2001
DOI: 10.1088/0305-4470/34/49/320
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Rigorous proof of the attractive nature for the Casimir force of ap-odd hypercube

Abstract: The Casimir effect giving rise to an attractive force between the configuration boundaries that confine the massless scalar field is rigorously proven for odd dimensional hypercube with the Dirichlet boundary conditions and different spacetime dimensions D by the Epstein zeta function regularization. PACS number(s): 04.62.+v, 03.65.Ge

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Cited by 20 publications
(19 citation statements)
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“…Now we just have to collect them all and integrate them over k z as indicated in Eq. (15). The integral of the three different kind of branch cuts can be easily calculated and the results for each are: The sum over j in the last equation comes from the Taylor expansion of the denominator of that particular branch-cut term Eq.…”
Section: Appendix a Electromagnetic Modes In Waveguidesmentioning
confidence: 99%
“…Now we just have to collect them all and integrate them over k z as indicated in Eq. (15). The integral of the three different kind of branch cuts can be easily calculated and the results for each are: The sum over j in the last equation comes from the Taylor expansion of the denominator of that particular branch-cut term Eq.…”
Section: Appendix a Electromagnetic Modes In Waveguidesmentioning
confidence: 99%
“…Inevitably a lot of attention has been focused on the role of boundary conditions and very recently on the interplay of material properties, temperature, and geometry. Some new methods have developed for computing the Casimir effect between a finite number of compact objects [8], inside a rectangular box or cavity [10][11][12]. When a topology of the flat spacetime was chosen to cause the helix boundary condition for a scalar field, the Casimir force behaves very much like the force on a spring that obeys the Hooke's law when the ratio of the pitch to the circumference of the helix is small, but in this case, the force comes from a quantum effect, so the author call it quantum spring [13] [14] or quantum anti-spring [15] corresponding to periodic-like and anti-periodic-like boundary condition, see also [16].…”
Section: Introductionmentioning
confidence: 99%
“…So, the regularized temperaturedependent parts of the free energy densities for these two BCs are 27) where the sign "+" corresponds to Dirichlet BCs and the sign "−" to Neumann BCs. It is obvious that the term proportional to T 4 is the blackbody radiation energy restricted in the volume L 3 , regardless of the BCs.…”
Section: Dirichlet and Neumann Bcsmentioning
confidence: 99%