<p>Eylee Jung <i>et.al</i>[<CitationRef CitationID="CR1">1</CitationRef>] had conjectured that <InlineEquation ID="IEq1"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11128_2025_4680_Article_IEq1.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="65" /> </InlineMediaObject> <EquationSource Format="TEX">\(P_{max}=\frac{1}{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>P</mi> <mrow> <mi mathvariant="italic">max</mi> </mrow> </msub> <mo>=</mo> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> </mrow> </math></EquationSource> </InlineEquation> is a necessary and sufficient condition for the perfect two-party teleportation, and consequently, the Groverian measure of entanglement for the entanglement resource must be <InlineEquation ID="IEq2"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11128_2025_4680_Article_IEq2.gif" Format="GIF" Height="26" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\(\frac{1}{\sqrt{2}}\)</EquationSource> <EquationSource Format="MATHML"><math> <mfrac> <mn>1</mn> <msqrt> <mn>2</mn> </msqrt> </mfrac> </math></EquationSource> </InlineEquation>. It is also known that prototype <i>W</i> state is not useful for standard teleportation. Agrawal and Pati[<CitationRef CitationID="CR2">2</CitationRef>] have successfully executed perfect (standard) teleportation with non-prototype <i>W</i> state. Aligned with the protocol mentioned in[<CitationRef CitationID="CR2">2</CitationRef>], we have considered here <i>Star</i> type tripartite states and have shown that perfect teleportation is suitable with such states. Moreover, we have taken the linear superposition of non-prototype <i>W</i> state and its spin-flipped version and shown that it belongs to <i>Star</i> class. Also, standard teleportation is possible with these states. It is observed that genuine tripartite entanglement is not necessary requirement for a state to be used as a channel for successful standard teleportation. We have also shown that these <i>Star</i> class states are <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11128_2025_4680_Article_IEq3.gif" Format="GIF" Height="22" Rendition="HTML" Resolution="72" Type="Linedraw" Width="65" /> </InlineMediaObject> <EquationSource Format="TEX">\(P_{max}=\frac{1}{4}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>P</mi> <mrow> <mi mathvariant="italic">max</mi> </mrow> </msub> <mo>=</mo> <mfrac> <mn>1</mn> <mn>4</mn> </mfrac> </mrow> </math></EquationSource> </InlineEquation> states and their Groverian entanglement is <InlineEquation ID="IEq4"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="11128_2025_4680_Article_IEq4.gif" Format="GIF" Height="26" Rendition="HTML" Resolution="72" Type="Linedraw" Width="21" /> </InlineMediaObject> <EquationSource Format="TEX">\(\frac{\sqrt{3}}{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mfrac> <msqrt> <mn>3</mn> </msqrt> <mn>2</mn> </mfrac> </math></EquationSource> </InlineEquation>, thus concluding that Jung conjecture is not a necessary condition.</p>

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Teleportation of unknown qubit via Star-type tripartite states

  • Anushree Bhattacharjee,
  • Abhijit Mandal,
  • Sovik Roy

摘要

Eylee Jung et.al[1] had conjectured that \(P_{max}=\frac{1}{2}\) P max = 1 2 is a necessary and sufficient condition for the perfect two-party teleportation, and consequently, the Groverian measure of entanglement for the entanglement resource must be \(\frac{1}{\sqrt{2}}\) 1 2 . It is also known that prototype W state is not useful for standard teleportation. Agrawal and Pati[2] have successfully executed perfect (standard) teleportation with non-prototype W state. Aligned with the protocol mentioned in[2], we have considered here Star type tripartite states and have shown that perfect teleportation is suitable with such states. Moreover, we have taken the linear superposition of non-prototype W state and its spin-flipped version and shown that it belongs to Star class. Also, standard teleportation is possible with these states. It is observed that genuine tripartite entanglement is not necessary requirement for a state to be used as a channel for successful standard teleportation. We have also shown that these Star class states are \(P_{max}=\frac{1}{4}\) P max = 1 4 states and their Groverian entanglement is \(\frac{\sqrt{3}}{2}\) 3 2 , thus concluding that Jung conjecture is not a necessary condition.