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Reachable sets for two-level open quantum systems driven by coherent and incoherent controls

Lev Lokutsievskiy, Alexander Pechen

TL;DR

This work analyzes reachable sets for a two-level open quantum system driven by coherent $u(t)$ and incoherent $n(t)$ controls, using a Bloch-vector formulation to study exact and asymptotic controllability. It proves that, for a qubit, incoherent control does not enlarge the reachable set, and characterizes the precision limit $δ\sim γ/ω$ with two lacunae of size $\sim δ$ around certain pure states when only one coherent control is available; with two coherent controls, the system becomes completely controllable within the density-matrix set. The reachable set as a function of final time exhibits a nontrivial structure, and the authors provide a fast numerical method for time-minimal coherent control via a reduced auxiliary system and a tabulation-based acceleration. These results imply high-precision state steering in open qubit systems and offer practical guidance for leveraging environmental (incoherent) controls alongside coherent drive in quantum control tasks.

Abstract

In this work, we study controllability in the set of all density matrices for a two-level open quantum system driven by coherent and incoherent controls. In [A. Pechen, Phys. Rev. A 84, 042106 (2011)] an approximate controllability, i.e., controllability with some precision, was shown for generic $N$-level open quantum systems driven by coherent and incoherent controls. However, the explicit formulation of this property, including the behavior of this precision as a function of transition frequencies and decoherence rates of the system, was not known. The present work provides a rigorous analytical study of reachable sets for two-level open quantum systems. First, it is shown that for $N=2$ the presence of incoherent control does not affect the reachable set (while incoherent control may affect the time necessary to reach particular state). Second, the reachable set in the Bloch ball is described and it is shown that already just for one coherent control any point in the Bloch ball can be achieved with precision $δ\sim γ/ω$, where $γ$ is the decoherence rate and $ω$ is the transition frequency. Typical values are $δ\lesssim10^{-3}$ that implies high accuracy of achieving any density matrix. Moreover, we show that most points in the Bloch ball can be exactly reached, except of two lacunae of size $\simδ$. For two coherent controls, the system is shown to be completely controllable in the set of all density matrices. Third, the reachable set as a function of the final time is found and shown to exhibit a non-trivial structure.

Reachable sets for two-level open quantum systems driven by coherent and incoherent controls

TL;DR

This work analyzes reachable sets for a two-level open quantum system driven by coherent and incoherent controls, using a Bloch-vector formulation to study exact and asymptotic controllability. It proves that, for a qubit, incoherent control does not enlarge the reachable set, and characterizes the precision limit with two lacunae of size around certain pure states when only one coherent control is available; with two coherent controls, the system becomes completely controllable within the density-matrix set. The reachable set as a function of final time exhibits a nontrivial structure, and the authors provide a fast numerical method for time-minimal coherent control via a reduced auxiliary system and a tabulation-based acceleration. These results imply high-precision state steering in open qubit systems and offer practical guidance for leveraging environmental (incoherent) controls alongside coherent drive in quantum control tasks.

Abstract

In this work, we study controllability in the set of all density matrices for a two-level open quantum system driven by coherent and incoherent controls. In [A. Pechen, Phys. Rev. A 84, 042106 (2011)] an approximate controllability, i.e., controllability with some precision, was shown for generic -level open quantum systems driven by coherent and incoherent controls. However, the explicit formulation of this property, including the behavior of this precision as a function of transition frequencies and decoherence rates of the system, was not known. The present work provides a rigorous analytical study of reachable sets for two-level open quantum systems. First, it is shown that for the presence of incoherent control does not affect the reachable set (while incoherent control may affect the time necessary to reach particular state). Second, the reachable set in the Bloch ball is described and it is shown that already just for one coherent control any point in the Bloch ball can be achieved with precision , where is the decoherence rate and is the transition frequency. Typical values are that implies high accuracy of achieving any density matrix. Moreover, we show that most points in the Bloch ball can be exactly reached, except of two lacunae of size . For two coherent controls, the system is shown to be completely controllable in the set of all density matrices. Third, the reachable set as a function of the final time is found and shown to exhibit a non-trivial structure.

Paper Structure

This paper contains 7 sections, 3 theorems, 39 equations, 5 figures.

Key Result

Theorem 1

For any starting point ${\mathbf{r}}^0$ the sets of asymptotically reachable points for system (eq:main_control system) with or without incoherent control coincide.

Figures (5)

  • Figure 1: The spiral grid in the polar coordinates.
  • Figure 2: The non-reachable triangle. Here $\alpha$ and $\beta$ are some sufficiently small parameters.
  • Figure 3: 2D in the $(z,R)$ cylindrical coordinates (upper row) and 3D in the Bloch ball (bottom row) plots of the reachable sets for $\gamma/\omega=0.1$ and $\omega T=0.1$ (1st column), $\omega T=0.5$ (2nd column), $\omega T=1$ (3rd column), $\omega T=1.5$ (4th column).
  • Figure 4: 2D in the $(z,R)$ cylindrical coordinates (upper row) and 3D in the Bloch ball (bottom row) plots of the reachable sets for $\gamma/\omega=0.1$ and $\omega T=2$ (1st column), $\omega T=4$ (2nd column), $\omega T=6$ (3rd column), $\omega T=7$ (4th column).
  • Figure 5: Evolution of the reachable set as a function of $T$ (see the ancillary file ReachableSets.mp4 and supplementary movie online at https://stacks.iop.org/JPA/54/395304/mmedia).

Theorems & Definitions (5)

  • Theorem 1
  • Remark 1
  • Theorem 2
  • Theorem 3
  • Remark 2