Optimal estimates of trace distance between bosonic Gaussian states and applications to learning
1Dahlem Center for Complex Quantum Systems, Freie Universität Berlin, 14195 Berlin, Germany
2NEST, Scuola Normale Superiore and Istituto Nanoscienze, Piazza dei Cavalieri 7, IT-56126 Pisa, Italy
3QuSoft, Science Park 123, 1098 XG Amsterdam, the Netherlands
4Korteweg–de Vries Institute for Mathematics, University of Amsterdam, Science Park 105-107, 1098 XG Amsterdam, the Netherlands
5Scuola Normale Superiore, Piazza dei Cavalieri 7, 56126 Pisa, Italy
6Institute for Theoretical Physics, University of Amsterdam, Science Park 904, 1098 XH Amsterdam, the Netherlands
| Published: | 2025-06-12, volume 9, page 1769 |
| Editor: | Daniel Malz |
| Eprint: | arXiv:2411.02368v4 |
| Doi: | https://doi.org/10.22331/q-2025-06-12-1769 |
| Citation: | Quantum 9, 1769 (2025). |
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Abstract
Gaussian states of bosonic quantum systems enjoy numerous technological applications and are ubiquitous in nature. Their significance lies in their simplicity, which in turn rests on the fact that they are uniquely determined by two experimentally accessible quantities, their first and second moments. But what if these moments are only known approximately, as is inevitable in any realistic experiment? What is the resulting error on the Gaussian state itself, as measured by the most operationally meaningful metric for distinguishing quantum states, namely, the trace distance? In this work, we fully resolve this question by demonstrating that if the first and second moments are known up to an error $\varepsilon$, the trace distance error on the state also scales as $\varepsilon$, and this functional dependence is optimal. To prove this, we establish tight bounds on the trace distance between two Gaussian states in terms of the norm distance of their first and second moments. As an application, we improve existing bounds on the sample complexity of tomography of Gaussian states.

Featured image: Trace distance upper bound between two Gaussian states in terms of their covariance matrices' distance.
Popular summary
Gaussian states—such as coherent and squeezed states—are among the most important states in quantum optics and continuous-variable quantum information. Their widespread use comes from a remarkable feature: a Gaussian state is completely determined by just two quantities—its first moments (like average position and momentum) and second moments (like variances and covariances). These are quantities that can, in principle, be measured directly in the lab.
But no real experiment can measure with perfect accuracy. So what happens when these moments are only known approximately—say, with error at most $\varepsilon$? How close is the corresponding Gaussian state to the true one?
In this work, we provide a complete and optimal answer to this fundamental question. We prove that if the first and second moments are known up to error $\varepsilon$, then the error on the full quantum state—measured using the trace distance, which quantifies how well two quantum states can be distinguished—also scales linearly with $\varepsilon$. This scaling is not just a bound: it is optimal. No better general relationship is possible.
As a key application, we sharpen existing bounds on the sample complexity of Gaussian state tomography—that is, the number of measurements required to reconstruct an unknown Gaussian state from experimental data.
To reach this result, we develop sharp bounds linking trace distance and moment errors, and introduce a new tool—the derivative of a Gaussian state—which sheds light on the differential geometry of the Gaussian state manifold.
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[4] Xiaobin Zhao, Pengcheng Liao, Francesco Anna Mele, Ulysse Chabaud, and Quntao Zhuang, "Complexity of quantum tomography from genuine non-Gaussian entanglement", Nature Communications 17 1, 373 (2025).
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