11 research outputs found

    Universal trend of the information entropy of a fermion in a mean field

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    We calculate the information entropy of single-particle states in position-space SrS_{r} and momentum-space SkS_{k} for a nucleon in a nucleus, a Λ\Lambda particle in a hypernucleus and an electron in an atomic cluster. It is seen that SrS_{r} and SkS_{k} obey the same approximate functional form as functions of the number of particles, SrS_{r} ({\rm or} Sk)=a+bN1/3S_{k}) = a+bN^{1/3} in all of the above many-body systems in position- and momentum- space separately. The net information content Sr+SkS_{r}+S_{k} is a slowly varying function of NN of the same form as above. The entropy sum Sr+SkS_{r}+S_{k} is invariant to uniform scaling of coordinates and a characteristic of the single-particle states of a specific system. The order of single-particle states according to Sr+SkS_r +S_k is the same as their classification according to energy keeping the quantum number nn constant. The spin-orbit splitting is reproduced correctly. It is also seen that Sr+SkS_{r}+S_{k} enhances with excitation of a fermion in a quantum-mechanical system. Finally, we establish a relationship of Sr+SkS_r +S_k with the energy of the corresponding single-particle state i.e. Sr+Sk=kln(μE+ν)S_r +S_k = k \ln (\mu E +\nu). This relation holds for all the systems under consideration.Comment: 9 pages, latex, 6 figure

    Deformed Harmonic Oscillators for Metal Clusters: Analytic Properties and Supershells

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    The analytic properties of Nilsson's Modified Oscillator (MO), which was first introduced in nuclear structure, and of the recently introduced, based on quantum algebraic techniques, 3-dimensional q-deformed harmonic oscillator (3-dim q-HO) with Uq(3) > SOq(3) symmetry, which is known to reproduce correctly in terms of only one parameter the magic numbers of alkali clusters up to 1500 (the expected limit of validity for theories based on the filling of electronic shells), are considered. Exact expressions for the total energy of closed shells are determined and compared among them. Furthermore, the systematics of the appearance of supershells in the spectra of the two oscillators is considered, showing that the 3-dim q-HO correctly predicts the first supershell closure in alkali clusters without use of any extra parameter.Comment: 25 pages LaTeX plus 21 postscript figure

    Rotationally Invariant Hamiltonians for Nuclear Spectra Based on Quantum Algebras

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    The rotational invariance under the usual physical angular momentum of the SUq(2) Hamiltonian for the description of rotational nuclear spectra is explicitly proved and a connection of this Hamiltonian to the formalisms of Amal'sky and Harris is provided. In addition, a new Hamiltonian for rotational spectra is introduced, based on the construction of irreducible tensor operators (ITO) under SUq(2) and use of q-deformed tensor products and q-deformed Clebsch-Gordan coefficients. The rotational invariance of this SUq(2) ITO Hamiltonian under the usual physical angular momentum is explicitly proved, a simple closed expression for its energy spectrum (the ``hyperbolic tangent formula'') is introduced, and its connection to the Harris formalism is established. Numerical tests in a series of Th isotopes are provided.Comment: 34 pages, LaTe

    Unified description of magic numbers of metal clusters in terms of the 3-dimensional q-deformed harmonic oscillator

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    Magic numbers predicted by a 3-dimensional q-deformed harmonic oscillator with Uq(3)>SOq(3) symmetry are compared to experimental data for atomic clusters of alkali metals (Li, Na, K, Rb, Cs), noble metals (Cu, Ag, Au), divalent metals (Zn, Cd), and trivalent metals (Al, In), as well as to theoretical predictions of jellium models, Woods-Saxon and wine bottle potentials, and to the classification scheme using the 3n+l pseudo quantum number. In alkali metal clusters and noble metal clusters the 3-dimensional q-deformed harmonic oscillator correctly predicts all experimentally observed magic numbers up to 1500 (which is the expected limit of validity for theories based on the filling of electronic shells), while in addition it gives satisfactory results for the magic numbers of clusters of divalent metals and trivalent metals, thus indicating that Uq(3), which is a nonlinear extension of the U(3) symmetry of the spherical (3-dimensional isotropic) harmonic oscillator, is a good candidate for being the symmetry of systems of several metal clusters. The Taylor expansions of angular momentum dependent potentials approximately producing the same spectrum as the 3-dimensional q-deformed harmonic oscillator are found to be similar to the Taylor expansions of the symmetrized Woods-Saxon and wine-bottle symmetrized Woods-Saxon potentials, which are known to provide successful fits of the Ekardt potentials.Comment: 23 pages including 7 table

    Two approximate formulae for the binding energies in Lambda hypernuclei and light nuclei

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    Two approximate formulae are given for the binding energies in Lambda-hypernuclei and light nuclei by means of the (reduced) Poeschl-Teller and the Gaussian central potentials. Those easily programmable formulae combine the eigenvalues of the transformed Jacobi eigenequation and an application of the hypervirial theorems.Comment: Accepted for publication in Europhysics Letter

    Approximate analytical solutions of the generalized Woods-Saxon potentials including the spin-orbit coupling term and spin symmetry

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    We study the approximate analytical solutions of the Dirac equation for the generalized Woods-Saxon potential with the pseudo-centrifugal term. In the framework of the spin and pseudospin symmetry concept, the approximately analytical bound state energy eigenvalues and the corresponding upper- and lower-spinor components of the two Dirac particles are obtained, in closed form, by means of the Nikiforov-Uvarov method which is based on solving the second-order linear differential equation by reducing it to a generalized equation of hypergeometric type. The special cases κ=±1\kappa =\pm 1 (l=l~=0,l=% \widetilde{l}=0, s-wave) and the non-relativistic limit can be reached easily and directly for the generalized and standard Woods-Saxon potentials. Also, the non-relativistic results are compared with the other works.Comment: 25 page
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