
The following singularly perturbed integral equation \[ \varepsilon u_\varepsilon(x) + \int_a^b K(x,y)u_\varepsilon(y)\,dy =f(x), \quad x\in[a,b]\tag{1} \] is considered, which becomes a Fredholm equation of first kind for \(\varepsilon=0\). The kernels \(K_\pm(x,y):=K(x,y)\) for \(\pm(x-y)>0\) are both smooth on \([a,b]\times[a,b]\) and might have jump on the diagonal \(K_+(x,x)-K_-(x,x)=a(x)\), or their derivatives have the jump \([\partial^n_yK_+(x,y)-\partial^n_yK_-(x,y)]| _{y=x} =a(x)\) and \(a\in C^\infty([a,b])\), \(a(x)\not=0\) for \(x\in[a,b]\) (an ellipticity condition). The author proves the unique solvability of equation (1) under condition that the ``unperturbed'' equation with \(\varepsilon=0\) is uniquely solvable. Moreover, the principal term of the asymptotic expansion with respect to \(\varepsilon\) is given by adapting the technique developed by \textit{G. I. Eskin} [Dokl. Akad. Nauk SSSR 211, 547--550 (1973; Zbl 0292.35068)] for similar problems for pseudodifferential equations. The results are applied to several examples including a Volterra equation.
asymptotic expansion, Fredholm equation, Applied Mathematics, Volterra equation, Asymptotic expansion, Fredholm integral equations, Singular perturbation, singular perturbation, Analysis
asymptotic expansion, Fredholm equation, Applied Mathematics, Volterra equation, Asymptotic expansion, Fredholm integral equations, Singular perturbation, singular perturbation, Analysis
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