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We address the following question: Which kinds of symmetry protected topological (SPT) Hamiltonians can be many-body localized? That is, which Hamiltonians with an SPT ground state have finite energy density excited states which are all localized by disorder? Based on the observation that a finite energy density state, if localized, can be viewed as the ground state of a local Hamiltonian, we propose a simple (though possibly incomplete) rule for many-body localization of SPT Hamiltonians: If the ground state and top state (highest energy state) belong to the same SPT phase, then it is possible to localize all the finite energy density states; If the ground and top state belong to different SPT phases, then most likely there are some finite energy density states which can not be fully localized.
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