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We present results for lattice QCD in the limit of infinite gauge coupling,obtained from a worm-type Monte Carlo algorithm on a discrete spatial latticebut with continuous Euclidean time. This is obtained by sending both theanisotropy parameter gamma^2 \sim a/a_t and the number of time-slices N_\tau toinfinity, keeping the ratio \gamma^2/N_\tau \sim aT fixed. The obvious gain isthat no continuum extrapolation N_\tau -> \infty has to be carried out.Moreover, the algorithm is faster and the sign problem disappears. We compareour computations with those on discrete lattices. We determine the phasediagram as a function of temperature and baryon chemical potential.

Continuous Time Monte Carlo for Lattice QCD in the Strong Coupling Limit