1,094 research outputs found

    Lowest eigenvalue of the nuclear shell model Hamiltonian

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    In this paper we investigate regular patterns of matrix elements of the nuclear shell model Hamiltonian HH, by sorting the diagonal matrix elements from the smaller to larger values. By using simple plots of non-zero matrix elements and lowest eigenvalues of artificially constructed "sub-matrices" hh of HH, we propose a new and simple formula which predicts the lowest eigenvalue with remarkable precisions.Comment: six pages, four figures, Physical Review C, in pres

    Coherent Pair State of Pion in Constituent Quark Model

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    A coherent state of pions is introduced to the nonrelativistic quark model. The coherent pair approximation is employed for the pion field in order to maintain the spin-isospin symmetry. In this approximation the pion is localized in the momentum space, and the vertex form factor in the pion-quark interaction is derived from this localization. The nucleon masses and wave functions are calculated using this model, and our results are compared to those of the quark model with the one pion exchange potential. Similar result is obtained for the mass spectrum, but there exists a clear difference in the internal structure of nucleon resonances.Comment: 17 pages, 2 figures, revtex, submitted to Phys. Rev.

    Theory of magnetoelectric resonance in two-dimensional S=3/2S=3/2 antiferromagnet Ba2CoGe2O7{\rm Ba_2CoGe_2O_7} via spin-dependent metal-ligand hybridization mechanism

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    We investigate magnetic excitations in an S=3/2S=3/2 Heisenberg model representing two-dimensional antiferromagnet Ba2CoGe2O7{\rm Ba_2CoGe_2O_7}. In terahertz absorption experiment of the compound, Goldstone mode as well as novel magnetic excitations, conventional magnetic resonance at 2 meV and both electric- and magnetic-active excitation at 4 meV, have been observed. By introducing a hard uniaxial anisotropy term Λ(Sz)2\Lambda (S^z)^2, three modes can be explained naturally. We also indicate that, via the spin-dependent metal-ligand hybridization mechanism, the 4 meV excitation is an electric-active mode through the coupling between spin and electric-dipole. Moreover, at 4 meV excitation, an interference between magnetic and electric responses emerges as a cross correlated effect. Such cross correlation effects explain the non-reciprocal linear directional dichroism observed in Ba2CoGe2O7{\rm Ba_2CoGe_2O_7}.Comment: 5 pages, 3 figure

    SU(3) realization of the rigid asymmetric rotor within the IBM

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    It is shown that the spectrum of the asymmetric rotor can be realized quantum mechanically in terms of a system of interacting bosons. This is achieved in the SU(3) limit of the interacting boson model by considering higher-order interactions between the bosons. The spectrum corresponds to that of a rigid asymmetric rotor in the limit of infinite boson number.Comment: 9 pages, 2 figures, LaTeX, epsfi

    Optical Spectra in the Ferromagnetic States near the Charge Ordering

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    The optical conductivity is studied numerically for the ferromagnetic metallic state close to the charge ordering observed in perovskite manganites.Comment: 11 pages, Latex, 6 ps figure

    One-Center Charge Transfer Transitions in Manganites

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    In frames of a rather conventional cluster approach, which combines the crystal field and the ligand field models we have considered different charge transfer (CT) states and O 2p-Mn 3d CT transitions in MnO69_{6}^{9-} octahedra. The many-electron dipole transition matrix elements were calculated using the Racah algebra for the cubic point group. Simple "local" approximation allowed to calculate the relative intensity for all dipole-allowed ππ\pi -\pi and σσ\sigma -\sigma CT transitions. We present a self-consistent description of the CT bands in insulating stoichiometric LaMn3+^{3+}O3_3 compound with the only Mn3+^{3+} valent state and idealized octahedral MnO69_{6}^{9-} centers which allows to substantially correct the current interpretation of the optical spectra. Our analysis shows the multi-band structure of the CT optical response with the weak low-energy edge at 1.7 eV, associated with forbidden t1g(π)egt_{1g}(\pi)-e_{g} transition and a series of the weak and strong dipole-allowed high-energy transitions starting from 2.5 and 4.5 eV, respectively, and extending up to nearly 11 eV. The most intensive features are associated with two strong composite bands near 4.6÷4.74.6\div 4.7 eV and 8÷98\div 9 eV, respectively, resulting from the superposition of the dipole-allowed σσ\sigma -\sigma and ππ\pi -\pi CT transitions. These predictions are in good agreement with experimental spectra. The experimental data point to a strong overscreening of the crystal field parameter DqDq in the CT states of MnO69_{6}^{9-} centers.Comment: 10 pages, 3 figure

    Quadrupole Collective States in a Large Single-J Shell

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    We discuss the ability of the generator coordinate method (GCM) to select collective states in microscopic calculations. The model studied is a single-jj shell with hamiltonian containing the quadrupole-quadrupole interaction. Quadrupole collective excitations are constructed by means of the quadrupole single-particle operator. Lowest collective bands for jj=31/2 and particle numbers NN=4,6,8,10,12, and 1414 are found. For lower values of jj, exact solutions are obtained and compared with the GCM results.Comment: submitted for publication in Phys. Rev. C, revtex, 28 pages, 15 PostScript figures available on request from [email protected], preprint No. IFT/17/9

    Direct observation of cycloidal spin modulation and field-induced transition in N\'eel-type skyrmion-hosting VOSe2_2O5_5

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    We investigate the spin rotational structure of magnetic skyrmions in a tetragonal polar magnet VOSe2O5 via polarized small-angle neutron scattering (SANS). Spin polarization analysis of the scattered neutrons provides consistent evidence for the cycloidal spin modulation in all the incommensurate phases at zero and non-zero magnetic field along the c axis, including the triangular skyrmion-lattice phase. In the vicinity of the skyrmion phase, we performed extensive SANS measurements to unravel a field-induced incommensurate phase (IC-2 state). We discuss the possibility of anisotropic double-q state as an alternative spin structure to provisional square skyrmion-lattice state.Comment: 27 pages, 5 figure
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