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aC Therefore, AC = CA = a2Cand, in the same way, BC = CB = c2C

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Problem 10930

(American Mathematical Monthly, Vol.109, March 2002) Proposed by P. Schweitzer (USA).

Show that there do not exist real 2-by-2 matices A and B such that their commutator is nonzero and commutes with both A and B. (The commutator C of A and B is defined by C = AB − BA.) Solution proposed by Roberto Tauraso, Dipartimento di Matematica, Universit`a di Roma “Tor Vergata”, via della Ricerca Scientifica, 00133 Roma, Italy.

By the Cayley-Hamilton theorem, the matrices A and B solve their characteristic polynomial:

A2= aA + b , B2= cB + d

where a = tr(A), b = −det(A) and c = tr(B), d = −det(B). Since C commutes with A

 AC − CA= 0

AC+ CA = A2B+ BA2= (aA + b)B − B(aA + b) = aC Therefore, AC = CA = a2Cand, in the same way, BC = CB = c2C. Thus

C2= (AB − BA)C = A(BC) − B(AC) = a 2 ·c

2C −c 2 ·a

2C= 0.

Assume that C 6= 0. Then there is a vector v 6= 0 such that u := Cv 6= 0. Note that u is a common eigenvector of C, A and B:

Cu= C2v= 0, Au = ACv = a

2Cv= a

2u, Bu= BCv = c

2Cv= c 2u.

The vectors u and v are linearly independent: let α, β ∈ R such that αu + βv = 0 then 0 = C(αu + βv) = αCu + βCv = αC2v+ βCv = βu,

which implies that α = β = 0. Since a = tr(A) and c = tr(B) then the representations of the matrices A and B with respect to the base < u, v > are

A=

 a

2 γ

0 a2



and B =

 c

2 δ

0 2c



for some γ, δ ∈ R. Then

C= AB − BA =

 ac 4

a 2δ+2cγ 0 ac4



 ac 4

c 2γ+a2δ 0 ac4



= 0

that is a contradiction. 

Remark. The statement does not hold in higher dimension: for example in R3×3

if A =

0 1 0 0 0 0 0 0 0

 and B =

0 0 0 0 0 1 0 0 0

 then C = AB − BA =

0 0 1 0 0 0 0 0 0

and AC = CA, BC = CB.

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