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Optimal tradeoffs for estimating Pauli observables

Sitan Chen, Weiyuan Gong, Qi Ye

TL;DR

For any subset of Paulis and any family of measurement strategies, the optimal sample complexity is completely characterize, up to <tex>$\log\vert A\vert$</tex> factors.

Abstract

We revisit the problem of Pauli shadow tomography: given copies of an unknown $n$-qubit quantum state $ρ$, estimate $\text{tr}(Pρ)$ for some set of Pauli operators $P$ to within additive error $ε$. This has been a popular testbed for exploring the advantage of protocols with quantum memory over those without: with enough memory to measure two copies at a time, one can use Bell sampling to estimate $|\text{tr}(Pρ)|$ for all $P$ using $O(n/ε^4)$ copies, but with $k\le n$ qubits of memory, $Ω(2^{(n-k)/3})$ copies are needed. These results leave open several natural questions. How does this picture change in the physically relevant setting where one only needs to estimate a certain subset of Paulis? What is the optimal dependence on $ε$? What is the optimal tradeoff between quantum memory and sample complexity? We answer all of these questions. For any subset $A$ of Paulis and any family of measurement strategies, we completely characterize the optimal sample complexity, up to $\log |A|$ factors. We show any protocol that makes $\text{poly}(n)$-copy measurements must make $Ω(1/ε^4)$ measurements. For any protocol that makes $\text{poly}(n)$-copy measurements and only has $k < n$ qubits of memory, we show that $\widetildeΘ(\min\{2^n/ε^2, 2^{n-k}/ε^4\})$ copies are necessary and sufficient. The protocols we propose can also estimate the actual values $\text{tr}(Pρ)$, rather than just their absolute values as in prior work. Additionally, as a byproduct of our techniques, we establish tight bounds for the task of purity testing and show that it exhibits an intriguing phase transition not present in the memory-sample tradeoff for Pauli shadow tomography.

Optimal tradeoffs for estimating Pauli observables

TL;DR

For any subset of Paulis and any family of measurement strategies, the optimal sample complexity is completely characterize, up to <tex></tex> factors.

Abstract

We revisit the problem of Pauli shadow tomography: given copies of an unknown -qubit quantum state , estimate for some set of Pauli operators to within additive error . This has been a popular testbed for exploring the advantage of protocols with quantum memory over those without: with enough memory to measure two copies at a time, one can use Bell sampling to estimate for all using copies, but with qubits of memory, copies are needed. These results leave open several natural questions. How does this picture change in the physically relevant setting where one only needs to estimate a certain subset of Paulis? What is the optimal dependence on ? What is the optimal tradeoff between quantum memory and sample complexity? We answer all of these questions. For any subset of Paulis and any family of measurement strategies, we completely characterize the optimal sample complexity, up to factors. We show any protocol that makes -copy measurements must make measurements. For any protocol that makes -copy measurements and only has qubits of memory, we show that copies are necessary and sufficient. The protocols we propose can also estimate the actual values , rather than just their absolute values as in prior work. Additionally, as a byproduct of our techniques, we establish tight bounds for the task of purity testing and show that it exhibits an intriguing phase transition not present in the memory-sample tradeoff for Pauli shadow tomography.
Paper Structure (56 sections, 43 theorems, 138 equations, 7 figures, 1 table, 5 algorithms)

This paper contains 56 sections, 43 theorems, 138 equations, 7 figures, 1 table, 5 algorithms.

Key Result

Theorem 1

The sample complexity of Pauli shadow tomography for any $A\subseteq\pazocal{P}_n$ using $(c, \pazocal{M})$-protocols is characterized by the following quantity: where $\pazocal{D}(A)$ denotes the set of probability distributions over $A$. Specifically, for any $A\subseteq\pazocal{P}_n$, we have that:

Figures (7)

  • Figure 1: Comparison of bounds in \ref{['thm:PauliShadowAllK']} and \ref{['thm:Purity']}, and chen2022exponential for shadow tomography and purity testing.
  • Figure : (a) Learning without quantum memory
  • Figure : (a) Learning without quantum memory
  • Figure : (c) Learning with $c$-copy measurements
  • Figure : (e) $(c, \pazocal{M})$ learning protocols
  • ...and 2 more figures

Theorems & Definitions (76)

  • Theorem 1: Master theorem
  • Theorem 2
  • Theorem 3
  • Theorem 4
  • Theorem 5: Informal, see Theorem \ref{['thm:ccopyLower']}
  • Theorem 6
  • Theorem 7
  • Lemma 1: E.g., Lemma 4.10 in chen2022exponential
  • Lemma 2
  • Lemma 3: See, e.g., meleIntroductionHaarMeasure2023
  • ...and 66 more