arXiv subjects
Publications and source records attributed to Waldemar Sieg.
The classical Borsuk's non-retract theorem asserts that a unit sphere in $\mathbb{R}^n$ is not a continuous retract of the unit closed ball. We will show that such a unit sphere is a piecewise continuous retract of the unit closed ball.
Let $X$ and $Y$ be the Hausdorff topological spaces and let $A$ be both an $\fs$- and $\gd$- subset of $X$. Let also $f\cn A\to Y$ be a function for which the inverse image of every open subset $U\subset Y$ is $\fs$ in $X$. We show that $f$ can be linearly extended to a function with the same property defined on $X$. A similar result is proved for Baire-one function defined on an analogous subset of $\mR$. We give also an answer when the extension map is (with a supremum norm) an isometry.
Let $\Omega$ be a perfectly normal topological space, let $A$ be a non-empty $G_\delta$-subset of $\Omega$ and let $B_1(A)$ denote the space of all functions $A\to\mathbb{R}$ of Baire-one class on $A$. Let also $\|\cdot\|_\infty$ be the supremum norm. The symbol $\chi_A$ stands for the characteristic function of $A$. We prove that for every bounded function $f\in B_1(A)$ there is a sequence $(H_n)$ of both $F_\sigma$- and $G_\delta$-subsets of $\Omega$ such that the function $\overline{f}\colon\Omega\to\mathbb{R}$ given by the uniformly convergent series on $\Omega$ with the formula: $\overline{f}:=c\sum_{n=0}^\infty\left(\frac{2}{3}\right)^{n+1}\left(\frac{1}{2}-\chi_{H_n}\right)$ extends $f$ with $\overline{f}\in B_1(\Omega)$ and the condition ($\triangle$) of the form: $\|f(A)\|_\infty=\|\overline{f}(\Omega)\|_\infty$. We apply the above series to obtain an extension of $f$ positive to $\overline{f}$ positive with the condition ($\triangle$). A similar technique allows us to obtain an extension of Baire-alpha function on $A$ to Baire-alpha function on $\Omega$.
We characterise the class of uniform limits of functions from Pawlak's class $\mathcal B_1^{**}$. The resulting class $u\mathscr S_1$, which contains functions with the oscillation rank one, is discussed in connection with its linear span. We apply a general, topological space, setting in our discussion.