<p>We propose a signal <InlineEquation ID="IEq1"> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mtext>∆</mtext> <mi>p</mi> <mfenced close=")" open="("> <mn>3</mn> </mfenced> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {\Delta }_p^{(3)} \)</EquationSource> </InlineEquation> for tripartite correlations in finite-dimensional quantum systems and <InlineEquation ID="IEq2"> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mtext>∆</mtext> <mi>w</mi> <mfenced close=")" open="("> <mn>3</mn> </mfenced> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {\Delta }_w^{(3)} \)</EquationSource> </InlineEquation> for holographic systems. We prove that <InlineEquation ID="IEq3"> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mtext>∆</mtext> <mi>p</mi> <mfenced close=")" open="("> <mn>3</mn> </mfenced> </msubsup> </math></EquationSource> <EquationSource Format="TEX">\( {\Delta }_p^{(3)} \)</EquationSource> </InlineEquation> is non-negative for any tripartite entangled mixed states and vanishes for mixed product states. It is a correlation signal because it is generally nonzero for a separable state containing a classical mixture. Based on the conjecture, the equality between an entanglement wedge cross section <i>E</i><sub><i>w</i></sub> and entanglement of purification <i>E</i><sub><i>p</i></sub>, i.e., <i>E</i><sub><i>w</i></sub> = <i>E</i><sub><i>P</i></sub> in the semiclassical limit, we apply the tripartite correlation signal to study the structures of tripartite entanglement in AdS<sub>3</sub>/CFT<sub>2</sub>, especially for pure AdS<sub>3</sub>. We comment on a generalization to <i>n</i>-partite correlation signals <InlineEquation ID="IEq4"> <EquationSource Format="MATHML"><math display="inline"> <msubsup> <mi mathvariant="normal">Δ</mi> <mi>p</mi> <mfenced close=")" open="("> <mi>n</mi> </mfenced> </msubsup> <mfenced close=")" open="("> <mrow> <msub> <mi>A</mi> <mn>1</mn> </msub> <mo>:</mo> <mo>⋯</mo> <mo>:</mo> <msub> <mi>A</mi> <mi>n</mi> </msub> </mrow> </mfenced> </math></EquationSource> <EquationSource Format="TEX">\( {\Delta}_p^{(n)}\left({A}_1:\cdots :{A}_n\right) \)</EquationSource> </InlineEquation>.</p>

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Tripartite correlation signal from multipartite entanglement of purification

  • Ning Bao,
  • Keiichiro Furuya,
  • Joydeep Naskar

摘要

We propose a signal p 3 \( {\Delta }_p^{(3)} \) for tripartite correlations in finite-dimensional quantum systems and w 3 \( {\Delta }_w^{(3)} \) for holographic systems. We prove that p 3 \( {\Delta }_p^{(3)} \) is non-negative for any tripartite entangled mixed states and vanishes for mixed product states. It is a correlation signal because it is generally nonzero for a separable state containing a classical mixture. Based on the conjecture, the equality between an entanglement wedge cross section Ew and entanglement of purification Ep, i.e., Ew = EP in the semiclassical limit, we apply the tripartite correlation signal to study the structures of tripartite entanglement in AdS3/CFT2, especially for pure AdS3. We comment on a generalization to n-partite correlation signals Δ p n A 1 : : A n \( {\Delta}_p^{(n)}\left({A}_1:\cdots :{A}_n\right) \) .