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On the topology of Diophantine approximation spectra

Published online by Cambridge University Press:  02 May 2017

Damien Roy*
Affiliation:
Département de Mathématiques, Université d’Ottawa, 585 King Edward, Ottawa, Ontario K1N 6N5, Canada email droy@uottawa.ca
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Abstract

Fix an integer $n\geqslant 2$ . To each non-zero point $\mathbf{u}$ in $\mathbb{R}^{n}$ , one attaches several numbers called exponents of Diophantine approximation. However, as Khintchine first observed, these numbers are not independent of each other. This raises the problem of describing the set of all possible values that a given family of exponents can take by varying the point  $\mathbf{u}$ . To avoid trivialities, one restricts to points  $\mathbf{u}$ whose coordinates are linearly independent over  $\mathbb{Q}$ . The resulting set of values is called the spectrum of these exponents. We show that, in an appropriate setting, any such spectrum is a compact connected set. In the case $n=3$ , we prove moreover that it is a semi-algebraic set closed under component-wise minimum. For $n=3$ , we also obtain a description of the spectrum of the exponents $(\text{}\underline{\unicode[STIX]{x1D711}}_{1},\text{}\underline{\unicode[STIX]{x1D711}}_{2},\text{}\underline{\unicode[STIX]{x1D711}}_{3},\overline{\unicode[STIX]{x1D711}}_{1},\overline{\unicode[STIX]{x1D711}}_{2},\overline{\unicode[STIX]{x1D711}}_{3})$ recently introduced by Schmidt and Summerer.

Information

Type
Research Article
Copyright
© The Author 2017 
Figure 0

Figure 1. The combined graph of the integral 3-system of Example 2.4.

Figure 1

Figure 2. A simple chain in $\bar{\unicode[STIX]{x1D6E5}}^{(3)}$.

Figure 2

Figure 3. Joining two closed chains into a single one.

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Figure 4. A strict elementary path in $\bar{\unicode[STIX]{x1D6E5}}^{(3)}$.

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Figure 5. A strict elementary path visiting $C_{i}^{\ast }$.

Figure 5

Figure 6. A strict elementary path visiting $C_{i}$.

Figure 6

Figure 7. The case where $G\in (A,D]$.

Figure 7

Figure 8. The case where $G\in (\mathbf{f}_{2},A]$.