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11.11-3. The Hopf–Fock Formula

               Let us give a useful formula that allows one to express the solution of Eq. (1) with an arbitrary
               right-hand side f(x) via the solution to a simpler auxiliary integral equation with an exponential
               right-hand side.
                   Assume that in Eq. (1) we have

                                       f(x)= e iζx ,  Im ζ >0,  y(x)= y ζ (x),             (32)

               and moreover, conditions (15) and (16) hold. In this case

                                                       ∞

                                         y ζ (x)= e iζx  +  R(x, t)e iζt  dt,              (33)
                                                      0
               where R(x, t) has the form (25). After some manipulations, we can see that


                                                         x
                                            ˇ
                                     y ζ (x)= M – (–ζ) 1+  R(t,0)e –iζt  dt e iζx .        (34)
                                                       0
               On setting x = 0 in (34), we have
                                                        ˇ
                                                y ζ (0) = M – (–ζ),                        (35)
               and if the function K(x) describing the kernel of the integral equation is even, then

                                                        ˇ
                                                 y ζ (0) = M + (ζ).                        (36)
                   On the basis of formula (34), we can obtain the solution of Eq. (1) for a general f(x) as well
               (see also Section 9.6):
                                    1     ∞                          ∞     iux
                                                            ˇ
                                           ˇ
                             y(x)=        F + (–ζ)y ζ (x) dζ,  F + (u)=  f(x)e  dx.        (37)
                                   2π                               0
                                       –∞
                   Remark 1. All results obtained in Section 11.11 concerning Wiener–Hopf equations of the sec-
               ond kind remain valid for continuous, square integrable, and some other classes of functions, which
               are discussed in detail in the paper by M. G. Krein (1958) and in the book by C. Corduneanu (1973).
                   Remark 2. The solution of the Wiener–Hopf equation can be also obtained in other classes of
                                                     ˇ
               functions for the exceptional case in which 1 – K(u) = 0 (see Subsections 11.9-1 and 11.10-5).
                •
                 References for Section 11.11: V. A. Fock (1942), M. G. Krein (1958), C. Corduneanu (1973), V. I. Smirnov (1974),
               P. P. Zabreyko, A. I. Koshelev, et al. (1975).

               11.12. Methods for Solving Equations With Difference
                         Kernels on a Finite Interval


                 11.12-1. Krein’s Method
               Consider a method for constructing exact analytic solutions of linear integral equations with an
               arbitrary right-hand side. The method is based on the construction of two auxiliary solutions of
               simpler equations with the right-hand side equal to 1. The auxiliary solutions are used to construct
               a solution of the original equation for an arbitrary right-hand side.




                 © 1998 by CRC Press LLC








               © 1998 by CRC Press LLC
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