Spontaneous symmetry breaking can persist at all temperatures in certain biconical
O(N)×Z2 vector models when the underlying field theories are ultraviolet complete. So far, the existence of such theories has been established in fractional dimensions for local but nonunitary models or in
2+1 dimensions but for nonlocal models. Here, we study local models at zero and finite temperature directly in
2+1 dimensions employing functional methods. At zero temperature, we establish that our approach describes the quantum critical behavior with good accuracy for all
N≥2. We then exhibit the mechanism of discrete symmetry breaking from
O(N)×Z2→O(N) for increasing temperature near the biconical critical point when
N is finite but large. We calculate the corresponding finite-temperature phase diagram and further show that the Hohenberg-Mermin-Wagner theorem is fully respected within this approach, i.e., symmetry breaking only occurs in the
Z2 sector. Finally, we determine the critical
N above which this phenomenon can be observed to be
Nc≈15. Published by the American Physical Society 2025