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The Hasse invariant of the Tate normal form \(E_7\) and the supersingular polynomial for the Fricke group \(\Gamma _0^*(7)\)

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Abstract

A formula is proved for the number of linear factors and irreducible cubic factors over \({\mathbb {F}}_l\) of the Hasse invariant \({\hat{H}}_{7,l}(a)\) of the elliptic curve \(E_7(a)\) in Tate normal form, on which the point (0, 0) has order 7, as a polynomial in the parameter a, in terms of the class number of the imaginary quadratic field \(K={\mathbb {Q}}(\sqrt{-l})\). Conjectural formulas are stated for the numbers of quadratic and sextic factors of \(\hat{H}_{7,l}(a)\) of certain specific forms in terms of the class number of \({\mathbb {Q}}(\sqrt{-7l})\), which are shown to imply a recent conjecture of Nakaya on the number of linear factors over \({\mathbb {F}}_l\) of the supersingular polynomial \(ss_l^{(7*)}(X)\) corresponding to the Fricke group \(\Gamma _0^*(7)\).

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Notes

  1. The equation of \( E_{7,7} \) is \( Y^2+(1+d-d^2)XY+7(d^2-d^3)Y=X^3 -d (d-1)(7d+6)X^2-6d(d-1)(d^5 -2d^4-7d^3 + 9d^2 -3d+1)X -d(d-1)(d^9-2d^8-34d^7+153d^6-229d^5+199d^4-111d^3+28d^2-7d+1)\).

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Appendix

Appendix

Let

$$\begin{aligned} \eta (\tau )=q^{1/24} \prod _{n \ge 1}{(1-q^n)}, \ \ q = e^{2\pi i \tau }, \end{aligned}$$

be the Dedekind \(\eta \)-function. Also, let

$$\begin{aligned} h(\tau ) = q^{-1} \prod _{n \ge 1}{\frac{(1-q^{7n-3})(1-q^{7n-4})(1-q^{7n-2})^2(1-q^{7n-5})^2}{(1-q^{7n-1})^3(1-q^{7n-6})^3}}, \end{aligned}$$

a modular function for \(\Gamma _1(7)\). See [10, p. 156].

Theorem 10

For \(\tau \) in the upper half-plane,

$$\begin{aligned} \left( \frac{\eta (\tau )}{\eta (7\tau )}\right) ^4=\frac{h^3-8h^2+5h+1}{h(h-1)}, \ \ h=h(\tau ). \end{aligned}$$
(8.1)

Also, if \(d(\tau )=h(\frac{-1}{7\tau })\), then

$$\begin{aligned} 49\left( \frac{\eta (7\tau )}{\eta (\tau )}\right) ^4=\frac{d^3-8d^2+5d+1}{d(d-1)}, \ \ d=d(\tau ). \end{aligned}$$
(8.2)

It is clear that (8.2) follows from (8.1), using the transformation formula

$$\begin{aligned} \eta \left( \frac{-1}{\tau }\right) = \sqrt{\frac{\tau }{i}} \eta (\tau ). \end{aligned}$$

Theorem 11

The function \(h(\tau )\) above satisfies the transformation formulas:

$$\begin{aligned} h\left( \frac{3\tau - 1}{7\tau - 2}\right) =&\ \frac{1}{1-h(\tau )}, \end{aligned}$$
(8.3)
$$\begin{aligned} h\left( \frac{2\tau -1}{7\tau -3}\right) =&\ \frac{h(\tau )-1}{h(\tau )}. \end{aligned}$$
(8.4)

Note that the map \(A(\tau )=\frac{2\tau -1}{7\tau -3}\) has order 3 and \(A^2(\tau )= \frac{3\tau - 1}{7\tau - 2}\). We first prove (8.4). We use the notation \(e(x) = exp(2 \pi i x)\).

Proof

Start with the formulas from [10, p. 157]:

(8.5)
(8.6)

From the infinite products in (8.5) and (8.6) we get

$$\begin{aligned} s(\tau ) t^2(\tau ) =&\ q^{-1} \prod _{n \ge 1}{\frac{(1-q^{7n-3})(1-q^{7n-4})(1-q^{7n-2})^2(1-q^{7n-5})^2}{(1-q^{7n-1})^3(1-q^{7n-6})^3}}\\ =&\ h(\tau ). \end{aligned}$$

Hence, the theta function representations in (8.5) and (8.6) yield

To prove the formula for \(h\left( \frac{2\tau -1}{7\tau -3}\right) = h(A(\tau ))\) we compute the transforms

First, we have from [10, p. 143, (4.5)], using the mapping \(B(\tau ) = \frac{2\tau -7}{\tau -3}\), that

where

$$\begin{aligned} \kappa _1 = e\left( \frac{-27}{4}+\frac{37}{56}\right) \kappa _0 = e\left( \frac{-5}{56}\right) \kappa _0, \end{aligned}$$

and \(\kappa _0\) is a fixed 8-th root of unity depending only on the mapping B. Now use [10, (4.3)] with \(\ell = 0\) and \(m=9\) and the lower sign, according to which

This gives that

Next, we have

where

$$\begin{aligned} \kappa _3 = e\left( \frac{-39}{4}+\frac{81}{56}\right) \kappa _0 = e\left( \frac{39}{56}\right) \kappa _0. \end{aligned}$$

Using [10, (4.3)] with \(\ell = 0\) and \(m=8\) and the lower sign gives

from which we obtain

Finally, for the third theta function we have

where

$$\begin{aligned} \kappa _5 = e\left( \frac{-51}{4}+\frac{141}{56}\right) \kappa _0 = e\left( \frac{-13}{56}\right) \kappa _0. \end{aligned}$$

Now using [10, (4.3)] with \(\ell =0, m=-6\) and the upper sign gives

from which we obtain

Putting this all together gives

Now using the product formula [10, (4.8)] for the theta functions yields that

$$\begin{aligned} h\left( \frac{2\tau -1}{7\tau -3}\right) = \prod _{n \ge 1}{\frac{(1-q^{7n-1})(1-q^{7n-6})(1-q^{7n-3})^2(1-q^{7n-4})^2}{(1-q^{7n-2})^3(1-q^{7n-5})^3}}. \end{aligned}$$
(8.7)

On the other hand, from the relation \(s^7(\tau ) = h(\tau ) (h(\tau )-1)^2\) we easily derive the product formula

$$\begin{aligned} h(\tau )-1 = q^{-1} \prod _{n \ge 1}{\frac{(1-q^{7n-3})^3(1-q^{7n-4})^3}{(1-q^{7n-1})^2(1-q^{7n-6})^2(1-q^{7n-2})(1-q^{7n-5})}}. \end{aligned}$$

Dividing by the product formula for \(h(\tau )\) yields that

$$\begin{aligned} \frac{h(\tau )-1}{h(\tau )} = \prod _{n \ge 1}{\frac{(1-q^{7n-1})(1-q^{7n-6})(1-q^{7n-3})^2(1-q^{7n-4})^2}{(1-q^{7n-2})^3(1-q^{7n-5})^3}} \end{aligned}$$

and proves the formula. From (8.4) it follows that

$$\begin{aligned} h\left( \frac{3\tau -1}{7\tau -2}\right) = h(A^2(\tau )) = \frac{h(A(\tau ))-1}{h(A(\tau ))} = \frac{1}{1-h(\tau )}, \end{aligned}$$

which is formula (8.3). This proves Theorem 11. \(\square \)

Remark

Alternatively, we could finish the above proof by noting that \(h\left( \frac{2\tau -1}{7\tau -3}\right) \) is a modular function for \(\Gamma _1(7)\), since \(T \in \Gamma _1(7)\) satisfies

$$\begin{aligned} h(A T(\tau )) = h(SA(\tau )) = h(A(\tau )), \ \ \text {for some} \ S \in \Gamma _1(7). \end{aligned}$$

Since \(h(\tau )\) is a Hauptmodul for \(\Gamma _1(7)\) and \(h(\tau ) \rightarrow h(A(\tau ))\) induces an automorphism of \(\textsf {K}_{\Gamma _1(7)}/\textsf {K}_{\Gamma _0(7)}\), it follows that \(h(A(\tau ))\) is also a Hauptmodul and therefore equal to a linear fractional expression in \(h(\tau )\). Furthermore, the six values of \(h(\tau )\) at the cusps of \(\Gamma _1(7)\) (namely, \(\infty , 1 ,0\) and the roots \(r_i\) of \(x^3-8x^2+5x+1\), by (4.4)), are permuted by this automorphism (as residues of h modulo the prime divisors of \(\textsf {K}_{\Gamma _1(7)}\) at infinity). Since the value \(\infty \) corresponding to \(\tau = \infty i\) is mapped to \(h(A(\tau )) = 1\), by the product formula (8.7), it follows that the value 1 must be mapped to 0. This holds because \(h(A(\tau )) = \frac{h+a}{h+b}\) cannot map a root \(r_i\) to 0: otherwise \(a = -r_i\), and applying the map twice sends 1 to \(\infty \) (A has order 3), which would yield that b satisfies the irreducible equation \(b^2+b+1-r_i = 0\) over \({\mathbb {Q}}(\zeta _7)\) (the norm of its discriminant is \(-43\)). But then \(\frac{1-r_i}{1+b} = r_j\), for some j, would be impossible and \(\frac{h+a}{h+b}\) could not map 1 to one of the \(r_j\). Hence, \(a = -1, b = 0\) and \(h(A(\tau )) = \frac{h-1}{h}\). From the resulting product formula for \((h(\tau )-1)/h(\tau )\) we can derive the equation \(s^7(\tau ) = h(\tau ) (h(\tau )-1)^2\).

Now we use the fact that \([\Gamma _0(7): \Gamma _1(7) \cup (-I)\Gamma _1(7)]=3\), from which it follows that \(1, A, A^2\) are representatives for the cosets of \(\Gamma _1[7] = \Gamma _1(7) \cup (-I)\Gamma _1(7)\) in \(\Gamma _0(7)\). It follows that the function

$$\begin{aligned} \nonumber z(\tau )&= h(\tau )+h(A(\tau ))+h(A^2(\tau ))\\&= h(\tau )+\frac{h(\tau )-1}{h(\tau )}+\frac{1}{1-h(\tau )} = \frac{h^3(\tau )-3h(\tau )+1}{h(\tau )(h(\tau )-1)} \end{aligned}$$
(8.8)

is a modular function for \(\Gamma _0(7)\) with a simple pole at \(\infty i\) and the value \(z(\tau ) = z(0) = 8\) at the other cusp of \(\Gamma _0(7)\) (since the values of \(h(\tau )\) at the cusps of \(\Gamma _1(7)\) lying above 0 are the roots \(r_i\) of \(x^3-8x^2+5x+1\)). It is clear that \(\left( \frac{\eta (\tau )}{\eta (7\tau )}\right) ^4\) is a Hauptmodul for \(\Gamma _0(7)\) [25, pp. 46, 51], and comparing q-expansions gives that

$$\begin{aligned} z(\tau ) = \left( \frac{\eta (\tau )}{\eta (7\tau )}\right) ^4+8. \end{aligned}$$

This shows that

$$\begin{aligned} \left( \frac{\eta (\tau )}{\eta (7\tau )}\right) ^4&= z(\tau )-8 = \frac{h^3(\tau )-3h(\tau )+1}{h(\tau )(h(\tau )-1)}-8\\&= \frac{h^3(\tau )-8h^2(\tau )+5h(\tau )+1}{h(\tau )(h(\tau )-1)}, \end{aligned}$$

which is (8.1). See [11, (4.24), p. 89].

These identities are closely related to several of Ramanujan’s entries in the unorganized material of his Notebooks. See entries 31 and 32 in [1, pp. 174–184]. In particular, the product representation of \(h(\tau )-1\) in the above proof is equivalent to Entry 32(ii) of [1, p. 176] (or [2, (1.2)]); and the relation \(f_7(h(\tau ),j_7^*(\tau )) = 0\) in Sect. 4 is, assuming Theorem 10, equivalent to Entry 32(iii) of [1, p. 176] (or [2, (1.3)]). Also see [6, Theorem 7.14, p. 440] and [19].

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Morton, P. The Hasse invariant of the Tate normal form \(E_7\) and the supersingular polynomial for the Fricke group \(\Gamma _0^*(7)\). Ramanujan J 63, 339–385 (2024). https://doi.org/10.1007/s11139-023-00764-8

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