[Levin, FOCS-88], studied invariant characteristics $ f(x) $ of strings $ x $. It set no restrictions at all (even computability) on $ f $, except invariance $ f(x)= f(c(x)) \pm O(1) $ under simple encodings (i.e. change of representation) $ c(x) $. In contrast, it restricted $ c $ severely, allowing only $ c $ computable and invertible in polynomial time and preserving length $ \|x\|\pm O(1) $. Two examples of $ f $ are $ \|x\| $ (artificially required to be invariant) and Kolmogorov complexity $ K(x) $. I first considered strings $ x $ generated with polynomial time computable probability distributions $ m $. On such $ x $ all invariants $ f $, despite their generality, turn out to be determined by $ \|x\|,K(x) $, i.e. $ f(x)=f'(K(x),\|x\|)\pm O(\log(r(x))) $, where the expectation $ \sum_x m(x)r(x) $ is $ \le1 $. It still remains a challenge to find an elementary proof of this general statement. (Known proof uses constructive expanders.) Strings with samplable distributions turn out to be much richer with many more invariants possible.
Several of my papers study models of computations. In [Gacs, Levin 81] we consider the general hardware-independent model: "causal nets". It allows to introduce general (but tight) measures of complexity and treat other measures as geometric issues of embedding the net into the space-time of a particular hardware. Causal nets also allow an exact characterization of computability of recursive functions which allow symmetric input configurations: some are not computable since initial symmetries cannot be broken deterministically.
[Itkis, Levin, FOCS-89] considers VLSI models. Traditional ones assume wires of constant width, taking most of chip's area, often squaring it. These models also assume switching time depending only on chip's diameter $ D $, even if all wires are much shorter than $ D $. Later models allow switching time $ f(d) $ to decrease with wires length $ d $ (e.g., linearly, or even quadratically.) We show that for superlinear (even slightly) $ f $, the chips' computational power loses any sensitivity to wires width. It is as strong as it would be if wires' were infinitesimally thin, all area used for nodes. We simulate such wires by arranging cooperation of nodes to transport data to each other in parallel so that no delays could occur even in the worst case.
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