled Cyclotron Facility at the National Superconducting Cyclotron Laboratory (NSCL) at Michigan State University.
Stuchbery AE, Benczer-Koller N, Kumbartzki G, Mertzimekis TJ. Gyromagnetic ratios and octupole collectivity in the structure of the $^{90-96}Zr isotopes. Phys. Rev. C. 2004;69:044302–1.Abstract
Shell model calculations have been performed for low-excitation states in the Zr isotopes between 90Zr and 96Zr with an emphasis on the g factors and electromagnetic decay rates for the lowest 2+ and 3- states. Overall the 2+ states are reasonably well described. In contrast, the 3- states present a puzzle because the measured g factors imply a single-particle configuration whereas the experimental E3 transition rates imply collective structures that cannot be explained by shell model calculations. A consistent description of the 3 - states in 90Zr and 96Zr is sought in terms of coupling between the single-particle structure and a collective octupole vibration.
Walters WB, Tomlin BE, Mantica PF, Brown BA, Rikovska Stone J, Davies AD, Estrade A, Hosmer PT, Hoteling N, Liddick SN, et al. Probing the sustainability of the N=82 and Z=50 shell closures for neutron-rich nuclides: Decay of $^{120}$Rh$^{75}$ to levels of $^{120}$Pd$^{74}$. Phys. Rev. C. 2004;70:0343141–0343145.Abstract
The low-energy levels of 120Pd74 were populated by ? decay of 120Rh75, which was produced via projectile fragmentation of a 136Xe82 beam at 120 MeV/nucleon. Delayed ?-gated ? rays with energies of 438 and 618 keV were observed in coincidence with 120Rh75 fragments and assigned to the 21+ ? 0+ and 41+ ? 21+ transitions, respectively, in 120Pd74. Isomeric ?-ray transitions are also reported for 120Rh75 and 126Cd78. The low-energy structure of 120Pd74 shows remarkable similarity to those of the isotopic 108Pd62 and isotonic 128Xe74 suggesting that these nuclides share the same Z=50 and N=82 closed shell structures with neutron-rich 120Pd 74.
Kumbartzki G, Cooper JR, Benczer-Koller N, Hiles K, Mertzimekis TJ, Taylor MJ, Speidel K-H, Maier-Komor P, Bernstein L, McMahan MA, et al. First g factor measurement using a radioactive $^{76}$Kr beam. Phys. Lett. B. 2004;591:213–219.Abstract
The g factor of the first 2+ state of radioactive 76Kr (T1/2=14.8 h) has been measured, extending the systematics of the previously measured stable 78,80,82,84,86Kr isotopes. The measurement was performed with a radioactive 76Kr ion beam applying projectile Coulomb excitation in inverse kinematics combined with the transient magnetic field technique. The 76Kr beam was produced and accelerated in batch mode (re-cyclotron method) at the Lawrence Berkeley National Laboratory 88-Inch Cyclotron. A total of three production and acceleration cycles yielded six hours of beam on target with peak rates of 108 particles/s. About 5.6×104 particle-? coincidence events were recorded. The g factor g(76Kr;2 +1)=+0.37(11) was obtained by direct comparison to the known g(78Kr;2+1) value re-measured immediately after the 76Kr runs with the same setup and under almost identical kinematic conditions. © 2004 Elsevier B.V. All rights reserved.
Benczer‐Koller N, Kumbartzki G, Mertzimekis TJ, Sharon YY, Speidel K ‐H, Taylor MJ, Zamick L. Stuart Pittel and the f$_{7/2}$ Shell Revisited: Magnetic Moments in the Ca Isotopes. In: AIP Conference Proceedings. Vol. 726. ; 2004. pp. 81-86.
Cooper JR, Bernstein L, McMahan MA, Powell J, Wutte D, Ahle L, Benczer-Koller N, Dashdorj D, Kumbartzki G, Mertzimekis TJ, et al. Production of a $^{76}$Kr radioactive ion beam using a batch mode method. Nucl. Instrum. Meth. Phys. Res. A. 2004;533:287–294.Abstract
A batch mode process has been developed to produce a 76Kr (T1/2 = 14.8 h) radioactive ion beam at the Lawrence Berkeley National Laboratory 88-in. Cyclotron. First, a 6 particle ?A ? beam is run for 17 h to produce approximately 101476Kr atoms via the reaction 74Se(?, 2n)76Kr. Then, the krypton is separated from the target material and injected into the AECR-U ion source. Beam intensities as high as 3 × 108 particles per second are observed with an integrated beam current of 6(2) × 1011 particles per 24-h batch cycle. © 2004 Published by Elsevier B.V.
Benczer-Koller N, Kumbartzki G, Hiles K, Cooper JR, Bernstein L, Ahle L, Schiller A, Mertzimekis TJ, Taylor MJ, McMahan MA, et al. First Measurement of a Magnetic Moment of a Short-Lived State with an Accelerated Radioactive Beam: $^{76}$Kr. In: Covello A "Key Topics in Nuclear Structure", Proceedings of the 8th International Spring Seminar on Nuclear Physics, Paestum, Italy, May 23-27. World Scientific, Singapore; 2004. pp. 63.