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Construction of PPT entangled state and its detection by using second-order moment of the partial transposition

Rohit Kumar, Satyabrata Adhikari

TL;DR

The paper develops a moment-based framework to detect PPT entangled states in bipartite systems via the second-order moment p2 of the partial transpose, establishing a dimension-dependent PPT bound and a Bloch-vector condition. It extends the toolkit with Newton’s identities to link eigenvalue structure to moments, derives a lower bound on p2 in PPT states, and analyzes convex mixtures of separable and PPT entangled states with witness-based entanglement detection. It further constructs a class of PPT entangled states formed from mixtures of Bell-state components and PPT entangled pieces and demonstrates that these states can achieve positive distillable key rates, highlighting potential cryptographic applications. The results collectively advance practical PPT-state detection and provide cryptographic relevance for bound entangled states in higher dimensions.

Abstract

We adopt a formalism by which we construct and detect a new family of positive partial transpose entangled states in $d_1\otimes d_2$ dimensional system. Our detection method is based on the second order moment $p_2(ρ^{T_B})$ as it is very easy to calculate and may be realizable in laboratory. We show that if the second order moment $p_2(ρ^{T_B})$ in $d_1\otimes d_2$ dimensional system satisfy $p_2(ρ^{T_B})\leq\frac{1}{d_1 d_2-1}$, then the state is a PPT state. We also derive an equivalent condition on the bloch vector. Then, we construct a quantum state by considering the mixture of a separable and an entangled state and obtain a condition on the mixing parameter for which the mixture represents a PPTES. Finally, applying our results, we have shown that the distillable key rate of the private state, prepared through our prescription, is positive. It suggests that our result also has potential applications in quantum cryptography.

Construction of PPT entangled state and its detection by using second-order moment of the partial transposition

TL;DR

The paper develops a moment-based framework to detect PPT entangled states in bipartite systems via the second-order moment p2 of the partial transpose, establishing a dimension-dependent PPT bound and a Bloch-vector condition. It extends the toolkit with Newton’s identities to link eigenvalue structure to moments, derives a lower bound on p2 in PPT states, and analyzes convex mixtures of separable and PPT entangled states with witness-based entanglement detection. It further constructs a class of PPT entangled states formed from mixtures of Bell-state components and PPT entangled pieces and demonstrates that these states can achieve positive distillable key rates, highlighting potential cryptographic applications. The results collectively advance practical PPT-state detection and provide cryptographic relevance for bound entangled states in higher dimensions.

Abstract

We adopt a formalism by which we construct and detect a new family of positive partial transpose entangled states in dimensional system. Our detection method is based on the second order moment as it is very easy to calculate and may be realizable in laboratory. We show that if the second order moment in dimensional system satisfy , then the state is a PPT state. We also derive an equivalent condition on the bloch vector. Then, we construct a quantum state by considering the mixture of a separable and an entangled state and obtain a condition on the mixing parameter for which the mixture represents a PPTES. Finally, applying our results, we have shown that the distillable key rate of the private state, prepared through our prescription, is positive. It suggests that our result also has potential applications in quantum cryptography.

Paper Structure

This paper contains 10 sections, 6 theorems, 69 equations.

Key Result

Theorem 1

Let us consider a $d_{1} \otimes d_{2}$ dimensional system expressed by the density operator $\rho_{AB}$, where the subsystems $A$ and $B$ described by the Hilbert spaces $H_{A}$ and $H_{B}$ respectively and $\rho_{AB}^{T_B}$ is the partial transposition of the density matrix $\rho_{AB}$. Suppose th

Theorems & Definitions (17)

  • Theorem 1
  • Example 1
  • Example 2
  • Example 3
  • Example 4
  • Corollary 2
  • Example 5
  • Example 6
  • Theorem 3
  • Theorem 4
  • ...and 7 more