“…Obviously, the unsharp measurement strategy used here is optimal. For Werner state, the classical bound C N = {1/ √ 2, 1/ √ 3, 1/ √ 3, 0.5393, 0.5236, 0.503, 0.5} when N = {2, 3, 4, 6, 10, 16, ∞}, respectively [42,44]. Since the classical bound of N = 16 is very close to that of infinite measurement settings, we implement N = {2, 3, 4, 6, 10, 16} to investigate the behavior of quantum steering in this work.…”