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Kyungpook Mathematical Journal 2023; 63(3): 345-353

Published online September 30, 2023 https://doi.org/10.5666/KMJ.2023.63.3.345

Copyright © Kyungpook Mathematical Journal.

On the Tarry-Escott and Related Problems for 2×2 matrices over

Supawadee Prugsapitak∗ and Walisa Intarapak, Vichian Laohakosol

Algebra and Applications Research Unit, Division of Computational Science, Faculty of Science, Prince of Songkla University, Hat Yai, Songkhla 90110, Thailand
e-mail : supawadee.p@psu.ac.th and walisa.p@hotmail.com

Department of Mathematics, Faculty of Science, Kasetsart University, Bangkok 10900, Thailand
e-mail : fscivil@ku.ac.th

Received: October 31, 2022; Revised: July 2, 2022; Accepted: July 5, 2023

Reduced solutions of size 2 and degree n of the Tarry-Escott problem over M2() are determined. As an application, the diophantine equation αAn+βBn=αCn+βDn, where α,β are rational numbers satisfying α+β0 and n{1,2}, is completely solved for A,B,C,DM2().

Keywords: Diophantine Equation, Matrix Equation, Tarry-Escott Problem

A Diophantine equation is an equation, usually with integral or rational coefficients, in which the sought-after unknowns are also integers. In 1989, Vaserstein [6] suggested solving classical problems of number theory substituting the ring by the ring M2() of 2×2 integral matrices. Some problems become easier and some give us interesting results. The Tarry-Escott problem is a classical problem in number theory which asks one to find two distinct multisets of integers {a1,,an} and {b1,,bn} such that

i=1naij= i=1nbij

for j=1,2,,k. We call n the size of the solution and k the degree. We abbreviate the above system by writing

{a1,,an}=k{b1,,bn}.

Solutions with k=n-1 are called ideal solutions. The Tarry-Escott problem has been extensively investigated in the literature; see for instance [1], [2] and also [5].

In 2006, Choudhry [3] introduced a matrix analog of the Tarry-Escott problem by considering the problem over M2(). The Tarry–Escott problem over Mm(R) for a given ring R can be stated as follows: given k,m,n and a ring R, two different multisets

A={A1,A2,,An}andB={B1,B2,,Bn},

where Ai,BiMm(R){0_}, constitute a non-trivial solution of the Tarry–Escott problem of size n and degree k over Mm(R) if

i=1nAij= i=1nBij  (j=1,2,,k),

abbreviated as {A1,,An}=k{B1,,Bn}. Choudhry [3] obtained, in parametric terms, two distinct pairs of matrices A1,A2 and B1,B2 in M2() such that A1n+A2n=B1n+B2n holds simultaneously for all integral values of n, whether positive or negative. This gives a non-trivial solution of the matrix analog of the Tarry-Escott problem of infinite degree and size 2. Using this solution, he obtained an arbitrarily long multigrade chain of matrices in M2() such that

A11n+A12n=A21n+A22n==Am1n+Am2n,

which also holds simultaneously for all integral values of n, whether positive or negative. Further, he obtained a parametric solution over M2() of the equation

A1n+A2n+A3n=B1n+B2n+B3n,

for all integral values of n. This solution leads to another arbitrarily long multigrade chain of matrices in M2().

In the present work, we present a different approach to obtain solutions of the Tarry-Escott problem over M2(); our approach also provides additional solutions different from those of Choudhry. As an application of our main result, general solutions, over M2(), are determined for the diophantine equation

αAn+βBn=αCn+βDn,

where α,β with α+β0 and n{1,2}.

First, we prove an auxiliary result which will be used later.

Lemma 2.1. Let m and n be positive integers,

let Ai,BiMm()(i=1,,n), and let αi. If

i=1nαiAi= i=1nαiBiand i=1nαiAi2= i=1nαiBi2,

then

i=1nαi(Ai+C)= i=1nαi(Bi+C)and i=1nαi(Ai+C)2= i=1nαi(Bi+C)2

for any CMm().

Proof. Since i=1nαiAi= i=1nαiBi and i=1nαiAi2= i=1nαiBi2, it is easy to see that

i=1nαi(Ai+C)= i=1nαi(Bi+C)

and

i=1nαi(Ai+C)2=i=1nαiAi2+(i=1nαiAi)C+C(i=1nαiAi)+i=1nαiC2=i=1nαiBi2+(i=1nαiBi)C+C(i=1nαiBi)+i=1nαiC2=i=1nαi(Bi+C)2.

Immediate from Lemma 2.1 is

Corollary 2.2. Let m and n be positive integers and let

A={A1,A2,,An}andB={B1,B2,,Bn}

be subsets of Mm(). If A=2B, then for any matrix CMm() we have

A+C=2B+C

where

A+C={A1+C,A2+C,,An+C},B+C={B1+C,B2+C,,Bn+C}.

We next define equivalent solutions.

Definition 2.3. Let k, m and n be positive integers. Let

A={A1,,An},B={B1,,Bn},X={X1,,Xn},Y={Y1,,Yn}

be subsets of Mm(). We say that A=kB and X=kY are equivalent if there exist M and N in Mm() such that for all i,

Xi=MAi+NandYi=MBi+N.

Definition 2.4. Let k, m and n be positive integers. Let A={A1,,An},B={B1,,Bn} be subsets of Mm(). Then a solution A=kB is called a reduced solution if

i=1nAi= i=1nBi=0_.

The concept of being reduced is useful because of the next result.

Theorem 2.5. Let m and n be positive integers. Every solution of size n and degree 2 of the Tarry-Escott Problem over Mm() is equivalent to a reduced solution.

Proof. Let A={A1,,An} and B={B1,,Bn} be two subsets of Mm() such that A=2B. Now let X={X1,X2,,Xn} and Y={Y1,Y2,,Yn}, where Xi=AiS, Yi=BiS for i=1,,n and S=(A1++An)/n. It is easy to see that

i=1nXi= i=1nYi=0_.

Thus X=2Y is a reduced solution. Since A=2B and X=2Y, by Lemma 2.1, A=2B is equivalent to a reduced solution X=2Y.

We now consider the so-called symmetric solutions of the Tarry-Escott Problem over M2(); these are integral matrices X and Y satisfying

Xn+(X)n=Yn+(Y)n,

for all positive integers n. It suffices to show that X2=Y2. We first recall a result from [4].

Theorem 2.6. Let c. Suppose that X and Y are two elements in M2() such that XYYX. If X2+Y2=cI where I is the identity matrix, then tr(X)=tr(Y)=0 and detX+detY=c.

We prove now another auxiliary result.

Lemma 2.7. Suppose X and Y are nonzero elements in M2() and XY. Then X2=Y2andXY=YX if and only if there exist nonzero matrices A,BM2() such that

AB=BA=0_,X=A+B2andY=AB2.

Proof. Suppose X2=Y2 and XY=YX. Next, we let A = X+Y and B=X-Y. Then the results follows easily. For the converse, we suppose that X=(A+B)/2 and Y=(AB)/2 where AB=BA=0_. Then it is easy to see that XY=YX and X2=Y2. Hence the converse holds as desired.

From Lemma 2.7, in order to find commutative solutions of Xn+(X)n=Yn+(Y)n for all positive integer n, it suffices to solve for matrices A and B such that AB=BA=0_, and this leads us to our first main result.

Theorem 2.8. Suppose X and Y are nonzero elements in M2(). Then {X,X}=2{Y,Y} if and only if X,Y belong to one of the following two classes.

  • 1. XYYX,X2=Y2, X=abcaandY=wxyw where

    a,b,c,w,x,y are rationals such that a2+bc=w2+xy and (bxcx or axbw or aycw).

  • 2. XY=YX,X2=Y2, and there exist nonzero matrices A,BM2() such that

    AB=BA=0_,X=A+B2andY=AB2.

    where A and B are of the following forms:

    • (a) A=amacmc and B=wxwmxm where acmw0 and aw+xc=0,

    • (b) A=00cd and B=w0cwd0 where cdw0,

    • (c) A=0b0d and B=wbwd00 where bdw≠ 0,

    • (d) A=000d and B=w000 where dw≠ 0,

    • (e) A=00c0 and B=00y0 where cy≠ 0,

    • (f) A=0b00 and B=0x00 where bx≠ 0.

Proof. Suppose X2=Y2.

Case 1: XYYX. Then by Theorem 2.6, tr(X)=tr(Y)=0 and detX+detiY=0. Let X=abca,Y=wxyw where a,b,c,w,x,y. Since detX+detiY=0, detX=detY. This implies that a2+bc=w2+xy as desired. Now note that XY=aw+byaxbwcwaycx+awandYX=aw+cxbwaxaycwby+aw. Thus we have bycx or axbw or aycw.

Case 2: XY=YX. By Lemma 2.7, there exist A,BM2() such that AB=BA=0_. Suppose A=abcd and B=wxyz. Thus we have the following system of equations:

aw+by=aw+cx=0
ax+bz=bw+xd=0
cw+dy=ay+cz=0
cx+dz=by+dz=0

Since AB=0_, this implies that detA=0 or detB=0. We may assume that detA=0. Thus ad-bc=0.

Case 2.1: abcd0. Since ad-bc=0, a/b=c/d. Let m=b/a. By (2.1), y=w/m. By (2.2), z=x/m. Thus A=amacmc and B=wxwmxm as desired.

Case 2.2: ad = bc =0. Thus there are 4 cases to consider.

Case 2.2.1: a=b=0. Then (2.1)-(2.4) imply that

cx=xd=cw+dy=cz=cx+dz=dz=0.

Since at least one of c and d is nonzero, we have x=z=0. If cd0 then cw+dy=0. Then y=cw/d. Thus we obtain solutions of the form A=00c0 and B=w0cwdd where cdw0.

Case 2.2.1(i): c=0. Then y=0. The fact that A,B are nonzero matrices implies dw0. Thus we obtain solutions of the form A=000d and B=w000 where dw0.

Case 2.2.1(ii): d=0. Then w=0. Again since A,B are nonzero matrices, we have cy0. So we obtain solutions of the form A=00c0 and B=00y0 where cy0.

Case 2.2.2: a=c=0. Then (2.1)-(2.4) imply that

by=bz=bw+dx=dy=dz=by+dz=0.

Since at least one of b and d is nonzero, we have y=z=0.

Case 2.2.2(i): bd0. Then bw+dx=0 and x=bw/d. Thus we obtain solutions of the form A=0b0d and B=wbwd00 where bdw0.

Case 2.2.2(ii): b=0. Then x=0. The fact that A,B are nonzero matrices implies dw0. Thus we obtain solutions of the form A=000d and B=w000 where dw0.

Case 2.2.2(iii): d=0. Then w=0. Again since A and B are nonzero matrices, we have bx0. So we obtain solutions of the form A=0b00 and B=0x00 where bx0.

For the case b=d=0 and c=d=0, we proceed similarly and obtain solutions as shown in the previous cases. The converse is easily checked.

We next provide an example.

Example 2.9. Let A=1212,B=4422. It is easy to see that AB=BA=0_. Next, we let X=(A+B)/2 and Y=(AB)/2. Then

X=5/233/22,Y=3/211/20.

By Lemma 2.7, XY = YX and X2=Y2. Thus {X,X}=n{Y,Y} for any positive integer n. Moreover, since X and Y are nonsingular matrices, {X,X}=n{Y,Y} for all integer n.

We proceed now to our final task which is to solve

α1X1n+α2X2n=α1Y1n+α2Y2n

for n=1 and 2 over M2(). We need two more auxiliary results.

Lemma 2.10. Let m be a positve integer. Let A1,A2,B1,B2 be matrices in Mm(). Let α1 and α2 be nonzero rational numbers such that α1+α20. If

α1A1n+α2A2n=α1B1n+α2B2n

for n=1,2 then there exist Ai and Bi in Mm() such that

α1A 1+α2A 2=0_=α1B 1+α2B 2andα1A 12+α2A 22=α1B 12+α2B 22.

Proof. Suppose α1A1n+α2A2n=α1B1n+α2B2n for n=1, 2 and α1α2(α1+α2)0.

For i=1, 2, we define

S=α1A1+α2A2,Ai=AiSα1+α2,Bi=BiSα1+α2.

Then α1A 1+α2A 2=α1B 1+α2B 2=0. Since α1A1n+α2A2n=α1B1n+α2B2n for n=1, 2, by Lemma 2.1, we have α1A 12+α2A 22=α1B 12+α2B 22.

Lemma 2.11. Let m be a positive integer. Let α1 and α2 be nonzero rational numbers such that α1+α20. There exist A1,A2,B1,B2Mm() such that α1A1+α2A2=α1B1+α2B2=0_ and α1A12+α2A22=α1B12+α2B22 if and only if A12=B12.

Proof. Suppose α1A1+α2A2=α1B1+α2B2=0_, A2=(α1A1)/α2 and B2=(α1B1)/α2. Then

(α1+α12/α2)A12=α1A12+α2A22=α1B12+α2B22=(α1+α12/α2)B12.

Thus A12=B12.

For the converse, suppose A2=(α1A1)/α2 and B2=(α1B1)/α2. Then

α2A2+α1A1=α1B1+α2B2=0_.

Since A12=B12, we obtain that

α1A12+α2A22=α1B12+α2B22.

Combining the results of Lemmas 2.10 and 2.11, we arrive at our final main result.

Theorem 2.12. Let α1 and α2 be nonzero rational numbers such that α1+α20. Then all solutions of the diophantine equation

α1X1n+α2X2n=α1Y1n+α2Y2n

for n=1 and 2 over M2() are the form X1=A1+C, X2=(α1A1)/α2+C, Y1=B1+C, Y2=(α1B1)/α2+C where A12=B12 and CM2().

We end this paper with an example.

Example 2.13. We show how to solve the following system of equations

2X1n+3X2n=2Y1n+3Y2n  (1n2)

over M2().

By Lemma 2.10, we can restrict our attention to find solutions A1,A2,B1,B2 in M2() such that

2A1+3A2=2B1+3B2=0_and2A12+3A22=2B12+3B22.

By Theorem 2.8, it suffices to find A1,B1M2() such that A12=B12. We work out some solutions for two different cases.

Case 1: A1B1=B1A1. Let A1=5/233/22 and B1=3/211/20. Then we have

A2=23A1=5/3214/3 and B2=23B112/31/30.

Case 2: A1B1B1A1. Let A1=2142 and B1=3193. Then

A2=23A1=4/32/38/34/3 and B2=23B1=22/362.

Therefore,

2(A1+C)n+3(A2+C)n=2(B1+C)n+3(B2+C)n

for n=1, 2 where CM2().

We would like to express our gratitude to the referee(s) for comments and suggestions.

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