Random projection reduces the dimension of data while approximately preserving distances, and the Johnson–Lindenstrauss lemma states how many dimensions suffice. I derive three results and test them on 20,000 pairs of points from the UCI Spambase data (4,601 e-mails, 57 standardised features). First, for Gaussian projections the squared distortion ratio of every pair is exactly chi-squared with k degrees of freedom divided by k, whatever the data; per-pair Kolmogorov–Smirnov tests reject this at 5% in 2.4% to 5.8% of pairs, consistent with the nominal rate. Second, for any projection with independent entries of unit variance and fourth moment mu4, the variance of the ratio is [2 + (mu4 − 3)q]/k, where q = sum of x_i^4 over ||x||^4 measures how concentrated the pair's difference is on few coordinates. The empirical slopes of variance on q match (mu4 − 3)/k for Gaussian, Rademacher, Achlioptas and very sparse projections (for example −0.397 against −0.400 for Rademacher at k = 5). Third, the Dasgupta–Gupta union bound requires k = 254 to keep all 20,000 pairs within 50% distortion; in simulation 93% of Gaussian matrices already achieve this at k = 200 and 68% at k = 160. The bound's per-pair tail is loose by a factor of 15 at k = 40: it gives 0.378 where the exact probability is 0.025.
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Manoj Kumar Aguru (2026) studied this question.
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