<p>We propose a phenomenon of discrete-time quantum walks on graphs called the pulsation, which is a generalization of a phenomenon in the quantum searches. This phenomenon is discussed on a composite graph formed by two connected graphs <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(G_{1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>G</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(G_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>G</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation>. The pulsation means that the state periodically transfers between <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(G_{1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>G</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(G_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>G</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> with the initial state of the uniform superposition on <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(G_1\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>G</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation>. In this paper, we focus on the case for the Grover walk where <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(G_{1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>G</mi> <mn>1</mn> </msub> </math></EquationSource> </InlineEquation> is the Johnson graph and <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(G_{2}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>G</mi> <mn>2</mn> </msub> </math></EquationSource> </InlineEquation> is a star graph. Also, the composite graph is constructed by identifying an arbitrary vertex of the Johnson graph with the internal vertex of the star graph. In that case, we find the pulsation with <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(O(\sqrt{N^{1+1/k}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>O</mi> <mo stretchy="false">(</mo> <msqrt> <msup> <mi>N</mi> <mrow> <mn>1</mn> <mo>+</mo> <mn>1</mn> <mo stretchy="false">/</mo> <mi>k</mi> </mrow> </msup> </msqrt> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> periodicity, where <i>N</i> and <i>k</i> are the number of vertices and the diameter of the Johnson graph, respectively. The proof is based on Kato’s perturbation theory in finite-dimensional vector spaces.</p>

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Pulsation of quantum walk on Johnson graph

  • Taisuke Hosaka,
  • Etsuo Segawa

摘要

We propose a phenomenon of discrete-time quantum walks on graphs called the pulsation, which is a generalization of a phenomenon in the quantum searches. This phenomenon is discussed on a composite graph formed by two connected graphs \(G_{1}\) G 1 and \(G_{2}\) G 2 . The pulsation means that the state periodically transfers between \(G_{1}\) G 1 and \(G_{2}\) G 2 with the initial state of the uniform superposition on \(G_1\) G 1 . In this paper, we focus on the case for the Grover walk where \(G_{1}\) G 1 is the Johnson graph and \(G_{2}\) G 2 is a star graph. Also, the composite graph is constructed by identifying an arbitrary vertex of the Johnson graph with the internal vertex of the star graph. In that case, we find the pulsation with \(O(\sqrt{N^{1+1/k}})\) O ( N 1 + 1 / k ) periodicity, where N and k are the number of vertices and the diameter of the Johnson graph, respectively. The proof is based on Kato’s perturbation theory in finite-dimensional vector spaces.