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...
Gespeichert in:
Veröffentlicht in: | IEEE transactions on information theory 2015-09, Vol.61 (9), p.5012-5027 |
---|---|
1. Verfasser: | |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext bestellen |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
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 |