9 research outputs found

    Helium- and Lithium-like ionic sequences: Critical charges

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    In non-relativistic quantum mechanics we study the Coulomb systems of infinitely massive center of charge Z and two-three electrons: (Z,e,e)(Z,e,e) and (Z,e,e,e)(Z,e,e,e). It is shown that in both cases the total energy curve in ZZ is smooth, without any visible irregularities. Thus, for both systems the physical integer charges Z=1,2,...Z=1,2,... do not play a distinguished role as would be associated with charge quantization. By definition, a critical charge ZcrZ_{cr} is a charge which separates a domain of the existence of bound states from a domain of unbound ones (continuum). For both systems the critical charges are found, Zcr,2e=0.91085Z_{cr,2e}=0.91085 and Zcr,3e=2.009Z_{cr,3e}=2.009, respectively. Based on numerical analysis, the Puiseux expansion in fractional powers of (ZZcr)(Z-Z_{cr}) is constructed for both systems. Our results indicate the existence of a square-root branch point singularity at ZcrZ_{cr} with exponent 3/2. A connection between the critical charge and the radius of convergence of 1/Z-expansion is briefly discussed.Comment: 10 pages, LaTeX, typos corrected, Fig.1 added, a Note Added with calculated critical charge for 21S2^1S state for (Z,e,e)(Z,e,e) system, $Z_{cr,2e}^{(2^1S)}\ =\ 1.02

    A note about the ground state of the H3+{\rm H}_3^+ hydrogen molecular ion

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    Three simple 7,(7+3),107-, (7+3)-, 10-parametric trial functions for the H3+{\rm H}_3^+ molecular ion are presented. Each of them provides subsequently the most accurate approximation for the Born-Oppenheimer ground state energy among several-parametric trial functions. These trial functions are chosen following a criterion of physical adequacy and includes the electronic correlation in the exponential form exp(γr12)\sim\exp{(\gamma r_{12})}, where γ\gamma is a variational parameter. The Born-Oppenheimer energy is found to be E=1.34034,1.34073,1.34159E=-1.340 34, -1.340 73, -1.341 59\,a.u., respectively, for optimal equilateral triangular configuration of protons with the equilibrium interproton distance R=1.65R=1.65\,a.u. The variational energy agrees in three significant digits (s.d.) with most accurate results available at present as well as for major expectation values.Comment: 12 pages, 1 figure, 3 table

    Charged Hydrogenic, Helium and Helium-Hydrogenic Molecular Chains in a Strong Magnetic Field

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    A non-relativistic classification of charged molecular hydrogenic, helium and mixed helium-hydrogenic chains with one or two electrons which can exist in a strong magnetic field B1016B \lesssim 10^{16} G is given. It is shown that for both 1e2e1e-2e cases at the strongest studied magnetic fields the longest hydrogenic chain contains at most five protons indicating to the existence of the H54+\rm{H}_5^{4+} and H53+\rm{H}_5^{3+} ions, respectively. In the case of the helium chains the longest chains can exist at the strongest studied magnetic fields with three and four \al-particles for 1e2e1e-2e cases, respectively. For mixed helium-hydrogenic chains the number of heavy centers can reach five for highest magnetic fields studied. In general, for a fixed magnetic field two-electron chains are more bound than one-electron ones.Comment: 32 pages, 2 figures, 9 table

    The HeH+HeH^+ molecular ion in a magnetic field

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    A detailed study of the low-lying electronic states {}^1\Si,{}^3\Si,{}^3\Pi,{}^3\De of the HeH+\rm{HeH}^+ molecular ion in parallel to a magnetic field configuration (when \al-particle and proton are situated on the same magnetic line) is carried out for B=04.414×1013B=0-4.414\times 10^{13} G in the Born-Oppenheimer approximation. The variational method is employed using a physically adequate trial function. It is shown that the parallel configuration is stable with respect to small deviations for \Si-states. The quantum numbers of the ground state depend on the magnetic field strength. The ground state evolves from the spin-singlet {}^1\Si state for small magnetic fields B0.5B\lesssim 0.5 a.u. to the spin-triplet {}^3\Si unbound state for intermediate fields and to the spin-triplet strongly bound 3Π^3\Pi state for B15B \gtrsim 15 a.u. When the HeH+\rm{HeH}^+ molecular ion exists, it is stable with respect to a dissociation.Comment: 13 pages, 5 figures, 4 table

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