<p>In this paper, the notion of quaternionic Balakrishnan operator <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(J^{\alpha }\)</EquationSource> </InlineEquation> with the quaternionic power (<InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\alpha \in {\mathbb {H}}\)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\textrm{Re}(\alpha )&gt;0\)</EquationSource> </InlineEquation>) is introduced via quaternionic non-negative operator <i>T</i> and the inclusion relations of the domains and ranges of these two types of operators are demonstrated. The unique unified integral representation of <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(J^{\alpha }\)</EquationSource> </InlineEquation> is obtained through the slice Cauchy kernels and the slice regularity of the exponent mapping is proved. Further, the limits of <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(J^{\alpha }x\)</EquationSource> </InlineEquation> as <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\alpha \rightarrow 0\)</EquationSource> </InlineEquation> and <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\alpha \rightarrow 1\)</EquationSource> </InlineEquation> are investigated under some fixed spherical sectors. By obtaining moment inequality, we prove that <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(J^{\alpha }\)</EquationSource> </InlineEquation> is a closable operator and introduce the power with base <i>T</i> and exponent <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\alpha \)</EquationSource> </InlineEquation> as the operator <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\overline{J^{\alpha }}\)</EquationSource> </InlineEquation>, then the integral representation of <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\overline{J^{\alpha }}\)</EquationSource> </InlineEquation> is given by the limit of <i>S</i>-resolvent operator of <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(-T\)</EquationSource> </InlineEquation>. Besides, the related integral expressions of <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(J^{\alpha }\)</EquationSource> </InlineEquation> are established via quaternionic semigroup when <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(-T\)</EquationSource> </InlineEquation> is the infinitesimal generator of an equibounded strongly continuous quaternionic semigroup. It is crucial to note that the fractional quaternionic operator set <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\{\overline{J_{T}^{\alpha }}:\alpha \in {\mathbb {H}}^{+}\}\)</EquationSource> </InlineEquation> has a nice semigroup property under the <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(*\)</EquationSource> </InlineEquation>-<i>product</i> we introduced under the noncommutative setting. In addition, for the space consisting of right linear bounded quaternionic operators with a Schauder basis, we also obtained the semigroup property for <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(J^{\alpha }\)</EquationSource> </InlineEquation> through introducing the <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(\star \)</EquationSource> </InlineEquation>-<i>product</i>.</p>

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Quaternionic Balakrishnan operator and related semigroup property

  • Guangzhou Qin,
  • Chao Wang,
  • Jibin Li

摘要

In this paper, the notion of quaternionic Balakrishnan operator \(J^{\alpha }\) with the quaternionic power ( \(\alpha \in {\mathbb {H}}\) and \(\textrm{Re}(\alpha )>0\) ) is introduced via quaternionic non-negative operator T and the inclusion relations of the domains and ranges of these two types of operators are demonstrated. The unique unified integral representation of \(J^{\alpha }\) is obtained through the slice Cauchy kernels and the slice regularity of the exponent mapping is proved. Further, the limits of \(J^{\alpha }x\) as \(\alpha \rightarrow 0\) and \(\alpha \rightarrow 1\) are investigated under some fixed spherical sectors. By obtaining moment inequality, we prove that \(J^{\alpha }\) is a closable operator and introduce the power with base T and exponent \(\alpha \) as the operator \(\overline{J^{\alpha }}\) , then the integral representation of \(\overline{J^{\alpha }}\) is given by the limit of S-resolvent operator of \(-T\) . Besides, the related integral expressions of \(J^{\alpha }\) are established via quaternionic semigroup when \(-T\) is the infinitesimal generator of an equibounded strongly continuous quaternionic semigroup. It is crucial to note that the fractional quaternionic operator set \(\{\overline{J_{T}^{\alpha }}:\alpha \in {\mathbb {H}}^{+}\}\) has a nice semigroup property under the \(*\) -product we introduced under the noncommutative setting. In addition, for the space consisting of right linear bounded quaternionic operators with a Schauder basis, we also obtained the semigroup property for \(J^{\alpha }\) through introducing the \(\star \) -product.