1 Introduction
The general Erdős distance problem is to determine the number of distinct distances spanned by a finite set of points. In the Euclidean space, it is conjectured that for any finite set
$E \subset \mathbb {R}^d$
,
$d\ge 2$
, we have
$|\Delta (E)| \gtrapprox |E|^{{2}/{d}}$
, where
$\Delta (E)=\{\|x-y\| : x,y \in E\}$
. Here and throughout,
$X\ll Y$
means that there exists
$C>0$
such that
$X\le CY$
, and
$X\lessapprox Y$
with the parameter N means that for any
$\varepsilon>0$
, there exists
$C_{\varepsilon }>0$
such that
$X\,\le \,C_{\varepsilon }N^{\varepsilon }Y$
.
The finite field analogue of the distance problem was first studied by Bourgain et al. [Reference Bourgain, Katz and Tao2] over prime fields. In this setting, the Euclidean distance between any two points
$x=(x_1,\ldots , x_d), y=(y_1,\ldots ,y_d) \in \mathbb {F}_q^d$
, the d-dimensional vector space over the finite field
$\mathbb F_q$
of order q, is
$\|x-y\|=\sum _{i=1}^d(x_i-y_i)^2\in \mathbb F_q$
. For prime fields
$\mathbb {F}_p$
with
$p\equiv 1 \pmod 4$
, they showed that if
$E \subset \mathbb {F}_p^2$
with
$|E|=p^{\delta }$
for some
$0<\delta <2$
, then the distance set satisfies
$|\Delta (E)| \gg |E|^{{1}/{2}+\varepsilon }$
for some
$\varepsilon>0$
depending only on
$\delta $
.
This bound does not hold in general for arbitrary finite fields
$\mathbb {F}_q$
, as shown by Iosevich and Rudnev [Reference Iosevich and Rudnev9]. In this general setting, they considered the Erdős–Falconer distance problem to determine how large
$E \subset \mathbb {F}_q^d$
needs to be so that
$\Delta (E)$
spans all possible distances or at least a positive proportion of them. More precisely, they proved that
$\Delta (E)=\mathbb {F}_q$
if
$|E|> 2q^{{(d+1)}/{2}}$
in the all distances case, and also conjectured that
$|\Delta (E)| \gg q$
if
$|E| \gg _{\varepsilon } q^{{d}/{2}+\varepsilon }$
in the positive proportion case. In [Reference Hart, Iosevich, Koh and Rudnev6], it was shown that the exponent in the all distances case is sharp for odd d, and the conjecture for the positive proportion case holds for all
$E \subset \{x\in \mathbb {F}_q^d : \|x\|=1\}$
. It is conjectured that in even dimensions, the optimal exponent is
${d}/{2}$
for the all distances case. In particular for
$d=2$
, it was shown in [Reference Chapman, Erdogan, Hart, Iosevich and Koh3] that if
$E \subseteq \mathbb {F}_q^2$
satisfies
$|E| \gg q^{{4}/{3}}$
, then
$|\Delta (E)| \gg q$
, improving the positive proportion case. The proofs in [Reference Chapman, Erdogan, Hart, Iosevich and Koh3] use extension estimates for circles. Therefore, one would expect to get improvements for distance problems if one can obtain improved estimates for extension problems.
There have been a recent series of other improvements and generalisations on the Erdős–Falconer distance problem. In [Reference Hieu and Pham7], a generalisation for subsets of regular varieties was studied. Extension theorems and their connection to the Erdős–Falconer problem are the main focus of [Reference Koh, Pham and Vinh10]. The exponents
${(d+1)}/{2}$
and
${d}/{2}$
were improved in [Reference Pham and Suk13, Reference Pham and Vinh14] for subsets E with Cartesian product structure in the all distances case for
$|\Delta (E)|$
and in the positive proportion case for the quotient distance set
$|{\Delta (E)}/{\Delta (E)}|$
.
A two-parameter variant of the Erdős–Falconer distance problem for the Euclidean distance was studied by Birklbauer and Iosevich in [Reference Birklbauer and Iosevich1]. More precisely, given
$E \subseteq \mathbb {F}_q^d \times \mathbb {F}_q^d$
, where
$d\ge 2$
, define the two-parameter distance set as
![](https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20230509150418721-0640:S0004972722000818:S0004972722000818_eqnu1.png?pub-status=live)
They proved the following results.
Theorem 1.1 [Reference Birklbauer and Iosevich1]
Let E be a subset in
$\mathbb {F}_q^d \times \mathbb {F}_q^d$
. If
$|E| \gg q^{{(3d+1)}/{2}}$
, then
$ |\Delta _{d, d}(E)| = q^2$
.
Theorem 1.2 [Reference Birklbauer and Iosevich1]
Let E be a subset in
$\mathbb {F}_q^2 \times \mathbb {F}_q^2$
. If
$|E| \gg q^{{10}/{3}}$
, then
$ |\Delta _{2, 2}(E)| \gg q^2$
.
In this short note, we provide an extension and an improvement of these results. Unlike [Reference Birklbauer and Iosevich1], which relies heavily on Fourier analytic techniques, we use an elementary counting approach.
Let
$P(x)=\sum _{i=1}^da_ix_i^s\in \mathbb F_q[x_1,\ldots , x_d]$
be a fixed diagonal polynomial in d variables of degree
$s\ge 2$
. For
$x=(x_1,\ldots ,x_d), y=(y_1,\ldots ,y_d) \in \mathbb {F}_q^d$
, we introduce
![](https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20230509150418721-0640:S0004972722000818:S0004972722000818_eqnu2.png?pub-status=live)
For any set
$E\subset \mathbb {F}_q^d\times \mathbb {F}_q^d$
, define
![](https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20230509150418721-0640:S0004972722000818:S0004972722000818_eqnu3.png?pub-status=live)
Our first result reads as follows.
Theorem 1.3. Let E be a subset in
$\mathbb {F}_q^d \times \mathbb {F}_q^d$
. If
$|E| \gg q^{{(3d+1)}/{2}}$
, then
$ |\Delta _{d, d}^s(E)| \gg q^2$
.
Our method also works for the multi-parameter distance set for
$E \subseteq \mathbb {F}_q^{d_1+\cdots +d_k}$
, but we do not discuss such extensions here. For
$d=2$
, we get an improved version of Theorem 1.2 for the Euclidean distance function over prime fields.
Theorem 1.4. Let
$E \subseteq \mathbb {F}_p^2 \times \mathbb {F}_p^2$
. If
$|E| \gg p^{{13}{/4}}$
, then
$ |\Delta _{2,2}(E)| \gg p^2$
.
The continuous versions of Theorems 1.3 and 1.4 have been studied in [Reference Du, Ou and Zhang4, Reference Hambrook, Iosevich and Rice5, Reference Iosevich, Janczak and Passant8]. We do not know whether our method can be extended to that setting. It follows from our approach that the conjectured exponent
${d}/{2}$
of the (one-parameter) distance problem would imply the sharp exponent for the two-parameter analogue, namely
${3d}/{2}$
, for even dimensions. We refer to [Reference Birklbauer and Iosevich1] for constructions and more discussions.
2 Proof of Theorem 1.3
By using the following auxiliary result whose proof relies on Fourier analytic methods (see [Reference Vinh15, Theorem 2.3] and [Reference Koh and Shen11, Corollaries 3.1 and 3.4]), we are able to give an elegant proof for Theorem 1.3. Compared with the method in [Reference Birklbauer and Iosevich1], ours is more elementary.
Lemma 2.1. Let
$X, Y \subseteq \mathbb {F}_q^d$
. Define
$\Delta ^s(X, Y)=\{\|x-y\|_s\colon x\in X, y\in Y\}$
. If
$|X||Y|\gg q^{d+1}$
, then
$|\Delta ^s(X, Y)|\gg q$
.
Proof of Theorem 1.3
By assumption,
$|E|\ge Cq^{d+{(d+1)}/{2}}$
for some constant
$C>0$
. For
$y\in \mathbb {F}_q^d$
, let
$E_y:=\{x\in \mathbb F_q^d : (x, y)\in E\}$
and define
![](https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20230509150418721-0640:S0004972722000818:S0004972722000818_eqnu4.png?pub-status=live)
We first show that
$ |Y|\,\ge \, \tfrac 12C q^{{(d+1)}/{2}}$
. Note that
![](https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20230509150418721-0640:S0004972722000818:S0004972722000818_eqnu5.png?pub-status=live)
where the last inequality holds since
$|E_y|\,\le \,q^d$
for
$y\in \mathbb {F}_q^d$
. Combining it with the assumption on
$|E|$
gives the lower bound
![](https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20230509150418721-0640:S0004972722000818:S0004972722000818_eqnu6.png?pub-status=live)
However, by definition,
$|E_y|\,\le \,\tfrac 12C q^{{(d+1)}/{2}}$
for
$y \in \mathbb {F}^d_q\setminus Y$
, yielding the upper bound
![](https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20230509150418721-0640:S0004972722000818:S0004972722000818_eqnu7.png?pub-status=live)
These two bounds together give
$Cq^{d+{(d+1)}/{2}} - q^d|Y|\,\le \,\tfrac 12C q^{d+{(d+1)}/{2}}$
, proving the claimed bound
$|Y|\,\ge \, \tfrac 12C q^{{(d+1)}/{2}}$
.
In particular, Lemma 2.1 implies
$|\Delta ^s(Y,Y)|\gg q$
, as
$|Y||Y| \gg q^{d+1}$
. However, for each
$u\in \Delta ^s(Y,Y)$
, there are
$z, t\in Y$
such that
$\|z-t\|_s=u$
. One has
$|E_z|, |E_t|\gg q^{{(d+1)}/{2}}$
, therefore, again by Lemma 2.1,
$|\Delta ^s(E_z, E_t)|\gg q$
. Furthermore, for
$v\in \Delta ^s(E_z, E_t)$
, there are
$x\in E_z$
and
$y\in E_t$
satisfying
$\|x-y\|_s=v$
. Note that
$x\in E_z$
and
$y\in E_t$
mean that
$(x,z), (y,t)\in E$
. Thus,
$(v,u)=(\|x-y\|_s, \|z-t\|_s)\in \Delta _{d, d}^s(E)$
. From this, we conclude that
$|\Delta _{d, d}^s(E)|\gg q|\Delta ^s(Y,Y)|\gg q^2$
, which completes the proof.
3 Proof of Theorem 1.4
To improve the exponent over prime fields
$\mathbb {F}_p$
, we strengthen Lemma 2.1 as shown in Lemma 3.1 below. Following the proof of Theorem 1.3 and using Lemma 3.1 proves Theorem 1.4.
Lemma 3.1. Let
$X, Y \subseteq \mathbb {F}_p^2$
. If
$|X|, |Y|\gg p^{5/4}$
, then
$|\Delta (X, Y)|\gg p$
.
Proof. It is clear that if
$X' \subseteq X$
and
$Y' \subseteq Y$
, then
$\Delta (X',Y')\subseteq \Delta (X,Y)$
. Thus, without loss of generality, we may assume that
$|X|=|Y|=N$
with
$N\gg p^{5/ 4}$
. Let Q be the number of quadruples
$(x, y, x', y')\in X\times Y\times X\times Y$
such that
$\|x-y\|=\|x'-y'\|$
. It follows easily from the Cauchy–Schwarz inequality that
![](https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20230509150418721-0640:S0004972722000818:S0004972722000818_eqnu8.png?pub-status=live)
Let T be the number of triples
$(x, y, y')\in X\times Y\times Y $
such that
$\|x-y\|=\|x-y'\|$
. By the Cauchy–Schwarz inequality again, one gets
$Q\ll |X|\cdot T$
. Next, we need to bound T. For this, denote
$Z=X\cup Y$
, so that
$N\le |Z|\le 2N$
. Let
$T'$
be the number of triples
$(a, b, c)\in Z\times Z\times Z$
such that
$\|a-b\|=\|a-c\|$
. Obviously,
$T\le T'$
. However, it was recently proved (see [Reference Murphy, Petridis, Pham, Rudnev and Stevens12, Theorem 4]) that
![](https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20230509150418721-0640:S0004972722000818:S0004972722000818_eqnu9.png?pub-status=live)
which gives
![](https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20230509150418721-0640:S0004972722000818:S0004972722000818_eqnu10.png?pub-status=live)
and then
$T\ll {N^3}/p$
(since
$N\gg p^{5 /4}$
). Putting all the bounds together, we obtain
![](https://static.cambridge.org/binary/version/id/urn:cambridge.org:id:binary:20230509150418721-0640:S0004972722000818:S0004972722000818_eqnu11.png?pub-status=live)
or equivalently,
$|\Delta (X,Y)|\gg p$
, as required.
Acknowledgement
The authors are grateful to Dr. Thang Pham for sharing insights and new ideas.