“…In a quantum circuit, frequent local measurements, which do not commute with the generators of the unitary dynamics induce a phase transition in the dynamics of entanglement [1][2][3]. This phenomenon has been observed in random quantum circuits, where the unitary evolution is generated by Clifford [2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17] or Haar [1,3,[18][19][20][21][22][23][24][25][26] random gates and in Hamiltonian systems, where the unitary time evolution is continuous [27][28][29][30][31][32][33][34][35][36][37][38][39]. Due to the inherent randomness of the measurement process, the entanglement phase transitions do not manifest on the level of ensemble averaged, local order parameters but only in higher moments, or replicas of the state [11,20,31,<...>…”