Hostname: page-component-78c5997874-94fs2 Total loading time: 0 Render date: 2024-11-10T11:28:29.829Z Has data issue: false hasContentIssue false

A UNIQUE PERFECT POWER DECAGONAL NUMBER

Published online by Cambridge University Press:  06 August 2021

PHILIPPE MICHAUD-RODGERS*
Affiliation:
Mathematics Institute, University of Warwick, Coventry, CV4 7AL, UK
Rights & Permissions [Opens in a new window]

Abstract

Let $\mathcal {P}_s(n)$ denote the nth s-gonal number. We consider the equation

$$ \begin{align*}\mathcal{P}_s(n) = y^m \end{align*} $$

for integers $n,s,y$ and m. All solutions to this equation are known for $m>2$ and $s \in \{3,5,6,8,20 \}$ . We consider the case $s=10$ , that of decagonal numbers. Using a descent argument and the modular method, we prove that the only decagonal number greater than 1 expressible as a perfect mth power with $m>1$ is $\mathcal {P}_{10}(3) = 3^3$ .

Type
Research Article
Creative Commons
Creative Common License - CCCreative Common License - BY
This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (https://creativecommons.org/licenses/by/4.0/), which permits unrestricted re-use, distribution, and reproduction in any medium, provided the original work is properly cited.
Copyright
© The Author(s), 2021. Published by Cambridge University Press on behalf of Australian Mathematical Publishing Association Inc.

1. Introduction

The nth s-gonal number, with $s \geq 3$ , which we denote by $\mathcal {P}_s(n)$ , is given by the formula

$$ \begin{align*} \mathcal{P}_s(n) = \frac{(s-2)n^2-(s-4)n}{2}. \end{align*} $$

Polygonal numbers have been studied since antiquity [Reference Dickson6, pages 1–39] and relations between different polygonal numbers and perfect powers have received much attention (see, for example, [Reference Kim, Park and Pintér7] and the references cited therein). Kim et al. [Reference Kim, Park and Pintér7, Theorem 1.2] found all solutions to the equation $\mathcal {P}_s(n) = y^m$ when $m>2$ and $s \in \{3,5,6,8,20 \}$ for integers n and y. We extend this result (for $m>1$ ) to the case $s=10$ , that of decagonal numbers.

Theorem 1.1. All solutions to the equation

(1.1) $$ \begin{align} \mathcal{P}_{10}(n) = y^m,\quad n,y,m \in \mathbb{Z},\quad m> 1 \end{align} $$

satisfy $n=y=0, n=|y|=1$ or $n=y=m=3$ .

In particular, the only decagonal number greater than 1 expressible as a perfect mth power with $m>1$ is $\mathcal {P}_{10}(3) = 3^3$ .

We will prove Theorem 1.1 by carrying out a descent argument to obtain various ternary Diophantine equations, to which one may associate Frey elliptic curves. The difficulty in solving the equation $\mathcal {P}_{s}(n) = y^m$ for a fixed value of s is due to the existence of the trivial solution $n=y=1$ (for any value of m). We note that adapting our method of proof also works for the cases $s \in \{3,5,6,8,20 \}$ mentioned above, but will not extend to any other values of s (see Remark 3.1).

2. Descent and small values of m

We note that it will be enough to prove Theorem 1.1 in the case $m=p$ , prime. We write (1.1) as

(2.1) $$ \begin{align} n(4n-3) = y^p, \quad n,y \in \mathbb{Z},\quad p \text{ prime}\end{align} $$

and suppose that $n,y \in \mathbb {Z}$ satisfy this equation with $n \ne 0$ .

Case 1: $3 \nmid n$

If $3 \nmid n$ , then n and $4n-3$ are coprime, so there exist coprime integers a and b such that

$$ \begin{align*} n = a^p \quad \text{ and } \quad 4n-3 = b^p. \end{align*} $$

It follows that

(2.2) $$ \begin{align} 4a^p-b^p = 3. \end{align} $$

If $p=2$ , we see that $(2a-b)(2a+b)=3$ , so that $a = b = \pm 1$ and so $n=|y|=1$ . If $p=3$ or $p=5$ , then using the Thue equation solver in Magma [Reference Bosma, Cannon and Playoust5], we also find that $a=b=1$ .

Case 2: $3 \parallel n$

Suppose that $3 \parallel n$ (that is, $\mathrm {ord}_3(n)=1$ ). Then, after dividing (2.1) by $3^{\mathrm {ord}_3(y)p}$ , we see that there exist coprime integers t and u with $3 \nmid t$ such that

$$ \begin{align*}n = 3t^p \quad \text{ and } \quad 4n-3 = 3^{p-1}u^p. \end{align*} $$

Then

(2.3) $$ \begin{align} 4t^p-3^{p-2}u^p = 1. \end{align} $$

If $p=2$ , we have $(2t-u)(2t+u)=1$ , which has no solutions. If $p=3$ , then we have $4t^3-3u^3=1$ and, using the Thue equation solver in Magma [Reference Bosma, Cannon and Playoust5], we verify that $u=t=1$ is the only solution to this equation. This gives $n=y=3$ . If $p=5$ , Magma’s Thue equation solver shows that there are no solutions.

Case 3: $3^2 \mid n$

If $3^2 \mid n$ , then $3 \parallel 4n-3$ and, arguing as in Case 2, there exist coprime integers v and w with $3 \nmid w$ such that

$$ \begin{align*}n = 3^{p-1}v^p \quad \text{ and } \quad 4n-3 = 3w^p. \end{align*} $$

So,

(2.4) $$ \begin{align} 4 \cdot 3^{p-2}v^p- w^p = 1. \end{align} $$

If $p=2$ , then as in Case 2 we obtain no solutions. If $p=3$ or $p=5$ , then we use Magma’s Thue equation solver to verify that there are no solutions with $v \ne 0$ .

3. Frey curves and the modular method

To prove Theorem 1.1, we will associate Frey curves to equations (2.2), (2.3) and (2.4) and apply Ribet’s level-lowering theorem [Reference Ribet8, Theorem 1.1] to obtain a contradiction. We describe this process as level-lowering the Frey curve. We have considered the cases $p=2,3$ and $5$ in Section 2 and so we will assume that $m=p$ is prime with $p \geq 7$ .

We note that at this point we could directly apply [Reference Bennett and Skinner3, Theorem 1.2] to conclude that the only solutions to (3.1) are $a=b=1$ , giving $n=1$ , and apply [Reference Bennett2, Theorem 1.2] to show that (3.2) and (3.3) have no solutions. The computations for (3.1) are not explicitly carried out in [Reference Bennett and Skinner3], so for the convenience of the reader and to highlight why the case $s=10$ is somewhat special, we provide some details of the arguments.

Case 1: $3 \nmid n$

We write (2.2) as

(3.1) $$ \begin{align} -b^p +4a^p = 3 \cdot 1^2, \end{align} $$

which we view as a generalised Fermat equation of signature $(p,p,2)$ . We note that the three terms are integral and coprime.

We suppose that $ab \ne \pm 1$ . Following the recipes of [Reference Bennett and Skinner3, pages 26–31], we associate Frey curves to (3.1). We first note that b is odd, since $b^p = 4n-3$ . If $a \equiv 1 \pmod {4}$ , we set

$$ \begin{align*}E_1: Y^2 = X^3 -3X^2+3a^pX. \end{align*} $$

If $a \equiv 3 \pmod {4}$ , we set

$$ \begin{align*}E_2: Y^2 = X^3 + 3X^2+3a^pX. \end{align*} $$

If a is even, we set

$$ \begin{align*}E_3: Y^2+XY = X^3 - X^2 + \frac{3a^p}{16} X. \end{align*} $$

We level-lower each Frey curve and find that for $i=1,2,3,$ we have $E_i \sim _p f_i$ for $f_i$ a newform at level $N_{p_i}$ , where $N_{p_1} = 36, N_{p_2} = 72$ and $N_{p_3} = 18$ . The notation $E \sim _p f$ means that the mod-p Galois representation of E arises from f. There are no newforms at level $18$ and so we focus on the curves $E_1$ and $E_2$ . There is a unique newform, $f_1$ , at level $36$ , and a unique newform, $f_2$ , at level $72$ .

The newform $f_1$ has complex multiplication by the imaginary quadratic field $\mathbb {Q}(\!\sqrt {-3})$ . This allows us to apply [Reference Bennett and Skinner3, Proposition 4.6]. Since $2 \nmid ab$ and $3 \nmid ab$ , we conclude that $p=7$ or $13$ and that all elliptic curves of conductor $2p$ have positive rank over $\mathbb {Q}(\!\sqrt {-3})$ . However, it is straightforward to check that this is not the case for $p=7$ and $13$ . We conclude that $E_1 \not \sim _p f_1$ .

Let $F_2$ denote the elliptic curve with Cremona label 72a2 whose isogeny class corresponds to $f_2$ . This elliptic curve has full two-torsion over the rationals and has j-invariant $2^{4} \cdot 3^{-2} \cdot 13^{3}$ . We apply [Reference Bennett and Skinner3, Proposition 4.4], which uses an image of inertia argument, to obtain a contradiction in this case too.

Remark 3.1. The trivial solution $a=b=1$ (or $n=y=1$ ) corresponds to the case $i=1$ above. The only reason we are able to discard the isomorphism $E_1 \sim _p f_1$ is because the newform $f_1$ has complex multiplication. The modular method would fail to eliminate the newform $f_1$ otherwise. For each value of s, we can associate to (1.1) generalised Fermat equations of signature $(p,p,2)$ , $(p,p,3)$ and $(p,p,p)$ . We found we could only obtain newforms with complex multiplication (when considering the case corresponding to the trivial solution) when $s = 3, 6, 8, 10$ or $20$ . A similar strategy of proof also works for $s=5$ using the work of Bennett [Reference Bennett1, page 3] on equations of the form $(a+1)x^n-ay^n = 1$ to deal with the trivial solution.

Case 2: $3 \parallel n$

We rewrite (2.3) as

(3.2) $$ \begin{align} 4t^p-3^{p-2}u^p = 1 \cdot 1^3, \end{align} $$

which we view as a generalised Fermat equation of signature $(p,p,3)$ . The three terms are integral and coprime. We suppose that $tu \ne \pm 1$ . Using the recipes of [Reference Bennett, Vatsal and Yazdani4, pages 1401–1406], we associate to (3.2) the Frey curve

$$ \begin{align*}E_4: Y^2 + 3XY - 3^{p-2}u^p \, Y = X^3. \end{align*} $$

We level-lower $E_4$ and find that $E_4 \sim _p f$ , where f is a newform at level $6$ , an immediate contradiction, as there are no newforms at level $6$ .

Case 3: $3^2 \mid n$

We rewrite (2.4) as

(3.3) $$ \begin{align} -w^p + 4 \cdot 3^{p-2}v^p = 1 \cdot 1^3, \end{align} $$

which we view as a generalised Fermat equation of signature $(p,p,3)$ . The three terms are integral and coprime. We suppose that $vw \ne \pm 1$ . The Frey curve we attach to (3.3) is

$$ \begin{align*} E_5: Y^2 + 3XY + 4 \cdot 3^{p-2} v^p \, Y = X^3. \end{align*} $$

We level-lower and find that $E_5 \sim _p f$ , where f is a newform at level $6$ , a contradiction as in Case 2.

This completes the proof of Theorem 1.1.

Footnotes

The author is supported by an EPSRC studentship.

References

Bennett, M., ‘Rational approximation to algebraic numbers of small height: the Diophantine equation $\mid\! a{x}^n+by^n\!\mid\ =1$ ’, J. reine angew. Math. 535 (2001), 149.10.1515/crll.2001.044CrossRefGoogle Scholar
Bennett, M., ‘Products of consecutive integers’, Bull. Lond. Math. Soc. 36(5) (2004), 683694.10.1112/S0024609304003480CrossRefGoogle Scholar
Bennett, M. and Skinner, C., ‘Ternary Diophantine equations via Galois representations and modular forms’, Canad. J. Math. 56(1) (2004), 2354.10.4153/CJM-2004-002-2CrossRefGoogle Scholar
Bennett, M., Vatsal, V. and Yazdani, S., ‘Ternary Diophantine equations of signature $\left(p,p,3\right)$ ’, Compos. Math. 140(6) (2004), 13991416.10.1112/S0010437X04000983CrossRefGoogle Scholar
Bosma, W., Cannon, J. and Playoust, C., ‘The Magma algebra system. I. The user language’, J. Symbolic Comput. 24(3–4) (1997), 235265.10.1006/jsco.1996.0125CrossRefGoogle Scholar
Dickson, L., History of the Theory of Numbers, Vol. II, Diophantine Analysis (Dover, New York, 2005).Google Scholar
Kim, D., Park, K. and Pintér, A., ‘A Diophantine problem concerning polygonal numbers’, Bull. Aust. Math. Soc. 88(2) (2013), 345350.10.1017/S0004972712001050CrossRefGoogle Scholar
Ribet, K., ‘On modular representations of $\mathrm{Gal}(\overline{\mathbb{Q}}/ \mathbb{Q})$ arising from modular forms’, Invent. Math. 100 (1990), 431476.CrossRefGoogle Scholar