As it was already mentioned by Christophe Leuridan for classical continued fraction
we have extended Gauss measure
$$d\overline{\nu}(x,y)=\frac{1}{\log2}\cdot\frac{dx\,dy}{(1+xy)^2}=\frac{1}{\log2}\cdot\begin{vmatrix} 1 & \mp x\\
\pm y & 1
\end{vmatrix}^{-2} dx\,dy,\qquad (x,y)\in[0,1]^2,$$
which is invariant under the map
$$\overline{T}:(x,y)\to\begin{cases}(\{1/x\},([1/x]+y)^{-1},&\text{ if }x\ne 0;\\
(x,y),&\text{ if }x= 0.
\end{cases}$$
Details can be found in the book
M. Iosifescu and C. Kraaikamp, Metrical theory of continued fractions, 2002.
From geometrical point of view this extended Gauss measure describes the distribution of reduced Voronoi bases $(b_1,b_2)$ with $b_1=(1,\mp x)$, $b_2=(\pm y,1)$ on the boundary of the unit square.
In dimension $3$ something similar is knowт for Voronoi-Minkowski continued fractions(see Three-dimensional continued fractions and Kloosterman sums). The measure has the form
$$\mathrm{const} \int_{\Pi}\frac{d\alpha'd\beta'd\gamma'}{(\det X)^3},$$
where $X=\begin{pmatrix}
1 & \alpha_2' & \pm\alpha_3'\\
-\beta_1' & 1 & \beta_3'\\
\gamma_1'&-\gamma_2'&1\\
\end{pmatrix}$ are matricies of reduced Minkowski bases and
$\alpha'=(\alpha_2',\alpha_3')$,
$\beta'=(\beta_1',\beta_3')$,
$\gamma'=(\gamma_1',\gamma_2')$.