Fingerprinting Codes Meet Geometry: Improved Lower Bounds for Private Query Release and Adaptive Data Analysis

December 18, 2024 Β· Declared Dead Β· πŸ› Symposium on the Theory of Computing

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Authors Xin Lyu, Kunal Talwar arXiv ID 2412.14396 Category cs.DS: Data Structures & Algorithms Cross-listed cs.CR, cs.LG Citations 2 Venue Symposium on the Theory of Computing Last Checked 4 months ago
Abstract
Fingerprinting codes are a crucial tool for proving lower bounds in differential privacy. They have been used to prove tight lower bounds for several fundamental questions, especially in the ``low accuracy'' regime. Unlike reconstruction/discrepancy approaches however, they are more suited for query sets that arise naturally from the fingerprinting codes construction. In this work, we propose a general framework for proving fingerprinting type lower bounds, that allows us to tailor the technique to the geometry of the query set. Our approach allows us to prove several new results, including the following. First, we show that any (sample- and population-)accurate algorithm for answering $Q$ arbitrary adaptive counting queries over a universe $\mathcal{X}$ to accuracy $Ξ±$ needs $Ξ©(\frac{\sqrt{\log |\mathcal{X}|}\cdot \log Q}{Ξ±^3})$ samples, matching known upper bounds. This shows that the approaches based on differential privacy are optimal for this question, and improves significantly on the previously known lower bounds of $\frac{\log Q}{Ξ±^2}$ and $\min(\sqrt{Q}, \sqrt{\log |\mathcal{X}|})/Ξ±^2$. Second, we show that any $(\varepsilon,Ξ΄)$-DP algorithm for answering $Q$ counting queries to accuracy $Ξ±$ needs $Ξ©(\frac{\sqrt{ \log|\mathcal{X}| \log(1/Ξ΄)} \log Q}{\varepsilonΞ±^2})$ samples, matching known upper bounds up to constants. Our framework allows for proving this bound via a direct correlation analysis and improves the prior bound of [BUV'14] by $\sqrt{\log(1/Ξ΄)}$. Third, we characterize the sample complexity of answering a set of random $0$-$1$ queries under approximate differential privacy. We give new upper and lower bounds in different regimes. By combining them with known results, we can complete the whole picture.
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