<p>In this paper we discuss about convex combinations of the form <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathcal {K}_{n,\lambda }^{\alpha ,\beta }=(1-\lambda )\Psi _{n,\alpha }+\lambda \Psi _{n,\beta }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi mathvariant="script">K</mi> <mrow> <mi>n</mi> <mo>,</mo> <mi>λ</mi> </mrow> <mrow> <mi>α</mi> <mo>,</mo> <mi>β</mi> </mrow> </msubsup> <mo>=</mo> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo>-</mo> <mi>λ</mi> <mo stretchy="false">)</mo> </mrow> <msub> <mi mathvariant="normal">Ψ</mi> <mrow> <mi>n</mi> <mo>,</mo> <mi>α</mi> </mrow> </msub> <mo>+</mo> <mi>λ</mi> <msub> <mi mathvariant="normal">Ψ</mi> <mrow> <mi>n</mi> <mo>,</mo> <mi>β</mi> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation> of Graham-Kohr type extension operators <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\Psi _{n,\alpha }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Ψ</mi> <mrow> <mi>n</mi> <mo>,</mo> <mi>α</mi> </mrow> </msub> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\lambda \in [0,1]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>λ</mi> <mo>∈</mo> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">]</mo> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\alpha ,\beta \in [0,1]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>,</mo> <mi>β</mi> <mo>∈</mo> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">]</mo> </mrow> </math></EquationSource> </InlineEquation>. The operators <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\Psi _{n,\alpha }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Ψ</mi> <mrow> <mi>n</mi> <mo>,</mo> <mi>α</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> were defined by I. Graham and G. Kohr in Complex Variables Theory Appl. 47 (2002), 59-72. They proved that the extension operator <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\Psi _{n,\alpha }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Ψ</mi> <mrow> <mi>n</mi> <mo>,</mo> <mi>α</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> preserve the starlikeness for all <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(n\ge {2}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>≥</mo> <mn>2</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\alpha \in [0,1]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>α</mi> <mo>∈</mo> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">]</mo> </mrow> </math></EquationSource> </InlineEquation>. The main idea of this paper is to obtain new extension operators defined by convex combinations of Graham-Kohr type operators <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\Psi _{n,\alpha }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Ψ</mi> <mrow> <mi>n</mi> <mo>,</mo> <mi>α</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> that preserve the starlikeness. We prove that a starlike function <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(f\in S^*\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>f</mi> <mo>∈</mo> <msup> <mi>S</mi> <mo>∗</mo> </msup> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\mathfrak {Re}f'(z_1)&gt;0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi mathvariant="fraktur">Re</mi> <msup> <mi>f</mi> <mo>′</mo> </msup> <mrow> <mo stretchy="false">(</mo> <msub> <mi>z</mi> <mn>1</mn> </msub> <mo stretchy="false">)</mo> </mrow> <mo>&gt;</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, for all <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(z_1\in \mathbb {U}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>z</mi> <mn>1</mn> </msub> <mo>∈</mo> <mi mathvariant="double-struck">U</mi> </mrow> </math></EquationSource> </InlineEquation>, is taken to a starlike mapping on the Euclidean unit ball <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\mathbb {B}^n\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">B</mi> </mrow> <mi>n</mi> </msup> </math></EquationSource> </InlineEquation> by the operators <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\mathcal {K}_{\lambda }^{0}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi mathvariant="script">K</mi> <mrow> <mi>λ</mi> </mrow> <mn>0</mn> </msubsup> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\mathcal {K}_{\lambda }^{1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi mathvariant="script">K</mi> <mrow> <mi>λ</mi> </mrow> <mn>1</mn> </msubsup> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq16"> <EquationSource Format="TEX">\(\mathcal {K}_{\lambda }^{0}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi mathvariant="script">K</mi> <mrow> <mi>λ</mi> </mrow> <mn>0</mn> </msubsup> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq17"> <EquationSource Format="TEX">\(\mathcal {K}_{\lambda }^{1}\)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mi mathvariant="script">K</mi> <mrow> <mi>λ</mi> </mrow> <mn>1</mn> </msubsup> </math></EquationSource> </InlineEquation> are particular forms of the operator <InlineEquation ID="IEq18"> <EquationSource Format="TEX">\(\mathcal {K}_{n,\lambda }^{\alpha ,\beta }.\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi mathvariant="script">K</mi> <mrow> <mi>n</mi> <mo>,</mo> <mi>λ</mi> </mrow> <mrow> <mi>α</mi> <mo>,</mo> <mi>β</mi> </mrow> </msubsup> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation></p>

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Convex Combinations of Graham-Kohr Type Extension Operators

  • Eduard Ştefan Grigoriciuc

摘要

In this paper we discuss about convex combinations of the form \(\mathcal {K}_{n,\lambda }^{\alpha ,\beta }=(1-\lambda )\Psi _{n,\alpha }+\lambda \Psi _{n,\beta }\) K n , λ α , β = ( 1 - λ ) Ψ n , α + λ Ψ n , β of Graham-Kohr type extension operators \(\Psi _{n,\alpha }\) Ψ n , α , where \(\lambda \in [0,1]\) λ [ 0 , 1 ] and \(\alpha ,\beta \in [0,1]\) α , β [ 0 , 1 ] . The operators \(\Psi _{n,\alpha }\) Ψ n , α were defined by I. Graham and G. Kohr in Complex Variables Theory Appl. 47 (2002), 59-72. They proved that the extension operator \(\Psi _{n,\alpha }\) Ψ n , α preserve the starlikeness for all \(n\ge {2}\) n 2 and \(\alpha \in [0,1]\) α [ 0 , 1 ] . The main idea of this paper is to obtain new extension operators defined by convex combinations of Graham-Kohr type operators \(\Psi _{n,\alpha }\) Ψ n , α that preserve the starlikeness. We prove that a starlike function \(f\in S^*\) f S with \(\mathfrak {Re}f'(z_1)>0\) Re f ( z 1 ) > 0 , for all \(z_1\in \mathbb {U}\) z 1 U , is taken to a starlike mapping on the Euclidean unit ball \(\mathbb {B}^n\) B n by the operators \(\mathcal {K}_{\lambda }^{0}\) K λ 0 and \(\mathcal {K}_{\lambda }^{1}\) K λ 1 , where \(\mathcal {K}_{\lambda }^{0}\) K λ 0 and \(\mathcal {K}_{\lambda }^{1}\) K λ 1 are particular forms of the operator \(\mathcal {K}_{n,\lambda }^{\alpha ,\beta }.\) K n , λ α , β .