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Learning Quantum Processes and Hamiltonians via the Pauli Transfer Matrix

Matthias C. Caro

TL;DR

The paper demonstrates that learning an unknown $n$-qubit quantum process via Pauli transfer matrices is exponentially easier with a quantum memory than without one. By recasting PTM learning as shadow tomography on the Choi state and employing Pauli shadow tomography, it achieves $O\left((n+\log(1/\delta))/\varepsilon^4\right)$ copies to learn all PTM entries, while memoryless strategies require $\Omega\left(4^n/\varepsilon^2\right)$ queries. It extends these results to predicting expectation values under sparsity constraints, and shows how PTM learning serves as a subroutine for learning arbitrary Hamiltonians via short-time dynamics and polynomial interpolation. The work situates these results within shadow tomography, classical shadows, and channel-learning literature, and provides explicit lower bounds for memoryless models under channel-promises such as doubly-stochasticity and entanglement-breaking behavior. Overall, the results highlight a robust quantum memory–enabled advantage for learning highly complex quantum dynamics, with practical implications for efficiently characterizing quantum processes and Hamiltonians on near-term devices.

Abstract

Learning about physical systems from quantum-enhanced experiments, relying on a quantum memory and quantum processing, can outperform learning from experiments in which only classical memory and processing are available. Whereas quantum advantages have been established for a variety of state learning tasks, quantum process learning allows for comparable advantages only with a careful problem formulation and is less understood. We establish an exponential quantum advantage for learning an unknown $n$-qubit quantum process $\mathcal{N}$. We show that a quantum memory allows to efficiently solve the following tasks: (a) learning the Pauli transfer matrix of an arbitrary $\mathcal{N}$, (b) predicting expectation values of bounded Pauli-sparse observables measured on the output of an arbitrary $\mathcal{N}$ upon input of a Pauli-sparse state, and (c) predicting expectation values of arbitrary bounded observables measured on the output of an unknown $\mathcal{N}$ with sparse Pauli transfer matrix upon input of an arbitrary state. With quantum memory, these tasks can be solved using linearly-in-$n$ many copies of the Choi state of $\mathcal{N}$, and even time-efficiently in the case of (b). In contrast, any learner without quantum memory requires exponentially-in-$n$ many queries, even when querying $\mathcal{N}$ on subsystems of adaptively chosen states and performing adaptively chosen measurements. In proving this separation, we extend existing shadow tomography upper and lower bounds from states to channels via the Choi-Jamiolkowski isomorphism. Moreover, we combine Pauli transfer matrix learning with polynomial interpolation techniques to develop a procedure for learning arbitrary Hamiltonians, which may have non-local all-to-all interactions, from short-time dynamics. Our results highlight the power of quantum-enhanced experiments for learning highly complex quantum dynamics.

Learning Quantum Processes and Hamiltonians via the Pauli Transfer Matrix

TL;DR

The paper demonstrates that learning an unknown -qubit quantum process via Pauli transfer matrices is exponentially easier with a quantum memory than without one. By recasting PTM learning as shadow tomography on the Choi state and employing Pauli shadow tomography, it achieves copies to learn all PTM entries, while memoryless strategies require queries. It extends these results to predicting expectation values under sparsity constraints, and shows how PTM learning serves as a subroutine for learning arbitrary Hamiltonians via short-time dynamics and polynomial interpolation. The work situates these results within shadow tomography, classical shadows, and channel-learning literature, and provides explicit lower bounds for memoryless models under channel-promises such as doubly-stochasticity and entanglement-breaking behavior. Overall, the results highlight a robust quantum memory–enabled advantage for learning highly complex quantum dynamics, with practical implications for efficiently characterizing quantum processes and Hamiltonians on near-term devices.

Abstract

Learning about physical systems from quantum-enhanced experiments, relying on a quantum memory and quantum processing, can outperform learning from experiments in which only classical memory and processing are available. Whereas quantum advantages have been established for a variety of state learning tasks, quantum process learning allows for comparable advantages only with a careful problem formulation and is less understood. We establish an exponential quantum advantage for learning an unknown -qubit quantum process . We show that a quantum memory allows to efficiently solve the following tasks: (a) learning the Pauli transfer matrix of an arbitrary , (b) predicting expectation values of bounded Pauli-sparse observables measured on the output of an arbitrary upon input of a Pauli-sparse state, and (c) predicting expectation values of arbitrary bounded observables measured on the output of an unknown with sparse Pauli transfer matrix upon input of an arbitrary state. With quantum memory, these tasks can be solved using linearly-in- many copies of the Choi state of , and even time-efficiently in the case of (b). In contrast, any learner without quantum memory requires exponentially-in- many queries, even when querying on subsystems of adaptively chosen states and performing adaptively chosen measurements. In proving this separation, we extend existing shadow tomography upper and lower bounds from states to channels via the Choi-Jamiolkowski isomorphism. Moreover, we combine Pauli transfer matrix learning with polynomial interpolation techniques to develop a procedure for learning arbitrary Hamiltonians, which may have non-local all-to-all interactions, from short-time dynamics. Our results highlight the power of quantum-enhanced experiments for learning highly complex quantum dynamics.
Paper Structure (34 sections, 34 theorems, 105 equations, 3 figures)

This paper contains 34 sections, 34 theorems, 105 equations, 3 figures.

Key Result

Theorem 1.1

There is a learning algorithm with quantum memory that uses $\mathcal{O}(n/\varepsilon^4)$ copies of the Choi state of an unknown $n$-qubit quantum channel $\mathcal{N}$ to output simultaneously $\varepsilon$-accurate estimates for all the $16^n$ entries $\tfrac{1}{2^n}\tr[\sigma_A \mathcal{N}(\sigm

Figures (3)

  • Figure 1: Illustration of learning quantum channels from general channel access, each panel to be read from left to right. Panel (a) depicts a learner without quantum memory, panel (b) depicts a learner with quantum memory.
  • Figure 2: Illustration of learning quantum channels from Choi access, each panel to be read from bottom to top. Panel (a) depicts a learner without quantum memory, panel (b) depicts a learner with quantum memory.
  • Figure 3: Illustration of learning quantum channels from parallel access, each panel to be read from bottom to top. Panel (a) depicts a learner without quantum memory, panel (b) depicts a learner with quantum memory.

Theorems & Definitions (92)

  • Theorem 1.1: Pauli transfer matrix learning with and without quantum memory
  • Corollary 1.2: Predicting Pauli-sparse expectation values for arbitrary channels
  • Theorem 1.3: Learning arbitrary Hamiltonians with quantum memory
  • Definition 2.1: Quantum channels
  • Proposition 2.2: Choi-Jamiolkowski isomorphism jamiolkowski1972linearchoi1975completely
  • Proposition 2.3: Properties of the Choi-Jamiolkowski isomorphism (see, e.g., wolf2012quantumchannels)
  • Definition 2.4: General transfer matrices
  • Definition 2.5: Local transfer matrices
  • Example 2.6: Pauli transfer matrix
  • Definition 2.7: Learning quantum channels without quantum memory chen2021exponential-arxiv
  • ...and 82 more