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Many model quantum spin systems have been proposed to realize critical points or phases described by 2+1 dimensional conformal gauge theories. On a torus of size and modular parameter , the energy levels of such gauge theories equal times universal functions of . We compute the universal spectrum of QED, a U(1) gauge theory with two-component massless Dirac fermions, in the large limit. We also allow for a Chern-Simons term at level , and show how the topological -fold ground state degeneracy in the absence of fermions transforms into the universal spectrum in the presence of fermions; these computations are performed at fixed in the large limit.

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