M. Waroquier

The U(5) → O(6) transition in the U(612) supersymmetry scheme and its application to the odd-A Rh isotopes

P. Van Isacker, J. Jolie, K. Heyde, M. Waroquier, J. Moreau, O. Scholten
Physics Letters B
149 (1-3), 26-30
1984
A1
Published while none of the authors were employed at the CMM

Abstract 

We discuss the U(5) → O(6) transition in the supersymmetry scheme of the interacting boson model. An application to the odd-A Rh isotopes is presented and includes a discussion of energy spectra, one-nucleon transfer properties and E2 transition rates.

M1 transition strengths in the neutron-proton interacting boson model

P. Van Isacker, K. Heyde, J. Jolie, M. Waroquier, J. Moreau, O. Scholten
Physics Letters B
144 (1-2), 1-4
1984
A1
Published while none of the authors were employed at the CMM

Abstract 

We study the U(5), SU(3), SU∗(3) and O(6) limits of the neutron-proton interacting boson model. A group theoretical interpretation of the Majorana term is discussed. The B(M1;01+→11+) values are calculated in the four limits and in differen t classes of translational nuclei.

An effective Skyrme-type interaction for nuclear structure calculations: (I). Ground-state properties

M. Waroquier, K. Heyde, G. Wenes
Nuclear Physics A
404 (2), 269-297
1983
A1
Published while none of the authors were employed at the CMM

Abstract 

A “universal” effective NN interaction of the Skyrme type has been proposed which is suitable for both ground and excited states in nuclei throughout the nuclear mass table. The analytical structure of the proposed interaction SkE is presented and discussed. The spin stability of the force is studied by deriving the corresponding Landau-Migdal interaction for uniform nuclear matter. An equivalent set of force parameters starting from a realistic interaction after application of the local-density approximation (LDA) and the density-matrix expansion (DME) is derived. The behavior of the SkE interaction in describing charge properties is extensively discussed by carrying out a detailed and elaborate study of nucleon and charge distributions in 58Ni, the Ca and Pb isotopes.

An effective Skyrme-type interaction for nuclear structure calculations: (II). Excited-state properties

M. Waroquier, G. Wenes, K. Heyde
Nuclear Physics A
404 (2), 298-332
1983
A1
Published while none of the authors were employed at the CMM

Abstract 

A universal effective NN interaction SkE of the Skyrme type has been proposed, suitable for both ground and excited states in nuclei throughout the nuclear mass table. In this second part (II) the behaviour of the SkE force as a particle-particle and particle-hole effective interaction is studied. We show the ability of SkE to reproduce all two-particle (two-hole) valence nucleon spectra. A detailed study for 18O and 130Sn is carried out. The definitely determined SkE interaction is also applied as a particle-hole interaction and detailed shell-model calculations for the light 16O and heavy 208Pb nuclei are discussed. We also concentrate on the description of giant multipole resonances throughout the whole nuclear mass region.

Structure of the energy levels of 53, 55, 57Mn from the (d, 3He) reaction on iron isotopes at 80 MeV

N.G. Puttaswamy, W. Oelert, A. Djaloeis, C. Mayer-Böricke, P. Turek, P.W.M. Glaudemans, B.C. Metsch, K. Heyde, M. Waroquier, P. Van Isacker, G. Wenes, V. Lopac, V. Paar
Nuclear Physics A
401 (2), 269-302
1983
A1
Published while none of the authors were employed at the CMM

g-boson excitations in the interacting boson model

K. Heyde, P. Van Isacker, M. Waroquier, G. Wenes, Y. Gigase, J. Stachel
Nuclear Physics A
398 (2), 235-252
1983
A1
Published while none of the authors were employed at the CMM

Abstract 

We have extended the interacting boson model (IBM) by including the g-boson degree of freedom. Schematic model calculations have been carried out in the two different limits: SU(5) and O(6). Particular applications have been carried out for 104Ru, a nucleus intermediate between SU(5) and O(6). In all cases, energy spectra, E2 and E4 transition rates have been studied in detail and compared with the most recent experimental data for 104Ru.

Nuclear temperature effects in the scission-point model of nuclear fission

J. Moreau, K. Heyde, M. Waroquier
Physical Review C
28 (4), 1640-1647
1983
A1
Published while none of the authors were employed at the CMM

Abstract 

According to the scission-point model, the probability for a particular fission event can be expressed in terms of the collective potential and the collective kinetic energy at the scission point. Two additional assumptions make the scission-point model an easily calculable model: the assumption of equal collective kinetic energies for constant distances d between the tips of the fragments, and the assumption that one is able to characterize the excitation energy of the fragments with a nuclear temperature T, independent of both the mass ratio and the charge ratio, and of the deformations of the fragments. It is pointed out that the latter assumption violates energy conservation. A modified, recursive procedure is proposed, resulting in an "energy conservation consistent" scission-point method. Mass and charge distributions for the fission of 235U and 252Cf compound systems have been calculated and compared with distributions following the "standard" scission-point method of Wilkins, Steinberg, and Chasman.
NUCLEAR REACTIONS Scission-point model. Collective potential and intrinsic excitation energy. Nuclear temperature T. Mass and charge distributions. Fission of 235U and 252C.

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