<p>We determine completely the analytic functions <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\varphi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>φ</mi> </math></EquationSource> </InlineEquation> in the unit disk <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathbb {D}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">D</mi> </math></EquationSource> </InlineEquation> such that for all (normalized) orientation-preserving harmonic mappings <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(f=h+\overline{g}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>f</mi> <mo>=</mo> <mi>h</mi> <mo>+</mo> <mover> <mi>g</mi> <mo>¯</mo> </mover> </mrow> </math></EquationSource> </InlineEquation> produced by the shear construction with <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(h+ g=\varphi \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>h</mi> <mo>+</mo> <mi>g</mi> <mo>=</mo> <mi>φ</mi> </mrow> </math></EquationSource> </InlineEquation>, the condition that each <i>f</i> maps <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(\mathbb {D}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">D</mi> </math></EquationSource> </InlineEquation> onto a convex domain holds. As a consequence, we obtain the following more general result: for a given complex number <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\eta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>η</mi> </math></EquationSource> </InlineEquation>, with <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(|\eta |=1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">|</mo> <mi>η</mi> <mo stretchy="false">|</mo> <mo>=</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation>, we characterize those holomorphic mappings <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\varphi \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>φ</mi> </math></EquationSource> </InlineEquation> in <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\mathbb {D}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">D</mi> </math></EquationSource> </InlineEquation> such that every harmonic function <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(f=h+\overline{g}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>f</mi> <mo>=</mo> <mi>h</mi> <mo>+</mo> <mover> <mi>g</mi> <mo>¯</mo> </mover> </mrow> </math></EquationSource> </InlineEquation> as above with <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(h-\eta g=\varphi \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>h</mi> <mo>-</mo> <mi>η</mi> <mi>g</mi> <mo>=</mo> <mi>φ</mi> </mrow> </math></EquationSource> </InlineEquation> maps <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(\mathbb {D}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">D</mi> </math></EquationSource> </InlineEquation> onto a convex domain. The resulting functions are mappings onto a half-plane and mappings onto a strip, and the shear direction, determined by the parameter <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(\eta \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>η</mi> </math></EquationSource> </InlineEquation> above, is parallel to the linear boundaries of the half-planes and strips.</p>

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Always-convex Harmonic Shears

  • Rodrigo Hernández,
  • María J. Martín,
  • Fernando Pérez-González,
  • Magdalena Wołoszkiewicz-Cyll

摘要

We determine completely the analytic functions \(\varphi \) φ in the unit disk \(\mathbb {D}\) D such that for all (normalized) orientation-preserving harmonic mappings \(f=h+\overline{g}\) f = h + g ¯ produced by the shear construction with \(h+ g=\varphi \) h + g = φ , the condition that each f maps \(\mathbb {D}\) D onto a convex domain holds. As a consequence, we obtain the following more general result: for a given complex number \(\eta \) η , with \(|\eta |=1\) | η | = 1 , we characterize those holomorphic mappings \(\varphi \) φ in \(\mathbb {D}\) D such that every harmonic function \(f=h+\overline{g}\) f = h + g ¯ as above with \(h-\eta g=\varphi \) h - η g = φ maps \(\mathbb {D}\) D onto a convex domain. The resulting functions are mappings onto a half-plane and mappings onto a strip, and the shear direction, determined by the parameter \(\eta \) η above, is parallel to the linear boundaries of the half-planes and strips.