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JOURNALS // Zhurnal Matematicheskoi Fiziki, Analiza, Geometrii [Journal of Mathematical Physics, Analysis, Geometry] // Archive

Zh. Mat. Fiz. Anal. Geom., 2012 Volume 8, Number 3, Pages 248–259 (Mi jmag537)

On the universal models of commutative systems of linear operators

R. Hatamleha, V. A. Zolotarevbc

a Department of Mathematics, Jadara University, Irbid-Jordan
b Mathematics Division, B. Verkin Institute for Low Temperature Physics and Engineering, National Academy of Sciences of Ukraine, 47 Lenin Ave., Kharkiv 61103, Ukraine
c V. N. Karazin Kharkiv National University, Faculty of Mathematics and Mechanics, 4 Svobody Sq., Kharkiv 61077, Ukraine

Abstract: The universal models are constructed for a system of linear bounded non-selfadjoint operators $\{A_1,A_2\}$ acting in a Hilbert space $H$ such that 1) $[A_1,A_2]=0$, $[A_1^*,A_2]=0$; 2) $\displaystyle{\frac{A_k-A_k^*}i\geq0}$ ($k=1, 2$); 3) the function $A(\lambda)=A_1(\lambda_1)A_2(\lambda_2)$ ($A_k(\lambda_k)=A_k(I-\lambda_kA_k)^{-1}$, $k=1, 2$) is an entire function of the exponential type. It is proved that this class of linear operator systems is realized by the restriction on invariant subspaces of systems of operator of integration by independent variables in $L^2(\Omega)\otimes l^2$ where $\Omega$ is a rectangle in $\mathbb{R}^2$.

Key words and phrases: non-selfadjoint operators, universal models.

MSC: 47A45

Received: 07.10.2011



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