November 2023
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Publications (467)
March 2013
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14 Reads
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1 Citation
In rotating nuclei, backbending appears to be a large increase in the moment of inertia of a band, accompanied by a decrease in the rotational frequency. This has been shown to be a band crossing where one band (e.g. the ground or vacuum band) is crossed by a band in which the Coriolis force has unpaired two high-j nucleons and aligned their angular momentum with the rotation axis of the nucleus. With increasing spin this force gradually quenches the nuclear pairing correlations, with one or two of these band crossings in the process. © 2013 by World Scientific Publishing Co. Pte. Ltd. All rights reserved.
December 2012
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25 Reads
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8 Citations
Physical Review C
Over a period of several years we have performed three separate experiments at Lawrence Berkeley National Laboratory's 88-Inch Cyclotron in which 235U (thick target) was Coulomb-excited. The program involved stand-alone experiments with Gammmasphere and with the 8pi Spectrometer using 136Xe beams at 720 MeV, and a CHICO-Gammasphere experiment with a 40Ca beam at 184 MeV. In addition to extending the known negative-parity bands to high spin, we have assigned levels in some seven positive-parity bands which are in some cases (e.g., [631]1/2, [624]7/2, and [622]5/2) strongly populated by E3 excitation. The CHICO data have been analyzed to extract E2 and E3 matrix elements from the observed yields. Additionally, many M1 matrix elements could be extracted from the γ-ray branching ratios. A number of new features have emerged, including the unexpected attenuation of magnetic transitions between states of the same Nilsson multiplet, the breakdown of Coriolis staggering at high spin, and the effect of E3 collectivity on Coriolis interactions.
September 2011
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81 Reads
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2 Citations
Journal of Physics Conference Series
Recently it has become possible to perform detailed spectroscopy on nuclei beyond Z = 100 with the aim of understanding the underlying single-particle structure of superheavy elements. A number of such experiments have been performed at the 88-Inch Cyclotron of the Lawrence Berkeley National Laboratory using the Berkeley Gas-filled Separator (BGS), coupled with delayed γ-ray and electron-decay spectroscopy. Experiments have been performed on 254No (Z = 102), 257Rf (Z = 104), and 261Sg (Z = 106). The results provide new information on the properties of transactinide nuclei, which is important for testing models of the heaviest elements.
June 2010
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51 Reads
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70 Citations
Physics Letters B
We report results from an experiment on the decay of the high-K isomers in 254No. We have been able to establish the decay from the known high-lying four-quasiparticle isomer, which we assign as a Kπ=16+ state at an excitation energy of Ex=2.928(3) MeV. The decay of this state passes through a rotational band based on a previously unobserved state at Ex=2.012(2) MeV, which we suggest is based on a two-quasineutron configuration with Kπ=10+. This state in turn decays to a rotational band based on the known Kπ=8− isomer, which we infer must also have a two quasineutron configuration. We are able to assign many new gamma-rays associated with the decay of the Kπ=8− isomer, including the identification of a highly K-forbidden ΔK=8 E1 transition to the ground-state band. These results provide valuable new information on the orbitals close to the Fermi surface, pairing correlations, deformation and rotational response, and K-conservation in nuclei of the deformed trans-fermium region.
September 2009
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33 Reads
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33 Citations
Physical Review C
Two isomeric states have been identified in 255Lr. The decay of the isomers populates rotational structures. Comparison with macroscopic-microscopic calculations suggests that the lowest observed sequence is built upon the [624]9/2+ Nilsson state. However, microscopic cranked relativistic Hartree-Bogoliubov (CRHB) calculations do not reproduce the moment of inertia within typical accuracy. This is a clear challenge to theories describing the heaviest elements.
February 2009
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28 Reads
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55 Citations
Physical Review C
Excited states in Rf256 were populated via the Pb208(Ti50,2n) fusion-evaporation reaction. Delayed γ-ray and electron decay spectroscopy was performed and three isomeric states in Rf256 have been identified. A fourth low-energy nonyrast state was identified from the γ-ray decay of one of the higher lying isomers. The states are interpreted as multi-quasiparticle excitations.
January 2009
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9 Reads
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7 Citations
October 2008
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6 Reads
New techniques in the use of highly-segmented HPGe detectors enable the tracking of the path of a scattered gamma ray in the detector. This enables precision Doppler correction of gamma rays emitted from fast-moving sources for high-resolution spectroscopy at radioactive beam facilities. Critical to these applications is a knowledge of the position resolution to which the scattering points can be determined. We directly measured the position resolution of using a highly collimated Cs source. Signal decomposition was used to determine the position and charge deposition of the interaction points from the scattered gamma ray in the crystal, followed by tracking to identify the first interaction point. The set of first interaction points form a line through the detector and their dispersion gives the position resolution of the crystal in two dimensions. Such a measurement was performed with the 36-way segmented GRETINA P3 prototype detector the position resolution was found to be sigmax = 1.5 mm and sigmay = 1.7 mm.
September 2008
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20 Reads
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19 Citations
Physical Review C
The structure of the neutron-rich N=20 nucleus 35P has been investigated through nucleon transfer experiments using the 208Pb(36,Xγ) reaction at 230 MeV. The level structure, of mainly 1ℏω excitations in 35P, has been significantly expanded. The measurements are compared with shell model calculations. Experimental branching ratio limits are reported for predicted transitions to the 2ℏω bandheads in 35P and 34Si.
Citations (49)
... U is generally renormalized to U −2∆ p , where 2∆ p , known as the backshift parameter, takes the pairing interaction into account. Recently, however, detailed analyses [153,172] have suggested that the magnitude of ∆ p should be much smaller than usually used, or neglected entirely. This, then, is an additional factor which adds uncertainty to current knowledge of Γ N . ...
- Citing Article
March 2000
... Zirkonyum diborür (ZrB 2 ), pota ve termokupl astarı yapımında, alüminyum elektrolizinde katot kaplamasında, kesme ve aşındırma takımlarında, hipersonik uçakların ve roket atış sistemlerinin termal korumasında, nozullarda, zırh uygulamalarında ve nükleer reaktörlerde durdurucu olarak kullanılmakta veya kullanıma aday görülmektedir [3][4][5]. Ayrıca zirkonyum diborürün süperiletkenlik davranışları literatürde incelenmiş ve güncel olarak da incelenmeye devam etmektedir [6][7]. Çeşitli oksit ya da karbür katkıları ile geliştirilen zirkonyum borür esaslı kompozit malzemeler (ZrB 2 -ZrC, ZrB 2 -ZrO 2 , ZrB 2 -SiC, ZrB 2 -SiO 2 , ZrB 2 -B 4 C, vb.) mükemmel fiziksel ve mekanik özellikler göstermektedirler [8]. ...
- Citing Article
December 2012
Physical Review C
... Numerous studies were performed within the surrogate approach [23,[25][26][27][28][29][30][31] yielding encouraging results in a few particular cases: neutron capture, fission, and, recently, also the (n, p) channel [32]. The surrogate method generates the nucleus of interest that undergoes fission or γ decay through a direct reaction induced by a high-energy charged particle. ...
- Citing Article
May 2006
Physical Review C
... The rotational band resulting from this mechanism possesses increasing B(M1)/B(E 2) ratio, and decreasing B(M1) value with increasing rotational frequency. While the presence of the MR band is a very common phenomenon around the neutron-deficient Pb region [5][6][7], the observation of the MR band [8][9][10][11] in the above Pb region (Z = 82) around N = 126 neutron shell closure is rare due to insufficient experimental data at the high spin. The presence of the MR band in this region has already been reported for 203,204 At (Z = 85) [12,13], 202 Bi (Z = 83) [14], 201,202 Pb (Z = 82) [15], and 206 Fr (Z = 87) [16]. ...
Reference:
High-spin level structure of 209Rn
- Citing Article
February 2001
Nuclear Physics A
... It has been demonstrated that the additional spectral line widening due to charge trapping depends not only on CCE but also on the electronic and Fano noises, so that higher causes a higher excess line widening for the same CCE [55]. Effects of charge trapping have been observed both in detectors made with compound semiconductors as with germanium and silicon, due to several different causes as: significant defect or impurity density both native as due to radiation damage, presence of volumes with low electric field [56][57][58][59][60][61][62] ...
- Citing Article
June 2005
Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment
... Most tracking algorithms attempt to reconstruct the tracks of photons, which have been fully absorbed in the Ge detectors (there is the notable exception of the TANGO algorithm [9], which also identifies Compton escape events, see section 4). There are two categories of tracking algorithms: forward-tracking algorithms [10], which start from the known position of the source and reconstruct the track of photons as they interact in the detector and back-tracking algorithms [11], which start from the potential photoelectric interaction point and reconstruct the track backwards to the source. Forward-tracking algorithms have been demonstrated to be more efficient than back-tracking algorithms [12] and are therefore used both at AGATA [1] and GRETINA [13]. ...
- Citing Article
June 1999
Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment
... Several other candidates have been suggested, reviewed in Refs. [347,356,464], with relevant references given in the caption of Figure 2. ...
- Citing Article
September 2003
Physical Review C
... As the mass number increases in these Pd nuclei, the deformation is expected to gradually change toward an oblate shape beyond 111 Pd [3]. However, past experiments have shown that the yrast structures in 113,115,117 Pd nuclei correspond to rotational bands arising from a prolate deformation [4][5][6]. The present experiment investigates these bands with very high statistics data to better determine the energy levels of odd-A Pd nuclei in this region. ...
- Citing Article
August 1999
Physical Review C
... The energy-level staggering in γ-bands in the chain of the Pd isotopes was analyzed in Ref. [7]. The levels of the γ-bands in 108 Pd [7], 110 Pd [7], 112 Pd [8] are grouped as 2 + , (3 + ,4 + ), (5 + ,6 + ) and etc., which is consistent with γ-soft behavior accordingly to the model of Wilets and Jean [9]. While the γ-bands are not so well developed in 102,104,106 Pd as in the heavier Pd isotopes, the amplitude of the staggering effect decreases in 114 Pd and 116 Pd with respect to that in 108,110,112 Pd, where it reaches its maximum [7]. ...
- Citing Article
February 2001
European Physical Journal A
... Custom readout electronics provided amplified, differential pulses from the HPGe detector charge collection process [29]. These signals were recorded by digitizers developed for the GRETINA experiment [30,31] which were read out using the Object-oriented Real-time Control and Acquisition (ORCA) software package [32][33][34]. ...
- Citing Article
December 2004
Nuclear Physics A