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Clemenger-Nilsson model

Recently it has been shown [21] that the spectrum of this g-deformed, 3-dimensional harmonic oscillator (Q30) reproduces very well that of the modified harmonic oscillator introduced by Nilsson [12, 15] without the spin-orbit coupling term. Since the Nilsson model without spin-orbit coupling is essentially the Nilsson-Clemenger model used for the description of metal clusters [11], it is worth examining whether the Q30 model can be used to reproduce the magic numbers and some other properties of simple metal clusters. [Pg.281]

It has been proven [21] that the spectrum obtained with the Q30 model closely resembles that of the modified harmonic oscillator of Nilsson and Clemenger. In both cases, the effect of the 1(14-1) term is to flatten the bottom of the harmonic oscillator potential, making it resemble the Woods-Saxon potential [18]. [Pg.295]


See other pages where Clemenger-Nilsson model is mentioned: [Pg.280]    [Pg.280]    [Pg.301]    [Pg.279]    [Pg.258]    [Pg.11]    [Pg.142]    [Pg.143]    [Pg.143]    [Pg.276]   
See also in sourсe #XX -- [ Pg.40 , Pg.40 , Pg.280 , Pg.293 , Pg.294 ]




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