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Now system (1) can be rewritten as the single Fredholm equation

                                     nb–(n–1)a
                           Y (x) – λ       K(x, t)Y (t) dt = F(x),  a ≤ x ≤ nb – (n – 1)a.
                                   a

                   If the kernels K ij (x, t) are square integrable on the square S = {a ≤ x ≤ b, a ≤ t ≤ b} and the
               right-hand sides f i (x) are square integrable on [a, b], then the kernel K(x, t) is square integrable on
               the new square
                                  S n = {a < x < nb – (n – 1)a, a < t < nb – (n – 1)a},

               and the right-hand side F(x) is square integrable on [a, nb – (n – 1)a].
                   If condition (4) is satisfied, then the kernel K(x, t) satisfies the inequality

                                      b
                                        2
                                       K (x, t) dt ≤ A ∗ ,  a < x < nb – (n – 1)a,
                                     a
               where A ∗ is a constant.
                •
                 Reference for Section 11.19: S. G. Mikhlin (1960).


               11.20. Regularization Method for Equations With Infinite
                         Limits of Integration

                 11.20-1. Basic Equation and Fredholm Theorems
               Consider an integral equation of the second kind in the form

                        1     ∞                1      0                 ∞
                y(x)+ √        K 1 (x – t)y(t) dt + √  K 2 (x – t)y(t) dt +  M(x, t)y(t) dt = f(x), (1)
                        2π  0                   2π  –∞                –∞

               where –∞ < x < ∞. We assume that the functions y(x) and f(x) and the kernels K 1 (x) and K 2 (x)
               are such that their Fourier transforms belong to L 2 (–∞, ∞) and satisfy the H¨ older condition. We
               also assume that the Fourier transforms of the kernel M(x, t) with respect to each variable belong
               to L 2 (–∞, ∞) and satisfy the H¨ older condition and, in addition,


                                            ∞   ∞
                                                         2
                                                  |M(x, t)| dx dt < ∞.
                                           –∞  –∞
               It should be noted that Eq. (1) with M(x, t) ≡ 0 is the convolution-type integral equation with two
               kernels which was discussed in Subsection 11.9-2.
                   The transposed homogeneous equation has the form

                         1     ∞                 1     0                  ∞
                 ϕ(x)+ √        K 1 (t – x)ϕ(t) dt + √  K 2 (t – x)ϕ(t) dt +  M(t, x)ϕ(t) dt = 0, (2)
                         2π  0                   2π  –∞                 –∞

               where –∞ < x < ∞.
                   Assume that the normality conditions (see Subsection 11.9-2) hold, that is,

                                   1+ K 1 (u) ≠ 0,  1 + K 2 (u) ≠ 0,  –∞ < u < ∞.           (3)

                   THEOREM 1. The number of linearly independent solutions of the homogeneous (f(x) ≡ 0)
               equation (1) and that of the transposed homogeneous (g(x) ≡ 0) equation (2) are finite.




                 © 1998 by CRC Press LLC








               © 1998 by CRC Press LLC
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