2021
DOI: 10.1007/s13324-021-00507-2
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Casimir pistons with generalized boundary conditions: a step forward

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Cited by 3 publications
(2 citation statements)
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“…If the two objects lie outside of each other, the Casimir energy has the same form as in (1) but the force between them is defined as the variation of the total energy with respect to the distance between the objects (although the force can also be defined in this way when one object is inside the other, see for instance [8]). Since, in most cases, the divergent parts of the energies E 1 , E 2 , and E int is independent of this distance, the Casimir force is well-defined (even if the energy might be divergent [2,6,9]).…”
Section: Introductionmentioning
confidence: 99%
“…If the two objects lie outside of each other, the Casimir energy has the same form as in (1) but the force between them is defined as the variation of the total energy with respect to the distance between the objects (although the force can also be defined in this way when one object is inside the other, see for instance [8]). Since, in most cases, the divergent parts of the energies E 1 , E 2 , and E int is independent of this distance, the Casimir force is well-defined (even if the energy might be divergent [2,6,9]).…”
Section: Introductionmentioning
confidence: 99%
“…to define the self-adjoint extensions of ĤV , one could recover the Bloch semi-periodicity condition (3.4) from the boundary conditions in (3.6). This approach enables to interpret the comb as a oneparameter family of quantum pistons [148][149][150] where 1. The middle piston membrane is represented by the individual potential V(z) given in (3.1) placed at the middle point of the primitive cell.…”
Section: On Any Intervalmentioning
confidence: 99%