<p>The two-dimensional moment problem consists of finding a positive Borel measure <InlineEquation ID="IEq1"> <EquationSource Format="TEX">\(\mu \)</EquationSource> <EquationSource Format="MATHML"><math> <mi>μ</mi> </math></EquationSource> </InlineEquation> in <InlineEquation ID="IEq2"> <EquationSource Format="TEX">\(\mathbb {R}^2\)</EquationSource> <EquationSource Format="MATHML"><math> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> </math></EquationSource> </InlineEquation> such that <InlineEquation ID="IEq3"> <EquationSource Format="TEX">\(\int _{\mathbb {R}^2} t_1^m t_2^n d\mu = s_{m,n}\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <msub> <mo>∫</mo> <msup> <mrow> <mi mathvariant="double-struck">R</mi> </mrow> <mn>2</mn> </msup> </msub> <msubsup> <mi>t</mi> <mn>1</mn> <mi>m</mi> </msubsup> <msubsup> <mi>t</mi> <mn>2</mn> <mi>n</mi> </msubsup> <mi>d</mi> <mi>μ</mi> <mo>=</mo> <msub> <mi>s</mi> <mrow> <mi>m</mi> <mo>,</mo> <mi>n</mi> </mrow> </msub> </mrow> </math></EquationSource> </InlineEquation>, <InlineEquation ID="IEq4"> <EquationSource Format="TEX">\(m,n=0,1,2,...\)</EquationSource> <EquationSource Format="MATHML"><math> <mrow> <mi>m</mi> <mo>,</mo> <mi>n</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo>,</mo> <mn>2</mn> <mo>,</mo> <mo>.</mo> <mo>.</mo> <mo>.</mo> </mrow> </math></EquationSource> </InlineEquation>, where <InlineEquation ID="IEq5"> <EquationSource Format="TEX">\(s_{m,n}\)</EquationSource> <EquationSource Format="MATHML"><math> <msub> <mi>s</mi> <mrow> <mi>m</mi> <mo>,</mo> <mi>n</mi> </mrow> </msub> </math></EquationSource> </InlineEquation> are prescribed real constants (moments). We study this moment problem in the case when the sequence <InlineEquation ID="IEq6"> <EquationSource Format="TEX">\(\{ s_{m,n} \}_{m,n=0}^\infty \)</EquationSource> <EquationSource Format="MATHML"><math> <msubsup> <mrow> <mo stretchy="false">{</mo> <msub> <mi>s</mi> <mrow> <mi>m</mi> <mo>,</mo> <mi>n</mi> </mrow> </msub> <mo stretchy="false">}</mo> </mrow> <mrow> <mi>m</mi> <mo>,</mo> <mi>n</mi> <mo>=</mo> <mn>0</mn> </mrow> <mi>∞</mi> </msubsup> </math></EquationSource> </InlineEquation> is positive semi-definite, and the following Carleman-type conditions hold: <Equation ID="Equ72"> <EquationSource Format="TEX">\(\begin{aligned} \sum _{k=1}^\infty \frac{1}{ \root 2k \of { s_{2m,2k} + s_{2m+2,2k} } } = \infty ,\quad m=0,1,2,.... \end{aligned}\)</EquationSource> <EquationSource Format="MATHML"><math display="block"> <mrow> <mtable> <mtr> <mtd columnalign="right"> <mrow> <munderover> <mo>∑</mo> <mrow> <mi>k</mi> <mo>=</mo> <mn>1</mn> </mrow> <mi>∞</mi> </munderover> <mfrac> <mn>1</mn> <mroot> <mrow> <msub> <mi>s</mi> <mrow> <mn>2</mn> <mi>m</mi> <mo>,</mo> <mn>2</mn> <mi>k</mi> </mrow> </msub> <mo>+</mo> <msub> <mi>s</mi> <mrow> <mn>2</mn> <mi>m</mi> <mo>+</mo> <mn>2</mn> <mo>,</mo> <mn>2</mn> <mi>k</mi> </mrow> </msub> </mrow> <mrow> <mn>2</mn> <mi>k</mi> </mrow> </mroot> </mfrac> <mo>=</mo> <mi>∞</mi> <mo>,</mo> <mspace width="1em" /> <mi>m</mi> <mo>=</mo> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo>,</mo> <mn>2</mn> <mo>,</mo> <mo>.</mo> <mo>.</mo> <mo>.</mo> <mo>.</mo> </mrow> </mtd> </mtr> </mtable> </mrow> </math></EquationSource> </Equation>In this case all solutions of the moment problem are parameterized by a class of analytic contractive operator-valued functions. The special case of the determinate moment problem is characterized. We introduce a notion of a generalized resolvent for a pair of commuting symmetric operators. We use basic properties of such generalized resolvents as a main tool in studying the above moment problem.</p>

错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

An Analytical Parameterization for all Solutions of the Two-Dimensional Moment Problem Under Carleman-Type Conditions

  • S. M. Zagorodnyuk

摘要

The two-dimensional moment problem consists of finding a positive Borel measure \(\mu \) μ in \(\mathbb {R}^2\) R 2 such that \(\int _{\mathbb {R}^2} t_1^m t_2^n d\mu = s_{m,n}\) R 2 t 1 m t 2 n d μ = s m , n , \(m,n=0,1,2,...\) m , n = 0 , 1 , 2 , . . . , where \(s_{m,n}\) s m , n are prescribed real constants (moments). We study this moment problem in the case when the sequence \(\{ s_{m,n} \}_{m,n=0}^\infty \) { s m , n } m , n = 0 is positive semi-definite, and the following Carleman-type conditions hold: \(\begin{aligned} \sum _{k=1}^\infty \frac{1}{ \root 2k \of { s_{2m,2k} + s_{2m+2,2k} } } = \infty ,\quad m=0,1,2,.... \end{aligned}\) k = 1 1 s 2 m , 2 k + s 2 m + 2 , 2 k 2 k = , m = 0 , 1 , 2 , . . . . In this case all solutions of the moment problem are parameterized by a class of analytic contractive operator-valued functions. The special case of the determinate moment problem is characterized. We introduce a notion of a generalized resolvent for a pair of commuting symmetric operators. We use basic properties of such generalized resolvents as a main tool in studying the above moment problem.