Fractals and Universal Spaces in Dimension Theory - download pdf or read online

By Stephen Lipscomb

ISBN-10: 0387854932

ISBN-13: 9780387854939

ISBN-10: 0387854940

ISBN-13: 9780387854946

For metric areas the search for common areas in size concept spanned nearly a century of mathematical study. The historical past breaks evidently into sessions — the classical (separable metric) and the fashionable (not unavoidably separable metric). whereas the classical concept is now good documented in different books, this can be the 1st ebook to unify the fashionable thought (1960 – 2007). just like the classical conception, the fashionable thought essentially consists of the unit interval.

By the Seventies, the writer of this monograph generalized Cantor’s 1883 building (identify adjacent-endpoints in Cantor’s set) of the unit period, acquiring — for any given weight — a one-dimensional metric area that comprises rationals and irrationals as opposite numbers to these within the unit interval.

Following the advance of fractal geometry throughout the Eighties, those new areas became out to be the 1st examples of attractors of limitless iterated functionality structures — “generalized fractals.” using snap shots to demonstrate the fractal view of those areas is a distinct characteristic of this monograph. moreover, this publication offers ancient context for similar study that comes with imbedding theorems, graph concept, and closed imbeddings.

This monograph may be priceless to topologists, to mathematicians operating in fractal geometry, and to historians of arithmetic. it could possibly additionally function a textual content for graduate seminars or self-study — the reader will locate many suitable open difficulties that may encourage extra examine into those topics.

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Extra resources for Fractals and Universal Spaces in Dimension Theory

Example text

Xb1 xb2 · · · = θb = ψβ ◦ πβ (θ) (b ∈ A ; β = p(b)) such that xbi = 1 implies (xci = 0 for each c ∈ A \ {b}). Moreover, from this no-carry property, Σb∈A θb ≤ 1, and consequently (θb )b∈A ∈ l2 (A ). Proof. Let φ : JA → N (A) be a “choice function” such that φ(θ) = a1 a2 · · · ∈ θ selects a member φ(θ) of the equivalence class θ ∈ JA . 1, we have θb = ψβ ◦ πβ (θ) = p1 ◦ ψb ◦ πb (a1 a2 · · · ) = p1 ◦ ψb (ab1 ab2 · · · ) = ∞ b i i=1 xi /2 , where (2) xbi = 1 ⇔ abi = b ⇔ ai = b and xbi = 0 ⇔ abi = b ⇔ ai = b.

4 The “no-carry property” encoded in N ({z, a, b}). Let δ = ba ∈ N (A). Then viewing “z” as “zero” and “zeroing out all letters not equal to a” we project δ = ba → δ a = za ∈ N ({z, a}) where N ({z, a}) is a copy of Cantor’s set with endpoints z and a. Similarly, by “zeroing out all letters not equal to b” we project δ = ba → δ b = bz ∈ N ({z, b}). 5 Example. We illustrate how the no-carry property in N ({z, a, b}) encodes the no-carry property of the Sierpi´ nski triangle T : First, identify the letter “a” with “1” and the letter “z” with “0”, inducing a homeomorphism §12 25 STAR SPACES N ({z, a}) ↔ N ({0, 1}).

JA πβ ψb ..................................................... I(ζ, β) ψβ C(0, 1) ... ... p 1 ... ... [0, 1] Fig. 2 For b ∈ A , the mapping gb maps N (A) into [0, 1]. , if θ = p(δ), then each gb (δ) = θb and g(δ) = (gb (δ)) = (θb ) = f (θ). g ................................................................ N (A) ωA . .... .... . ... ... .... ... ..... . p f JA Since f is injective and g = f ◦ p we see that g and p have the same fibers g −1 (f (θ)) = p−1 ◦ f −1 (f (θ)) = p−1 (θ).

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