2014
DOI: 10.11648/j.ajmp.20140302.16
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Boundary Conditions Effects on the Ground State of a Two-Electron Atom in a Vacuum Cavity

Abstract: Abstract:The ground state properties of the two-electron atom with atomic number 2 Z ≥ in the spherical vacuum cavity with general boundary conditions of "not going out" are studied. It is shown that for certain parameters of the cavity such atom could either decay into the one-electron atom with the same atomic number and an electron or be in stable state with the binding and ionization energies several times bigger than the same energies of the free atom. By analogy with the Wigner-Seitz model of metallic bo… Show more

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Cited by 3 publications
(4 citation statements)
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References 31 publications
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“…In accordance with [30], the limiting value (a) is obtained from the equation (25) Now, let us study the behavior of the lowest elec tronic energy term of the molecular hydrogen ion as a function of R, depending on the specific values of a, V 0 , and d. The shell parameters are chosen so that they correspond to the scale of the real sizes of microvoids, in which the confinement of the atomic system can occur (see the discussion in [29][30][31]). For V 0 , the opti mal characteristic of the general case is Ӎ10 eV and the lowest energy level has an exponential dependence on distance.…”
Section: A Molecular Hydrogen Ion In a Cavity With A Finite Width Boumentioning
confidence: 99%
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“…In accordance with [30], the limiting value (a) is obtained from the equation (25) Now, let us study the behavior of the lowest elec tronic energy term of the molecular hydrogen ion as a function of R, depending on the specific values of a, V 0 , and d. The shell parameters are chosen so that they correspond to the scale of the real sizes of microvoids, in which the confinement of the atomic system can occur (see the discussion in [29][30][31]). For V 0 , the opti mal characteristic of the general case is Ӎ10 eV and the lowest energy level has an exponential dependence on distance.…”
Section: A Molecular Hydrogen Ion In a Cavity With A Finite Width Boumentioning
confidence: 99%
“…a C < < a 2 , we introduce the following sampling functions (31) The f L, R φ functions are the eigen functions of H L, R with an exponential accuracy [35], where φ is the nor malized wave function of a double well Schrodinger operator that corresponds to E 0 . The probability, P L , of finding the particle in the left well is given by (32) since the integral in the range a 1 < a < a 2 is exponen tially small.…”
Section: The Tunnel Splitting Of the Lowest Level Of An Ion In A Shellmentioning
confidence: 99%
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