Identities for matrix commutators

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Verify the validity of the identity (see problem 15. 18):

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(1)

[A,B]=−[B,A]\left[A, B\right] = - \left[B, A\right]

(2)

[A,A]=O\left[A, A\right] = O

(3)

[A,E]=[E,A]=O\left[A, E\right] = \left[E, A\right] = O

(4)

[A,(B+C)]=[A,B]+[A,C]\left[A, (B + C)\right] = \left[A, B\right] + \left[A, C\right]

Prove that for any square matrices A,B,CA, B, C the following equalities hold:

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(a)

[A,BC]=[A,B]C+B[A,C][A, B C]=[A, B] C+B[A, C];

(b)

[[A,B],C]+[[B,C],A]+[[C,A],B]=0[[A, B], C]+[[B, C], A]+[[C, A], B]=0.

Prove that [[X,Y]2,Z]=0\left[[X, Y]^{2}, Z\right]=0 for any three matrices X,Y,Z∈M2(K)X, Y, Z \in M_{2}(\mathfrak {K}). Here [X,Y]=XY−YX[X, Y]=X Y-Y X is the commutator of the matrices X,YX, Y.

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(i)

Let AA, BB be n×nn \times n matrices. Show that

tr⁡((A+B)(A−B))≡tr⁡(A2)−tr⁡(B2). \operatorname {tr}((A+B)(A-B)) \equiv \operatorname {tr}(A^{2})-\operatorname {tr}(B^{2}).
(ii)

Let AA, BB, CC be n×nn \times n matrices. Show that tr⁡([A,B]C)=tr⁡(A[B,C])\operatorname {tr}([A,B]C) = \operatorname {tr}(A[B,C]).

Let AA, BB, HH be n×nn \times n matrices over C\mathbb {C} such that [A,H]=0n[A, H] = 0_n, [B,H]=0n[B, H] = 0_n. Find [[A,B],H][[A, B], H].

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(i)

Let AA, BB be n×nn \times n matrices over C\mathbb {C}. Let SS be an invertible n×nn \times n matrix over C\mathbb {C} with A~=S−1AS\widetilde{A} = S^{-1}AS, B~=S−1BS\widetilde{B} = S^{-1}BS. Show that [A~,B~]=S−1[A,B]S[\widetilde{A}, \widetilde{B}] = S^{-1}[A, B]S.

(ii)

Let AA, BB be n×nn \times n matrices over C\mathbb {C}. Assume that [A,B]=0n[A, B] = 0_n. Let UU be a unitary matrix. Calculate [U∗AU,U∗BU][U^{*}AU, U^{*}BU].

(iii)

Let TT be an invertible matrix. Show that T−1AT≡A+T−1[A,T]T^{-1}AT \equiv A + T^{-1}[A, T].

Let AA, BB be n×nn \times n matrices. Given the expression

A2B+AB2+B2A+BA2−2ABA−2BAB. A^{2}B + AB^{2} + B^{2}A + BA^{2} - 2ABA - 2BAB.

Write the expression in a more compact form using commutators.

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Let A1A_1, A2A_2, A3A_3 be n×nn \times n matrices over C\mathbb {C}. The ternary commutator [A1,A2,A3][A_1, A_2, A_3] (also called the ternutator) is defined as

[A1,A2,A3]:=∑π∈S3sign⁡(π)Aπ(1)Aπ(2)Aπ(3)≡A1A2A3+A2A3A1+A3A1A2−A1A3A2−A2A1A3−A3A2A1. [A_1, A_2, A_3] := \sum _{\pi \in S_3} \operatorname {sign}\left(\pi \right) A_{\pi (1)}A_{\pi (2)}A_{\pi (3)} \equiv A_1A_2A_3 + A_2A_3A_1 + A_3A_1A_2 - A_1A_3A_2 - A_2A_1A_3 - A_3A_2A_1.

Let n=2n = 2 and consider the Pauli spin matrices σ1\sigma_1, σ2\sigma_2, σ3\sigma_3. Calculate the ternutator [σ1,σ2,σ3][\sigma_1, \sigma_2, \sigma_3].

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Let AA, BB be n×nn \times n matrices over C\mathbb {C}. Assume that BB is invertible. Show that

[A,B−1]≡−B−1[A,B]B−1. [A, B^{-1}] \equiv -B^{-1}[A, B]B^{-1}.
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Let n≥1n \geq 1 and AA, BB be n×nn \times n matrices over C\mathbb {C}. Show that

[A,Bn]=∑j=0n−1Aj[A,B]Bn−1−j. [A, B^{n}] = \sum _{j=0}^{n-1} A^{j}[A, B]B^{n-1-j}.
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Let AA, BB be n×nn \times n matrices and TT a (fixed) invertible n×nn \times n matrix. We define the bracket

[A,B]T:=ATB−BTA. [A, B]_T := ATB - BTA.

Let

T=(0110),X=(0100),Y=(0010),H=(100−1). T = \begin{pmatrix} 0 & 1 \\ 1 & 0 \end{pmatrix}, \qquad X = \begin{pmatrix} 0 & 1 \\ 0 & 0 \end{pmatrix}, \qquad Y = \begin{pmatrix} 0 & 0 \\ 1 & 0 \end{pmatrix}, \qquad H = \begin{pmatrix} 1 & 0 \\ 0 & -1 \end{pmatrix}.

Find [X,Y]T[X, Y]_T, [X,H]T[X, H]_T, [Y,H]T[Y, H]_T.

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Let AA, BB, CC be n×nn \times n matrices. Show that

tr⁡([A,B]C)≡tr⁡(A[B,C]) \operatorname {tr}([A, B]C) \equiv \operatorname {tr}(A[B, C])

applying cyclic invariance.

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(i)

Let AA be an associative algebra over a field F\mathbb {F}. We define the commutator

[a,b]:=ab−ba [a,b] := ab - ba

for all a,b∈Aa, b \in A. Show that with this definition of the commutator we have a Lie algebra.

(ii)

Give an example.

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(i)

Let U,VU, V be n×nn \times n unitary matrices such that the commutator [U,V]=W[U,V] = W is again a unitary matrix, i.e. W∗=W−1W^{*} = W^{-1}. Show that

R+R−1=In R + R^{-1} = I_{n}

where R=U−1V−1UVR = U^{-1}V^{-1}UV is the group commutator of U−1U^{-1} and V−1V^{-1}.

(ii)

Give an example for such matrices U,VU, V for the case n=2n=2.

Let A1,A2,A3A_{1}, A_{2}, A_{3} be n×nn \times n matrices over C\mathbb {C}. The ternary commutator [A1,A2,A3][A_{1},A_{2},A_{3}] (also called the ternutator) is defined as

[A1,A2,A3]:=∑π∈S3sgn⁡(π)Aπ(1)Aπ(2)Aπ(3)≡A1A2A3+A2A3A1+A3A1A2−A1A3A2−A2A1A3−A3A2A1 . \begin{align} [A_{1},A_{2},A_{3}] & := \sum _{\pi \in S_{3}} \operatorname {sgn}(\pi ) A_{\pi (1)}A_{\pi (2)}A_{\pi (3)} \\ & \equiv A_{1}A_{2}A_{3} + A_{2}A_{3}A_{1} + A_{3}A_{1}A_{2} - A_{1}A_{3}A_{2} - A_{2}A_{1}A_{3} - A_{3}A_{2}A_{1} \, . \end{align}
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(i)

Let n=2n=2 and consider the Pauli spin matrices σx,σy,σz\sigma_{x}, \sigma_{y}, \sigma_{z}. Calculate the ternutator

[σx,σy,σz] . [\sigma _{x}, \sigma _{y}, \sigma _{z}] \, .
(ii)

Calculate

A1⊗A2⊗A3+A2⊗A3⊗A1+A3⊗A1⊗A2−A1⊗A3⊗A2−A2⊗A1⊗A3−A3⊗A2⊗A1 . A_{1}\otimes A_{2}\otimes A_{3} + A_{2}\otimes A_{3}\otimes A_{1} + A_{3}\otimes A_{1}\otimes A_{2} - A_{1}\otimes A_{3}\otimes A_{2} - A_{2}\otimes A_{1}\otimes A_{3} - A_{3}\otimes A_{2}\otimes A_{1} \, .

References

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[Кос15] Кострикин А.И. Сборник задач по алгебре. МЦНМО, 2015.
[Кос00] Кострикин А.И. Линейная алгебра. ФИЗМАТЛИТ, 2000.
[StHa17] Steeb W., Hardy Y. Problems and Solutions in Introductory and Advanced Matrix Calculus. 2nd ed., World Scientific Publishing, 2017.
[STH12] Steeb W., Tanski I., Hardy Y. Problems and Solutions for Groups, Lie Groups, Lie Algebras with Applications. World Scientific Publishing, 2012.