Displaying similar documents to “Sets of determination for solutions of the Helmholtz equation”

Endpoint bounds for convolution operators with singular measures

E. Ferreyra, T. Godoy, M. Urciuolo (1998)

Colloquium Mathematicae

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Let S n + 1 be the graph of the function ϕ : [ - 1 , 1 ] n defined by ϕ ( x 1 , , x n ) = j = 1 n | x j | β j , with 1< β 1 β n , and let μ the measure on n + 1 induced by the Euclidean area measure on S. In this paper we characterize the set of pairs (p,q) such that the convolution operator with μ is L p - L q bounded.

Vector integral equations with discontinuous right-hand side

Filippo Cammaroto, Paolo Cubiotti (1999)

Commentationes Mathematicae Universitatis Carolinae

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We deal with the integral equation u ( t ) = f ( I g ( t , z ) u ( z ) d z ) , with t I = [ 0 , 1 ] , f : 𝐑 n 𝐑 n and g : I × I [ 0 , + [ . We prove an existence theorem for solutions u L ( I , 𝐑 n ) where the function f is not assumed to be continuous, extending a result previously obtained for the case n = 1 .

Characterization of sets of determination for parabolic functions on a slab by coparabolic (minimal) thinness

Jarmila Ranošová (1996)

Commentationes Mathematicae Universitatis Carolinae

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Let T be a positive number or + . We characterize all subsets M of n × ] 0 , T [ such that inf X n × ] 0 , T [ u ( X ) = inf X M u ( X ) i for every positive parabolic function u on n × ] 0 , T [ in terms of coparabolic (minimal) thinness of the set M δ = ( x , t ) M B p ( ( x , t ) , δ t ) , where δ ( 0 , 1 ) and B p ( ( x , t ) , r ) is the “heat ball” with the “center” ( x , t ) and radius r . Examples of different types of sets which can be used instead of “heat balls” are given. It is proved that (i) is equivalent to the condition sup X n × + u ( X ) = sup X M u ( X ) for every bounded parabolic function on n × + and hence to all equivalent conditions given in the article...