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首页> 外文期刊>Integral Equations and Operator Theory >C*-Algebras of Integral Operators with Piecewise Slowly Oscillating Coefficients and Shifts Acting Freely
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C*-Algebras of Integral Operators with Piecewise Slowly Oscillating Coefficients and Shifts Acting Freely

机译:具有分段缓慢振荡系数和移位的积分算子的C *-代数

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摘要

We establish a symbol calculus for the C*-subalgebra $mathcal{A}$ of $mathcal{B}left( {L^2 left( mathbb{T} right)} right)$ generated by the operators of multiplication by slowly oscillating and piecewise continuous functions and the operators $e_{h,lambda } S_mathbb{T} e_{h,lambda }^{ - 1} Ileft( {h in mathbb{R},lambda in mathbb{T}} right)$ where $S_{mathbb{T}} $ is the Cauchy singular integral operator and $e_{{h,lambda }} (t): = exp {left( {h(t + lambda )/(t - lambda )} right)},t in mathbb{T}backslash {left{ lambda right}}.$ The C*-algebra $mathcal{A}$ is invariant under the transformations $$A mapsto U_{z} A{user1{U}}^{{{user1{ - 1}}}}_{{user1{z}}} quad {text{and}}quad A mapsto e_{{h,lambda }} Ae^{{ - 1}}_{{h,lambda }} I{left( {z,lambda in mathbb{T},;h in mathbb{R}} right)},$$ where U z is the rotation operator ${left( {U_{z} varphi } right)}(t): = varphi (zt),;t in mathbb{T}.$ Using the localtrajectory method, which is a natural generalization of the Allan-Douglas local principle to nonlocal type operators, we construct symbol calculi and establish Fredholm criteria for the C*-algebra $mathfrak{B}$ generated by the operators $A in mathcal{A}$ and $U_{z} (z in mathbb{T}),$ for the C*-algebra $mathfrak{C}$ generated by the operators $A in mathcal{A}$ and $e_{{h,lambda }} I{left( {h in mathbb{R},;lambda in mathbb{T}} right)},$ and for the C*-algebra $mathfrak{D}$ generated by the algebras $mathfrak{B}$ and $mathfrak{C}.$ The C*-algebra $mathfrak{B}$ can be considered as an algebra of convolution type operators with piecewise slowly oscillating coefficients and shifts acting freely.
机译:我们为C *次代数$ mathcal {A} $ of $ mathcal {B} left({L ^ 2 left(mathbb {T} right)} right)$建立符号演算,该乘法由乘法运算符通过缓慢振荡生成和分段连续函数,以及运算符$ e_ {h,lambda} S_mathbb {T} e_ {h,lambda} ^ {-1} Ileft({Mathbb {R}中的h,mathbb {T}}中的lambda right)$其中$ S_ {mathbb {T}} $是柯西奇异积分运算符,$ e _ {{h,lambda}}(t):= exp {left({h(t + lambda)/(t-lambda)} right) },t in mathbb {T}反斜杠{left {lambda right}}。$ C *代数$ mathcal {A} $在$$ A映射到U_ {z} A {user1 {U}} ^的变换下不变。 {{{user1 {-1}}}} _ {{user1 {z}}} quad {text {and}} quad一个映射到e _ {{h,lambda}} Ae ^ {{-1}} _ {{h ,lambda}} I {left({z,mathbb {T}中的lambda,; h mathbb {R}}中right)}},$$其中U z 是旋转运算符$ {left({U_ { z} varphi} right)}(t):= varphi(zt),; t in mathbb {T}。$使用localtrajectory方法,这是Allan-Douglas局部原则的自然概括从非本地类型运算符开始,我们构造符号计算并为运算符$ A在mathcal {A} $和$ U_ {z}中生成的C *-代数$ mathfrak {B} $(在mathbb {T中为z }),$由运算符$ A在mathcal {A} $和$ e _ {{h,lambda}} I {left({h在mathbb {R}中,)中生成的C *代数$ mathfrak {C} $ ; lambda in mathbb {T}} right)},$和由代数$ mathfrak {B} $和$ mathfrak {C}生成的C *-代数$ mathfrak {D} $。$ C *-代数$ mathfrak {B} $可以看作是卷积类型算子的代数,它具有分段缓慢振荡的系数,并且移位可以自由地起作用。

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