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arXiv:1804.03840 · Physical Review A

Triangle inequalities in coherence measures and entanglement concurrence

Yue Dai, Wen‐Long You, Yuli Dong, Chengjie Zhang

Published Dec 6, 2017• 8 citations
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Abstract

We provide detailed proofs of triangle inequalities in coherence measures and entanglement concurrence. If a rank-2 state $\ensuremath{\varrho}$ can be expressed as a convex combination of two pure states, i.e., $\ensuremath{\varrho}={p}_{1}|{\ensuremath{\psi}}_{1}\ensuremath{\rangle}\ensuremath{\langle}{\ensuremath{\psi}}_{1}|+{p}_{2}|{\ensuremath{\psi}}_{2}\ensuremath{\rangle}\ensuremath{\langle}{\ensuremath{\psi}}_{2}|$, a triangle inequality can be established as $|E(|{\mathrm{\ensuremath{\Psi}}}_{1}\ensuremath{\rangle})\ensuremath{-}E(|{\mathrm{\ensuremath{\Psi}}}_{2}\ensuremath{\rangle})|\ensuremath{\le}E(\ensuremath{\varrho})\ensuremath{\le}E(|{\mathrm{\ensuremath{\Psi}}}_{1}\ensuremath{\rangle})+E(|{\mathrm{\ensuremath{\Psi}}}_{2}\ensuremath{\rangle})$, where $|{\mathrm{\ensuremath{\Psi}}}_{1}\ensuremath{\rangle}=\sqrt{{p}_{1}}|{\ensuremath{\psi}}_{1}\ensuremath{\rangle}$ and $|{\mathrm{\ensuremath{\Psi}}}_{2}\ensuremath{\rangle}=\sqrt{{p}_{2}}|{\ensuremath{\psi}}_{2}\ensuremath{\rangle}$; $E$ can be considered either coherence measures or entanglement concurrence. This inequality displays mathematical beauty for its similarity to the triangle inequality in plane geometry. An illustrative example is given after the proof.

DOI
10.1103/physreva.96.062308

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We provide detailed proofs of triangle inequalities in coherence measures and entanglement concurrence. If a rank-2 state \ensuremathϱ\ensuremath{\varrho}\ensuremathϱ can be expressed as a convex combination of two pure states, i.e., \ensuremathϱ=p1∣\ensuremathψ1\ensuremath⟩\ensuremath⟨\ensuremathψ1∣+p2∣\ensuremathψ2\ensuremath⟩\ensuremath⟨\ensuremathψ2∣\ensuremath{\varrho}={p}_{1}|{\ensuremath{\psi}}_{1}\ensuremath{\rangle}\ensuremath{\langle}{\ensuremath{\psi}}_{1}|+{p}_{2}|{\ensuremath{\psi}}_{2}\ensuremath{\rangle}\ensuremath{\langle}{\ensuremath{\psi}}_{2}|\ensuremathϱ=p1​∣\ensuremathψ1​\ensuremath⟩\ensuremath⟨\ensuremathψ1​∣+p2​∣\ensuremathψ2​\ensuremath⟩\ensuremath⟨\ensuremathψ2​∣, a triangle inequality can be established as ∣E(∣\ensuremathΨ1\ensuremath⟩)\ensuremath−E(∣\ensuremathΨ2\ensuremath⟩)∣\ensuremath≤E(\ensuremathϱ)\ensuremath≤E(∣\ensuremathΨ1\ensuremath⟩)+E(∣\ensuremathΨ2\ensuremath⟩)|E(|{\mathrm{\ensuremath{\Psi}}}_{1}\ensuremath{\rangle})\ensuremath{-}E(|{\mathrm{\ensuremath{\Psi}}}_{2}\ensuremath{\rangle})|\ensuremath{\le}E(\ensuremath{\varrho})\ensuremath{\le}E(|{\mathrm{\ensuremath{\Psi}}}_{1}\ensuremath{\rangle})+E(|{\mathrm{\ensuremath{\Psi}}}_{2}\ensuremath{\rangle})∣E(∣\ensuremathΨ1​\ensuremath⟩)\ensuremath−E(∣\ensuremathΨ2​\ensuremath⟩)∣\ensuremath≤E(\ensuremathϱ)\ensuremath≤E(∣\ensuremathΨ1​\ensuremath⟩)+E(∣\ensuremathΨ2​\ensuremath⟩), where ∣\ensuremathΨ1\ensuremath⟩=p1∣\ensuremathψ1\ensuremath⟩|{\mathrm{\ensuremath{\Psi}}}_{1}\ensuremath{\rangle}=\sqrt{{p}_{1}}|{\ensuremath{\psi}}_{1}\ensuremath{\rangle}∣\ensuremathΨ1​\ensuremath⟩=p1​​∣\ensuremathψ1​\ensuremath⟩ and ∣\ensuremathΨ2\ensuremath⟩=p2∣\ensuremathψ2\ensuremath⟩|{\mathrm{\ensuremath{\Psi}}}_{2}\ensuremath{\rangle}=\sqrt{{p}_{2}}|{\ensuremath{\psi}}_{2}\ensuremath{\rangle}∣\ensuremathΨ2​\ensuremath⟩=p2​​∣\ensuremathψ2​\ensuremath⟩; EEE can be considered either coherence measures or entanglement concurrence. This inequality displays mathematical beauty for its similarity to the triangle inequality in plane geometry. An illustrative example is given after the proof.
Quantum coherence and entanglement are two key features in quantum mechanics and play important roles in quantum information processing and quantum computation. We provide a general triangle-like inequality satisfied by the l1l_1l1​-norm measure of coherence for convex combination of arbitrary n pure states of a quantum state ρ\rho ρ. Furthermore, we present triangle-like inequality for the convex-roof extended negativity for any states of rank 2, which gives a positive answer to a conjecture raised in Dai et al. (Phys. Rev. A 96:062308, 2017). Detailed examples are given to illustrate the relations characterized by the triangle-like inequalities.
The quantification of multipartite entanglement remains a long-standing open challenge in quantum information theory with major implications for quantum foundations and quantum technologies. In the context of three-qubit pure states, the concurrence triangle underlies geometric interpretations for a variety of multipartite entanglement measures. In particular, the concurrence fill, which is proportional to the square root of the area of the concurrence triangle, has been shown to be a valid measure of genuine tripartite entanglement. As a result, there is now significant interest in extending the concurrence triangle and concurrence fill to three-qubit mixed states. In this work, we show that any rank-2 three-qubit mixed state can be visualized in terms of concurrence prisms associated with their pure state decompositions. Thus, the concurrence fill of the mixed state obtained through convex-roof extension is proportional to the total prism fill area, defined as the square root of the base area times the height, associated with the prisms minimized over all pure state decompositions. We then consider three-qubit mixed states that are incoherent mixtures of Greenberger-Horne-Zeilinger (GHZ) and W states and analytically perform their convex-roof extension to obtain a closed-form expression for the concurrence fill of these rank-2 mixtures. Finally, we apply the geometric picture of concurrence prisms to these mixtures and their pure state decomposition corresponding to minimum concurrence fill as a tool for visualization.
Although genuine multipartite entanglement has already been generated and verified by experiments, most of the existing measures cannot detect genuine entanglement faithfully. In this work, by exploiting for the first time a previously overlooked constraint for the distribution of entanglement in three-qubit systems, we reveal a new genuine tripartite entanglement measure, which is related to the area of a so-called concurrence triangle. It is compared with other existing measures and is found superior to previous attempts for different reasons. A specific example is illustrated to show that two tripartite entanglement measures can be inequivalent due to the high dimensionality of the Hilbert space. The properties of the triangle measure make it a candidate in potential quantum tasks and available to be used in any multiparty entanglement problems.
We derive a simple lower bound on the geometric measure of entanglement for mixed quantum states in the case of a general multipartite system. The main ingredient of the presented derivation is the triangle inequality applied to the root infidelity distance in the space of density matrices. The obtained bound leads to entanglement criteria with a straightforward interpretation. The proposed criteria provide an experimentally accessible, powerful entanglement test. This article is part of a special issue of Journal of Physics A: Mathematical and Theoretical devoted to '50 years of Bell's theorem'.
Concurrence is a widely used entanglement measure of bipartite mixed states. We propose to consider the concurrence as being defined by a quadratic form on the space of self-adjoint operators. The square root of this form determines the values of the concurrence on the pure states, while the values on the mixed states are obtained as the largest convex extension, the convex roof. This viewpoint admits a generalization. Namely, the space of self-adjoint operators and the convex cone of positive semidefinite operators contained therein can be replaced by an arbitrary real vector space containing a convex cone. Then the concurrence is determined on the extreme rays of the cone by the square root of a quadratic form, and on the rest of the cone by the convex roof. We compute this generalized concurrence in the case when the cone is a second order cone. This enables us to compute the concurrence of arbitrary bipartite mixed states of rank 2. As an application, we compute the concurrences of the density matrices of all graphs with two edges or with three edges forming a triangle. We also consider the problem of maximizing the concurrence on the set of mixed states having a fixed spectrum.
The entanglement content of superpositions of quantum states is investigated based on a measure called concurrence. Given a bipartite pure state in arbitrary dimension written as the quantum superposition of two other such states, we find simple inequalities relating the concurrence of the state to that of its components. We derive an exact expression for the concurrence when the component states are biorthogonal and provide elegant upper and lower bounds in all other cases. For quantum bits, our upper bound is tighter than the previously derived bound [N. Linden et al., Phys. Rev. Lett. 97, 100502 (2006)].