<p>In the present article we obtain the approximation properties of Szász-type operators by use of wavelets in quantum calculus. We construct the Szász-type operators by <i>q</i>-calculus and introduce the Kantrovich variant of this operator by wavelets, then obtain the <InlineEquation ID="IEq1"> <EquationSource Format="MATHML"><math> <msub> <mi>L</mi> <mi>p</mi> </msub> </math></EquationSource> <EquationSource Format="TEX">$L_{p}$</EquationSource> </InlineEquation>-approximation for <InlineEquation ID="IEq2"> <EquationSource Format="MATHML"><math> <mn>1</mn> <mo>≤</mo> <mi>p</mi> <mo>≤</mo> <mi mathvariant="normal">∞</mi> </math></EquationSource> <EquationSource Format="TEX">$1\leq p \leq \infty $</EquationSource> </InlineEquation>. We obtain some characterization of second-order Lipschitz function spaces. We use the Ditzian-Totik <i>K</i>-functional and obtain some inequalities in <InlineEquation ID="IEq3"> <EquationSource Format="MATHML"><math> <msub> <mi>L</mi> <mi>p</mi> </msub> </math></EquationSource> <EquationSource Format="TEX">$L_{p}$</EquationSource> </InlineEquation> spaces. Finally, in the sense of Haar basis for all <InlineEquation ID="IEq4"> <EquationSource Format="MATHML"><math> <mn>1</mn> <mo>≤</mo> <mi>k</mi> <mo>≤</mo> <mi mathvariant="script">L</mi> <mo>∈</mo> <mi mathvariant="double-struck">N</mi> </math></EquationSource> <EquationSource Format="TEX">$1\leq k \leq \mathcal{L} \in \mathbb{N}$</EquationSource> </InlineEquation>, <InlineEquation ID="IEq5"> <EquationSource Format="MATHML"><math> <mn>0</mn> <mo>&lt;</mo> <mi>q</mi> <mo>&lt;</mo> <mn>1</mn> </math></EquationSource> <EquationSource Format="TEX">$0&lt; q&lt;1$</EquationSource> </InlineEquation> and <InlineEquation ID="IEq6"> <EquationSource Format="MATHML"><math> <mn>0</mn> <mo>≤</mo> <mi>x</mi> <mo>≤</mo> <mfrac> <mn>2</mn> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo>−</mo> <mi>q</mi> <mo stretchy="false">)</mo> <msub> <mrow> <mo stretchy="false">[</mo> <mi>m</mi> <mo stretchy="false">]</mo> </mrow> <mi>q</mi> </msub> </mrow> </mfrac> </math></EquationSource> <EquationSource Format="TEX">$0\leq x \leq \frac{2}{(1-q)[m]_{q}}$</EquationSource> </InlineEquation>, the <i>q</i>-Szász type operators by wavelets as follows: <Equation ID="Equa"> <EquationSource Format="MATHML"><math> <mrow> <mo>(</mo> <msub> <mi mathvariant="script">W</mi> <mrow> <mi>m</mi> <mo>,</mo> <mi>k</mi> <mo>,</mo> <mi>q</mi> </mrow> </msub> <mspace width="0.25em" /> <mi>g</mi> <mo>)</mo> </mrow> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> <mo>=</mo> <mfrac> <mn>1</mn> <msubsup> <mi mathvariant="script">E</mi> <mi>q</mi> <mrow> <msub> <mrow> <mo stretchy="false">[</mo> <mi>m</mi> <mo stretchy="false">]</mo> </mrow> <mi>q</mi> </msub> <mi>x</mi> </mrow> </msubsup> </mfrac> <munderover> <mo movablelimits="false">∑</mo> <mrow> <mi>k</mi> <mo>=</mo> <mn>0</mn> </mrow> <mi mathvariant="normal">∞</mi> </munderover> <msup> <mi>q</mi> <mfrac> <mrow> <mi>k</mi> <mo stretchy="false">(</mo> <mi>k</mi> <mo>−</mo> <mn>1</mn> <mo stretchy="false">)</mo> </mrow> <mn>2</mn> </mfrac> </msup> <mfrac> <msup> <mrow> <mo stretchy="false">(</mo> <msub> <mrow> <mo stretchy="false">[</mo> <mi>m</mi> <mo stretchy="false">]</mo> </mrow> <mi>q</mi> </msub> <mi>x</mi> <mo stretchy="false">)</mo> </mrow> <mi>k</mi> </msup> <mrow> <msub> <mrow> <mo stretchy="false">[</mo> <mi>k</mi> <mo stretchy="false">]</mo> </mrow> <mi>q</mi> </msub> <mo>!</mo> </mrow> </mfrac> <msubsup> <mo>∫</mo> <mn>0</mn> <mi mathvariant="normal">Ω</mi> </msubsup> <mi>g</mi> <mrow> <mo>(</mo> <mfrac> <mrow> <mi>t</mi> <mo>+</mo> <msub> <mrow> <mo stretchy="false">[</mo> <mi>k</mi> <mo stretchy="false">]</mo> </mrow> <mi>q</mi> </msub> </mrow> <msub> <mrow> <mo stretchy="false">[</mo> <mi>m</mi> <mo stretchy="false">]</mo> </mrow> <mi>q</mi> </msub> </mfrac> <mo>)</mo> </mrow> <mi>λ</mi> <mrow> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> <msub> <mi mathvariant="normal">d</mi> <mi>q</mi> </msub> <mi>t</mi> <mo>.</mo> </math></EquationSource> <EquationSource Format="TEX">\( \left (\mathcal{W}_{m,k,q} \; g\right )(x)= \frac{1}{\mathcal{E}_{q}^{[m]_{q} x}} \sum _{k=0}^{\infty } q^{\frac{k(k-1)}{2}} \frac{([m]_{q} x)^{k}}{[k]_{q}!} \int _{0}^{\Omega } g\left ( \frac{t+[k]_{q}}{[m]_{q}}\right )\lambda \left (t\right )\mathrm{d}_{q}t. \)</EquationSource> </Equation></p>

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Function preserving the wavelets-associated approximation by Szász-type operators in quantum calculus

  • Md. Nasiruzzaman

摘要

In the present article we obtain the approximation properties of Szász-type operators by use of wavelets in quantum calculus. We construct the Szász-type operators by q-calculus and introduce the Kantrovich variant of this operator by wavelets, then obtain the L p $L_{p}$ -approximation for 1 p $1\leq p \leq \infty $ . We obtain some characterization of second-order Lipschitz function spaces. We use the Ditzian-Totik K-functional and obtain some inequalities in L p $L_{p}$ spaces. Finally, in the sense of Haar basis for all 1 k L N $1\leq k \leq \mathcal{L} \in \mathbb{N}$ , 0 < q < 1 $0< q<1$ and 0 x 2 ( 1 q ) [ m ] q $0\leq x \leq \frac{2}{(1-q)[m]_{q}}$ , the q-Szász type operators by wavelets as follows: ( W m , k , q g ) ( x ) = 1 E q [ m ] q x k = 0 q k ( k 1 ) 2 ( [ m ] q x ) k [ k ] q ! 0 Ω g ( t + [ k ] q [ m ] q ) λ ( t ) d q t . \( \left (\mathcal{W}_{m,k,q} \; g\right )(x)= \frac{1}{\mathcal{E}_{q}^{[m]_{q} x}} \sum _{k=0}^{\infty } q^{\frac{k(k-1)}{2}} \frac{([m]_{q} x)^{k}}{[k]_{q}!} \int _{0}^{\Omega } g\left ( \frac{t+[k]_{q}}{[m]_{q}}\right )\lambda \left (t\right )\mathrm{d}_{q}t. \)