High-spin level structure of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msup><mml:mrow /><mml:mn>35</mml:mn></mml:msup><mml:mi>S</mml:mi></mml:math>

Aydin, S.; Ionescu‐Bujor, M.; Recchia, F.; Lenzi, S. M.; Bazzacco, D.; Bizzeti, P. G.; Bizzeti‐Sona, A. M.; Angelis, G. de; Deloncle, I.; Farnea, E.; Gadea, A.; Gottardo, A.; Haas, F.; Hüyük, T.; Laftchiev, H.; Lunardi, S.; Mengoni, D.; Menegazzo, R.; Michelagnoli, C.; Napoli, D. R.; Poves, A.; Şahin, E.; Singh, Pardeep; Tonev, D.; Ur, C. A.; Valiente-Dobón, J.J.

doi:10.1103/physrevc.89.014310

Cited by 15 publications

(23 citation statements)

References 40 publications

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“…The [2,1] configurations in 34 S are similar to the [1,1] ones in 32 S; they are SD at low spin but lose the collectivity with increasing spin so that they are better described as highly-deformed at the highest calculated spins (Fig. 31).…”

Section: S Nucleusmentioning

confidence: 73%

“…Third, in experiment the high spin structures in this mass region are better populated in the N ∼ Z nuclei. Note also that at present high spin studies are quite active in this mass region [30,[32][33][34][35].…”

Section: Introductionmentioning

confidence: 89%

“…The general features of rotational spectra along the yrast line are discussed in Sec. V. Section VI is devoted to the discussion of the appearance of super-, hyper-and megadeformed configurations along the yrast line of the 32,34 …”

Section: Introductionmentioning

confidence: 99%

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From superdeformation to extreme deformation and clusterization in theN≈Znuclei of theA≈40mass region

Ray¹,

Afanasjev²

2016

Phys. Rev. C

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From superdeformation to extreme deformation and clusterization in the N ∼ Z nuclei of the A ∼ 40 mass region. A systematic search for extremely deformed structures in the N ∼ Z nuclei of the A ∼ 40 mass region has been performed for the first time in the framework of covariant density functional theory. At spin zero such structures are located at high excitation energies which prevents their experimental observation. The rotation acts as a tool to bring these exotic shapes to the yrast line or its vicinity so that their observation could become possible with future generation of γ−tracking (or similar) detectors such as GRETA and AGATA. The major physical observables of such structures (such as transition quadrupole moments as well as kinematic and dynamic moments of inertia), the underlying single-particle structure and the spins at which they become yrast or near yrast are defined. The search for the fingerprints of clusterization and molecular structures is performed and the configurations with such features are discussed. The best candidates for observation of extremely deformed structures are identified. For several nuclei in this study (such as 36 Ar), the addition of several spin units above currently measured maximum spin of 16 will inevitably trigger the transition to hyper-and megadeformed nuclear shapes.

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Section: S Nucleusmentioning

confidence: 73%

Section: Introductionmentioning

confidence: 89%

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From superdeformation to extreme deformation and clusterization in theN≈Znuclei of theA≈40mass region

Ray¹,

Afanasjev²

2016

Phys. Rev. C

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show abstract

“…The overlap of the SRIM calculated stopping powers with the measured values, for heavy-ions, is presently quoted around 5% with 69% of the data within 5% of the TRIM calculated value and 86% within 10% [7]. This is significantly better than the stopping powers calculated using the models of Ziegler [10] and Northcliffe-Schilling [11], used in the conventional LINESHAPE program, that can have uncertainty as high as 15-20% [20,21].…”

Section: Programming and Methodologymentioning

confidence: 99%

“…The current methodology was first used for analysis of data acquired with thick elemental target that is presumably a simpler medium for stopping simula- An uncertainty of 5% on the stopping power has been included for the TRIM results while that in the results obtained using the Ziegler and the Northcliffe-Schilling models has been assigned to be 15% [20,21]. = 34 MeV, with a thick (∼ 200 mg/cm 2 ) elemental 27 Al foil as the target and 16 O beam provided by the 15UD Pelletron at the Inter University Accelerator Center (IUAC), New Delhi.…”

Section: Thick Elemental Targetmentioning

confidence: 99%