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arxiv: 2506.03453 · v3 · pith:W7MCWXLWnew · submitted 2025-06-03 · 🪐 quant-ph · math-ph· math.MP· nucl-th· physics.atom-ph· physics.optics

Permutation-Invariant N-body gates via Tavis-Cummings Hamiltonian

classification 🪐 quant-ph math-phmath.MPnucl-thphysics.atom-phphysics.optics
keywords gatesglobalswapinteractionmulti-qubitqubitscontrolcontrolled-z
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Global control provides a promising route to implementing multi-qubit gates without individual qubit addressing. This is especially appealing for permutation-invariant (PI) gates, whose symmetry is often broken when they are compiled into individually addressed one- and two-qubit gates. Important examples include SWAP, $\sqrt{i\text{SWAP}}$, and the n-qubit controlled-Z gate, which is equivalent, up to two single-qubit Hadamard gates, to the multi-qubit Toffoli gate. Motivated by this global-control perspective, we show that all PI unitaries on an arbitrary number of qubits can be realized using the Tavis-Cummings (TC) interaction, the multi-qubit version of the Jaynes-Cummings interaction, together with global uniform z and x fields. Here, the $n$ qubits are identically coupled to a single bosonic mode (oscillator), which is initialized in and returned to its vacuum state. A corollary is that all PI states, including GHZ and Dicke states, can be prepared using the same global control. For the case n=2 qubits, which is particularly important in quantum computing, we also find explicit pulse sequences for implementing all PI qubit unitaries that conserve angular momentum in the z direction, using only the TC interaction and global z fields. This includes controlled-Z, SWAP, and $\sqrt{i\text{SWAP}}$.

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