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  • 1980-1984  (4)
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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    The European physical journal 301 (1981), S. 137-140 
    ISSN: 1434-601X
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract Theg-factor of theJ π=21/2+ isomeric state in111In (T 1/2=13.3 ns) and of theJ π=6+ isomeric state in112Sn (T 1/2=13.7 ns) were measured using the spin rotation method. The result obtained for theJ π=21/2+ level in111In,g=+0.47 (2), indicates that this state has an almost pure ((πg 9/2)−1 νg 7/2 νd 5/2) shell model configuration. The experimental valueg=+0.04 (3) for theJ π=6+ isomer in112Sn agrees with the theoretical value calculated within the frame of the BCS model.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    Springer
    The European physical journal 304 (1982), S. 245-255 
    ISSN: 1434-601X
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract Like in earlier work by Schiffer et al. the effective interaction is derived from experimental two-body multiplets. However, now the assumption is that a multiplet state is formed by two unpaired fermions relative to a core of correlatedJ=0 pairs. Then the need for two ranges, as proposed by Schiffer, disappears for the force between identical nucleons in a model space which is large enough to include pairing correlations. A form with a single attractive medium range is preferred for the identical nucleon interaction in order to reproduce collective 2+ states in even-even nuclei. In contrast, the proton-neutron force requires a very short range or two ranges to reproduce the empirical values of multipole coefficients, observed in odd-odd nuclei. Therefore we discuss the fact that the effective interaction is not always isospin invariant. As a typical case broken-pair calculations in theN=50 region are considered. But the conclusions drawn, will also apply to other regions of the periodic table.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    Springer
    The European physical journal 313 (1983), S. 213-225 
    ISSN: 1434-601X
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The broken-pair model is used to study the nature of collective pair structure in even nuclei and a possible connection with the interacting-boson model IBM-2. In our self-consistent treatment there is no particle-hole ambiguity, such as has been reported in recent literature. We find that about four particles away from a closed shell, for both protons and neutrons, the collective 2+ (D-pair) structure becomes roughly independent of mass number due to the proton-neutron force. Only near the closed shell pronounced fermion configurations show up. The same is true for the 3− (F-pair). In lighter nuclei, the 20≦N≦50 shell, no really collective 4+ (G-pair) is formed but in heavier nuclei, 50≦N≦82, it begins to develop. No other types of collective-pair structure appear, such as a collective 0 2 + (S′-pair). When microscopically computed quantities are compared with currently used parameters in IBM fits, we find not only a considerable renormalization of boson energies, but also of the proton-neutron interaction. One effect responsible for this is Pauli blocking which makes the interaction seniority dependent. The trend of the proton-neutron interaction parameterk agrees with single-shell formulas, but for the IBM parameters χ ρ single-shell predictions are of little value. With some rules of thumb for renormalization the calculated parameters come close to those found in empirical fits.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    Springer
    The European physical journal 300 (1981), S. 323-327 
    ISSN: 1434-601X
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract Low lying energy levels and transition probabilities of63,65,67Zn are calculated in the Quasicluster-vibration model (QCVM). This model is an extension of the Clustervibration model (CVM) for three-particle-cluster vibration coupling. Instead of a three-particle cluster, now a one broken pair (number projected three quasiparticle) cluster is coupled to phonon states. It turns out that the sequence of isotopes may be described with one set of parameters, along the same line as previously used in the CVM. The resulting spectra and electromagnetic properties, for positive and negative parity states of odd Zn isotopes, compare with experimental data equally well as large shell-model calculations; this seems to justify the extension of the CVM to these nuclei with more than three particles or holes beyond a closed shell.
    Type of Medium: Electronic Resource
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