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Intrinsic-Dimensional Wasserstein Guarantees for Private Synthetic Measures

Abstract

We study an ε-differentially private synthetic measure for n points in [0,1]d by applying the existing PrivTree algorithm to construct an adaptive binary partition and then privately releasing its leaf masses. We consider the worst-case data model without any sampling or population-distribution assumption. The 1-Wasserstein error of the synthetic measure is Õd((ε n)−1/d) for d≥2, which is optimal compared to the minimax lower bound up to a logarithmic factor. Moreover, for d≥3 and 2<s≤ d, if the data set has covering number at most Ar−s over the relevant finite range of scales r, the expected error improves to Õd,s((ε n)−1/s). Thus the rate depends on a finite-scale intrinsic dimension rather than the ambient dimension, without requiring the recovery of a low-dimensional manifold. We also introduce a shifting technique to further avoid the exponential dependence of the constant on the ambient dimension d.

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BibTeX
@misc{he2026intrinsicdimensional,
  title = {{Intrinsic-Dimensional Wasserstein Guarantees for Private Synthetic Measures}},
  author = {Yiyun He},
  howpublished = {arXiv},
  year = {2026},
  month = sep,
  doi = {10.48550/arxiv.2609.17624},
  eprint = {2609.17624},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2609.17624},
}
RIS
TY  - UNPB
TI  - Intrinsic-Dimensional Wasserstein Guarantees for Private Synthetic Measures
AU  - Yiyun He
PY  - 2026
DA  - 2026/09/15
PB  - arXiv
DO  - 10.48550/arxiv.2609.17624
UR  - https://arxiv.org/abs/2609.17624
AB  - We study an ε-differentially private synthetic measure for n points in [0,1]^d by applying the existing PrivTree algorithm to construct an adaptive binary partition and then privately releasing its leaf masses. We consider the worst-case data model without any sampling or population-distribution assumption. The 1-Wasserstein error of the synthetic measure is Õ_d((ε n)^−1/d) for d≥2, which is optimal compared to the minimax lower bound up to a logarithmic factor. Moreover, for d≥3 and 2<s≤ d, if the data set has covering number at most Ar^−s over the relevant finite range of scales r, the expected error improves to Õ_d,s((ε n)^−1/s). Thus the rate depends on a finite-scale intrinsic dimension rather than the ambient dimension, without requiring the recovery of a low-dimensional manifold. We also introduce a shifting technique to further avoid the exponential dependence of the constant on the ambient dimension d.
ER  -