Odd-Parity Topological Superconductors: Theory and Application to Cu$_x$Bi$_2$Se$_3$

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Microscopically, these additional terms are proportional to the square of the wavefunction overlap of orbitals localized on the top and bottom of the five-atom unit cell, about 9 A ̊ 9\mathrm{\mathring{A}} apart. Therefore they are expected to be small
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