Abstract
We study a random unitary quantum circuit with only reset channels, which has high feasibility for real quantum devices. In particular, we investigate the many-body statistical physics properties, "reset-induced" entanglement phase transitions comparing the classical statistical picture in the large "d" limit of qudits. In the property of the reset-induced phase transition the parameter of qudit d is essential. That is, the transition properties induced by the reset channel significantly depend on d. We numerically elucidate this statement employing efficient stabilizer circuit simulations for d=2. Specifically, large fluctuations are observed near the critical point, indicating that the reset-induced phase transition is continuous. We obtain clear data collapses, consistent with a second-order mixed phase transition. This behavior differs from expectations based on the classical statistical mapping in the large-d limit.