A borderline case function
$f$ for
${{Q}_{\alpha }}\left( {{\mathbb{R}}^{n}} \right)$ spaces is defined as a Haar wavelet decomposition, with the coefficients depending on a fixed parameter
$\beta \,>\,0$ . On its support
${{I}_{0}}\,=\,{{\left[ 0,\,1 \right]}^{n}},\,f\left( x \right)$ can be expressed by the binary expansions of the coordinates of
$x$ . In particular,
$f\,=\,{{f}_{\beta }}\,\in \,{{Q}_{\alpha }}\left( {{\mathbb{R}}^{n}} \right)$ if and only if
$\alpha \,<\,\beta \,<\frac{n}{2}$ , while for
$\beta \,=\,\alpha $ , it was shown by Yue and Dafni that
$f$ satisfies a John–Nirenberg inequality for
${{Q}_{\alpha }}\left( {{\mathbb{R}}^{n}} \right)$ . When
$\beta \,\ne \,1$ ,
$f$ is a self-affine function. It is continuous almost everywhere and discontinuous at all dyadic points inside
${{I}_{0}}$ . In addition, it is not monotone along any coordinate direction in any small cube. When the parameter
$\beta \,\in \,\left( 0,\,1 \right)$ ,
$f$ is onto from
${{I}_{0}}$ to
$\left[ -\frac{1}{1-{{2}^{-\beta }}},\,\frac{1}{1-{{2}^{-\beta }}} \right]$ , and the graph of
$f$ has a non-integer fractal dimension
$n\,+\,1\,-\beta$ .