In two space-time dimensions, there is a theory of Lorentzian quantum gravi
ty which can be defined by a rigorous, non-perturbative path integral and i
s inequivalent to the well-known theory of (Euclidean) quantum Liouville gr
avity. It has a number of appealing features: i) its quantum geometry is no
n-fractal, ii) it remains consistent when coupled to matter, even beyond th
e c=1 barrier, iii) it is closer to canonical quantization approaches than
previous path-integral formulations, and iv) its construction generalizes t
o higher dimensions.