Experimental and theoretical investigations of quadrupole collective degrees of freedom in 104Ru

Srebrny, J.; Czosnyka, T.; Droste, Ch.; Rohoziński, S. G.; Próchniak, L.; Zaja̧c, K.; Pomorski, K.; Cline, D.; Wu, C. Y.; Bäcklin, A.; Hasselgren, L.; Diamond, R.M.; Habs, D.; Körner, H. J.; Stephens, F. S.; Baktash, C.; Kostecki, Ryszard Paweł

doi:10.1016/j.nuclphysa.2005.11.013

Cited by 77 publications

(98 citation statements)

References 23 publications

Supporting

Mentioning

Contrasting

Order By: Relevance

“…Let us remark that the quasi-γ band systematics can only be reproduced by including the three-boson term in the IBM Hamiltonian [33]. The previous results compare well with the ones obtained using the 5D collective Hamiltonian approach, based on the deformed Nilsson potential and the Strutinsky's shell correction [67]. …”

supporting

confidence: 76%

Structural evolution inA≈100nuclei within the mapped interacting boson model based on the Gogny energy density functional

2016

View full text Add to dashboard Cite

The structure of even-even neutron-rich Ru, Mo, Zr and Sr nuclei in the A ≈ 100 mass region is studied within the interacting boson model (IBM) with microscopic input from the self-consistent mean-field approximation based on the Gogny-D1M energy density functional. The deformation energy surface in the quadrupole deformation space (β, γ), computed within the constrained HartreeFock-Bogoliubov framework, is mapped onto the expectation value of the appropriately chosen IBM Hamiltonian with configuration mixing in the boson condensate state. The mapped IBM Hamiltonian is used to study the spectroscopic properties of 98−114 Ru, 96−112 Mo, 94−110 Zr and 92−108 Sr. Several cases of γ-soft behavior are predicted in Ru and Mo nuclei while a pronounced coexistence between strongly-prolate and weakly-oblate deformed shapes is found for Zr and Sr nuclei. The method describes well the evolution of experimental yrast and non-yrast states as well as selected B(E2) transition probabilities.

show abstract

supporting

confidence: 76%

Structural evolution inA≈100nuclei within the mapped interacting boson model based on the Gogny energy density functional

2016

View full text Add to dashboard Cite

show abstract

“…In the same way one obtains for the coupling of three operators analogous to invariant P (3) s of equation (4) [81,94]:…”

Section: B Recent Analyses Methods: Cline-flaum Approachmentioning

confidence: 82%

“…An extensive study has been carried out by Srebrny et al [94] describing deformed nuclei by a Nilsson ellipsoidal deformed potential [106][107][108], equating the experimental (or theoretical, as derived from our present LSSM calculations) P …”

Section: B Recent Analyses Methods: Cline-flaum Approachmentioning

confidence: 99%

“…These methods have been used in a large number of recent papers (in particular in the region of the Ge, Kr, Mo, Ru and Pd nuclei [90][91][92][93][94][95], as well as in the much heavier Pb mass region (W, Os, Pt, Hg, Po isotopes) [96][97][98][99][100][101].…”

Section: Shape Invariantsmentioning

confidence: 99%

“…The only other possible particle distribution producing positive parity states is, when the two proton holes are placed in the 2p 1/2 orbital, making up for a 0 Using the concept that most nuclei exhibit some softness and, consequently, exhibit a tendency for deformation (be it static as for strongly deformed nuclei, or, in a dynamic way for soft nuclei in transitional regions and near to closed shells), any excited state is prone to be described using collective modes of motion (rotation, shape oscillations), implying that a nuclear shape is not a net "observable". Although the magnitude of the overall nuclear deformation β remains a well defined variable, the uncertainty in the nuclear shape γ (which can be quantified by calculating the variance, defined as σ( Q 3 ) ≡ Q 6 − ( Q 3 ) 2 (see also references [81,94,97])) is in general increasing with the increasing nuclear spin. Thus we do not consider γ values of other states than 0 + 1 , though they could in principle be calculated from the shell-model results.…”

Section: Deformation Analysismentioning

confidence: 99%

See 2 more Smart Citations

Shell-model-based deformation analysis of light cadmium isotopes

et al. 2017

View full text Add to dashboard Cite

Large-scale shell-model calculations for the even-even Cadmium isotopes 98 Cd -108 Cd have been performed with the ANTOINE code in the π(2p 1/2 ; 1g 9/2 ) ν(2d 5/2 ; 3s 1/2 ; 2d 3/2 ; 1g 7/2 ; 1h 11/2 ) model space without further truncation. Known experimental energy levels and B(E2) values could be well reproduced. Taking these calculations as a starting ground we analyze the deformation parameters predicted for the Cd isotopes as a function of neutron number N and spin J using the methods of model independent invariants introduced by K. Kumar and D. Cline.

show abstract

Weakly Deformed Systems with Triaxial Dynamics

Nomura

2013

Springer Theses

View full text Add to dashboard Cite

Experimental and theoretical investigations of quadrupole collective degrees of freedom in 104Ru

Cited by 77 publications

References 23 publications

Structural evolution inA≈100nuclei within the mapped interacting boson model based on the Gogny energy density functional

Structural evolution inA≈100nuclei within the mapped interacting boson model based on the Gogny energy density functional

Shell-model-based deformation analysis of light cadmium isotopes

Weakly Deformed Systems with Triaxial Dynamics

Contact Info

Product

Resources

About