j_max dependence of the running coupling in 2+1D SU(2) Hamiltonian lattice gauge theory
Determine whether the renormalization group running of the dimensionless coupling ag^2 in the 2+1-dimensional SU(2) Hamiltonian lattice gauge theory depends non-trivially on the local Hilbert space truncation parameter j_max as the lattice spacing a approaches zero, and, if so, characterize this dependence analytically and validate it with numerical calculations along the continuum limit trajectory.
References
Whether the running coupling has a non-trivial dependence on $j_{\rm max}$ should be studied analytically and tested against numerical calculations, which are left for future work.
However, it is an interesting question of how large this truncation has to be to retrieve the continuum physics and whether there is some assistance provided by gauge invariance and universality in this context. For example, in one dimension, we found that one can obtain an accurate central charge even with $j_\text{max}=1/2$. We leave these questions regarding higher dimensions for future work.
A systematic quantitative characterization of the scaling of observables with $R_{\rm max}$ and the gauge coupling $g$, particularly toward the weak-coupling regime, remains an open question.