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arXiv:2409.00878 · Physical Review A

Gaussian unsteerable channels and computable quantifications of Gaussian steering

Taotao Yan, Jie Guo, Jinchuan Hou, Xiaofei Qi, Kan He

Published Nov 20, 2024• 2 citations
arXivHTMLPDF

Abstract

The current quantum resource theory for Gaussian steering in continuous-variable systems is flawed and incomplete. Its primary shortcoming stems from an inadequate comprehension of the architecture of Gaussian channels transforming Gaussian unsteerable states into Gaussian unsteerable states, resulting in a restricted selection of free operations. In the present paper we explore in depth the structure of such $(m+n)$-mode Gaussian channels and introduce a class of Gaussian unsteerable channels and a class of maximal Gaussian unsteerable channels, both of which may be chosen as free operations, which completes the resource theory for Gaussian steering from $A$ to $B$ by using Alice's Gaussian measurements. We also propose two quantifications ${\mathcal{J}}_{j}$ ($j=1,2$) of $(m+n)$-mode Gaussian steering from $A$ to $B$. The computation of the value of ${\mathcal{J}}_{j}$ is straightforward and efficient, as it relies solely on the covariance matrices of Gaussian states, eliminating the need for any optimization procedures. Though the ${\mathcal{J}}_{j}$ are not genuine Gaussian steering measures, they have some nice properties such as being nonincreasing under certain Gaussian unsteerable channels. Additionally, we compare ${\mathcal{J}}_{2}$ with the Gaussian steering measure ${\mathcal{N}}_{3}$, which is based on the Uhlmann fidelity, revealing that ${\mathcal{J}}_{2}$ is an upper bound of ${\mathcal{N}}_{3}$ for a certain class of $(1+1)$-mode Gaussian pure states. As an illustration, we apply ${\mathcal{J}}_{2}$ to discuss the behavior of Gaussian steering for a special class of $(1+1)$-mode Gaussian states in Markovian environments, which uncovers the intriguing phenomenon of rapid decay in quantum steering.

DOI
10.1103/physreva.110.052427

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The current quantum resource theory for Gaussian steering in continuous-variable systems is flawed and incomplete. Its primary shortcoming stems from an inadequate comprehension of the architecture of Gaussian channels transforming Gaussian unsteerable states into Gaussian unsteerable states, resulting in a restricted selection of free operations. In the present paper we explore in depth the structure of such (m+n)(m+n)(m+n)-mode Gaussian channels and introduce a class of Gaussian unsteerable channels and a class of maximal Gaussian unsteerable channels, both of which may be chosen as free operations, which completes the resource theory for Gaussian steering from AAA to BBB by using Alice's Gaussian measurements. We also propose two quantifications Jj{\mathcal{J}}_{j}Jj​ (j=1,2j=1,2j=1,2) of (m+n)(m+n)(m+n)-mode Gaussian steering from AAA to BBB. The computation of the value of Jj{\mathcal{J}}_{j}Jj​ is straightforward and efficient, as it relies solely on the covariance matrices of Gaussian states, eliminating the need for any optimization procedures. Though the Jj{\mathcal{J}}_{j}Jj​ are not genuine Gaussian steering measures, they have some nice properties such as being nonincreasing under certain Gaussian unsteerable channels. Additionally, we compare J2{\mathcal{J}}_{2}J2​ with the Gaussian steering measure N3{\mathcal{N}}_{3}N3​, which is based on the Uhlmann fidelity, revealing that J2{\mathcal{J}}_{2}J2​ is an upper bound of N3{\mathcal{N}}_{3}N3​ for a certain class of (1+1)(1+1)(1+1)-mode Gaussian pure states. As an illustration, we apply J2{\mathcal{J}}_{2}J2​ to discuss the behavior of Gaussian steering for a special class of (1+1)(1+1)(1+1)-mode Gaussian states in Markovian environments, which uncovers the intriguing phenomenon of rapid decay in quantum steering.
Quantum steering is a crucial quantum resource that lies intermediate between entanglement and Bell nonlocality. Gaussian channels, meanwhile, play a foundational role in diverse quantum protocols, secure communication, and related fields. In this paper, we focus on several classes of Gaussian channels associated with quantum steering: Gaussian steering-annihilating channels, Gaussian steering-breaking channels, Gaussian unsteerable channels, and maximal Gaussian unsteerable channels. We give the concepts of these channels, derive the necessary and sufficient conditions for a Gaussian channel to belong to each class, and explore the intrinsic relationships among them. Additionally, since quantifying the steering capability of Gaussian channels in continuous-variable systems requires an understanding of the structure of free superchannels, we also provide a detailed characterization of Gaussian unsteerable superchannels and maximal Gaussian unsteerable superchannels.
Quantum steering is an important quantum resource, which is intermediate between entanglement and Bell nonlocality. In this paper, we study steering witnesses for Gaussian states in continuous-variable systems. We give a definition of steering witnesses by covariance matrices of Gaussian states, and then obtain a steering criterion by steering witnesses to detect steerability of any (m+n)-mode Gaussian states. In addition, the conditions for two steering witnesses to be comparable and the optimality of steering witnesses are also discussed.
Einstein-Podolsky-Rosen steering incarnates a useful nonclassical correlation which sits between entanglement and Bell nonlocality. While a number of qualitative steering criteria exist, very little has been achieved for what concerns quantifying steerability. We introduce a computable measure of steering for arbitrary bipartite Gaussian states of continuous variable systems. For two-mode Gaussian states, the measure reduces to a form of coherent information, which is proven never to exceed entanglement, and to reduce to it on pure states. We provide an operational connection between our measure and the key rate in one-sided device-independent quantum key distribution. We further prove that Peres' conjecture holds in its stronger form within the fully Gaussian regime: namely, steering bound entangled Gaussian states by Gaussian measurements is impossible.
Quantum steering-a strong correlation to be verified even when one party or its measuring device is fully untrusted-not only provides a profound insight into quantum physics but also offers a crucial basis for practical applications. For continuous-variable (CV) systems, Gaussian states among others have been extensively studied, however, mostly confined to Gaussian measurements. While the fulfilment of Gaussian criterion is sufficient to detect CV steering, whether it is also necessary for Gaussian states is a question of fundamental importance in many contexts. This critically questions the validity of characterizations established only under Gaussian measurements like the quantification of steering and the monogamy relations. Here, we introduce a formalism based on local uncertainty relations of non-Gaussian measurements, which is shown to manifest quantum steering of some Gaussian states that Gaussian criterion fails to detect. To this aim, we look into Gaussian states of practical relevance, i.e. two-mode squeezed states under a lossy and an amplifying Gaussian channel. Our finding significantly modifies the characteristics of Gaussian-state steering so far established such as monogamy relations and one-way steering under Gaussian measurements, thus opening a new direction for critical studies beyond Gaussian regime.
Continuous-variable systems realized in quantum optics play a major role in quantum information processing, and it is also one of the promising candidates for a scalable quantum computer. We introduce a resource theory for continuous-variable systems relevant to universal quantum computation. In our theory, easily implementable operations---Gaussian operations combined with feed-forward---are chosen to be the free operations, making the convex hull of the Gaussian states the natural free states. Since our free operations and free states cannot perform universal quantum computation, genuine non-Gaussian states---states not in the convex hull of Gaussian states---are the necessary resource states for universal quantum computation together with free operations. We introduce a monotone to quantify the genuine non-Gaussianity of resource states, in analogy to the stabilizer theory. A direct application of our resource theory is to bound the conversion rate between genuine non-Gaussian states. Finally, we give a protocol that probabilistically distills genuine non-Gaussianity---increases the genuine non-Gaussianity of resource states---only using free operations and postselection on Gaussian measurements, where our theory gives an upper bound for the distillation rate. In particular, the same protocol allows the distillation of cubic phase states, which enable universal quantum computation when combined with free operations.
The diverse range of resources which underlie the utility of quantum states in practical tasks motivates the development of universally applicable methods to measure and compare resources of different types. However, many of such approaches were hitherto limited to the finite-dimensional setting or were not connected with operational tasks. We overcome this by introducing a general method of quantifying resources for continuous-variable quantum systems based on the robustness measure, applicable to a plethora of physically relevant resources such as optical nonclassicality, entanglement, genuine non-Gaussianity, and coherence. We demonstrate in particular that the measure has a direct operational interpretation as the advantage enabled by a given state in a class of channel discrimination tasks. We show that the robustness constitutes a well-behaved, bona fide resource quantifier in any convex resource theory, contrary to a related negativity-based measure known as the standard robustness. Furthermore, we show the robustness to be directly observable-it can be computed as the expectation value of a single witness operator-and establish general methods for evaluating the measure. Explicitly applying our results to the relevant resources, we demonstrate the exact computability of the robustness for several classes of states.