Abstract

We present an extensive quantum Monte Carlo study of the Néel-valence bond solid (VBS) phase transition on rectangular and honeycomb lattice SU(NN) antiferromagnets in sign problem free models. We find that in contrast to the honeycomb lattice and previously studied square lattice systems, on the rectangular lattice for small NN a first order Néel-VBS transition is realized. On increasing N≥4N\geq 4, we observe that the transition becomes continuous and with the {\em same} universal exponents as found on the honeycomb and square lattices (studied here for N=5,7,10N=5,7,10), providing strong support for a deconfined quantum critical point. Combining our new results with previous numerical and analytical studies we present a general phase diagram of the stability of CPN−1\mathbb{CP}^{N-1} fixed points with qq-monopoles.

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