<p>Consider the set <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathcal {V}_p(\lambda )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">V</mi> <mi>p</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>λ</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>, which is defined as the collection of those functions <i>f</i> on the open unit disc <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathbb {D}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">D</mi> </math></EquationSource> </InlineEquation> in the plane of complex numbers which have a simple pole at <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(z=p\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>z</mi> <mo>=</mo> <mi>p</mi> </mrow> </math></EquationSource> </InlineEquation>, provided <i>p</i> is in the interval (0,&#xa0;1). They are analytic in <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(\mathbb {D}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">D</mi> </math></EquationSource> </InlineEquation> except at <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(z=p\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>z</mi> <mo>=</mo> <mi>p</mi> </mrow> </math></EquationSource> </InlineEquation>. Additionally, they satisfy the normalizations <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(f(0)=0, f'(0)-1=0\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mn>0</mn> <mo>,</mo> <msup> <mi>f</mi> <mo>′</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mn>0</mn> <mo stretchy="false">)</mo> </mrow> <mo>-</mo> <mn>1</mn> <mo>=</mo> <mn>0</mn> </mrow> </math></EquationSource> </InlineEquation>, and for all <i>z</i> in <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\mathbb {D} \)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">D</mi> </math></EquationSource> </InlineEquation> and <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(\lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>λ</mi> </math></EquationSource> </InlineEquation> in the interval (0,&#xa0;1], the inequality <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(\left| (z/f(z))^2 f'(z)-1\right| &lt; \lambda \)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mfenced close="|" open="|"> <msup> <mrow> <mo stretchy="false">(</mo> <mi>z</mi> <mo stretchy="false">/</mo> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>z</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">)</mo> </mrow> <mn>2</mn> </msup> <msup> <mi>f</mi> <mo>′</mo> </msup> <mrow> <mo stretchy="false">(</mo> <mi>z</mi> <mo stretchy="false">)</mo> </mrow> <mo>-</mo> <mn>1</mn> </mfenced> <mo>&lt;</mo> <mi>λ</mi> </mrow> </math></EquationSource> </InlineEquation> is satisfied. Every function <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(f\in \mathcal {V}_p(\lambda )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>f</mi> <mo>∈</mo> <msub> <mi mathvariant="script">V</mi> <mi>p</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>λ</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> can be expressed as a Taylor series expansion: <Equation ID="Equ21"> <EquationSource Format="TEX">\( f(z)=z+\sum _{n=2}^{\infty }a_n z^n, \quad |z|&lt;p. \)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mi>f</mi> <mrow> <mo stretchy="false">(</mo> <mi>z</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mi>z</mi> <mo>+</mo> <munderover> <mo>∑</mo> <mrow> <mi>n</mi> <mo>=</mo> <mn>2</mn> </mrow> <mi>∞</mi> </munderover> <msub> <mi>a</mi> <mi>n</mi> </msub> <msup> <mi>z</mi> <mi>n</mi> </msup> <mo>,</mo> <mspace width="1em" /> <mrow> <mo stretchy="false">|</mo> <mi>z</mi> <mo stretchy="false">|</mo> </mrow> <mo>&lt;</mo> <mi>p</mi> <mo>.</mo> </mrow> </math></EquationSource> </Equation>This paper initially determines the regions of variability of the difference of subsequent coefficients <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\((a_{n+1}-a_n)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mo stretchy="false">(</mo> <msub> <mi>a</mi> <mrow> <mi>n</mi> <mo>+</mo> <mn>1</mn> </mrow> </msub> <mo>-</mo> <msub> <mi>a</mi> <mi>n</mi> </msub> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> for <InlineEquation ID="IEq12"> <EquationSource Format="TEX">\(n\ge 1\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>n</mi> <mo>≥</mo> <mn>1</mn> </mrow> </math></EquationSource> </InlineEquation> within a specific range of values of <InlineEquation ID="IEq13"> <EquationSource Format="TEX">\(p\in (0,1)\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>p</mi> <mo>∈</mo> <mo stretchy="false">(</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> </math></EquationSource> </InlineEquation> for functions in the class <InlineEquation ID="IEq14"> <EquationSource Format="TEX">\(\mathcal {V}_p(\lambda )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">V</mi> <mi>p</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>λ</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>. As a result of this analysis, we also obtain sharp upper bounds for the determinants of Toeplitz and Hermitian Toeplitz matrices, where the entries of these matrices correspond to the Taylor coefficients of functions in <InlineEquation ID="IEq15"> <EquationSource Format="TEX">\(\mathcal {V}_p(\lambda )\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">V</mi> <mi>p</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>λ</mi> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation>.</p>

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Successive coefficients, Toeplitz and Hermitian Toeplitz determinant for certain meromorphic univalent functions

  • Alana John,
  • Firdoshi Parveen

摘要

Consider the set \(\mathcal {V}_p(\lambda )\) V p ( λ ) , which is defined as the collection of those functions f on the open unit disc \(\mathbb {D}\) D in the plane of complex numbers which have a simple pole at \(z=p\) z = p , provided p is in the interval (0, 1). They are analytic in \(\mathbb {D}\) D except at \(z=p\) z = p . Additionally, they satisfy the normalizations \(f(0)=0, f'(0)-1=0\) f ( 0 ) = 0 , f ( 0 ) - 1 = 0 , and for all z in \(\mathbb {D} \) D and \(\lambda \) λ in the interval (0, 1], the inequality \(\left| (z/f(z))^2 f'(z)-1\right| < \lambda \) ( z / f ( z ) ) 2 f ( z ) - 1 < λ is satisfied. Every function \(f\in \mathcal {V}_p(\lambda )\) f V p ( λ ) can be expressed as a Taylor series expansion: \( f(z)=z+\sum _{n=2}^{\infty }a_n z^n, \quad |z|<p. \) f ( z ) = z + n = 2 a n z n , | z | < p . This paper initially determines the regions of variability of the difference of subsequent coefficients \((a_{n+1}-a_n)\) ( a n + 1 - a n ) for \(n\ge 1\) n 1 within a specific range of values of \(p\in (0,1)\) p ( 0 , 1 ) for functions in the class \(\mathcal {V}_p(\lambda )\) V p ( λ ) . As a result of this analysis, we also obtain sharp upper bounds for the determinants of Toeplitz and Hermitian Toeplitz matrices, where the entries of these matrices correspond to the Taylor coefficients of functions in \(\mathcal {V}_p(\lambda )\) V p ( λ ) .