Clifford group dipoles and the enactment of Weyl/Coxeter group W(E8) by entangling gates
Michel Planat (FEMTO-ST)

TL;DR
This paper explores how specific entangling Clifford gates can generate representations of complex Coxeter and Weyl groups, including W(E8), revealing deep connections between quantum entanglement, group theory, and quantum gate structures.
Contribution
It introduces a novel link between entangling Clifford gates and the realization of Weyl/Coxeter groups like W(E8) through unitary representations, expanding understanding of quantum symmetries.
Findings
Representation of W(D5) and W(F4) from Clifford gates
W(E8) representation via three-qubit Clifford group and Toffoli gate
Connections between entangled states and complex reflection groups
Abstract
Peres/Mermin arguments about no-hidden variables in quantum mechanics are used for displaying a pair (R, S) of entangling Clifford quantum gates, acting on two qubits. From them, a natural unitary representation of Coxeter/Weyl groups W(D5) and W(F4) emerges, which is also reflected into the splitting of the n-qubit Clifford group Cn into dipoles Cn . The union of the three-qubit real Clifford group C+ 3 and the Toffoli gate ensures a orthogonal representation of the Weyl/Coxeter group W(E8), and of its relatives. Other concepts involved are complex reflection groups, BN pairs, unitary group designs and entangled states of the GHZ family.
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Taxonomy
TopicsQuantum Computing Algorithms and Architecture · Quantum-Dot Cellular Automata
