1973
DOI: 10.1016/0003-4916(73)90420-x
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Toroidal and spherical bubble nuclei

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Cited by 138 publications
(169 citation statements)
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“…In 1967, Siemens and Bethe studied spherical bubble nuclei using a liquid drop model [5]. And later on, based on a liquid drop model (LDM) with shell correction energy, Wong studied known β-stable nuclei and found spherical bubbles [10]. Furthermore, Moretto et al showed that bubbles at finite temperature may be stabilized by the inner vapor pressure [13].…”
Section: Introductionmentioning
confidence: 99%
“…In 1967, Siemens and Bethe studied spherical bubble nuclei using a liquid drop model [5]. And later on, based on a liquid drop model (LDM) with shell correction energy, Wong studied known β-stable nuclei and found spherical bubbles [10]. Furthermore, Moretto et al showed that bubbles at finite temperature may be stabilized by the inner vapor pressure [13].…”
Section: Introductionmentioning
confidence: 99%
“…E.g., a region of relatively higher stability against spontaneous fission was obtained at Z = 164 and N = 318 in [8]. The properties of toroidal and spherical bubble nuclei were presented in [159]. Although speculative, the highly advanced experimental technology should be used also for some experiments to search for such really exotic phenomena in the accessible region of nuclei between Z = 126, N = 184 and Z = 190, N = 297.…”
Section: Discussionmentioning
confidence: 99%
“…The values of J appearing are 20, 60, and 100, but only for J=60 the configuration remains stable for a very large number of iterations. The values occurring here can be understood quite simply from the radially displaced harmonic oscillator model [9]. In practice the wave functions can be approximated quite well as Gaussians in the distance from the central circle of the torus, and by azimuthal factors like exp(imφ).…”
Section: Torus Stabilization By Rotationmentioning
confidence: 99%
“…In the present study, search for the stable state using the equivalent cranked rme HF equation, δ Ĥ − ωĴ z = 0 [14, 15], by scana large range of ω. efore the HF calculations, we here discuss the shell cture of the torus configuration using the radial dised harmonic oscillator (RDHO) model [9]. For the s configuration, not only Ω but also the z component of orbital angular momentum, Λ, are good quantum num-(Ω = Λ + Σ, where Σ denotes the z component of the values, ±1/2).…”
Section: Torus Stabilization By Rotationmentioning
confidence: 99%