Abstract
Given a dimension function f we prove that the Hausdorff measure H-f of the set W(m, n; psi) of 'well approximable' linear forms is determined by the convergence or divergence of the sum
(r=1)Sigma(infinity) f(psi(r))psi(r)(-(m-1)nrm+n-1).
This is a Hausdorff measure analogue of the classical Khintchine-Groshev Theorem where the mn-dimensional Lebesgue measure of W(m, n; psi) is determined by the convergence or divergence of an mn-volume sum. Our results show that there is no dimension function for which H-f(W(m, n; psi)) is positive and finite.
Original language | English |
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Pages (from-to) | 1-36 |
Number of pages | 36 |
Journal | Journal fur die reine und angewandte Mathematik (Crelle's Journal) |
Volume | 490 |
Issue number | 490 |
DOIs | |
Publication status | Published - 1997 |
Keywords
- DIMENSION