The quantum theory of general relativity at low energies

In quantum field theory there is now a well developed technique, effective field theory, which allows one to obtain low energy quantum predictions in ''non-renormalizable'' theories, using only the degrees of freedom and interactions appropriate for those energies. Whether or not general relativity is truly fundamental, at low energies it is automatically described as a quantum effective field theory and this allows a consistent framework for quantum gravity at ordinary energies. I briefly describe the nature and limits of the technique.