2010
DOI: 10.1103/physrevd.82.085033
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Fermionic current densities induced by magnetic flux in a conical space with a circular boundary

Abstract: We investigate the vacuum expectation value of the fermionic current induced by a magnetic flux in a (2 þ 1)-dimensional conical spacetime in the presence of a circular boundary. On the boundary the fermionic field obeys the MIT bag boundary condition. For irregular modes, a special case of boundary conditions at the cone apex is considered, when the MIT bag boundary condition is imposed at a finite radius, which is then taken to zero. We observe that the vacuum expectation values for both the charge density a… Show more

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Cited by 66 publications
(110 citation statements)
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“…The wave functions (2.16) are eigenfunctions of the projection of total angular momentum operator along the cosmic string, 19) with the eigenvalues j + α. The constants C (±) σ in (2.16) are determined by the orthonormalization condition 20) where γ is the determinant of the spatial metric tensor.…”
Section: Geometry and The Fermionic Modesmentioning
confidence: 99%
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“…The wave functions (2.16) are eigenfunctions of the projection of total angular momentum operator along the cosmic string, 19) with the eigenvalues j + α. The constants C (±) σ in (2.16) are determined by the orthonormalization condition 20) where γ is the determinant of the spatial metric tensor.…”
Section: Geometry and The Fermionic Modesmentioning
confidence: 99%
“…The azimuthal current density for scalar and fermionic fields, induced by a magnetic flux in the geometry of a straight cosmic string, has been investgated in [14]- [18]. The fermionic current induced by a magnetic flux in a (2 + 1)-dimensional conical spacetime with a circular boundary has been analyzed in [19]. The compactification of the cosmic string along its axis may lead to the appearance of the axial current density [17,18] (for the vacuum expectation value of the current density in models with compact dimensions see [20] in the case of flat background geometry and [21,22] for de Sitter and anti-de Sitter bulks).…”
Section: Introductionmentioning
confidence: 99%
“…Note that the radius of the magnetic flux should also be taken to zero. For j + α = 0 one has 22) and, hence, the part (4.21) vanishes as a 2|j+α| . For half-odd integer values of α, the exceptional case corresponds to the mode with j = −α.…”
Section: Charge Densitymentioning
confidence: 99%
“…[22]: (4.32) Similarly to the boundary-induced contributions, this part is an odd function of the parameter α 0 . For a massless field the boundary-free contribution in the charge density vanishes for r = 0.…”
Section: Charge Densitymentioning
confidence: 99%
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