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The metallic surface states of a strong topological insulator become superconducting with the proximity of an s-wave superconductor. Due to the magnetic field the states undergo Landau quantization. A zero-energy Majorana state arises for the Landau level n=0 together with an equally spaced sequence of fermion excitations. The spin-momentum locking due to the Rashba spin-orbit coupling is key to the formation of the Majorana state. The local density of states for the bound states and their spin-polarization is obtained.
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