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How Far do Lindbladians Go?

Jihong Cai, Advith Govindarajan, Marius Junge

TL;DR

The paper investigates how little dissipation is needed to make the full state space $\\mathcal{D}(\\mathcal{H})$ reachable when unitary control is already powerful (Hörmander generation of $\\mathfrak{su}(n)$). It develops a geometric and algebraic framework around Lindbladians, tangent cones, and lifting to characterize reachability, proving that a small number of non-self-adjoint jump operators suffices for transitivity in many cases, while purely self-adjoint jumps fail. It further incorporates environment-assisted resources and a gradient-form perspective to expand the set of attainable evolutions, and it provides constructive algorithms for state transport using sparse Lindbladians and amplitude damping, including finite-time reachability results and obstructions. The results reframe dissipation as a controllable resource for universal state preparation and reservoir engineering, with practical implications for designing efficient open-system control protocols.

Abstract

We study controllability of finite-dimensional open quantum systems under a general Markovian control model combining full coherent (unitary) control with tunable dissipative channels. Assuming the Hamiltonian controls is a Hörmander system that generate $\mathfrak{su}(n)$, we ask how little dissipation suffices to make the full state space $\mathcal{D}(\mathcal{H})$ controllable. We show that minimal non-unital noise can break unitary-orbit invariants and, in many cases, a very small set of jump operators yields transitivity on $\mathcal{D}(\mathcal{H})$. For multi-qubit systems we prove explicit transitivity results for natural resources such as a single-qubit amplitude-damping jump together with a dephasing channel, and we identify obstructions when only self-adjoint jump operators are available (yielding only unital evolutions). We further develop a geometric viewpoint and ask the ``lifting'' question: when can a path of densities be obtained from applying a time-dependent family of Lindbladian to an initial state? For this, we have to analyze the tangent structure of the ``manifold with corners'' and how this tangent structure reflects Lindbldian evolution. Building on this framework, we derive reachability criteria and no-go results based on a norm-decrease alignment condition, including a geometric obstruction arising from the incompatibility between admissible tangent directions and dissipative contraction.

How Far do Lindbladians Go?

TL;DR

The paper investigates how little dissipation is needed to make the full state space reachable when unitary control is already powerful (Hörmander generation of ). It develops a geometric and algebraic framework around Lindbladians, tangent cones, and lifting to characterize reachability, proving that a small number of non-self-adjoint jump operators suffices for transitivity in many cases, while purely self-adjoint jumps fail. It further incorporates environment-assisted resources and a gradient-form perspective to expand the set of attainable evolutions, and it provides constructive algorithms for state transport using sparse Lindbladians and amplitude damping, including finite-time reachability results and obstructions. The results reframe dissipation as a controllable resource for universal state preparation and reservoir engineering, with practical implications for designing efficient open-system control protocols.

Abstract

We study controllability of finite-dimensional open quantum systems under a general Markovian control model combining full coherent (unitary) control with tunable dissipative channels. Assuming the Hamiltonian controls is a Hörmander system that generate , we ask how little dissipation suffices to make the full state space controllable. We show that minimal non-unital noise can break unitary-orbit invariants and, in many cases, a very small set of jump operators yields transitivity on . For multi-qubit systems we prove explicit transitivity results for natural resources such as a single-qubit amplitude-damping jump together with a dephasing channel, and we identify obstructions when only self-adjoint jump operators are available (yielding only unital evolutions). We further develop a geometric viewpoint and ask the ``lifting'' question: when can a path of densities be obtained from applying a time-dependent family of Lindbladian to an initial state? For this, we have to analyze the tangent structure of the ``manifold with corners'' and how this tangent structure reflects Lindbldian evolution. Building on this framework, we derive reachability criteria and no-go results based on a norm-decrease alignment condition, including a geometric obstruction arising from the incompatibility between admissible tangent directions and dissipative contraction.

Paper Structure

This paper contains 12 sections, 25 theorems, 123 equations, 2 figures.

Key Result

Proposition 2.2

[proposition]chan_membership Let $S$ be a Hörmander system of $\mathfrak{su}(2^k)$. Then

Figures (2)

  • Figure 1: Illustration of the alignment condition of \ref{['p2condition']}
  • Figure 2: A choice of raising Lindbladians on the commutative state space of $\mathbb C^3$.

Theorems & Definitions (61)

  • Definition 2.1
  • Proposition 2.2
  • proof
  • Lemma 2.3
  • proof
  • Definition 2.4
  • Definition 2.5
  • Theorem 2.6
  • proof
  • Proposition 2.7
  • ...and 51 more