<p>Let <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mathbb {D}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">D</mi> </math></EquationSource> </InlineEquation> be the open unit disk in the complex plane <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathbb {C}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="double-struck">C</mi> </math></EquationSource> </InlineEquation> and let <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\mathcal {M}\)</EquationSource> <EquationSource Format="MATHML"><math> <mi mathvariant="script">M</mi> </math></EquationSource> </InlineEquation> be a semifinite von Neumann algebra. The main result of this paper is the weak type (1,&#xa0;1) inequality of the weighted Bergman projection <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(P_{w}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>P</mi> <mi>w</mi> </msub> </math></EquationSource> </InlineEquation> induced by reproducing kernels <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(K_z(\zeta )=\frac{1}{(1-\bar{z} \zeta )^\gamma } \int _0^1 \frac{d \nu (r)}{1-r \bar{z} \zeta }\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi>K</mi> <mi>z</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi>ζ</mi> <mo stretchy="false">)</mo> </mrow> <mo>=</mo> <mfrac> <mn>1</mn> <msup> <mrow> <mo stretchy="false">(</mo> <mn>1</mn> <mo>-</mo> <mover accent="true"> <mrow> <mi>z</mi> </mrow> <mrow> <mo stretchy="false">¯</mo> </mrow> </mover> <mi>ζ</mi> <mo stretchy="false">)</mo> </mrow> <mi>γ</mi> </msup> </mfrac> <msubsup> <mo>∫</mo> <mn>0</mn> <mn>1</mn> </msubsup> <mfrac> <mrow> <mi>d</mi> <mi>ν</mi> <mo stretchy="false">(</mo> <mi>r</mi> <mo stretchy="false">)</mo> </mrow> <mrow> <mn>1</mn> <mo>-</mo> <mi>r</mi> <mover accent="true"> <mrow> <mi>z</mi> </mrow> <mrow> <mo stretchy="false">¯</mo> </mrow> </mover> <mi>ζ</mi> </mrow> </mfrac> </mrow> </math></EquationSource> </InlineEquation>, that is, if <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(v\in B_{1,w}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>v</mi> <mo>∈</mo> <msub> <mi>B</mi> <mrow> <mn>1</mn> <mo>,</mo> <mi>w</mi> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation>, then: <Equation ID="Equ25"> <EquationSource Format="TEX">\(\Vert P_{w}(f)\Vert _{L^{v}_{1, \infty }(\mathcal {N}_{\mathbb {D}})}\le CB_{1,w}(v)^2\Vert f\Vert _{L^{v}_1(\mathcal {N}_{\mathbb {D}})},\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mrow> <mo stretchy="false">‖</mo> </mrow> <msub> <mi>P</mi> <mi>w</mi> </msub> <msub> <mrow> <mrow> <mo stretchy="false">(</mo> <mi>f</mi> <mo stretchy="false">)</mo> </mrow> <mo stretchy="false">‖</mo> </mrow> <mrow> <msubsup> <mi>L</mi> <mrow> <mn>1</mn> <mo>,</mo> <mi>∞</mi> </mrow> <mi>v</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <msub> <mi mathvariant="script">N</mi> <mi mathvariant="double-struck">D</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </msub> <mo>≤</mo> <mi>C</mi> <msub> <mi>B</mi> <mrow> <mn>1</mn> <mo>,</mo> <mi>w</mi> </mrow> </msub> <msup> <mrow> <mo stretchy="false">(</mo> <mi>v</mi> <mo stretchy="false">)</mo> </mrow> <mn>2</mn> </msup> <msub> <mrow> <mo stretchy="false">‖</mo> <mi>f</mi> <mo stretchy="false">‖</mo> </mrow> <mrow> <msubsup> <mi>L</mi> <mn>1</mn> <mi>v</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <msub> <mi mathvariant="script">N</mi> <mi mathvariant="double-struck">D</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </msub> <mo>,</mo> </mrow> </math></EquationSource> </Equation>where <InlineEquation ID="IEq7"> <EquationSource Format="TEX">\(\mathcal {N}_{\mathbb {D}}=L_{\infty }(\mathbb {D},A_{w})\bar{\otimes } \mathcal {M}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mi mathvariant="script">N</mi> <mi mathvariant="double-struck">D</mi> </msub> <mo>=</mo> <msub> <mi>L</mi> <mi>∞</mi> </msub> <mrow> <mo stretchy="false">(</mo> <mi mathvariant="double-struck">D</mi> <mo>,</mo> <msub> <mi>A</mi> <mi>w</mi> </msub> <mo stretchy="false">)</mo> </mrow> <mover accent="true"> <mrow> <mo>⊗</mo> </mrow> <mrow> <mo stretchy="false">¯</mo> </mrow> </mover> <mi mathvariant="script">M</mi> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq8"> <EquationSource Format="TEX">\(A_{w}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>A</mi> <mi>w</mi> </msub> </math></EquationSource> </InlineEquation> is the normalized Lebesgue area measure related to weight <i>w</i>. Moreover, <InlineEquation ID="IEq9"> <EquationSource Format="TEX">\(P_{w}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>P</mi> <mi>w</mi> </msub> </math></EquationSource> </InlineEquation> is bounded on <InlineEquation ID="IEq10"> <EquationSource Format="TEX">\(L^{v}_{p }(\mathcal {N}_{\mathbb {D}})\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msubsup> <mi>L</mi> <mi>p</mi> <mi>v</mi> </msubsup> <mrow> <mo stretchy="false">(</mo> <msub> <mi mathvariant="script">N</mi> <mi mathvariant="double-struck">D</mi> </msub> <mo stretchy="false">)</mo> </mrow> </mrow> </math></EquationSource> </InlineEquation> with <InlineEquation ID="IEq11"> <EquationSource Format="TEX">\(1&lt;p&lt;\infty .\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mn>1</mn> <mo>&lt;</mo> <mi>p</mi> <mo>&lt;</mo> <mi>∞</mi> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation></p>

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Weighted Bergman Projections Induced By Kernel With Integral Representation in Operator-Valued Setting

  • Chengshu Tian

摘要

Let \(\mathbb {D}\) D be the open unit disk in the complex plane \(\mathbb {C}\) C and let \(\mathcal {M}\) M be a semifinite von Neumann algebra. The main result of this paper is the weak type (1, 1) inequality of the weighted Bergman projection \(P_{w}\) P w induced by reproducing kernels \(K_z(\zeta )=\frac{1}{(1-\bar{z} \zeta )^\gamma } \int _0^1 \frac{d \nu (r)}{1-r \bar{z} \zeta }\) K z ( ζ ) = 1 ( 1 - z ¯ ζ ) γ 0 1 d ν ( r ) 1 - r z ¯ ζ , that is, if \(v\in B_{1,w}\) v B 1 , w , then: \(\Vert P_{w}(f)\Vert _{L^{v}_{1, \infty }(\mathcal {N}_{\mathbb {D}})}\le CB_{1,w}(v)^2\Vert f\Vert _{L^{v}_1(\mathcal {N}_{\mathbb {D}})},\) P w ( f ) L 1 , v ( N D ) C B 1 , w ( v ) 2 f L 1 v ( N D ) , where \(\mathcal {N}_{\mathbb {D}}=L_{\infty }(\mathbb {D},A_{w})\bar{\otimes } \mathcal {M}\) N D = L ( D , A w ) ¯ M , \(A_{w}\) A w is the normalized Lebesgue area measure related to weight w. Moreover, \(P_{w}\) P w is bounded on \(L^{v}_{p }(\mathcal {N}_{\mathbb {D}})\) L p v ( N D ) with \(1<p<\infty .\) 1 < p < .