<p>In this paper we focus our attention on the Graham–Kohr extension operator <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\Psi _{\alpha }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Ψ</mi> <mi>α</mi> </msub> </math></EquationSource> </InlineEquation> (introduced by Graham and Kohr in Complex Var. Theory Appl. 47:59–72, 2002) defined by <Equation ID="Equ28"> <EquationSource Format="TEX">\(\begin{aligned} \Psi _{\alpha }(f)(z_1,w)=\bigg (f(z_1),\bigg (\dfrac{f(z_1)}{z_1}\bigg )^{\alpha }w \bigg ), \quad (z_1,w)\in \Omega _{p,r}, \, \alpha \in [0,1] \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <msub> <mi mathvariant="normal">Ψ</mi> <mi>α</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>f</mi> <mo stretchy="false">)</mo> </mrow> <mrow> <mo stretchy="false">(</mo> <msub> <mi>z</mi> <mn>1</mn> </msub> <mo>,</mo> <mi>w</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mrow> <mo maxsize="2.047em" minsize="2.047em" stretchy="true">(</mo> </mrow> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <msub> <mi>z</mi> <mn>1</mn> </msub> <mo stretchy="false">)</mo> </mrow> <mo>,</mo> <mrow> <mo maxsize="2.047em" minsize="2.047em" stretchy="true">(</mo> </mrow> <mstyle displaystyle="true" scriptlevel="0"> <mfrac> <mrow> <mi>f</mi> <mo stretchy="false">(</mo> <msub> <mi>z</mi> <mn>1</mn> </msub> <mo stretchy="false">)</mo> </mrow> <msub> <mi>z</mi> <mn>1</mn> </msub> </mfrac> </mstyle> <msup> <mrow> <mo maxsize="2.047em" minsize="2.047em" stretchy="true">)</mo> </mrow> <mi>α</mi> </msup> <mi>w</mi> <mrow> <mo maxsize="2.047em" minsize="2.047em" stretchy="true">)</mo> </mrow> <mo>,</mo> <mspace width="1em" /> <mrow> <mo stretchy="false">(</mo> <msub> <mi>z</mi> <mn>1</mn> </msub> <mo>,</mo> <mi>w</mi> <mo stretchy="false">)</mo> </mrow> <mo>∈</mo> <msub> <mi mathvariant="normal">Ω</mi> <mrow> <mi>p</mi> <mo>,</mo> <mi>r</mi> </mrow> </msub> <mo>,</mo> <mspace width="0.166667em" /> <mi>α</mi> <mo>∈</mo> <mrow> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">]</mo> </mrow> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>and its properties on the domain <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\Omega _{p,r}=\{(z_1,w)\in \mathbb {C}\times X:\vert z_1\vert ^p+\Vert w\Vert ^r_X&lt;1\}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="normal">Ω</mi> <mrow> <mi>p</mi> <mo>,</mo> <mi>r</mi> </mrow> </msub> <mrow> <mo>=</mo> <mo stretchy="false">{</mo> </mrow> <mrow> <mo stretchy="false">(</mo> <msub> <mi>z</mi> <mn>1</mn> </msub> <mo>,</mo> <mi>w</mi> <mo stretchy="false">)</mo> </mrow> <mrow> <mo>∈</mo> <mi mathvariant="double-struck">C</mi> <mo>×</mo> <mi>X</mi> <mo>:</mo> <mo stretchy="false">|</mo> </mrow> <msub> <mi>z</mi> <mn>1</mn> </msub> <msup> <mrow> <mo stretchy="false">|</mo> </mrow> <mi>p</mi> </msup> <mo>+</mo> <msubsup> <mrow> <mo stretchy="false">‖</mo> <mi>w</mi> <mo stretchy="false">‖</mo> </mrow> <mi>X</mi> <mi>r</mi> </msubsup> <mrow> <mo>&lt;</mo> <mn>1</mn> <mo stretchy="false">}</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, where <i>X</i> is a complex Banach space and <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(p,r\ge {1}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>,</mo> <mi>r</mi> <mo>≥</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>. In the main part of the paper we will prove that the Graham–Kohr extension operator <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\Psi _{\alpha }\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Ψ</mi> <mi>α</mi> </msub> </math></EquationSource> </InlineEquation> preserves the first elements of <i>g</i>-Loewner chains from the unit disc <i>U</i> to the domain <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\Omega _{p,r}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Ω</mi> <mrow> <mi>p</mi> <mo>,</mo> <mi>r</mi> </mrow> </msub> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(p,r\ge {1}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>,</mo> <mi>r</mi> <mo>≥</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq7"> <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>. As consequences of this result, we obtain that the Graham–Kohr extension operator preserves, in particular, the first elements of Loewner chains, the <i>g</i>-starlike mappings, the strongly starlike mappings of order <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(d\in (0,1]\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>d</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">]</mo> </mrow> </math></EquationSource> </InlineEquation>, the parabolic starlike mappings of order <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(d\in [0,1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>d</mi> <mo>∈</mo> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, the starlike mappings of complex order <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation>, the almost starlike mappings of order <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(\mu \in [0,1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>μ</mi> <mo>∈</mo> <mo stretchy="false">[</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation>, respectively the spirallike mappings of order <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\delta \in (-\pi /2,\pi /2)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>δ</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mo>-</mo> <mi>π</mi> <mo stretchy="false">/</mo> <mn>2</mn> <mo>,</mo> <mi>π</mi> <mo stretchy="false">/</mo> <mn>2</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> on the same domain <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\Omega _{p,r}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi mathvariant="normal">Ω</mi> <mrow> <mi>p</mi> <mo>,</mo> <mi>r</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(p,r\ge {1}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>,</mo> <mi>r</mi> <mo>≥</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>.</p>

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g-Loewner Chains and the Graham–Kohr Extension Operator in Complex Banach Spaces

  • Eduard Ştefan Grigoriciuc

摘要

In this paper we focus our attention on the Graham–Kohr extension operator \(\Psi _{\alpha }\) Ψ α (introduced by Graham and Kohr in Complex Var. Theory Appl. 47:59–72, 2002) defined by \(\begin{aligned} \Psi _{\alpha }(f)(z_1,w)=\bigg (f(z_1),\bigg (\dfrac{f(z_1)}{z_1}\bigg )^{\alpha }w \bigg ), \quad (z_1,w)\in \Omega _{p,r}, \, \alpha \in [0,1] \end{aligned}\) Ψ α ( f ) ( z 1 , w ) = ( f ( z 1 ) , ( f ( z 1 ) z 1 ) α w ) , ( z 1 , w ) Ω p , r , α [ 0 , 1 ] and its properties on the domain \(\Omega _{p,r}=\{(z_1,w)\in \mathbb {C}\times X:\vert z_1\vert ^p+\Vert w\Vert ^r_X<1\}\) Ω p , r = { ( z 1 , w ) C × X : | z 1 | p + w X r < 1 } , where X is a complex Banach space and \(p,r\ge {1}\) p , r 1 . In the main part of the paper we will prove that the Graham–Kohr extension operator \(\Psi _{\alpha }\) Ψ α preserves the first elements of g-Loewner chains from the unit disc U to the domain \(\Omega _{p,r}\) Ω p , r , where \(p,r\ge {1}\) p , r 1 and \(\alpha \in [0,1]\) α [ 0 , 1 ] . As consequences of this result, we obtain that the Graham–Kohr extension operator preserves, in particular, the first elements of Loewner chains, the g-starlike mappings, the strongly starlike mappings of order \(d\in (0,1]\) d ( 0 , 1 ] , the parabolic starlike mappings of order \(d\in [0,1)\) d [ 0 , 1 ) , the starlike mappings of complex order \(\lambda \) λ , the almost starlike mappings of order \(\mu \in [0,1)\) μ [ 0 , 1 ) , respectively the spirallike mappings of order \(\delta \in (-\pi /2,\pi /2)\) δ ( - π / 2 , π / 2 ) on the same domain \(\Omega _{p,r}\) Ω p , r for \(p,r\ge {1}\) p , r 1 .