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Balanced Tripartite Entanglement, the Alternating Group A4 and the Lie Algebra sl(3,C)u(1)sl(3,C) \oplus u(1)

Abstract

We discuss three important classes of three-qubit entangled states and their encoding into quantum gates, finite groups and Lie algebras. States of the GHZ and W-type correspond to pure tripartite and bipartite entanglement, respectively. We introduce another generic class B of three-qubit states, that have balanced entanglement over two and three parties. We show how to realize the largest cristallographic group W(E8)W(E_8) in terms of three-qubit gates (with real entries) encoding states of type GHZ or W [M. Planat, {\it Clifford group dipoles and the enactment of Weyl/Coxeter group W(E8)W(E_8) by entangling gates}, Preprint 0904.3691 (quant-ph)]. Then, we describe a peculiar "condensation" of W(E8)W(E_8) into the four-letter alternating group A4A_4, obtained from a chain of maximal subgroups. Group A4A_4 is realized from two B-type generators and found to correspond to the Lie algebra sl(3,C)u(1)sl(3,\mathbb{C})\oplus u(1). Possible applications of our findings to particle physics and the structure of genetic code are also mentioned.Comment: 14 page

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    Last time updated on 02/01/2020