Let ( X , a , m ) (X,\,\mathcal {a},\,m) be a standard finite measure space. A bounded operator T on L 2 ( X ) {L^2}(X) is called a pseudo-integral operator if ( T f ) ( x ) = ∫ f ( y ) μ ( x , d y ) (Tf)(x)\, = \,\int {f(y)\,\mu (x,\,dy)} , where, for every x, μ ( x , ⋅ ) \mu (x,\, \cdot \,) is a bounded Borel measure on X. Main results: 1. A bounded operator T on L 2 {L^2} is a pseudo-integral operator with a positive kernel if and only if T maps positive functions to positive functions. 2. On nonatomic measure spaces every operator unitarily equivalent to T is a pseudo-integral operator if and only if T is the sum of a scalar and a Hilbert-Schmidt operator. 3. The class of pseudo-integral operators with absolutely bounded kernels form a selfadjoint (nonclosed) algebra, and the class of integral operators with absolutely bounded kernels is a two-sided ideal. 4. An operator T satisfies ( T f ) ( x ) = ∫ f ( y ) μ ( x , d y ) (Tf)(x)\, = \,\int {f(y)\,\mu (x,\,dy)} for f ∈ L ∞ f\, \in \,{L^\infty } if and only if there exists a positive measurable (almost-everywhere finite) function Ω \Omega such that | ( T f ) ( x ) | ⩽ ‖ f ‖ ∞ Ω ( x ) \left | {(Tf)(x)} \right |\, \leqslant \,{\left \| f \right \|_\infty }\Omega (x) .
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