Skip to main content

4.1 Elliptic curves

def: Elliptic curve

PnEEE=S(E)gen(E)=1OE(E,O)E(E,O)elliptic curve\begin{align*} &\sphericalangle \\ &\mathbb P^n \\ &E \in \mathfrak E \\ &E = \cancel S(E) \\ &\text{gen}(E) = 1 \\ &O \in E \\ \hline \\ &(E,O) \in \mathcal E \\ &(E,O) - \text{elliptic curve} \end{align*}
note

We designate a special point OO to be able to define a group over elliptic curve later in this section.

Weierstrass form

Further we're going to use affine polynomials to describe projective curves. That means that we're actually describing a curve on a projective open set Uz={[x,y,1],x,yF}U_z=\{[x,y,1], x,y \in \overline F \} and then there are some points of infinity that we can analyze using homogeneization.

For example affine equation yx2=1y-x^2=1 describes a projective equation yzx2=z2yz-x^2=z^2.

def: Weierstrass curve

P2f(x,y)=y2+a1xy+a3yx3a2x2a4xa6aiFC:I(C)=fICW/FCis a curve in Weierstrass formeqW(C):=fWeierstrass curve equation\begin{align*} &\sphericalangle \\ &\mathbb P^2 \\ &f(x,y) = y^2+a_1xy+a_3y-x^3-a_2x^2-a_4x-a_6 \\ &a_i \in F \\ &C: I(C)=\lang f \rang_I \\ \hline \\ &C \in \mathcal W/F \\ &C - \text{is a curve in Weierstrass form} \\ &\text{eq}_W(C):=f - \text{Weierstrass curve equation} \end{align*}

Proposition 4.1.1: Elliptic curve is a Weierstrass curve

Pn(E,O)E/F    f,gF(E)F,CW/F:ϕ:EP2,P[f(P),g(P),1],O[0,1,0],EϕCEE/F,e1=eqW(E),e2=eqW(E)    uF,r,s,tF:e1(x,y)=e2(u2x+r,u3y+su2x+t)CW/F,C=S(C)    (C,[0,1,0])E\begin{align*} &\sphericalangle \\ &\mathbb P^n \\ \hline \\ &\begin{align*} &(E,O) \in \mathcal E/F \implies \exists f, g \in F(E)_F, C \in \mathcal W / F: \\ &\phi: E \to \mathbb P^2, P \mapsto [f(P),g(P),1], O \mapsto [0,1,0], \\ &E \cong_{\phi}C \hspace{0.5cm} \tag{a}\\ &E \in \mathcal E/F, e_1 = \text{eq}_W(E), e_2 = \text{eq}_W(E)\implies \\ &\exists u \in F^*, r,s,t \in F: \\ &e_1(x,y)=e_2(u^2x+r, u^3y+su^2x+t) \hspace{0.5cm} \tag{b}\\ &C \in \mathcal W/F, C = \cancel S(C) \implies (C, [0,1,0]) \in \mathcal E \hspace{0.5cm} \tag{c}\\ \end{align*} \end{align*}

Proof

a.

The plan for the proof will be

  1. Find a mapping to a curve in Weierstrass form
  2. Prove that it's a morphism
  3. Prove that it's surjective
  4. Prove that it has degree 1
  5. Hence it's isomopshism
  6. Prove that image is smooth

From (3.4.13)(3.4.13) we have dimL(n(O))=n\dim L(n(O))=n. Note that L(n(O))L(n(O)) contains functions that don't have a pole more than of order nn. So dimL(2(O))=2\dim L(2(O))=2 and it will have basis {1,f}\{1,f\} and dimL(3(O))=3\dim L(3(O))=3 and it will have a basis {1,f,g}\{1,f,g\} for some functions f,gF(E)Ff, g \in F(E)_F. Note that ff has a pole of order 2 and gg has a pole of order 3. Thus {1,f,f2,f3,g,g2,fg}L(6(O))\{1,f, f^2, f^3, g, g^2, fg \}\subseteq L(6(O)) But we know that dimL(6(O))=6\dim L(6(O))=6 so there's a linear relations between these fuctions:

A1+A2f+A3g+A4f2+A5fg+A6g2+A7f3=0,AiF,Ai0A_1 + A_2f+A_3g+A_4f^2+A_5fg+A_6g^2+A_7f^3=0, \\A_i \in F, \exists A_i \ne 0\\

Note that A6A70A_6A_7 \ne 0, otherwise each other term would have a pole of different order so all AiA_i must be 00 in this case. Now assume f=A6A7f,g=A6A72gf=-A_6A_7f, g=A_6A_7^2g then dividing by A63A74A^3_6A^4_7 we'll get:

g2+a1fg+a3g=f3+a2f2+a4f+a6g^2+a_1fg+a_3g=f^3+a_2f^2+a_4f+a_6

So if we consider a map:

ϕ:EP2,P[f(P),g(P),1]\phi: E \to \mathbb P^2, P \mapsto [f(P),g(P),1]

Then it's image will be a curve CC subject to Weierstrass equation. Since EE is smooth by (3.4.3)(3.4.3) it's a morphism. And since it's non-constant it's surjective by (3.4.4)(3.4.4). Finally note that ordOg=3,ordOf=2\text{ord}_Og = -3, \text{ord}_Of = -2 so if we assume g=g1/g2,f=f1/f2g=g_1/g_2, f=f_1/f_2 we can make ϕ(O)=[g2(O)f1(O)/f2(O),g1(O),g2(O)]=[0,1,0]\phi(O)=[g_2(O)\cdot f_1(O)/f_2(O),g_1(O), g_2(O)] = [0,1,0]

Next, we want to show that degϕ=1\deg \phi = 1. By definition this means that [F(E):ϕF(C)]=1[F(E):\phi^*F(C)]=1. Let's recall how we define pullback of a function hF(C)h \in F(C):

h(x,y,z)=h1(x,y,z)/h2(x,y,z)ϕh(P)=h1(f(P),g(P),1)/h2(f(P),g(P),1)h(x,y,z)=h_1(x,y,z)/h_2(x,y,z) \\ \phi^*h(P) = h_1(f(P),g(P),1)/h_2(f(P),g(P),1)

This means that ϕF(C)\phi^*F(C) will have some rational functions of ff and gg, in other words ϕF(C)=F(f,g)\phi^*F(C)=F(f,g). Additional note for clarity of notation: F(C)F(C) means a functional field of a curve CC so here FF stands for functional, while F(f,g)F(f,g) is a field extension of the base field FF, so FF here is a field.

Now let's consider a map: ϕf:EP1,P[f(P),1]\phi_f: E \to \mathbb P^1, P \mapsto [f(P),1]. In this case ϕx1([1,0])=O\phi_x^{-1}([1,0])=O (since ff has the only pole in OO) and eϕf(O)=ordOϕft[1,0]=ordOf=2e_{\phi_f}(O)=\text{ord}_O\phi_f^*t_{[1,0]}=-\text{ord}_Of=2. So by (3.4.5)(3.4.5) we have degϕf=2\deg \phi_f=2. Knowing that ϕfF(P1)=F(f)\phi_f^*F(\mathbb P^1)=F(f) implies [F(E):F(f)]=2[F(E):F(f)]=2.

Similarly [F(E):F(g)]=3[F(E):F(g)]=3. But since we have tower of extensions F(E)/F(f,g)/F(f)F(E)/F(f,g)/F(f) and F(E)/F(f,g)/F(g)F(E)/F(f,g)/F(g) we know that:

2=[F(E):F(f)]=[F(E):F(f,g)][F(f,g):F(f)]3=[F(E):F(g)]=[F(E):F(f,g)][F(f,g):F(g)]2=[F(E):F(f)]=[F(E):F(f,g)][F(f,g):F(f)] \\ 3=[F(E):F(g)]=[F(E):F(f,g)][F(f,g):F(g)] \\

This implies that [F(E):F(f,g)]=1[F(E):F(f,g)]=1 and thus degϕ=1\deg \phi = 1. So by (3.4.4)(3.4.4) we have EϕCE \cong_\phi C.

Now let's prove CC is smooth. Assume otherwise - there exist some singular point. By linear change of variables we can assume it's (0,0)(0,0). Then using partial derivatives criterion we can check that the equation in this case is:

y2+a1xy=x3+a2xy^2+a_1xy=x^3+a_2x

Then we can make a rational map ψ:CP1,(x,y)[x,y]\psi: C \to \mathbb P^1, (x,y) \mapsto [x,y]. Then degψ=1\deg \psi = 1 since it has an inverse [1,t](t2+a1ta2,t3+a1t2a2t)[1,t] \mapsto (t^2+a_1t-a_2, t^3+a_1t^2-a_2t)

So we built a rational map of degree 1 ϕψ:EP1\phi \circ \psi: E \to \mathbb P^1. So by (3.4.4)(3.4.4) it's an isomopshism. But it cannot be the case since gen(E)=1\text{gen}(E)=1 and by (3.4.13)(3.4.13) gen(P1)=0\text{gen}(\mathbb P^1)=0. So we arrived at contradiction and thus CC is smooth

b.

As in (a)(a) we consider two maps ϕ=[f,g,1],ϕ=[f,g,1]\phi=[f,g,1], \phi'=[f',g',1] where both f,gf,g and f,gf',g' are the bases for L(2(O))L(2(O)) and L(3(O))L(3(O)) respectively. Since they're the bases of the same spaces we can write:

f=u1f+r,g=u2g+s2f+tf = u_1f'+r, g=u_2g'+s_2f'+t

Since in Weierstrass form f3f^3 and g2g^2 has coefficents 11 it follows u13=u22u_1^3=u_2^2. Letting u=u2/u1u=u_2/u_1 and s=s2/u2s=s_2/u^2 we have:

f=u2f+r,g=u3g+su2f+tf=u^2f'+r, g=u^3g'+su^2f'+t

Thus defining x=f(P),y=g(P),PEx = f(P), y=g(P), P \in E we finish the proof.

c.

Consider some point P0=(x0,y0)P_0=(x_0,y_0). Denote F(x,y):=eq(C)F(x,y):=\text{eq}(C). Since F(x,y)0F(x,y)\equiv 0 we know that 0=dF(x,y)=Fx(x,y)dx+Fy(x,y)dy0=dF(x,y)=F_x(x,y)dx+F_y(x,y)dy so we can define

ω:=d(xx0)Fy(x,y)=d(yy0)Fx(x,y)\omega:=\frac{d(x-x_0)}{F_y(x,y)}=-\frac{d(y-y_0)}{F_x(x,y)}

Note that ω\omega cannot have pole in PP, otherwise Fx(x0,y0)=Fy(x0,y0)=0F_x(x_0,y_0) = F_y(x_0,y_0)=0 and PP is singular. Consider a map:

ϕ:EP1,[x,y,1][x,1]\phi: E \to \mathbb P^1, [x,y,1] \to [x,1]

F(E)=F(x,y),ϕF(P1)=F(x)F(E)=F(x,y), \phi^*F(\mathbb P^1)=F(x). Since in Weierstrass form y2y^2 is a polynomial of xx we'll have degϕ=[F(x,y):F(x)]=2\deg \phi=[F(x,y):F(x)]=2. The other way to think about it is that the preimage of any point in P1\mathbb P^1 is two points (because we solve for y2y^2) or 1 points in which case it's ramified with index 2.

The uniformizer in P1\mathbb P^1 at point ϕ(P)=[x0,1]\phi(P)=[x_0,1] is tϕ(P)=xx0t_\phi(P)=x-x_0, so ϕtϕ(P)=xx0\phi^*t_{\phi(P)}=x-x_0. Since 2=degϕ=Qϕ1(ϕ(P))ordQ(ϕtϕ(Q))2=\deg \phi=\sum_{Q \in \phi^{-1}(\phi(P))}\text{ord}_Q(\phi^*t_{\phi(Q)}) and one of QQ is PP itself, we have ordP(xx0)2\text{ord}_{P}(x-x_0) \le 2. It also follows that we either have one point in pre-image and then ordP(xx0)=2\text{ord}_{P}(x-x_0)=2 or two points and then ordP(xx0)=1\text{ord}_{P}(x-x_0)=1. In the first case the polynomial F(x0,y)F(x_0,y) has double root and so Fy(x0,y0)=0F_y(x_0,y_0)=0, in the second case two distincts roots and Fy(x0,y0)0F_y(x_0,y_0) \ne 0. In any case:

ordP(ω)=ordP(xx0)ordP(Fy)1=0 \text{ord}_P(\omega) = \text{ord}_P(x-x_0)-\text{ord}_P(F_y)-1=0

Note that in case Fy(x0,y0)=0F_y(x_0,y_0)=0 we know that ordP(Fy)1\text{ord}_P(F_y) \ge 1 but it cannot be strictly greater because that order of ω\omega would be strictly less than 00 and we establised above that in cannot be the case.

So we proved that ω\omega has zero order in any PP in affine plane. One last thing is we need to consider its order in OO. We know that ordOx=2\text{ord}_Ox=-2 and ordOy=3\text{ord}_Oy=-3 so x=utO2,y=vtO3x=ut_O^{-2}, y = vt_O^{-3} where u(O),v(O)0,u(O),v(O)\ne 0, \infty (units in local ring at OO) and:

ω=dx2y+a1x+a3=2ut3+ut22vt3+a1ut2+a3dt==2u+ut2v+a1ut+a3t3dt\omega = \frac{dx}{2y+a_1x+a_3}=\frac{-2ut^{-3}+u't^{-2}}{2vt^{-3}+a_1ut^{-2}+a_3}dt=\\ =\frac{-2u+u't}{2v+a_1ut+a_3t^3}dt

Since uu is regular, by (3.4.11.f)(3.4.11.f) uu' is regular as well, t(O)=0t(O)=0 meaning the neither numerator nor denominator goes to 00 at OO and thus ordO(ω)=0\text{ord}_O(\omega)=0. So we proved:

div(ω)=0\text{div}(\omega) = 0

Finally by (3.4.13.b)(3.4.13.b) we have

2gen(C)2=degdivω=0    gen(C)=12\text{gen}(C)-2=\deg \text{div} \omega = 0 \implies \\ \text{gen}(C)=1

and taking O=[0,1,0]O = [0,1,0] we finish the proof

\square.

note

(b)(b) show that having this form of linear transformation is necessary condition for the curve to be the same

Short Weierstrass form

Consider a curve in Weierstrass form:

y2+a1xy+a3y=x3+a2x2+a4x+a6y^2+a_1xy+a_3y=x^3+a_2x^2+a_4x+a_6

We can simplify the equation using linear transformations. First, let's map y12(ya1xa3)y \mapsto \frac{1}{2}(y-a_1x-a_3). Note that transformation matrix is (a1110)\begin{pmatrix}-a_1 & 1 \\ 1 & 0\end{pmatrix} with detA=1\det A=1 so it's invertible and thus isomopshism. Then the equation becomes:

y2=4x3+b2x2+2b4x+b6,b2=a12+4a4b4=2a4+a1a3b6=a32+4a6y^2 = 4x^3+b_2x^2+2b_4x+b_6, \\ b_2=a_1^2+4a_4 \\ b_4=2a_4+a_1a_3 \\ b_6=a_3^2+4a_6

We define some auxiliary quantities for future reference:

b8=(b2b6b42)/4c4=b2224b4c6=b23+36b2b4216b6Δ=(c43c62)/1728j=c43/Δω=dx2y+a1x+a3=dy3x2+2a2x+a4a1yb_8=(b_2b_6-b_4^2)/4 \\ c_4=b_2^2-24b_4 \\ c_6=-b_2^3+36b_2b_4-216b_6 \\ \Delta=(c_4^3-c_6^2)/1728 \\ j=c_4^3/\Delta \\ \omega = \frac{dx}{2y+a_1x+a_3}=\frac{dy}{3x^2+2a_2x+a_4-a_1y}

Next, we can eliminate the x2x^2 term by applying the substitution (x,y)(x3b236,y108) (x, y) \mapsto \left(\frac{x-3b_2}{36}, \frac{y}{108}\right). Again the transformation matrix is (1/36001/108)\begin{pmatrix}1/36 & 0 \\ 0 & 1/108\end{pmatrix} so this is isomopshism. Then if charF2,3\text{char} F \ne 2,3 we get:

y2=x3+Ax+B,A=27c4,B=54c6y^2 = x^3 + Ax + B, \\ A=-27c_4, B=-54c_6

This form of the elliptic curve is called a Short Weiestrass form that we'll denote eqWs(E)\text{eq}_{Ws}(E). Note that when we transform the curve from Weierstrass curve to Short Weierstrass curve we actually change the curve so it's not the same curve anymore. But we do it via P2\mathbb P^2 automorphism so we can actually take some points on the original curve, transform these points via automorphism to Short Weierstrass curve, do some operations there and then come back to original curve via the inverse automorphism.

Thus essentially we can consider only Short Weiestrass curves. If it happens that the curve is not Short Weierstrass then we just use the algorithm above and thus we need to learn to deal with only the Short Weierstrass curves.

Singularity and invariants

Consider some transformation in the form of (4.1.1.b)(4.1.1.b):

x=u2x+r,y=u3y+u2sx+t\begin{align*} x' &= u^2 x + r, \\ y' &= u^3 y + u^2 s x + t \end{align*}

In can be checked that in this case we have the following transformations of the coefficents:

ua1=a1+2s,u2a2=a2sa1+3rs2,u3a3=a3+ra1+2t,u4a4=a4sa3+2ra2(t+rs)a1+3r22st,u6a6=a6+ra4+r2a2+r3ta3t2rta1,u2b2=b2+12r,u4b4=b4+rb2+6r2,u6b6=b6+2rb4+r2b2+4r3,u8b8=b8+3rb6+3r2b4+r3b2+3r4,u4c4=c4,u6c6=c6,u12Δ=Δ,j=j,u1ω=ω.\begin{align*} u a'_1 &= a_1 + 2s, \\ u^2 a'_2 &= a_2 - s a_1 + 3r - s^2, \\ u^3 a'_3 &= a_3 + r a_1 + 2t, \\ u^4 a'_4 &= a_4 - s a_3 + 2r a_2 - (t + rs)a_1 + 3r^2 - 2st, \\ u^6 a'_6 &= a_6 + r a_4 + r^2 a_2 + r^3 - t a_3 - t^2 - r t a_1, \\ u^2 b'_2 &= b_2 + 12r, \\ u^4 b'_4 &= b_4 + r b_2 + 6r^2, \\ u^6 b'_6 &= b_6 + 2r b_4 + r^2 b_2 + 4r^3, \\ u^8 b'_8 &= b_8 + 3r b_6 + 3r^2 b_4 + r^3 b_2 + 3r^4, \\ u^4 c'_4 &= c_4, \\ u^6 c'_6 &= c_6, \\ u^{12} \Delta' &= \Delta, \\ j' &= j, \\ u^{-1} \omega' &= \omega. \end{align*}

For the Short Weierstrass curve we have the following values for Δ,j\Delta, j:

Δ=16(4A3+27B2)j=1728(4A)3Δ\Delta = -16(4A^3+27B^2) \\ j=-1728\frac{(4A)^3}{\Delta}

Proposition 4.1.2: Singularity criterion

(E,O)EE=S(E)    Δ0\begin{align*} &\sphericalangle \\ &(E,O) \in \mathcal E \\ \hline \\ &E = \cancel S(E) \iff \Delta \ne 0 \end{align*}

Proof

    \implies

Note that in the table of transformation above we see that at this particular transformation Δ\Delta just scales by u12u^{12}. It can be shown that the transformation y12(ya1xa3)y \mapsto \frac{1}{2}(y-a_1x-a_3) does the same thing. So it doesn't change Δ\Delta being zero or non-zero. Thus we can consider the equation in the form:

y2=4x3+b2x2+2b4x+b6y^2 = 4x^3+b_2x^2+2b_4x+b_6 \\

The point (x0,y0)(x_0, y_0) is singular iff partial derivatives are zero, that is

2y0=12x02+2b2x0+2b4=02y_0=12x_0^2+2b_2x_0+2b_4=0

So singular point has a form (x0,0)(x_0, 0), moreover polynomial p(x):=4x3+b2x2+2b4x+b6p(x):=4x^3+b_2x^2+2b_4x+b_6 has p(x0)=0p(x_0)=0, px(x0)=0p'_x(x_0)=0 so x0x_0 should be a root of order at least 2 and thus discriminant of the cubic should go to zero. But it's discriminant is 16Δ16\Delta so we finished the proof. As a side note since cubic can have only one root of order 2, there could be only one singular point in Weiestrass.

    \impliedby

Consider an elliptic curve in the Long Weierstrass form:

f(x,y)=y2+a1xy+a3yx3a2x2a4xa6f(x,y)=y^2+a_1xy+a_3y-x^3-a_2x^2-a_4x-a_6

And its projective form:

F(x,y,z)=y2z+a1xyz+a3yz2x3a2x2za4xz2a6z3F(x,y,z)=y^2z+a_1xyz+a_3yz^2-x^3-a_2x^2z-a_4xz^2-a_6z^3

At point OO it has F/z(O)=1\partial F/\partial z(O)=1, so OS(E)O \in \cancel S(E).

Next, consider some singular point PS(E)P \notin \cancel S(E) and P=(x0,y0)P=(x_0,y_0). We can consider transformation x=x+x0,y=y+y0x'=x+x_0, y'=y+y_0. Under this transformation we have Δ\Delta not changing (see above for u=1,s=0,r=x0,t=y0u=1, s = 0, r=x_0, t=y_0). So we may assume that the singular point is (0,0)(0,0). Since the curve is singular at (0,0)(0,0) it means that fx(0,0)=0f'_x(0,0)=0 and fy(0,0)=0f'_y(0,0)=0. Since (0,0)E(0,0) \in E it also means that f(0,0)=0f(0,0)=0. But we know that

a6=f(0,0)=0a4=fx(0,0)=0a3=fy(0,0)=0a_6=-f(0,0)=0 \\ a_4=-f_x(0,0)=0 \\ a_3=f_y(0,0)=0 \\

So the equation becomes:

f(x,y)=y2+a1xyx3a2x2f(x,y)=y^2+a_1xy-x^3-a_2x^2

In this case we can calculate:

b2=a12+4a4=a12b4=2a4+a1a3=0b6=a32+4a6=0b8=(b2b6b42)/4=0c4=b2224b4=a14c6=b23+36b2b4216b6=a16Δ=(c43c62)/1728=(a112a112)/1728=0b_2=a_1^2+4a_4=a_1^2 \\ b_4=2a_4+a_1a_3=0 \\ b_6=a_3^2+4a_6=0 \\ b_8=(b_2b_6-b_4^2)/4=0 \\ c_4=b_2^2-24b_4=a_1^4 \\ c_6=-b_2^3+36b_2b_4-216b_6=-a_1^6 \\ \Delta=(c_4^3-c_6^2)/1728=(a_1^{12}-a_1^{12})/1728=0 \\

So we proved PS(E)    Δ=0\exists P \notin \cancel S(E) \implies \Delta = 0

\square

Proposition 4.1.3: j-invariant

(E,O),(E,O)EEE    j(E)=j(E)jF:(E,O)E:j(E)=j\begin{align*} &\sphericalangle \\ &(E,O), (E',O') \in \mathcal E \\ \hline \\ &\begin{align*} & E \cong E' \iff j(E)=j(E') \hspace{0.5cm} \tag{a} \\ & \forall j \in \overline F: \exists (E,O) \in \mathcal E: j(E)=j \hspace{0.5cm} \tag{b} \\ \end{align*} \end{align*}

Proof

a.

    \implies

If we take two Weierstrass forms of E1E_1 and E2E_2 they will be isomorphic. Thus by (4.1.1.b)(4.1.1.b) they're related by transformation that doesn't change the j-invariant.

    \impliedby

We will prove for char F5\text{char } F\ge 5 and curves in short Weierstrass form:

E:y2=x3+Ax+BE:y2=x3+Ax+BE: y^2=x^3+Ax+B \\ E': y^2=x^3+A'x+B' \\

Then

(4A)34A3+27B2=(4A)34A3+27B2    A3B2=A3B2\frac{(4A)^3}{4A^3 + 27B^2} = \frac{(4A')^3}{4A'^3 + 27B'^2} \implies \\ A^3B'^2=A'^3B^2

We want to build isomopshism in the form:

xu2x,yu3yx \mapsto u^2x', y \mapsto u^3y'

Consider 3 cases:

  1. A=0(j=0)A = 0\, (j=0) then since Δ0\Delta \ne 0 it follows that B0B\ne 0 so A=0A'=0 so we can make an isomopshism using u=(B/B)1/6u = (B/B')^{1/6}

  2. B=0(j=1728)B = 0\, (j=1728). Then likewise B=0B'=0 so we can take u=(A/A)1/4u = (A/A')^{1/4}

  3. A,B0(j0,1728)A,B \ne 0\, (j\ne 0, 1728). Then A,B0A', B' \ne 0 because if one of them is 00 then another one is 00 as well and Δ=0\Delta = 0 which is a contradiction of smoothness of EE. So we can take u=(A/A)1/4=(B/B)1/6u = (A/A')^{1/4}=(B/B')^{1/6}

b.

If j00,1728j_0 \ne 0, 1728 then consider equation:

E:y2+xy=x336j01728x1j01728E: y^2+xy=x^3-\frac{36}{j_0-1728}x-\frac{1}{j_0-1728}

In this case j(E)=j0,Δ=j03(j01728)3j(E)=j_0, \Delta=\frac{j_0^3}{(j_0-1728)^3}. The following curves work for other values of jj:

E:y2+y=x3,Δ=27,j=0E:y2=x3+x,Δ=64,j=1728E: y^2+y=x^3, \Delta = -27, j=0 \\ E: y^2=x^3+x, \Delta = -64, j=1728 \\

\square

Proposition 4.1.4: Invariant differential

(E,O)Eω=dx2y+a1x+a3=dy3x2+2a2x+a4a1ydivω=0\begin{align*} &\sphericalangle \\ &(E,O) \in \mathcal E \\ &\omega = \frac{dx}{2y+a_1x+a_3}=\frac{dy}{3x^2+2a_2x+a_4-a_1y} \\ \hline \\ &\text{div}\omega = 0 \end{align*}

Proof

Was proved in (4.1.1.c)(4.1.1.c)

\square