Page 272 -
P. 272

§7. Expansions Near the Origin and the Formal Group  249

        where zero on E has coordonates (t, s) = (0, 0),and t is a local parameter at 0 on
        E. This (t, s)-plane version of the cubic equation generates a formal series relations
        for s as a function of t by iterated substitution of the six-term expression for s into
        each term of s on the right-hand side of the above equation. The formal expansion
        has the following form:

                         3
                                                3
                                    2
                                           5
                               4
                     s = t + a 1 t + (a + a 2 )t + (a + 2a 1 a 2 + a 3 )t 6
                                    1           1
                            4    2             2     7
                        + (a + 3a a 2 + 3a 1 a 3 + a + a 4 )t + ···
                            1
                                 1
                                               2
                         3             2
                      = t (1 + A 1 t + A 2 t +· · · ),
        where A n is a polynomial of weight n in the a i with positive integer coefficients.
        (7.1) Proposition. In terms of the local uniformizing parameter t =−x/yat 0 on
        E the following formal expansions hold in Z[a 1 , a 2 , a 3 , a 4 , a 6 ][[t]]:
                                                    2
                 x = t −2  − a 1 t −1  − a 2 − a 3 t − (a 4 + a 1 a 3 )t − ··· ,
                      x      −3     −2     −1
                 y =−   =−t    + a 1 t  + a 2 t  + a 3 +· · · ,
                      t

                                      2
                                           3
                                                         3
                                2
                 ω = 1 + a 1 t + (a + a 2 )t + (a + 2a 1 a 2 + a 3 )t +· · · dt.
                                1          1
                        i
        The coefficients of t are isobaric of weight i + 2,i + 3, and i, respectively, for x, y,
        ω. Further, if the coefficients a j are in a ring R, then the expansions lie in R[[t]].
                                                                  3
        Proof. The formal expansions for x and y come from the expansion s = t (1+A 1 t+
        ··· ), y =−1/s,and x−ty, and it is clear that x and y are in Z[a 1 , a 2 , a 3 , a 4 , a 6 ][[t]].
        The formal expansion for ω is derived from this in two ways:
                                   dx        −2t −3  + ···
                          ω =              =    −3     dt,
                              2y + a 1 x + a 3  −2t  + ···
        which has coefficients in Z[1/2, a 1 , a 2 , a 3 , a 4 , a 6 ][[t]], and
                                    dy           3t −4  + ···
                       ω =                     =          dt,
                             2
                           3x + 2a 2 x + a 4 − a 1 y  3t −4  + ···
        which has coefficients in Z[1/3, a 1 , a 2 , a 3 , a 4 , a 6 ][[t]]. This proves the assertion
        about the coefficients of the above expression.
           The expansion x(t) and y(t) in the previous proposition are an algebraic analogue

        of the complex analytic expansions of ℘(u) and ℘ (u). In Chapter 13 we will see that
        these formal expressions have p-adic convergence properties.
           We can go further to analyze the group law near 0 formally also. The line joining
        two points (t 1 , s 1 ) and (t 2 , s 2 ) in the (t, s)-plane has slope given by

                                 3
                                            4
                                t − t 3    t − t 4
                       s 2 − s 1  2  1      2   1
                   λ =        =        + A 1     +· · ·
                        t 2 − t 1  t 2 − t 1  t 2 − t 1
   267   268   269   270   271   272   273   274   275   276   277