Existence of locally maximally entangled quantum states via geometric invariant theory
arXiv:1708.01645 · doi:10.1007/s00023-018-0682-6
Abstract
We study a question which has natural interpretations in both quantum mechanics and in geometry. Let be complex vector spaces of dimension and let . Geometrically, we ask given , when is the geometric invariant theory quotient non-empty? This is equivalent to the quantum mechanical question of whether the multipart quantum system with Hilbert space has a locally maximally entangled state, i.e. a state such that the density matrix for each elementary subsystem is a multiple of the identity. We show that the answer to this question is yes if and only if where \[ R(d_1,...,d_n) = \prod_i d_i +\sum_{k=1}^n (-1)^k \sum_{1\leq i_1<\dotsb <i_k\leq n} (\gcd(d_{i_1},\dotsc ,d_{i_k}) )^{2}. \] We also provide a simple recursive algorithm which determines the answer to the question, and we compute the dimension of the resulting quotient in the non-empty cases.
Improved the exposition and streamlined some proofs using results of Littelmann and Sato-Kimura
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