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Titlebook: Symmetries and Semiclassical Features of Nuclear Dynamics; Invited Lectures of A. A. Raduta Conference proceedings 1987 Springer-Verlag Be

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11#
發(fā)表于 2025-3-23 10:06:52 | 只看該作者
M. S. M. Nour El-Din,S. G. Rohoziński,J. A. Maruhn,W. Greiner styling features such as freeform curves and surfaces. In a typical scenario, the user begins by constructing the base wireframe model of the design object. For this, the user first sketches the initial feature curves on a very rough and simplified 3D template model. This template model acts as a p
12#
發(fā)表于 2025-3-23 15:33:01 | 只看該作者
13#
發(fā)表于 2025-3-23 19:12:10 | 只看該作者
J. Fink,L. Neise,M. Rufa,J. Maruhn,W. Greiner,P. G. Reinhard,J. Friedrichy providing an efficient medium for expressing ideas. However, despite the importance of sketches in engineering practice, current engineering software still relies on traditional mouse and keyboard interfaces, with little or no capabilities to handle free-form sketch input. With recent advances in
14#
發(fā)表于 2025-3-24 02:02:41 | 只看該作者
A. S?ndulescuognize and interpret what is drawn. Most commonly, a drawing is first processed to obtain a low-level representation of that drawing in terms of lines or strokes, and this representation is then searched for matches to known object templates. In this chapter we propose two template-based methods for
15#
發(fā)表于 2025-3-24 03:35:50 | 只看該作者
16#
發(fā)表于 2025-3-24 07:00:41 | 只看該作者
17#
發(fā)表于 2025-3-24 11:36:09 | 只看該作者
18#
發(fā)表于 2025-3-24 14:52:15 | 只看該作者
H. Rebel, how the evolution towards so-called ‘learning environments’ affects the kind of gathering or association that is staged and configured within families, schools and universities. In addition, it addresses the question of how to articulate what is educational in the context of ‘making’ family, schoo
19#
發(fā)表于 2025-3-24 20:10:37 | 只看該作者
20#
發(fā)表于 2025-3-25 01:35:35 | 只看該作者
,Excitation and decay of electric giant resonances — especially the isoscalar giant monopole resonanussed. The compressibility of nuclear matter Kn.m. will be determined from the newest experimental data on the GMR over the mass range 24 < A < 208 using a semiphenomenological expression for the nuclear compressibility K. in terms of a volume, surface, asymmetry and Coulomb contribution. The result
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