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In this paper, we investigate the edge Majorana modes in the simplest possible $p{}_{x}+ip_{y}$ superconductor defined on surfaces with different geometry - the annulus, the cylinder, the M\"obius band and a cone (by cone we mean a cone with the tip cut away so it is topologically equivalent to the annulus and cylinder)- and with different configuration of magnetic fluxes threading holes in these surfaces.
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For any physical system the Hamiltonian would also have terms which does not depend on the intrinsic geometry, but for simplicity we do not consider such terms here
Cited in the paper.
For the interaction to be well defined, the Fourier transform V ( q ) V(q) of the potential V ( r ) V(r) , where r r is the geodesic distance, have to vanish as q → ∞ q\rightarrow\infty . However, the precise behaviour at large momenta is not important for the long wave-length physics
Cited in the paper.
Adding higher-order terms would also mean that the ansatz Δ ϕ = c o n s t . \Delta\phi=const. is not a self-consistent solution close to vortices or edges
Cited in the paper.
There are many such flat embeddings, and it is interesting to ask which one would minimize the elastic energy for a real physical Möbius band. This problem was recently solved numerically in Ref. \rev@citealpnum
Cited in the paper.
2012
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Y. Maeno, S. Kittaka, T. Nomura, S. Yonezawa, and K. Ishida, Journal of the Physical Society of Japan 81
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