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§5. Points of Order p and Supersingular Curves  265

        §5. Points of Order p and Supersingular Curves


        Recall that the degree of an endomorphism λ : E → E is deg(λ) = [k(E) : k(E )]


        coming from the induced embedding k(E ) → k(E) factors into separable and
        purely inseparable parts
                               deg(λ) = deg(λ) s deg(λ) i ,


        where deg(λ) s = [k(E) : k(E )] s and deg(λ) i = [k(E) : k(E )] i . The purely

                                                       h
        inseperable degree is always a power of p, deg(λ) i = p , where h is called the
        height of λ. The kernel ker(λ)of λ is a finite subgroup of E(k s ).
        (5.1) Remark. The number of elements in the kernel is the separable degree. Let
        k = k s . Given a finite subgroup G in E(k s ) there exists a unique separable isogeny
                                         G
        λ G : E → E/G where k(E/G) = k(E) , the subfield invariant by the action of G
        on D(E) induced by translations of G on E. The isogeny and the quotient elliptic
        curve are defined over an intermediate field k 1 between k and its separable algebraic
                                                                         G
        closure k s . Then ker(λ G ) = G and deg(λ G ) = deg(λ g ) s = #G = [k(E) : k(E) ]
        by Galois theory. This is an indication of how to construct all separable isogenies.
        We do not supply the details of the construction of E/G except to give k(E/G) and
        the interested reader can consult Mumford, Abelian Varieties, Section 7 for further
        details.
                                                               h
        (5.2) Definition. The iterated absolute Frobenius Fr h  : E → E (p )  is defined by
                                                   E
                                    h
                          h
          h
                         p
        Fr (x, y) = (x  p h , y ) where E (p )  has Weierstrass equation with coefficients the
          E
          h
        p th power of the coefficients of E, i.e.,
                                                            h
                                                            p
                       2
                                         3
                                                 2
                      y + a p h  xy + a  p  h  y = x + a p h  x + a  p h x + a .
                           1      3           2      4     6
                                                              h
                        h                                   (p )       p h
           For k perfect Fr is purely inseparable of height h since k(E  ) = k(E)  in
                        E
                                                                          h
        k(E). Observe that E is defined over the finite field F h if and only if E and E (p )
                                                    p
                                   h
        are isomorphic and in this case Fr = π E .
                                   E
        (5.3) Lemma. Let K = k(x, y) be a separable algebraic extension of a purely tran-
                                                         p
        scendental extension k(x) of the perfect field k. Then [K : K ] = p.
                                       p
        Proof. Since K = k(x, y) = k(x, y ), the element x generates K over K  p  =
                p
            p
         p
                          p
                       p
        k (x , y ) = k(x , y ). Hence the degree is either p or 1. In the latter case x is in
          p
                    p
        K and x = t where t is both separable and purely inseparable over k(x), which is
                             p
        impossible. Hence [K : K ] = p.
        (5.4) Proposition. Let k be a perfect ground field, and let λ : E → E be a purely

                                                                          h

        inseparable isogeny of height h. Then there exists an isomorphism u : E → E (p )
                   h
        with uλ = Fr .
                   E
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