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III. The Erd˝ os–Fuchs Theorem
                        32


                                                                             1
                        Very deep arguments have even improved this to o
                                                                            n 2/3 , for ex-

                        ample, and the conjecture is that it is actually O  3 1  for every
                                                                         n 4  −1
                        1> 0. On the other hand, further difficult arguments show that it is

                        not O     3 1  .
                                 n 4  +1
                           Now all of these arguments were made for the very special case
                        of A   the perfect squares. What a surprise then, when Erd˝ os and
                        Fuchs showed, by simple analytic number theory, the following:

                        Theorem. For any set A,   r(0)+r(1)+r(2)+···+r(n)    C + O  1  is
                                                         n+1                      3  +1
                                                                                 n 4
                        impossible unless C   0.


                           This will be proved in the current chapter, but first an appetizer.
                        We prove that r − (n) can’t eventually be constant.
                           So let us assume that

                                                                    C
                                          2          2
                                        A (z) − A(z )   Pàz) +          ,             à 1)
                                                                  1 − z
                        P is a polynomial, and C is a positive constant. Now look for a con-
                        tradiction. The simple device of letting z → (−1) which worked
                                                                         +
                        so nicely for the r + problem, leads nowhere here. The exercises in
                        Chapter I were, after all, hand picked for their simplicity and involved
                        only the lightest touch of analysis. Here we encounter a slightly heav-
                        ier dose. We proceed, namely, by integrating the modulus around a
                        circle. From (1), we obtain, for 0 ≤ r< 1,

                                       π

                                               iθ
                                           2
                                        |A (re )|dθ
                                     −π
                                            π                   π

                                                  2 2iθ
                                       ≤      |A(r e   )|dθ +     |Pàre  iθ )|dθ      (2)
                                           −π                  −π
                                                π     dθ

                                         + C                 .
                                                          iθ
                                               −π  |1 − re |
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