A Quantized Johnson-Lindenstrauss Lemma: The Finding of Buffon's Needle

In 1733, Georges-Louis Leclerc, Comte de Buffon in France, set the ground of geometric probability theory by defining an enlightening problem: what is the probability that a needle thrown randomly on a ground made of equispaced parallel strips lies on two of them? In this paper, we show that the sol...

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Veröffentlicht in:IEEE transactions on information theory 2015-09, Vol.61 (9), p.5012-5027
1. Verfasser: Jacques, Laurent
Format: Artikel
Sprache:eng
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Zusammenfassung:In 1733, Georges-Louis Leclerc, Comte de Buffon in France, set the ground of geometric probability theory by defining an enlightening problem: what is the probability that a needle thrown randomly on a ground made of equispaced parallel strips lies on two of them? In this paper, we show that the solution to this problem, and its generalization to N dimensions, allows us to discover a quantized form of the Johnson-Lindenstrauss (JL) lemma, i.e., one that combines a linear dimensionality reduction procedure with a uniform quantization of precision δ > 0. In particular, given a finite set S ⊂ ℝ N of S points and a distortion level ϵ > 0, as soon as M > M 0 = O(ϵ -2 log S), we can (randomly) construct a mapping from (S, ℓ 2 ) to (δℤ M , ℓ 1 ) that approximately preserves the pairwise distances between the points of S. Interestingly, compared with the common JL lemma, the mapping is quasi-isometric and we observe both an additive and a multiplicative distortions on the embedded distances. These two distortions, however, decay as O((log S/M) 1/2 ) when M increases. Moreover, for coarse quantization, i.e., for high δ compared with the set radius, the distortion is mainly additive, while for small δ we tend to a Lipschitz isometric embedding. Finally, we prove the existence of a nearly quasi-isometric embedding of (S, ℓ 2 ) into (δℤ M , ℓ 2 ). This one involves a non-linear distortion of the ℓ 2 -distance in S that vanishes for distant points in this set. Noticeably, the additive distortion in this case is slower, and decays as O((log S/M) 1/4 ).
ISSN:0018-9448
1557-9654
DOI:10.1109/TIT.2015.2453355