Shadow Tomography of Quantum States 3: Shadow Tomography Needs Ω(min{D², log M}/ε²) CopiesResearch Paper
Why count copies of a quantum state
A mixed state of a -dimensional quantum system is a positive semidefinite matrix of trace . Writing down takes about real numbers, and is exponential in the number of qubits, so learning in full is expensive. Holevo's theorem and the random access code bounds of Ambainis, Nayak, Ta-Shma and Vazirani say that an -qubit state carries far fewer usable classical bits than its amplitudes suggest. Shadow tomography, introduced by S. Aaronson (arXiv:1711.01053), makes this quantitative: given known two-outcome measurements , how many copies of an unknown are needed to estimate every acceptance probability to within ?
Aaronson shows that copies suffice, polylogarithmic in and . The question this mission addresses is the converse: how many copies are necessary. Section 6 of the paper proves two lower bounds. Theorem 16 gives even when and the are diagonal (a classical distribution). Theorem 19, the goal here, strengthens the dimension term to for genuinely quantum states.
Timeline:
- 2016: full tomography of a -dimensional state to trace-distance accuracy needs copies up to logarithmic factors, with upper and lower bounds by O'Donnell and Wright (arXiv:1508.01907) and Haah, Harrow, Ji, Wu and Yu (arXiv:1508.01797).
- 2017–2018: Aaronson poses shadow tomography (Problem 1), proves the polylogarithmic upper bound (Theorem 2), and proves the lower bounds of Theorems 16 and 19.
- 2020 onward: classical shadows (Huang, Kueng and Preskill, arXiv:2002.08953) and later shadow-tomography algorithms study the same estimation task with other measurement models and improved upper bounds.
Setting
Fix a dimension . A two-outcome measurement is a Hermitian matrix with ; it accepts with probability . The tensor power is the matrix of independent copies. A strategy using copies is a measurement of with finitely many outcomes , given by positive semidefinite matrices with , together with outputs . It succeeds on when, with probability at least over , for every .
The proof works with these further objects, all defined in the mission:
- an orthogonal projection onto an -dimensional subspace of (Hermitian, idempotent, trace );
- , the maximally mixed state on that subspace;
- ;
- the von Neumann entropy in bits, over the eigenvalues of ;
- for states and , the quantum mutual information with the classical index, .
Formalization targets
Goal: Theorem 19 (p. 23)
There are a universal constant and a threshold such that for all , all with and all , some measurements on force every strategy that succeeds on every mixed state to use
copies. The goal fixes only the shape , not a constant, so a sharper constant does not invalidate it.
Milestones (pp. 23–24)
The milestones follow the proof, which sets and :
- Eq. (2): for some and all large even there are projections of rank with for all .
- .
- for .
- The exact entropy , with the binary entropy, and the bound .
- when all have equal entropy.
Significance
Theorem 19 shows that the dependence of shadow tomography cannot be removed, and that for shadow tomography is as hard as full tomography: as grows the bound becomes the tomography lower bound, which it therefore contains. Compared with the classical Theorem 16, it shows that quantum states need quadratically more copies in the dimension term. The factor matches the upper bound of Proposition 20 for the decision version, so the -dependence of the lower bound is tight in that setting.
The results are proved in the paper; none of them has a machine-checked proof that we know of. Formalizing the argument requires von Neumann entropy and its additivity on tensor products, the bound , a Holevo-plus-Fano step that turns successful estimation into mutual information, and the existence of many nearly orthogonal half-dimensional subspaces. Each is reusable well beyond this mission.
Difficulty
The obvious attempt adapts the classical argument of Theorem 16, which hides subsets of in a biased distribution. Quantum states allow hidden subspaces instead of subsets, which is where comes from, but two steps change character. First, the hiding family must be shown to exist: Eq. (2) is a concentration statement for random subspaces, and the lemma the paper cites for it (Lemma 18) is misstated, as explained below. Second, the information bound must be carried out for quantum states: the step "learning from requires " needs Holevo's bound and Fano's inequality, adjusted for success probability rather than certainty.
Formalization scope
Matrices are Matrix n n ℂ over a finite index type; the goal uses . Conventions committed to:
- A mixed state is the published
WildeQIT.IsDensityOperator(positive semidefinite, trace ), reused as a reference item. - A strategy is a finite-outcome POVM on , indexed by
Fin k → Fin D, with deterministic outputs ; classical randomness can be absorbed into the outcome set. - Probabilities and traces are real parts of complex traces. Entropies use ; Lean's gives , and
vnEntropyreturns on non-Hermitian matrices, which no statement uses. - Added to the goal: the threshold on and (for , succeeds) and (for , the output succeeds with ). Problem 1's is dropped, an equivalent statement under clipping.
- The measurements are chosen before the strategy (for every strategy, the same ), which is the meaning of a lower bound.
A trivializing formalization is ruled out: the goal does not mention , , , or , the success condition quantifies over all mixed states rather than a vacuous class, and the measurements are fixed before the strategy.
Not drafted:
- Lemma 18 (pp. 22–23) is false as printed. Since , concentrates at , not . The proof needs only Eq. (2), which is centred correctly and is a milestone.
- Eq. (2) is stated as existence, not as "probability over Haar-random subspaces", because Mathlib has no Haar measure on the unitary group or the Grassmannian; existence is what the proof uses.
- " must be at least " is not drafted: as stated it is imprecise for success probability , and the correct Holevo–Fano form is left to the solver.
- The final combination , is the goal's last step.
Contributions welcome: proofs of the milestones; a Haar-measure version of Eq. (2); von Neumann entropy infrastructure (additivity, the dimension bound, concavity); Holevo's bound and Fano's inequality for finite-dimensional states.
Selected references
- S. Aaronson, Shadow Tomography of Quantum States, arXiv:1711.01053v2, 2018; STOC 2018. https://arxiv.org/abs/1711.01053
- P. Hayden, D. Leung, A. Winter, Aspects of generic entanglement, Comm. Math. Phys. 265, 2006. https://arxiv.org/abs/quant-ph/0407049
- R. O'Donnell, J. Wright, Efficient quantum tomography, STOC 2016. https://arxiv.org/abs/1508.01907
- J. Haah, A. W. Harrow, Z. Ji, X. Wu, N. Yu, Sample-optimal tomography of quantum states, IEEE Trans. Inf. Theory 63, 2017. https://arxiv.org/abs/1508.01797
- A. Ambainis, A. Nayak, A. Ta-Shma, U. Vazirani, Dense quantum coding and quantum finite automata, J. ACM 49, 2002. https://arxiv.org/abs/quant-ph/9804043
- H.-Y. Huang, R. Kueng, J. Preskill, Predicting many properties of a quantum system from very few measurements, Nature Physics 16, 2020. https://arxiv.org/abs/2002.08953