I am currently reading the paper Quantum Group Particles and Non-Archimedean Geometry by Volovich and Aref'eva. Here they discuss the difference between $q$-deformation and $\hslash$-deformation. In a classical system, one has $$ \begin{align} x_ix_j&=x_jx_i\\ p_ip_j&=p_jp_i\\ p_ix_j&=x_jp_i, \end{align} $$ where $x_i$ and $p_i$ are position and momentum, respectively. Then an $\hslash$-deformation gives $$ \begin{align} [x_i,x_j]&=0\\ [p_i,p_j]&=0\\ [p_i,x_j]&=i\hslash \delta_{ij}, \end{align} $$ where $\delta_{ij}$ is the Kronecker delta. This is a quantum system, and I am familiar with this. Then they say that a $q$-deformation gives $$ \begin{align} x_ix_j&=qx_jx_i, \quad i<j,\\ p_ip_j&=qp_jp_i\\ p_ix_j&=qx_jp_i + ..., \end{align} $$ which is different from an $\hslash$-deformation. This seems to be in connection with what is called a quantum line or quantum plane.
My questions are:
1) What is the physical interpretation of $q$-deformation? It doesn't look like it is the same as going from classical mechanics to quantum mechanics. I have seen $q$-deformation in the case of quantum groups, though nothing was said about the physical interpretation.
2) What is the physical interpretation of a quantum line or quantum plane?
Thanks in advance!