2017
DOI: 10.1140/epjd/e2017-70503-6
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Spontaneous spherical symmetry breaking in atomic confinement

Abstract: The effect of spontaneous breaking of initial SO(3) symmetry is shown to be possible for an H-like atom in the ground state, when it is confined in a spherical box under general boundary conditions of "not going out" through the box surface (i.e. third kind or Robin's ones), for a wide range of physically reasonable values of system parameters. The reason is that such boundary conditions could yield a large magnitude of electronic wavefunction in some sector of the box boundary, what in turn promotes atomic di… Show more

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Cited by 4 publications
(15 citation statements)
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“…In a cavity with finite R, such situation also takes place when the equilibrium position of H shifts from the center to the border, that happens whenever λ < q with q being the nucleus charge. [34,35] In ℜ 3 / 2 the spherical symmetry restores only for infinite distances between the atom and plane and only in the case, when the atomic electron is localized in the nucleus vicinity, where it falls into the eigenstates of the free atom. But this is not the general case.…”
Section: The Problem Statement For Atomic H In ℜ 3 /mentioning
confidence: 99%
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“…In a cavity with finite R, such situation also takes place when the equilibrium position of H shifts from the center to the border, that happens whenever λ < q with q being the nucleus charge. [34,35] In ℜ 3 / 2 the spherical symmetry restores only for infinite distances between the atom and plane and only in the case, when the atomic electron is localized in the nucleus vicinity, where it falls into the eigenstates of the free atom. But this is not the general case.…”
Section: The Problem Statement For Atomic H In ℜ 3 /mentioning
confidence: 99%
“…[25][26][27][28][29][30][31][32][33] Moreover, such conditions are able to take into account the interaction of confined particles with medium, surrounding the cavity or demarcating the half-space. [29][30][31][32]34,35] It would be worth to note that the term "not going through," used here, underlines that these conditions do not necessarily originate from the actual confinement of particles inside the given volume, rather they may be caused by a significantly wider number of reasons, as it takes place, in particular, in the Wigner-Seitz model of an alkali metal, [4,5] where the valence electron state is principally delocalized. The latter circumstance turns out to be quite important, because in some cases the cavities, where a particle or an atom could reside, form a lattice, similar to that of an alkali metal, like certain interstitial sites of a metal supercell, for example, next-to-nearest octahedral positions of palladium face-centered-cubic lattice.…”
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confidence: 98%
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