Functions of perturbed pairs of noncommutative dissipative operators

IF 0.7 4区 数学 Q2 MATHEMATICS St Petersburg Mathematical Journal Pub Date : 2023-06-07 DOI:10.1090/spmj/1758
A. Aleksandrov, V. Peller
{"title":"Functions of perturbed pairs of noncommutative dissipative operators","authors":"A. Aleksandrov, V. Peller","doi":"10.1090/spmj/1758","DOIUrl":null,"url":null,"abstract":"<p>Let a function <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"f\">\n <mml:semantics>\n <mml:mi>f</mml:mi>\n <mml:annotation encoding=\"application/x-tex\">f</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> belong to the inhomogeneous analytic Besov space <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"left-parenthesis upper B Subscript normal infinity comma 1 Superscript 1 Baseline right-parenthesis Subscript plus Baseline left-parenthesis double-struck upper R squared right-parenthesis\">\n <mml:semantics>\n <mml:mrow>\n <mml:mo stretchy=\"false\">(</mml:mo>\n <mml:msubsup>\n <mml:mi>B</mml:mi>\n <mml:mrow class=\"MJX-TeXAtom-ORD\">\n <mml:mi mathvariant=\"normal\">∞<!-- ∞ --></mml:mi>\n <mml:mo>,</mml:mo>\n <mml:mn>1</mml:mn>\n </mml:mrow>\n <mml:mrow class=\"MJX-TeXAtom-ORD\">\n <mml:mspace width=\"thinmathspace\" />\n <mml:mn>1</mml:mn>\n </mml:mrow>\n </mml:msubsup>\n <mml:msub>\n <mml:mo stretchy=\"false\">)</mml:mo>\n <mml:mo>+</mml:mo>\n </mml:msub>\n <mml:mo stretchy=\"false\">(</mml:mo>\n <mml:msup>\n <mml:mrow class=\"MJX-TeXAtom-ORD\">\n <mml:mi mathvariant=\"double-struck\">R</mml:mi>\n </mml:mrow>\n <mml:mn>2</mml:mn>\n </mml:msup>\n <mml:mo stretchy=\"false\">)</mml:mo>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">(B_{\\infty ,1}^{\\,1})_+(\\mathbb {R}^2)</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula>. For a pair <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"left-parenthesis upper L comma upper M right-parenthesis\">\n <mml:semantics>\n <mml:mrow>\n <mml:mo stretchy=\"false\">(</mml:mo>\n <mml:mi>L</mml:mi>\n <mml:mo>,</mml:mo>\n <mml:mi>M</mml:mi>\n <mml:mo stretchy=\"false\">)</mml:mo>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">(L,M)</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> of not necessarily commuting maximal dissipative operators, the function <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"f left-parenthesis upper L comma upper M right-parenthesis\">\n <mml:semantics>\n <mml:mrow>\n <mml:mi>f</mml:mi>\n <mml:mo stretchy=\"false\">(</mml:mo>\n <mml:mi>L</mml:mi>\n <mml:mo>,</mml:mo>\n <mml:mi>M</mml:mi>\n <mml:mo stretchy=\"false\">)</mml:mo>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">f(L,M)</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> of <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"upper L\">\n <mml:semantics>\n <mml:mi>L</mml:mi>\n <mml:annotation encoding=\"application/x-tex\">L</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> and <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"upper M\">\n <mml:semantics>\n <mml:mi>M</mml:mi>\n <mml:annotation encoding=\"application/x-tex\">M</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> is defined as a densely defined linear operator. For <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"p element-of left-bracket 1 comma 2 right-bracket\">\n <mml:semantics>\n <mml:mrow>\n <mml:mi>p</mml:mi>\n <mml:mo>∈<!-- ∈ --></mml:mo>\n <mml:mo stretchy=\"false\">[</mml:mo>\n <mml:mn>1</mml:mn>\n <mml:mo>,</mml:mo>\n <mml:mn>2</mml:mn>\n <mml:mo stretchy=\"false\">]</mml:mo>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">p\\in [1,2]</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula>, it is proved that if <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"left-parenthesis upper L 1 comma upper M 1 right-parenthesis\">\n <mml:semantics>\n <mml:mrow>\n <mml:mo stretchy=\"false\">(</mml:mo>\n <mml:msub>\n <mml:mi>L</mml:mi>\n <mml:mn>1</mml:mn>\n </mml:msub>\n <mml:mo>,</mml:mo>\n <mml:msub>\n <mml:mi>M</mml:mi>\n <mml:mn>1</mml:mn>\n </mml:msub>\n <mml:mo stretchy=\"false\">)</mml:mo>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">(L_1,M_1)</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> and <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"left-parenthesis upper L 2 comma upper M 2 right-parenthesis\">\n <mml:semantics>\n <mml:mrow>\n <mml:mo stretchy=\"false\">(</mml:mo>\n <mml:msub>\n <mml:mi>L</mml:mi>\n <mml:mn>2</mml:mn>\n </mml:msub>\n <mml:mo>,</mml:mo>\n <mml:msub>\n <mml:mi>M</mml:mi>\n <mml:mn>2</mml:mn>\n </mml:msub>\n <mml:mo stretchy=\"false\">)</mml:mo>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">(L_2,M_2)</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> are pairs of not necessarily commuting maximal dissipative operators such that both differences <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"upper L 1 minus upper L 2\">\n <mml:semantics>\n <mml:mrow>\n <mml:msub>\n <mml:mi>L</mml:mi>\n <mml:mn>1</mml:mn>\n </mml:msub>\n <mml:mo>−<!-- − --></mml:mo>\n <mml:msub>\n <mml:mi>L</mml:mi>\n <mml:mn>2</mml:mn>\n </mml:msub>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">L_1-L_2</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> and <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"upper M 1 minus upper M 2\">\n <mml:semantics>\n <mml:mrow>\n <mml:msub>\n <mml:mi>M</mml:mi>\n <mml:mn>1</mml:mn>\n </mml:msub>\n <mml:mo>−<!-- − --></mml:mo>\n <mml:msub>\n <mml:mi>M</mml:mi>\n <mml:mn>2</mml:mn>\n </mml:msub>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">M_1-M_2</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> belong to the Schatten–von Neumann class <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"bold-italic upper S Subscript p\">\n <mml:semantics>\n <mml:msub>\n <mml:mrow class=\"MJX-TeXAtom-ORD\">\n <mml:mi mathvariant=\"bold-italic\">S</mml:mi>\n </mml:mrow>\n <mml:mi>p</mml:mi>\n </mml:msub>\n <mml:annotation encoding=\"application/x-tex\">{\\boldsymbol S}_p</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula>, then for an arbitrary function <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"f\">\n <mml:semantics>\n <mml:mi>f</mml:mi>\n <mml:annotation encoding=\"application/x-tex\">f</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> in <inline-formula content-type=\"math/tex\">\n<tex-math>\n(\\mathcyr {B}_{\\infty ,1}^{\\,1})_+(\\mathbb {R}^2)</tex-math></inline-formula>, the operator difference <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"f left-parenthesis upper L 1 comma upper M 1 right-parenthesis minus f left-parenthesis upper L 2 comma upper M 2 right-parenthesis\">\n <mml:semantics>\n <mml:mrow>\n <mml:mi>f</mml:mi>\n <mml:mo stretchy=\"false\">(</mml:mo>\n <mml:msub>\n <mml:mi>L</mml:mi>\n <mml:mn>1</mml:mn>\n </mml:msub>\n <mml:mo>,</mml:mo>\n <mml:msub>\n <mml:mi>M</mml:mi>\n <mml:mn>1</mml:mn>\n </mml:msub>\n <mml:mo stretchy=\"false\">)</mml:mo>\n <mml:mo>−<!-- − --></mml:mo>\n <mml:mi>f</mml:mi>\n <mml:mo stretchy=\"false\">(</mml:mo>\n <mml:msub>\n <mml:mi>L</mml:mi>\n <mml:mn>2</mml:mn>\n </mml:msub>\n <mml:mo>,</mml:mo>\n <mml:msub>\n <mml:mi>M</mml:mi>\n <mml:mn>2</mml:mn>\n </mml:msub>\n <mml:mo stretchy=\"false\">)</mml:mo>\n </mml:mrow>\n <mml:annotation encoding=\"application/x-tex\">f(L_1,M_1)-f(L_2,M_2)</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> belongs to <inline-formula content-type=\"math/mathml\">\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" alttext=\"bold-italic upper S Subscript p\">\n <mml:semantics>\n <mml:msub>\n <mml:mrow class=\"MJX-TeXAtom-ORD\">\n <mml:mi mathvariant=\"bold-italic\">S</mml:mi>\n </mml:mrow>\n <mml:mi>p</mml:mi>\n </mml:msub>\n <mml:annotation encoding=\"application/x-tex\">{\\boldsymbol S}_p</mml:annotation>\n </mml:semantics>\n</mml:math>\n</inline-formula> and the following Lipschitz type estimate holds: <disp-formula content-type=\"math/tex\">\n<tex-math>\n\\begin{equation*} \\|f(L_1,M_1)-f(L_2,M_2)\\|_{{\\boldsymbol S}_p} \\le const\\|f\\|_{\\mathcyr {B}_{\\infty ,1}^{\\,1}}\\max \\big \\{\\|L_1-L_2\\|_{{\\boldsymbol S}_p},\\|M_1-M_2\\|_{{\\boldsymbol S}_p}\\big \\}. \\end{equation*}</tex-math>\n</disp-formula></p>","PeriodicalId":51162,"journal":{"name":"St Petersburg Mathematical Journal","volume":" ","pages":""},"PeriodicalIF":0.7000,"publicationDate":"2023-06-07","publicationTypes":"Journal 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引用次数: 0

Abstract

Let a function f f belong to the inhomogeneous analytic Besov space ( B , 1 1 ) + ( R 2 ) (B_{\infty ,1}^{\,1})_+(\mathbb {R}^2) . For a pair ( L , M ) (L,M) of not necessarily commuting maximal dissipative operators, the function f ( L , M ) f(L,M) of L L and M M is defined as a densely defined linear operator. For p [ 1 , 2 ] p\in [1,2] , it is proved that if ( L 1 , M 1 ) (L_1,M_1) and ( L 2 , M 2 ) (L_2,M_2) are pairs of not necessarily commuting maximal dissipative operators such that both differences L 1 L 2 L_1-L_2 and M 1 M 2 M_1-M_2 belong to the Schatten–von Neumann class S p {\boldsymbol S}_p , then for an arbitrary function f f in (\mathcyr {B}_{\infty ,1}^{\,1})_+(\mathbb {R}^2), the operator difference f ( L 1 , M 1 ) f ( L 2 , M 2 ) f(L_1,M_1)-f(L_2,M_2) belongs to S p {\boldsymbol S}_p and the following Lipschitz type estimate holds: \begin{equation*} \|f(L_1,M_1)-f(L_2,M_2)\|_{{\boldsymbol S}_p} \le const\|f\|_{\mathcyr {B}_{\infty ,1}^{\,1}}\max \big \{\|L_1-L_2\|_{{\boldsymbol S}_p},\|M_1-M_2\|_{{\boldsymbol S}_p}\big \}. \end{equation*}

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扰动非交换耗散算子对的函数
设函数f属于非齐次解析Besov空间(B∞,11)+(R2)(B_。对于不必交换的极大耗散算子对(L,M)(L,M),L和M的函数f(L,M.)f(L、M)被定义为稠密定义的线性算子。对于[1,2]中的p∈[1,2]p\,证明了如果(L1,M1)(L_1,M_1)和(L2,M2)(L_2,M_22 L_1-L_2和M1−M2 M_1-M_2属于Schatten–von Neumann类S p{\boldsymbol S}_p,则对于(\mathcyr{B}_{infty,1}^{\,1})_+(\mathbb{R}^2),算子差f(L1,M1)−f(L2,M2)f(L_1,M_1)-f(L_2,M_2)属于S p{\boldsymbol S}_p,并且下面的Lipschitz型估计成立:开始{方程*}-f(L_2,M_2){B}_{infty,1}^{\,1}}}\max\big\{\|L_1-L_2\|_{\boldsymbol S}_p},\|M_1-M_2\|_。\结束{方程式*}
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CiteScore
1.00
自引率
12.50%
发文量
52
审稿时长
>12 weeks
期刊介绍: This journal is a cover-to-cover translation into English of Algebra i Analiz, published six times a year by the mathematics section of the Russian Academy of Sciences.
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Shape, velocity, and exact controllability for the wave equation on a graph with cycle On Kitaev’s determinant formula Resolvent stochastic processes Complete nonselfadjointness for Schrödinger operators on the semi-axis Behavior of large eigenvalues for the two-photon asymmetric quantum Rabi model
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