1975
DOI: 10.1016/0375-9474(75)91136-7
|View full text |Cite
|
Sign up to set email alerts
|

Potential-energy surfaces for the doubly even N = Z nuclei

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
2

Citation Types

4
81
0

Year Published

1988
1988
2007
2007

Publication Types

Select...
5
3

Relationship

0
8

Authors

Journals

citations
Cited by 209 publications
(90 citation statements)
references
References 26 publications
4
81
0
Order By: Relevance
“…As it is well known that the 0 + 2 state in 12 C (Hoyle state) has an excitation energy of 7.65 MeV and there is no evidence of low laying 0 + level at 3 MeV. Anywhere calculation predict for this nucleus an oblate ground state and prolate excited state [11] in agreement with our results. In 16 O the predicted level possible has the same energy as 2 − (8.87 MeV) state.…”
Section: Model Of Binding α-Particlessupporting
confidence: 91%
See 2 more Smart Citations
“…As it is well known that the 0 + 2 state in 12 C (Hoyle state) has an excitation energy of 7.65 MeV and there is no evidence of low laying 0 + level at 3 MeV. Anywhere calculation predict for this nucleus an oblate ground state and prolate excited state [11] in agreement with our results. In 16 O the predicted level possible has the same energy as 2 − (8.87 MeV) state.…”
Section: Model Of Binding α-Particlessupporting
confidence: 91%
“…Like for 24 Mg rotational band in [14] we can consider the potential-energy surface for 20 Ne. We can see [11] that really there are some minima in this potential surface and one of these have strong prolate deformation (see Fig. 4).…”
Section: Model Of Binding α-Particlesmentioning
confidence: 86%
See 1 more Smart Citation
“…It should be noted here that, although extensive theoretical calculations and rich experimental evidences have been accumulated for axially symmetric octupole (Y 30 ) deformations, as reviewed in [36,37], only a few calculations using WoodsSaxon Strutinsky methods are available [38][39][40][41] except for light nuclei, and no firm experimental evidence exists up to now concerning the non-axial octupole (Y 31 , Y 32 , Y 33 ) deformations in the mean fields. For light nuclei, non-axial octupole deformations have been discussed [42][43][44][45][46] in connection with alpha-cluster structures [47]; for instance, a triangular structure of 12 C [42,44] and a tetrahedral shape for 16 O [45, 46].…”
Section: Introductionmentioning
confidence: 99%
“…In particular, in collisions between two 12 C nuclei, these resonances have been interpreted in terms of nuclear molecules [ 1]. However, in many cases these structures have been connected to strongly deformed shapes and to the clustering phenomena, predicted from the α-cluster model [ 2], Hartree-Fock calculations [ 3], and the Nilsson-Strutinsky approach [ 4]. The question whether these molecular resonances represent true cluster states in the 24 Mg compound system, or whether they simply reflect scattering states in the ion-ion potential is still unresolved.…”
Section: Introductionmentioning
confidence: 99%