Search Results for « Quantum systems »

For a Markovian (in the strongest sense) open quantum system it is possible, by continuously monitoring the environment, to perfectly track the system; that is, to know the stochastically evolving pure state of the system without altering the master equation. In general, even for a system with a finite Hilbert space dimension D , the pure state trajectory will explore an infinite number of points in Hilbert space, meaning that the dimension K of the classical memory required for the tracking is infinite. However, Karasik and Wiseman [Phys. Rev. Lett., 106(2):020406, 2011] showed that tracking of a qubit ( D = 2 ) is always possible with a bit ( K = 2 ), and gave a heuristic argument implying that a finite K should be sufficient for any D , although beyond D = 2 it would be necessary to have K > D . Our paper is concerned with rigorously investigating the relationship between D and K m i n , the smallest feasible K . We confirm the long-standing conjecture of Karasik and Wiseman that, for generic systems with D > 2 , K m i n > D , by a computational proof (via Hilbert Nullstellensatz certificates of infeasibility). That is, beyond D = 2 , D -dimensional open quantum systems are provably harder to track than D -dimensional open classical systems. We stress that this result allows complete freedom in choice of monitoring scheme, including adaptive monitoring which is, in general, necessary to implement a physically realizable ensemble (as it is known) of just K pure states. Moreover, we develop, and better justify, a new heuristic to guide our expectation of K m i n as a function of D , taking into account the number L of Lindblad operators as well as symmetries in the problem. The use of invariant subspace and Wigner symmetries (that we recently introduced elsewhere, [New J. Phys. https://doi.org/10.1088/1367-2630/ab14b2]) makes it tractable to conduct a numerical search, using the method of polynomial homotopy continuation, to find finite physically realizable ensembles in D = 3 . The results of this search support our heuristic. We thus have confidence in the most interesting feature of our heuristic: in the absence of symmetries, K m i n ∼ D 2 , implying a quadratic gap between the classical and quantum tracking problems. Explicit adaptive monitoring schemes that realize the discovered finite ensembles are obtained numerically, thus facilitating future experimental investigations.