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On periodic in the plane solutions of second order linear hyperbolic systems

Tariel Kiguradze — 1997

Archivum Mathematicum

Sufficient conditions for the problem 2 u x y = P 0 ( x , y ) u + P 1 ( x , y ) u x + P 2 ( x , y ) u y + q ( x , y ) , u ( x + ω 1 , y ) = u ( x , y ) , u ( x , y + ω 2 ) = u ( x , y ) to have the Fredholm property and to be uniquely solvable are established, where ω 1 and ω 2 are positive constants and P j : R 2 R n × n ( j = 0 , 1 , 2 ) and q : R 2 R n are continuous matrix and vector functions periodic in x and y .

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