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Quantum Overlapping Tomography
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abstract
It is now experimentally possible to entangle thousands of qubits, and efficiently measure each qubit in parallel in a distinct basis. To fully characterize an unknown entangled state of $n$ qubits, one requires an exponential number of measurements in $n$, which is experimentally unfeasible even for modest system sizes. By leveraging (i) that single-qubit measurements can be made in parallel, and (ii) the theory of perfect hash families, we show that all $k$-qubit reduced density matrices of an $n$ qubit state can be determined with at most $e^{\mathcal{O}(k)} \log^2(n)$ rounds of parallel measurements. We provide concrete measurement protocols which realize this bound. As an example, we argue that with current experiments, the entanglement between every pair of qubits in a system of 1000 qubits could be measured and completely characterized in a few days. This corresponds to completely characterizing entanglement of nearly half a million pairs of qubits.
Forward citations
Cited by 2 Pith papers
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Optimal estimation of high-dimensional quantum states using locally gentle measurements
α-gentle tomography of rank-r qudits has minimax Frobenius rate Θ(rd²/(nα²)), with gentleness penalty scaling as ambient dimension d rather than parameter count rd.
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Locally Gentle State Certification for High Dimensional Quantum Systems
Locally α-gentle quantum state certification against the maximally mixed state has minimax sample complexity Θ(d^3/(ε^2 α^2)) for fixed unentangled measurements, a factor d/α^2 over the non-gentle rate.
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