<p>We consider the depolarizing channel in <i>d</i> dimension defined as <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(D_x(\rho )=(1-x)\rho +x\text {tr}(\rho ) \frac{I}{d}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>D</mi> <mi>x</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>ρ</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo>-</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mi>ρ</mi> <mo>+</mo> <mi>x</mi> <mtext>tr</mtext> <mrow> <mo stretchy="false">(</mo> <mi>ρ</mi> <mo stretchy="false">)</mo> </mrow> <mfrac> <mi>I</mi> <mi>d</mi> </mfrac> </mrow> </math></EquationSource> </InlineEquation>, and explicitly find a quantum channel <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathcal{N}_x\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="script">N</mi> <mi>x</mi> </msub> </math></EquationSource> </InlineEquation> which anti-degrades this, when <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(x\ge \frac{1}{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>x</mi> <mo>≥</mo> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> </mrow> </math></EquationSource> </InlineEquation>. This proves that the depolarizing channel <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(D_x\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>D</mi> <mi>x</mi> </msub> </math></EquationSource> </InlineEquation> has zero capacity when <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(x\ge \frac{1}{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>x</mi> <mo>≥</mo> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> </mrow> </math></EquationSource> </InlineEquation>. As a corollary, this implies that any quantum channel when contaminated by white noise stronger than this value loses its capacity completely. Although by arguments based on symmetric extendibility of the Choi matrix, it is known that the channel is anti-degradable when <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(x\ge \frac{d}{2(d+1)}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>x</mi> <mo>≥</mo> <mfrac> <mi>d</mi> <mrow> <mn>2</mn> <mo stretchy="false">(</mo> <mi>d</mi> <mo>+</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation>, [<CitationRef AdditionalCitationIDS="CR2" CitationID="CR1">1</CitationRef>–<CitationRef CitationID="CR3">3</CitationRef>], the explicit form of the anti-degrading channel in this larger interval is not known. We also calculate in closed form the capacity of the complementary channel <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\mathcal{D}_x^c\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi mathvariant="script">D</mi> <mi>x</mi> <mi>c</mi> </msubsup> </math></EquationSource> </InlineEquation> in the region <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(x\ge \frac{1}{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>x</mi> <mo>≥</mo> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> </mrow> </math></EquationSource> </InlineEquation>. This adds to the existing list of quantum channels for which the quantum capacity has been calculated in closed form, see [<CitationRef CitationID="CR4">4</CitationRef>, <CitationRef CitationID="CR5">5</CitationRef>], and [<CitationRef CitationID="CR6">6</CitationRef>].</p>

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Construction of channels which in every dimension anti-degrade the depolarizing channel

  • Shayan Roofeh,
  • Vahid Karimipour

摘要

We consider the depolarizing channel in d dimension defined as \(D_x(\rho )=(1-x)\rho +x\text {tr}(\rho ) \frac{I}{d}\) D x ( ρ ) = ( 1 - x ) ρ + x tr ( ρ ) I d , and explicitly find a quantum channel \(\mathcal{N}_x\) N x which anti-degrades this, when \(x\ge \frac{1}{2}\) x 1 2 . This proves that the depolarizing channel \(D_x\) D x has zero capacity when \(x\ge \frac{1}{2}\) x 1 2 . As a corollary, this implies that any quantum channel when contaminated by white noise stronger than this value loses its capacity completely. Although by arguments based on symmetric extendibility of the Choi matrix, it is known that the channel is anti-degradable when \(x\ge \frac{d}{2(d+1)}\) x d 2 ( d + 1 ) , [13], the explicit form of the anti-degrading channel in this larger interval is not known. We also calculate in closed form the capacity of the complementary channel \(\mathcal{D}_x^c\) D x c in the region \(x\ge \frac{1}{2}\) x 1 2 . This adds to the existing list of quantum channels for which the quantum capacity has been calculated in closed form, see [4, 5], and [6].