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Fission studies with ²⁵²Cf half-lives of excited states, isomeric structures in ¹¹³,¹¹⁵,¹¹⁷Pd, and neutron multiplicites /Fong, Dennis Ji-Bin. January 2005 (has links)
Thesis (Ph. D. in Physics)--Vanderbilt University, May 2005. / Title from title screen. Includes bibliographical references.
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Nuclear structure of 86Zr and 20O and beam pulsing techniquesWiedeking, Mathis. Tabor, Samuel L. Wiedenhoever, Ingo L. January 2004 (has links)
Thesis (Ph. D.)--Florida State University, 2004. / Advisor: Dr. Samuel L. Tabor and Dr. Ingo L. Wiedenhoever, Florida State University, College of Arts and Sciences, Dept. of Physics. Title and description from dissertation home page (viewed June 6, 2005). Document formatted into pages; contains xv, 143 pages. Includes bibliographical references (p. 138-142).
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Some problems in the theory of nuclear structureRoetter, Martyn F. January 1967 (has links)
No description available.
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Study of Excited Superdeformed Bands in 154Dy and High-spin Spectroscopy of 171HfIjaz, Qurant Ul Ann 09 December 2011 (has links)
The first project in this dissertation involves the search for and the study of excited superdeformed (SD) rotational bands in 154Dy. The data was obtained from an experiment at the 88-inch cyclotron of the Lawrence Berkeley National Laboratory via the fusion evaporation reaction 122Sn(36S, 4n) and using the Gammasphere spectrometer array to probe the high-spin states in 154Dy. With the help of large Compton-suppressed spectrometers such as GAMMASPHERE in the USA and EUROBALL in Europe, superdeformed nuclei have been identified in several regions of the chart of nuclides including 151Dy, 153Dy, 154Dy and 155Dy. The 154Dy nucleus, located in the center of A= 150 SD island, plays an important role in the study in this region. Only the lowest (yrast) SD band in 154Dy was known before this study. Three or four fold coincidence analysis was performed employing the conventional gating method as well as an automatic search routine. As the result, five excited SD bands were identified with intensities between 0.7 - 0.03 % of total reaction channel. Theoretical analysis based on Cranked Relativistic Mean Field calculations (CRMF) and the effective alignment method were carried out. The second project includes the spectroscopy of high-spin states in Hf nuclei, which were populated in another Gammasphere experiment using 128Te(48Ca, 5n) and 128Te(48Ca, 4n) reactions to obtain 171Hf and 172Hf, respectively. Three SD bands in 172Hf and one band with enhanced deformation (ED) in 171Hf have been extracted and published by our group. Subsequently, a complete highspin spectroscopy in 171Hf has been further carried out in which five new rotational bands have been identified. Their rotational properties, including spins, parities, excitation energies, aligned angular momentum and quasiparticle configurations were investigated within the framework of the cranked shell model, aided by a comparison with level structures in neighboring nuclei. The band crossings at very high rotational frequency (500 keV) are interpreted as the proton alignments. One band has been suggested to be associated with enhanced deformation based on the i13/2h9/2 proton orbitals and h9/2 neutron orbital. However, its decay pathways to known low-spin states could not be established.
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Nuclear structure near lg92 shell closureHuang, Haw. January 1978 (has links)
No description available.
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Octupole correlations in '2'2'5ThHughes, John Rhys January 1989 (has links)
No description available.
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Discrete gamma-ray spectroscopy of the N=90 isotones '1'5'4Gd and '1'5'6DyMorrison, J. D. January 1988 (has links)
No description available.
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Characterisation of the first 1/2+ excited state in 9B and isospin symmetry breaking studies in A = 9 nucleiMukwevho, Ndinannyi Justice January 2019 (has links)
>Magister Scientiae - MSc / The 9Be - 9B isospin doublet carries fundamental significance for both nuclear structure and nuclear astrophysics studies. The first excited 1/2+ state in 9Be is already well established. However, its isobaric analogue 1/2+ state in 9B has not been unambigously determined yet. Theoretically, two popular descriptions of the 9Bnucleus either use a cluster model with two unbound alpha particles held together by a covalent proton or using the shell model, as a 8Be core + proton in the sd shell. An experimental determination of the excitation energy of the first 1/2+ state in 9B will provide valuable information in validating the theoretical model that adequately describes such light unbound nuclei. Further, it will also provide a robust test of mirror (isospin) symmetry violations via measurements of mirror energy differences in the doublet. Although there have been several experimental attempts to characterize the first 1/2+ state in 9B several discrepancies still exist in reported values of the excitation energies. This thesis describes an experiment performed at iThemba LABS using the 9Be(3He,t)9B reaction to address the above issue. As a byproduct, the thesis also describes an additional determination of the excitation energy of the second J-pi = 1/2+, T = 3/2 state in 9B from the same experiment. This was performed in order to resolve a discrepancy related to the excitation energy of this state. The consequence of this measurement related to Isobaric Multiplet Mass Equation (IMME) for the excited T = 3/2, A = 9 quartet is discussed briefly.
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Level structure of ¹⁵²Gd populated in ¹⁵²Tb β decayStapels, Christopher John 20 September 2004 (has links)
As part of a research program to study the transitional region of N=88
isotones, ¹⁵²Tb was produced by the reaction ¹⁵¹Eu(α,3n)¹⁵²Tb in the 88" cyclotron
located at LBNL. Gamma-ray spectroscopy of the radiation emitted from excited
¹⁵²Gd following the β⁺ decay of ¹⁵²Tb has been performed using an array of 20
germanium detectors. The large Q-value (3990 keV) of the ¹⁵²Tb 2⁻ decay allows for
the population of many levels; study of coincidence and single events resulted in the
establishment of 54 new levels and 266 new transitions. Angular correlation of the
coincidences has determined spin and parity of many levels with several seen as key to
the band structure, including two new 0⁺ levels. One new rotational band including
the new 1475.2 keV 0⁺ level and the 1771.7 keV 2⁺ level is proposed. The overall
band structure compared to collective excitation models demonstrates the position of
¹⁵²Gd in the transition from a spherical to deformed shape, also seen in other N=88
isotones. Monopole transition strength among bands indicates the possibility of
mixing of both shapes among the excited states. The remarkable similarity of the band
structure among these isotones is discussed. / Graduation date: 2005
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Promyelocytic Leukemia Nuclear Bodies: A Meeting Place For Genomic LociChing, Reagan Wai Kit 15 November 2013 (has links)
The nucleus is a highly compartmentalized organelle where specific cellular activities are confined to discrete domains. One such domain is the promyelocytic leukemia nuclear body (PML NB). PML NBs are protein-based structures that make numerous contacts with neighboring chromatin domains. To elucidate the function of PML NBs, research has been focused on identifying the protein complement of PML NBs. More than 60 proteins have been shown to localize to PML NBs, implicating the bodies in numerous cellular activities such as transcription regulation, apoptosis, tumor suppression, and the antiviral response. This approach has not yielded a general model for PML NB function. Instead I have chosen to focus on the chromatin contacts made with PML NBs. Using live-cell microscopy, my observations support the hypothesis that changes in chromatin topology affect the structural integrity of PML NBs. Moreover, I have developed a technique, called immunoTRAP, which allows for the extraction of chromatin specifically associated with PML NBs. Analysis of these chromatin associations reveal that specific genes associate with PML NBs and these associations are cell type specific. Therefore, PML NBs make specific contacts with neighboring chromatin domains and these contacts are integral to PML NB morphology. Thus making PML NBs a meeting place for a specific set of genomic loci.
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