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Quantum Occam Learning: Sample-Supported Expressibility for Circuit-Based Quantum Learning
arXiv
Authors: Jeongho Bang, Kyoungho Cho, Jeongwoo Jae
Year
2026
Paper ID
68806
Status
Preprint
Abstract Read
~2 min
Abstract Words
231
Citations
N/A
Abstract
A central principle in quantum machine learning is that an ansatz should be expressive enough to represent the quantum data of interest. Yet, the expressibility is statistically meaningful only insofar as it can be learned from finitely many copies of an unknown quantum state. In this work, we develop an information-theoretic Occam theory for quantum data generated by finite-size quantum circuits. For the class Sn,G of n-qubit pure states preparable with at most G two-qubit gates, a metric-entropy argument gives the realizable sample law widetildeΘ\(G/ε2\) in the circuit-limited regime. For an arbitrary source hatρ, we introduce the best G-gate approximation error dG\(hatρ\) and the approximate circuit complexity C_η\(hatρ\). We prove an agnostic quantum Occam theorem: with M copies, one can learn up to the best G-gate approximation error plus a statistical penalty widetilde{O}\(sqrt{G/M}\). We then remove the need to know G in advance through an adaptive model-selection theorem whose oracle inequality selects the circuit complexity justified by the data. Matching lower bounds yield a sample-supported expressibility law: at trace-distance accuracy ε, M samples can support only Grm supported simeq Mε2 gates, up to logarithmic factors and tomography saturation at 2n. Thus, the circuit complexity becomes an adaptive statistical resource rather than a static promise. Our framework turns bounded circuit complexity into a model-selection principle for quantum machine learning.
Why This Paper Matters
- This paper contributes to the Quantum Machine Learning research area in the Quantum Articles archive.
- It adds a 2026 reference point for readers tracking recent quantum research.
- A central principle in quantum machine learning is that an ansatz should be expressive enough to represent the quantum data of interest.
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