The log log jam in Gaussian state tomography
- URL: http://arxiv.org/abs/2607.12983v1
- Date: Tue, 14 Jul 2026 17:25:43 GMT
- Title: The log log jam in Gaussian state tomography
- Abstract summary: We show that any protocol that uses Gaussian measurements, even entangled or adaptively chosen ones, must incur a $log log E$ dependence.<n>With highly entangled, non-Gaussian measurements, one can learn $n$-mode pure Gaussian states with $O(n2 / 2)$ samples, independent of $E$.<n>Our results shed new light on the intriguing interplay between adaptivity, entanglement, and magic in quantum learning.
- Score: 30.395638404311537
- License: http://arxiv.org/licenses/nonexclusive-distrib/1.0/
- Abstract: Unlike in finite dimensions, quantum information in continuous-variable systems has the peculiar feature that without imposing physical constraints, the sample complexity of state tomography can be unbounded. Remarkably, this is even the case for state-of-the-art protocols for learning Gaussian states, which have finite-dimensional descriptions: the best known rates scale with $\log \log E$, where $E$ is the energy of the system. We prove this is not an artifact of existing analyses, but a fundamental limitation of the measurements used. We show: (1) Any protocol that uses Gaussian measurements, even entangled or adaptively chosen ones, must incur a $\log \log E$ dependence. This answers an open question posed by a number of previous works. (2) There is a smooth tradeoff between the number of rounds of adaptivity and the energy dependence, and we give a matching protocol achieving this interpolated rate. (3) With highly entangled, non-Gaussian measurements, one can learn $n$-mode pure Gaussian states with $O(n^2 / ε^2)$ samples, independent of $E$. This answers an open question posed by Chen et al. (4) A simple protocol based on the single-copy canonical phase POVM of Holevo and Helstrom learns single-mode pure Gaussian states with $O(1/ε^2)$ samples, again independent of $E$. Our results clarify the role of energy in bosonic state tomography and shed new light on the intriguing interplay between adaptivity, entanglement, and magic in quantum learning.
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