Optimal lower bounds for quantum state tomography
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Abstract (arXiv)
We show that n = Omega(rd/varepsilon2) copies are necessary to learn a rank r mixed state ρ ∈ mathbbCd × d up to error varepsilon in trace distance. This matches the upper bound of n = O(rd/varepsilon2) from prior work, and therefore settles the sample complexity of mixed state tomography. We prove this lower bound by studying a special case of full state tomography that we refer to as projector tomography, in which ρ is promised to be of the form ρ = P/r, where P ∈ mathbbCd × d is a rank r projector. A key technical ingredient in our proof, which may be of independent interest, is a reduction which converts any algorithm for projector tomography which learns to error varepsilon in trace distance to an algorithm which learns to error O(varepsilon) in the more stringent Bures distance.
Key facts. Cited by 2 papers in the map (data through 14 Oct 2026). First posted on arXiv 9 Oct 2025.
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