Alphabeta Math
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The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.

  • Literature-sourced — the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted — a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated — a genuinely novel statement formulated by AI, with no source for the claim itself.

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21 results · all verified · 0 also independently AI-judged
Every result on this page is machine-checked by a proof checker and read in full and owner-audited; the judge is an additional, independent cross-model AI review of the proofs. The 21 not AI-judged were verified by owner audit (typically over a confirmed judge false positive), not failures.

Matrices, the Matrix of a Linear Map, and Change of Basis

1 · Prerequisites

2 · Summary

Finite sums in the scalar field and the published matrix-space structure make row-by-column multiplication meaningful, including empty index sets. Linear maps, finite-dimensional vector spaces, ordered bases, and unique coordinates supply the coordinate language, while composition, kernels, images, and dimension provide the structural setting in which matrices represent maps.

Matrix multiplication first yields matrix rings, units, matrix units, transpose, and noncommutativity. Pointwise operations make linear maps a vector space, and ordered bases turn matrix representation into a vector-space and ring isomorphism that respects composition and invertibility. Change-of-basis matrices then give the two-sided transformation law and similarity. Finally trace is defined, proved cyclic on rectangular products, shown invariant under similarity, and transferred to endomorphisms independently of basis.

3 · Logical flowchart

4 · Definitions, theorems and proofs

DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-08-11Open item page →

Rectangular matrix multiplication and the identity matrix InI_n, including zero-sized shapes

Definition

Let FF be a field, let m,n,pNm,n,p\in\mathbb N, and let A=(aij)Mm×n(F)A=(a_{ij})\in M_{m\times n}(F) and B=(bjk)Mn×p(F)B=(b_{jk})\in M_{n\times p}(F). Their matrix product is the matrix ABMm×p(F)AB\in M_{m\times p}(F) whose entries are

(AB)ik:=jnaijbjk.(AB)_{ik}:=\sum_{j\in n}a_{ij}b_{jk}.

The sum is the finite sum in the additive commutative monoid of FF. If n=0n=0, it is the empty sum, so ABAB is the zero matrix of shape mm by pp.

The identity matrix InMn(F)I_n\in M_n(F) has entry 11 when i=ji=j and entry 00 when iji\ne j. In particular, I0I_0 is the unique empty matrix in M0(F)M_0(F).

TheoremStatement: Literature-sourcedProof: AI-generatedprecheck passaudited 2026-08-11Open item page →

Matrix multiplication is associative, unital, distributive, and compatible with scalar multiplication

Statement

Matrix multiplication over a field is associative and unital, distributes over entrywise addition on both sides, and is compatible with scalar multiplication. Precisely, whenever the displayed products have compatible shapes,

A(BC)=(AB)C,ImA=A=AIn,A(BC)=(AB)C,\qquad I_mA=A=AI_n,

(A+A)B=AB+AB,A(B+B)=AB+AB,(A+A')B=AB+A'B,\qquad A(B+B')=AB+AB',

0B=0=A0,(λA)B=λ(AB)=A(λB).0B=0=A0,\qquad (\lambda A)B=\lambda(AB)=A(\lambda B).

These identities include every zero-sized shape.

Facts & Assumptions

Given: A field FF; matrices AMm×n(F)A\in M_{m\times n}(F), BMn×p(F)B\in M_{n\times p}(F), and CMp×q(F)C\in M_{p\times q}(F); conformable matrices A,BA',B'; and a scalar λF\lambda\in F.

[L1]

Matrix products and identity matrices are defined entrywise by finite row-by-column sums (Rectangular matrix multiplication and the identity matrix InI_n, including zero-sized shapes).

Proof

technique · direct
1.1

For i<mi<m and <q\ell<q, expansion by [L1] gives ((AB)C)i=k<pj<n(aijbjk)ck((AB)C)_{i\ell}=\sum_{k<p}\sum_{j<n}(a_{ij}b_{jk})c_{k\ell} and (A(BC))i=j<nk<paij(bjkck)(A(BC))_{i\ell}=\sum_{j<n}\sum_{k<p}a_{ij}(b_{jk}c_{k\ell}).

givenL1
2.1

Associativity and distributivity in FF, followed by [L2], identify the two sums in step 1.1, so (AB)C=A(BC)(AB)C=A(BC).

step 1.1L1L2
3.1

The entry formulas also give (ImA)ik=aik=(AIn)ik(I_mA)_{ik}=a_{ik}=(AI_n)_{ik}; splitting sums gives both distributive laws; pulling out λ\lambda gives scalar compatibility; and a sum of zero summands gives each zero law. Thus all stated identities hold entrywise.

step 2.1L1
4.1

If any indexing dimension is zero, every asserted matrix equality either has no entries to compare or reduces to an empty sum, whose value is 00. Hence the same calculations cover all zero-sized shapes, including I0I_0.

step 3.1L1L2
CorollaryStatement: AI-adaptedProof: AI-generatedprecheck passaudited 2026-08-11Open item page →

Mn(F)M_n(F) is a ring under entrywise addition and matrix multiplication, including the zero ring M0(F)M_0(F)

Statement

For every field FF and natural nn, Mn(F)M_n(F) is a ring under entrywise addition and matrix multiplication, with zero matrix as additive identity and InI_n as multiplicative identity. For n=0n=0, this is the one-element zero ring M0(F)M_0(F).

Facts & Assumptions

Given: A field FF and a natural nn.

[L1]

Matrix multiplication is associative and unital and distributes over entrywise addition on both sides (Matrix multiplication is associative, unital, distributive, and compatible with scalar multiplication).

Proof

technique · direct
1.1

The published pointwise vector-space structure on Mn(F)M_n(F) makes entrywise addition an abelian group operation, with the zero matrix and entrywise negatives.

givenL1
2.1

By [L1], matrix multiplication is associative, has identity InI_n, and satisfies both distributive laws over that addition.

step 1.1L1
3.1

These are exactly the ring axioms. If n=0n=0, there is one empty matrix, so its zero and identity coincide; the ring convention permits 0=10=1, making M0(F)M_0(F) the zero ring.

step 2.1L1
DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-08-11Open item page →

Matrix units EijE_{ij} and the Kronecker delta

Definition

For indices a,ba,b in the same finite index set, the Kronecker delta is

δab:={1,a=b,0,ab.\delta_{ab}:=\begin{cases}1,&a=b,\\0,&a\ne b.\end{cases}

Let i<mi<m and j<nj<n. The matrix unit EijMm×n(F)E_{ij}\in M_{m\times n}(F) is the matrix whose (r,s)(r,s)-entry is

(Eij)rs:=δriδsj.(E_{ij})_{rs}:=\delta_{ri}\delta_{sj}.

Thus EijE_{ij} has entry 11 in position (i,j)(i,j) and entry 00 everywhere else. When a dimension is zero, no index of that dimension exists and there are no matrix units of the corresponding shape.

LemmaStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-08-11Open item page →

EijEk=δjkEiE_{ij}E_{k\ell}=\delta_{jk}E_{i\ell}

Statement

For EijMm×n(F)E_{ij}\in M_{m\times n}(F) and EkMn×p(F)E_{k\ell}\in M_{n\times p}(F),

EijEk=δjkEi.E_{ij}E_{k\ell}=\delta_{jk}E_{i\ell}.

Facts & Assumptions

Given: A field FF and indices i<mi<m, j,k<nj,k<n, and <p\ell<p.

[L1]

The matrix unit EijE_{ij} has entry δriδsj\delta_{ri}\delta_{sj} in position (r,s)(r,s) (Matrix units EijE_{ij} and the Kronecker delta).

Proof

technique · direct
1.1

For r<mr<m and s<ps<p, the product entry is (EijEk)rs=t<nδriδtjδtkδs(E_{ij}E_{k\ell})_{rs}=\sum_{t<n}\delta_{ri}\delta_{tj}\delta_{tk}\delta_{s\ell}.

givenL1
2.1

If jkj\ne k, every summand is zero. If j=kj=k, only t=jt=j can contribute and the value is δriδs\delta_{ri}\delta_{s\ell}.

step 1.1L1
3.1

The two cases combine as (EijEk)rs=δjk(Ei)rs(E_{ij}E_{k\ell})_{rs}=\delta_{jk}(E_{i\ell})_{rs} for every entry, proving the matrix identity.

step 2.1L1
CorollaryStatement: Literature-sourcedProof: AI-generatedprecheck passaudited 2026-08-11Open item page →

Mn(F)M_n(F) is noncommutative for every n2n\ge2

Statement

For every field FF and every natural n2n\ge2, the ring Mn(F)M_n(F) is not commutative.

Facts & Assumptions

Given: A field FF and a natural n2n\ge2.

[L1]

Matrix units satisfy EijEk=δjkEiE_{ij}E_{k\ell}=\delta_{jk}E_{i\ell} (EijEk=δjkEiE_{ij}E_{k\ell}=\delta_{jk}E_{i\ell}).

Proof

technique · direct
1.1

By [L1], E01E10=E00E_{01}E_{10}=E_{00} while E10E01=E11E_{10}E_{01}=E_{11}; these products differ at entry (0,0)(0,0) because 101\ne0 in a field.

givenL1
2.1

Thus two elements of Mn(F)M_n(F) fail to commute, so the matrix ring is noncommutative.

step 1.1L1
DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-08-11Open item page →

The transpose ATA^{\mathsf T} of a matrix

Definition

For A=(aij)Mm×n(F)A=(a_{ij})\in M_{m\times n}(F), the transpose of AA is the matrix ATMn×m(F)A^{\mathsf T}\in M_{n\times m}(F) defined by

(AT)ji:=aij.(A^{\mathsf T})_{ji}:=a_{ij}.

Thus transposition interchanges rows and columns. The transpose of a zero-sized matrix is the unique matrix of the transposed zero-sized shape.

PropositionStatement: Literature-sourcedProof: AI-generatedprecheck passaudited 2026-08-11Open item page →

Transpose is linear and involutive, and (AB)T=BTAT(AB)^{\mathsf T}=B^{\mathsf T}A^{\mathsf T}

Statement

For matrices of the appropriate shapes and a scalar λ\lambda,

(A+B)T=AT+BT,(λA)T=λAT,(AT)T=A,(A+B)^{\mathsf T}=A^{\mathsf T}+B^{\mathsf T},\qquad (\lambda A)^{\mathsf T}=\lambda A^{\mathsf T},\qquad (A^{\mathsf T})^{\mathsf T}=A,

and

(AB)T=BTAT.(AB)^{\mathsf T}=B^{\mathsf T}A^{\mathsf T}.

Thus transpose is linear and involutive and reverses products.

Facts & Assumptions

Given: A field FF, matrices A,BA,B of the same shape, conformable matrices A,CA,C, and a scalar λF\lambda\in F.

[L1]

Transposition swaps the two entry indices (The transpose ATA^{\mathsf T} of a matrix).

Proof

technique · direct
1.1

Swapping indices in the entrywise sum and scalar product gives the two linearity identities, and swapping twice gives (AT)T=A(A^{\mathsf T})^{\mathsf T}=A.

givenL1
2.1

For conformable AMm×n(F)A\in M_{m\times n}(F) and CMn×p(F)C\in M_{n\times p}(F), one has ((AC)T)ki=(AC)ik=j<naijcjk((AC)^{\mathsf T})_{ki}=(AC)_{ik}=\sum_{j<n}a_{ij}c_{jk}.

step 1.1L1
3.1

Commutativity in FF rewrites the sum in step 2.1 as j<n(CT)kj(AT)ji=(CTAT)ki\sum_{j<n}(C^{\mathsf T})_{kj}(A^{\mathsf T})_{ji}=(C^{\mathsf T}A^{\mathsf T})_{ki}, proving the product law entrywise.

step 2.1L1
DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-08-11Open item page →

The space L(V,W)\mathcal L(V,W) of linear maps with pointwise addition and scalar multiplication

Definition

Let VV and WW be vector spaces over the same field FF. Write

L(V,W):={T:VW:T is linear}.\mathcal L(V,W):=\{T:V\to W:T\text{ is linear}\}.

For S,TL(V,W)S,T\in\mathcal L(V,W) and λF\lambda\in F, define pointwise operations by

(S+T)(v):=S(v)+T(v),(λT)(v):=λT(v).(S+T)(v):=S(v)+T(v),\qquad (\lambda T)(v):=\lambda T(v).

The zero function v0Wv\mapsto0_W is denoted by 00. Closure and the vector-space axioms for these operations are proved in L(V,W)\mathcal L(V,W) is a vector space over the common scalar field .

PropositionStatement: Literature-sourcedProof: AI-generatedprecheck passaudited 2026-08-11Open item page →

L(V,W)\mathcal L(V,W) is a vector space over the common scalar field

Statement

If VV and WW are vector spaces over a field FF, then L(V,W)\mathcal L(V,W) is a vector space over FF under pointwise addition and scalar multiplication.

Facts & Assumptions

Given: Vector spaces V,WV,W over the same field FF and the pointwise operations on L(V,W)\mathcal L(V,W).

[L1]

L(V,W)\mathcal L(V,W) is the set of linear maps, with pointwise addition and scalar multiplication (The space L(V,W)\mathcal L(V,W) of linear maps with pointwise addition and scalar multiplication).

Proof

technique · direct
1.1

If S,TS,T are linear, then (S+T)(au+bv)=a(S+T)(u)+b(S+T)(v)(S+T)(au+bv)=a(S+T)(u)+b(S+T)(v), and if λF\lambda\in F, then (λT)(au+bv)=a(λT)(u)+b(λT)(v)(\lambda T)(au+bv)=a(\lambda T)(u)+b(\lambda T)(v); hence the pointwise operations remain inside L(V,W)\mathcal L(V,W).

givenL1
2.1

Evaluating at an arbitrary vVv\in V reduces associativity, commutativity, both distributive laws, scalar associativity, and the scalar identity law to the corresponding vector-space laws in WW.

step 1.1L1
3.1

The zero function is the additive identity and (T)(v):=T(v)(-T)(v):=-T(v) is the additive inverse of TT. The same formulas cover the zero domain and zero codomain, so all vector-space axioms hold.

step 2.1L1
DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-08-11Open item page →

Invertible linear maps, linear isomorphisms, and inverse linear maps

Definition

Let T:VWT:V\to W be linear. It is invertible when there is a linear map S:WVS:W\to V such that

ST=idV,TS=idW.S\circ T=\operatorname{id}_V,\qquad T\circ S=\operatorname{id}_W.

Such an SS is the inverse linear map of TT, denoted T1T^{-1}. The two inverse equations make TT bijective and determine T1T^{-1} uniquely. An invertible linear map is also called a linear isomorphism, and VV and WW are linearly isomorphic, written VWV\cong W, when such a map exists.

LemmaStatement: Literature-sourcedProof: AI-generatedprecheck passaudited 2026-08-11Open item page →

Identity maps and composites of linear maps are linear

Statement

The identity map of a vector space is linear. If T:UVT:U\to V and S:VWS:V\to W are linear maps over the same field, then ST:UWS\circ T:U\to W is linear.

Facts & Assumptions

Given: Vector spaces U,V,WU,V,W over a field FF, scalars a,bFa,b\in F, vectors u,vUu,v\in U, and linear maps T:UVT:U\to V and S:VWS:V\to W.

[L1]

A map RR is linear when R(au+bv)=aR(u)+bR(v)R(au+bv)=aR(u)+bR(v) for all scalars and vectors (Linear map between vector spaces over the same field).

Proof

technique · direct
1.1

The identity satisfies idV(av+bw)=av+bw=aidV(v)+bidV(w)\operatorname{id}_V(av+bw)=av+bw=a\operatorname{id}_V(v)+b\operatorname{id}_V(w), so it is linear.

givenL1
2.1

Linearity of TT and then of SS gives S(T(au+bv))=S(aT(u)+bT(v))=aS(T(u))+bS(T(v))S(T(au+bv))=S(aT(u)+bT(v))=aS(T(u))+bS(T(v)).

step 1.1L1
3.1

The equality in step 2.1 is the defining linearity equation for STS\circ T, so the composite is linear.

step 2.1L1
DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-08-11Open item page →

Coordinate columns [v]B[v]_{\mathcal B} and matrices [T]BC[T]_{\mathcal B}^{\mathcal C} of linear maps relative to ordered bases

Definition

Let B=(b0,,bn1)\mathcal B=(b_0,\ldots,b_{n-1}) be an ordered basis of VV. The unique coordinates v=j<nxjbjv=\sum_{j<n}x_jb_j form the coordinate column [v]BMn×1(F)[v]_{\mathcal B}\in M_{n\times1}(F), whose jj-th entry is xjx_j.

Let C=(c0,,cm1)\mathcal C=(c_0,\ldots,c_{m-1}) be an ordered basis of WW and let T:VWT:V\to W be linear. The matrix of TT relative to B\mathcal B and C\mathcal C is the matrix [T]BCMm×n(F)[T]_{\mathcal B}^{\mathcal C}\in M_{m\times n}(F) whose jj-th column is [T(bj)]C[T(b_j)]_{\mathcal C}. Equivalently, if T(bj)=i<mtijciT(b_j)=\sum_{i<m}t_{ij}c_i, then ([T]BC)ij=tij([T]_{\mathcal B}^{\mathcal C})_{ij}=t_{ij}.

For an empty ordered basis, these definitions give the unique coordinate column or matrix of the corresponding zero-sized shape.

TheoremStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-08-11Open item page →

[T(v)]C=[T]BC[v]B[T(v)]_{\mathcal C}=[T]_{\mathcal B}^{\mathcal C}[v]_{\mathcal B}

Statement

Let T:VWT:V\to W be linear, let B\mathcal B be an ordered basis of VV, and let C\mathcal C be an ordered basis of WW. Then for every vVv\in V,

[T(v)]C=[T]BC[v]B.[T(v)]_{\mathcal C}=[T]_{\mathcal B}^{\mathcal C}[v]_{\mathcal B}.

Facts & Assumptions

Given: Ordered bases B=(bj)j<n\mathcal B=(b_j)_{j<n} and C=(ci)i<m\mathcal C=(c_i)_{i<m}, a linear map T:VWT:V\to W, and a vector vVv\in V.

[L1]

The coordinate column contains the unique coefficients in the ordered-basis expansion, and the jj-th column of [T]BC[T]_{\mathcal B}^{\mathcal C} is [T(bj)]C[T(b_j)]_{\mathcal C} (Coordinate columns [v]B[v]_{\mathcal B} and matrices [T]BC[T]_{\mathcal B}^{\mathcal C} of linear maps relative to ordered bases).

Proof

technique · direct
1.1

Write [v]B=(xj)j<n[v]_{\mathcal B}=(x_j)_{j<n}, so [L1] gives v=j<nxjbjv=\sum_{j<n}x_jb_j.

givenL1
2.1

By linearity, T(v)=j<nxjT(bj)T(v)=\sum_{j<n}x_jT(b_j); writing T(bj)=i<mtijciT(b_j)=\sum_{i<m}t_{ij}c_i gives T(v)=i<m(j<ntijxj)ciT(v)=\sum_{i<m}(\sum_{j<n}t_{ij}x_j)c_i.

step 1.1L1
3.1

The inner sum is the ii-th row-by-column entry of [T]BC[v]B[T]_{\mathcal B}^{\mathcal C}[v]_{\mathcal B}, and uniqueness of C\mathcal C-coordinates identifies this column with [T(v)]C[T(v)]_{\mathcal C}.

step 2.1L1
TheoremStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-08-11Open item page →

T[T]BCT\mapsto[T]_{\mathcal B}^{\mathcal C} is a vector-space isomorphism L(V,W)Mm×n(F)\mathcal L(V,W)\cong M_{m\times n}(F)

Statement

Let V,WV,W be finite-dimensional vector spaces over FF, with ordered bases B=(bj)j<n\mathcal B=(b_j)_{j<n} and C=(ci)i<m\mathcal C=(c_i)_{i<m}. The map

Φ:L(V,W)Mm×n(F),Φ(T)=[T]BC,\Phi:\mathcal L(V,W)\to M_{m\times n}(F),\qquad \Phi(T)=[T]_{\mathcal B}^{\mathcal C},

is a vector-space isomorphism.

Facts & Assumptions

Given: The finite-dimensional spaces and ordered bases in the Statement.

[L1]

L(V,W)\mathcal L(V,W) is a vector space under pointwise operations (L(V,W)\mathcal L(V,W) is a vector space over the common scalar field).

[L3]

A linear isomorphism is a linear map with a two-sided linear inverse (Invertible linear maps, linear isomorphisms, and inverse linear maps).

Proof

technique · direct
1.1

For every basis vector bjb_j, coordinate uniqueness in [L2] gives [(S+T)(bj)]C=[S(bj)]C+[T(bj)]C[(S+T)(b_j)]_{\mathcal C}=[S(b_j)]_{\mathcal C}+[T(b_j)]_{\mathcal C} and [(λT)(bj)]C=λ[T(bj)]C[(\lambda T)(b_j)]_{\mathcal C}=\lambda[T(b_j)]_{\mathcal C}, so Φ\Phi is linear column by column.

givenL1L2
2.1

If Φ(S)=Φ(T)\Phi(S)=\Phi(T), then [L2] gives S(bj)=T(bj)S(b_j)=T(b_j) for every jj; linearity and the unique expansion of every vector in B\mathcal B give S=TS=T, so Φ\Phi is injective.

step 1.1L1L2
3.1

Given A=(aij)Mm×n(F)A=(a_{ij})\in M_{m\times n}(F), prescribe T(bj):=i<maijciT(b_j):=\sum_{i<m}a_{ij}c_i and, for the unique expansion v=j<nxjbjv=\sum_{j<n}x_jb_j from [L2], define T(v):=j<nxjT(bj)T(v):=\sum_{j<n}x_jT(b_j). This is well defined and linear, and the jj-th matrix column is the jj-th column of AA; hence Φ(T)=A\Phi(T)=A. Together with steps 1.1 and 2.1, Φ\Phi is a linear bijection. Its set-theoretic inverse is linear: if A=Φ(S)A=\Phi(S) and B=Φ(T)B=\Phi(T), then injectivity and linearity give Φ1(A+B)=S+T\Phi^{-1}(A+B)=S+T and Φ1(λA)=λS\Phi^{-1}(\lambda A)=\lambda S. Thus Φ\Phi is a linear isomorphism by [L3].

step 1.1step 2.1L1L2L3
4.1

If n=0n=0, then VV is the zero space and both sides contain only their zero element; if m=0m=0, then WW and Mm×n(F)M_{m\times n}(F) are zero spaces and the only map is the zero map. Thus the construction also proves the isomorphism in every zero-dimensional case.

step 3.1L1L2L3
CorollaryStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-08-11Open item page →

dimFMm×n(F)=mn\dim_F M_{m\times n}(F)=mn and dimFL(V,W)=(dimFV)(dimFW)\dim_F\mathcal L(V,W)=(\dim_FV)(\dim_FW) for finite-dimensional V,WV,W

Statement

For a field FF and naturals m,nm,n, dimFMm×n(F)=mn\dim_FM_{m\times n}(F)=mn. Consequently, for finite-dimensional FF-vector spaces V,WV,W,

dimFL(V,W)=(dimFV)(dimFW).\dim_F\mathcal L(V,W)=(\dim_FV)(\dim_FW).

Facts & Assumptions

Given: A field FF, naturals m,nm,n, and finite-dimensional spaces V,WV,W with dimFV=n\dim_FV=n and dimFW=m\dim_FW=m.

[L1]

The matrix units EijE_{ij} have one entry equal to 11 and all other entries equal to 00 (Matrix units EijE_{ij} and the Kronecker delta).

[L3]

Relative to ordered bases, matrix representation is a vector-space isomorphism L(V,W)Mm×n(F)\mathcal L(V,W)\cong M_{m\times n}(F) (T[T]BCT\mapsto[T]_{\mathcal B}^{\mathcal C} is a vector-space isomorphism L(V,W)Mm×n(F)\mathcal L(V,W)\cong M_{m\times n}(F)).

Proof

technique · direct
1.1

Every matrix A=(aij)A=(a_{ij}) has the expansion A=(i,j)m×naijEijA=\sum_{(i,j)\in m\times n}a_{ij}E_{ij}, and a linear relation among the EijE_{ij} has each coefficient zero when its corresponding entry is read. Thus the matrix units form a basis.

givenL1
2.1

By [L2], the index set m×nm\times n has cardinality mnmn, so this basis has mnmn elements; if either dimension is zero, it is the empty basis of the zero matrix space. Hence dimFMm×n(F)=mn\dim_FM_{m\times n}(F)=mn.

step 1.1L1L2
3.1

The isomorphism in [L3] transports a basis and preserves dimension; substituting n=dimFVn=\dim_FV and m=dimFWm=\dim_FW gives the second formula.

step 2.1L3
TheoremStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-08-11Open item page →

[ST]BD=[S]CD[T]BC[S\circ T]_{\mathcal B}^{\mathcal D}=[S]_{\mathcal C}^{\mathcal D}[T]_{\mathcal B}^{\mathcal C}

Statement

Let T:UVT:U\to V and S:VWS:V\to W be linear, with ordered bases B\mathcal B of UU, C\mathcal C of VV, and D\mathcal D of WW. Then

[ST]BD=[S]CD[T]BC.[S\circ T]_{\mathcal B}^{\mathcal D}=[S]_{\mathcal C}^{\mathcal D}[T]_{\mathcal B}^{\mathcal C}.

Facts & Assumptions

Given: The composable linear maps and ordered bases in the Statement, and a vector uUu\in U.

[L1]

A composite of linear maps is linear (Identity maps and composites of linear maps are linear).

[L2]

Coordinate action gives [R(x)]Y=[R]XY[x]X[R(x)]_{\mathcal Y}=[R]_{\mathcal X}^{\mathcal Y}[x]_{\mathcal X} ([T(v)]C=[T]BC[v]B[T(v)]_{\mathcal C}=[T]_{\mathcal B}^{\mathcal C}[v]_{\mathcal B}).

[L3]

Matrix multiplication is associative whenever the shapes are compatible (Matrix multiplication is associative, unital, distributive, and compatible with scalar multiplication).

Proof

technique · direct
1.1

Apply [L2] to TT and then to SS: [S(T(u))]D=[S]CD[T(u)]C=[S]CD[T]BC[u]B[S(T(u))]_{\mathcal D}=[S]_{\mathcal C}^{\mathcal D}[T(u)]_{\mathcal C}=[S]_{\mathcal C}^{\mathcal D}[T]_{\mathcal B}^{\mathcal C}[u]_{\mathcal B}.

givenL1L2
2.1

Associativity from [L3] rewrites step 1.1 as [S(T(u))]D=([S]CD[T]BC)[u]B[S(T(u))]_{\mathcal D}=([S]_{\mathcal C}^{\mathcal D}[T]_{\mathcal B}^{\mathcal C})[u]_{\mathcal B} for every uu.

step 1.1L2L3
3.1

Evaluating at each vector of B\mathcal B makes [u]B[u]_{\mathcal B} a standard coordinate column, so the columns of [ST]BD[S\circ T]_{\mathcal B}^{\mathcal D} equal those of the displayed product. Therefore the matrices are equal.

step 2.1L1L2L3
CorollaryStatement: AI-adaptedProof: AI-generatedprecheck passaudited 2026-08-11Open item page →

EndF(V)\operatorname{End}_F(V) is a ring and matrix representation is a ring isomorphism EndF(V)Mn(F)\operatorname{End}_F(V)\cong M_n(F)

Statement

Let VV be an nn-dimensional vector space over FF. Then EndF(V):=L(V,V)\operatorname{End}_F(V):=\mathcal L(V,V) is a ring under pointwise addition and composition, and for every ordered basis B\mathcal B the map

T[T]BBT\longmapsto[T]_{\mathcal B}^{\mathcal B}

is a ring isomorphism EndF(V)Mn(F)\operatorname{End}_F(V)\cong M_n(F).

Facts & Assumptions

Given: A finite-dimensional FF-vector space VV and an ordered basis B\mathcal B of length nn.

[L1]

L(V,V)\mathcal L(V,V) is a vector space under pointwise operations (L(V,W)\mathcal L(V,W) is a vector space over the common scalar field).

Proof

technique · direct
1.1

Composition of endomorphisms is associative, has idV\operatorname{id}_V as identity, and distributes over pointwise addition; together with the additive group from [L1], this makes EndF(V)\operatorname{End}_F(V) a ring.

givenL1
2.1

By [L2], matrix representation is a bijective linear map, so it preserves addition and zero.

step 1.1L1L2
3.1

It preserves products by the composition formula in [L2], and [idV]BB=In[\operatorname{id}_V]_{\mathcal B}^{\mathcal B}=I_n by coordinate action. Thus it is a bijective unital ring homomorphism and hence a ring isomorphism.

step 2.1L2
DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-08-11Open item page →

Invertible matrices and the general linear group GLn(F)\operatorname{GL}_n(F)

Definition

A matrix AMn(F)A\in M_n(F) is invertible when there is a matrix BMn(F)B\in M_n(F) such that

AB=In=BA.AB=I_n=BA.

Such a BB is unique and is denoted A1A^{-1}. The general linear set is

GLn(F):={AMn(F):A is invertible}.\operatorname{GL}_n(F):=\{A\in M_n(F):A\text{ is invertible}\}.

It is the set of units of the ring Mn(F)M_n(F). The fact that it is a group under matrix multiplication is GLn(F)\operatorname{GL}_n(F) is a group under matrix multiplication, including the trivial group GL0(F)\operatorname{GL}_0(F) . For n=0n=0, the unique empty matrix is I0I_0 and is its own inverse.

TheoremStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-08-11Open item page →

A square matrix is invertible exactly when its multiplication map is a linear isomorphism; matrices preserve inverses of linear isomorphisms

Statement

For AMn(F)A\in M_n(F), let LA:Mn×1(F)Mn×1(F)L_A:M_{n\times1}(F)\to M_{n\times1}(F) be LA(x)=AxL_A(x)=Ax. Then AA is invertible if and only if LAL_A is a linear isomorphism.

More generally, if T:VWT:V\to W is a linear isomorphism between finite-dimensional spaces and B,C\mathcal B,\mathcal C are ordered bases, then [T]BC[T]_{\mathcal B}^{\mathcal C} is invertible and

[T1]CB=([T]BC)1.[T^{-1}]_{\mathcal C}^{\mathcal B}=([T]_{\mathcal B}^{\mathcal C})^{-1}.

Facts & Assumptions

Given: A field FF, a natural nn, and the matrix multiplication map LAL_A; for the general claim, an isomorphism TT and ordered bases B,C\mathcal B,\mathcal C.

[L1]

An invertible matrix has a two-sided matrix inverse, and a linear isomorphism has a two-sided linear inverse (Invertible matrices and the general linear group GLn(F)\operatorname{GL}_n(F), Invertible linear maps, linear isomorphisms, and inverse linear maps).

[L3]

Matrix multiplication distributes over addition and is compatible with scalar multiplication (Matrix multiplication is associative, unital, distributive, and compatible with scalar multiplication).

[L5]

The dimension of a finite-dimensional vector space is the common size of its finite bases (Finite-dimensional vector space, and its dimension dimFV\dim_F V; infinite-dimensional means having no finite basis).

Proof

technique · direct
1.1

By [L3], LAL_A and LBL_B are linear. If AB=BA=InAB=BA=I_n, then LALB=LAB=idL_AL_B=L_{AB}=\operatorname{id} and LBLA=LBA=idL_BL_A=L_{BA}=\operatorname{id}, so LAL_A is a linear isomorphism with inverse LBL_B. This includes n=0n=0, where the unique empty matrix and the unique zero-space map are their own inverses.

givenL1L3
2.1

Conversely, if LAL_A has a linear inverse SS, [L4] represents SS by a matrix BB in the standard coordinate basis. The two identity composites and [L2] give AB=In=BAAB=I_n=BA, so AA is invertible.

step 1.1L1L2L4
3.1

For a general linear isomorphism TT, the list T(B)T(\mathcal B) is an ordered basis of WW: T1T^{-1} transfers both linear independence and spanning back to B\mathcal B. Hence [L5] shows that B\mathcal B and C\mathcal C have the same length, so the two displayed representation matrices are square. Representing T1TT^{-1}\circ T and TT1T\circ T^{-1} in the chosen bases, [L2] gives both inverse equations for [T]BC[T]_{\mathcal B}^{\mathcal C} and [T1]CB[T^{-1}]_{\mathcal C}^{\mathcal B}.

step 2.1L1L2L5
CorollaryStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-08-11Open item page →

Two finite-dimensional vector spaces over FF are linearly isomorphic if and only if they have the same dimension

Statement

Two finite-dimensional vector spaces over the same field FF are linearly isomorphic if and only if they have the same dimension.

Facts & Assumptions

Given: Finite-dimensional FF-vector spaces V,WV,W.

Proof

technique · direct
1.1

If T:VWT:V\to W is an isomorphism and (bj)j<n(b_j)_{j<n} is a basis of VV, then (T(bj))j<n(T(b_j))_{j<n} is independent because applying T1T^{-1} to a vanishing linear combination makes every coefficient zero, and it spans because every ww equals T(v)T(v) and vv expands in the bjb_j. Thus it is a basis of WW, so the dimensions agree.

givenL1
2.1

Conversely, if the dimensions agree, choose ordered bases (bj)j<n(b_j)_{j<n} of VV and (cj)j<n(c_j)_{j<n} of WW and define T(jxjbj)=jxjcjT(\sum_jx_jb_j)=\sum_jx_jc_j. Unique coordinates make this a linear map with T(bj)=cjT(b_j)=c_j.

step 1.1L1
3.1

Defining S(jyjcj)=jyjbjS(\sum_jy_jc_j)=\sum_jy_jb_j gives a linear inverse to TT. For n=0n=0, both bases are empty and both spaces are zero, so the same formulas give the unique isomorphism.

step 2.1L1
CorollaryStatement: Literature-sourcedProof: AI-generatedprecheck passaudited 2026-08-11Open item page →

GLn(F)\operatorname{GL}_n(F) is a group under matrix multiplication, including the trivial group GL0(F)\operatorname{GL}_0(F)

Statement

For every field FF and natural nn, GLn(F)\operatorname{GL}_n(F) is a group under matrix multiplication. For n=0n=0, it is the trivial group containing the unique empty matrix.

Facts & Assumptions

Given: A field FF and a natural nn.

[L1]

GLn(F)\operatorname{GL}_n(F) is the set of invertible matrices, equivalently the units of Mn(F)M_n(F) (Invertible matrices and the general linear group GLn(F)\operatorname{GL}_n(F)).

Proof

technique · direct
1.1

By [L1], GLn(F)\operatorname{GL}_n(F) is exactly the unit set of the ring Mn(F)M_n(F).

givenL1
2.1

Applying [L2] gives closure, associativity inherited from the ring, identity InI_n, and inverse A1A^{-1} for every element, so GLn(F)\operatorname{GL}_n(F) is a group.

step 1.1L1L2
3.1

If n=0n=0, M0(F)M_0(F) has one element, the empty matrix I0I_0, which is its own inverse; hence its unit group is the trivial group.

step 2.1L1L2
DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-08-11Open item page →

The change-of-basis matrix PCB=[idV]BCP_{\mathcal C\leftarrow\mathcal B}=[\operatorname{id}_V]_{\mathcal B}^{\mathcal C}

Definition

Let B\mathcal B and C\mathcal C be ordered bases of the same finite-dimensional vector space VV. The change-of-basis matrix from B\mathcal B-coordinates to C\mathcal C-coordinates is

PCB:=[idV]BC.P_{\mathcal C\leftarrow\mathcal B}:=[\operatorname{id}_V]_{\mathcal B}^{\mathcal C}.

Its jj-th column is [bj]C[b_j]_{\mathcal C}. The arrow records the direction in which coordinate columns are converted.

TheoremStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-08-11Open item page →

[v]C=PCB[v]B[v]_{\mathcal C}=P_{\mathcal C\leftarrow\mathcal B}[v]_{\mathcal B} and PBC=PCB1P_{\mathcal B\leftarrow\mathcal C}=P_{\mathcal C\leftarrow\mathcal B}^{-1}

Statement

For ordered bases B,C\mathcal B,\mathcal C of a finite-dimensional vector space VV and every vVv\in V,

[v]C=PCB[v]B.[v]_{\mathcal C}=P_{\mathcal C\leftarrow\mathcal B}[v]_{\mathcal B}.

Moreover,

PBC=PCB1.P_{\mathcal B\leftarrow\mathcal C}=P_{\mathcal C\leftarrow\mathcal B}^{-1}.

Facts & Assumptions

Given: Ordered bases B,C\mathcal B,\mathcal C of VV and a vector vVv\in V.

[L1]

PCBP_{\mathcal C\leftarrow\mathcal B} is the matrix of idV\operatorname{id}_V from B\mathcal B-coordinates to C\mathcal C-coordinates (The change-of-basis matrix PCB=[idV]BCP_{\mathcal C\leftarrow\mathcal B}=[\operatorname{id}_V]_{\mathcal B}^{\mathcal C}).

Proof

technique · direct
1.1

Applying coordinate action from [L2] to idV\operatorname{id}_V and using [L1] gives [v]C=PCB[v]B[v]_{\mathcal C}=P_{\mathcal C\leftarrow\mathcal B}[v]_{\mathcal B}.

givenL1L2
2.1

Represent the identity composition idVidV\operatorname{id}_V\circ\operatorname{id}_V first from B\mathcal B through C\mathcal C back to B\mathcal B, and then from C\mathcal C through B\mathcal B back to C\mathcal C.

step 1.1L1L2
3.1

The composite-matrix formula in [L2] gives PBCPCB=IP_{\mathcal B\leftarrow\mathcal C}P_{\mathcal C\leftarrow\mathcal B}=I and PCBPBC=IP_{\mathcal C\leftarrow\mathcal B}P_{\mathcal B\leftarrow\mathcal C}=I, so the two matrices are inverses. Empty ordered bases give the same two equations in M0(F)M_0(F).

step 2.1L1L2
TheoremStatement: AI-adaptedProof: AI-adaptedprecheck passaudited 2026-08-11Open item page →

[T]BC=PCC[T]BCPBB[T]_{\mathcal B'}^{\mathcal C'}=P_{\mathcal C'\leftarrow\mathcal C}[T]_{\mathcal B}^{\mathcal C}P_{\mathcal B\leftarrow\mathcal B'}

Statement

Let T:VWT:V\to W be linear. If B,B\mathcal B,\mathcal B' are ordered bases of VV and C,C\mathcal C,\mathcal C' are ordered bases of WW, then

[T]BC=PCC[T]BCPBB.[T]_{\mathcal B'}^{\mathcal C'}=P_{\mathcal C'\leftarrow\mathcal C}[T]_{\mathcal B}^{\mathcal C}P_{\mathcal B\leftarrow\mathcal B'}.

Facts & Assumptions

Given: The linear map and four ordered bases in the Statement.

[L1]

PYXP_{\mathcal Y\leftarrow\mathcal X} is the matrix of the identity map converting X\mathcal X-coordinates to Y\mathcal Y-coordinates (The change-of-basis matrix PCB=[idV]BCP_{\mathcal C\leftarrow\mathcal B}=[\operatorname{id}_V]_{\mathcal B}^{\mathcal C}).

[L2]

Matrix representation sends a composite of linear maps to the product of their matrices in compatible intermediate bases ([ST]BD=[S]CD[T]BC[S\circ T]_{\mathcal B}^{\mathcal D}=[S]_{\mathcal C}^{\mathcal D}[T]_{\mathcal B}^{\mathcal C}).

Proof

technique · direct
1.1

Regard TT from B\mathcal B' to C\mathcal C' as the composite of the identity on VV from B\mathcal B' to B\mathcal B, then TT from B\mathcal B to C\mathcal C, then the identity on WW from C\mathcal C to C\mathcal C'.

givenL1
2.1

Applying [L2] twice, with the matrix of the last-applied map on the left, gives [T]BC=PCC[T]BCPBB.[T]_{\mathcal B'}^{\mathcal C'}=P_{\mathcal C'\leftarrow\mathcal C}[T]_{\mathcal B}^{\mathcal C}P_{\mathcal B\leftarrow\mathcal B'}.

step 1.1L1L2
3.1

The right factor is square of size dimV\dim V, the middle factor has shape (dimW)×(dimV)(\dim W)\times(\dim V), and the left factor is square of size dimW\dim W, so the product is defined and has the asserted shape, proving the formula.

step 2.1L1L2
DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-08-11Open item page →

Similar matrices: B=P1APB=P^{-1}AP for an invertible PP

Definition

Two matrices A,BMn(F)A,B\in M_n(F) are similar when there is an invertible matrix PGLn(F)P\in\operatorname{GL}_n(F) such that

B=P1AP.B=P^{-1}AP.

The matrix PP is a change-of-basis matrix or conjugating matrix for this similarity. Replacing PP by its inverse exchanges the roles of AA and BB.

TheoremStatement: AI-adaptedProof: AI-generatedprecheck passaudited 2026-08-11Open item page →

Similarity is an equivalence relation, and two matrices represent the same endomorphism in two bases exactly when they are similar

Statement

Similarity is an equivalence relation on Mn(F)M_n(F). Moreover, matrices A,BMn(F)A,B\in M_n(F) are similar if and only if there are an nn-dimensional FF-vector space VV, an endomorphism T:VVT:V\to V, and ordered bases B,C\mathcal B,\mathcal C such that A=[T]BBA=[T]_{\mathcal B}^{\mathcal B} and B=[T]CCB=[T]_{\mathcal C}^{\mathcal C}.

Facts & Assumptions

Given: A field FF, a natural nn, and matrices A,B,CMn(F)A,B,C\in M_n(F).

[L1]

AA and BB are similar when B=P1APB=P^{-1}AP for some invertible PP (Similar matrices: B=P1APB=P^{-1}AP for an invertible PP).

[L3]

The matrices Ei0E_{i0} are the standard coordinate columns in Mn×1(F)M_{n\times1}(F) (Matrix units EijE_{ij} and the Kronecker delta).

[L4]

Matrix multiplication is associative, unital, distributive, and compatible with scalar multiplication (Matrix multiplication is associative, unital, distributive, and compatible with scalar multiplication).

[L5]

A finite ordered list is an ordered basis exactly when it is linearly independent and spans the space (Basis of a vector space: a linearly independent spanning subset; and ordered basis: an injective finite list whose image is a basis).

Proof

technique · direct
1.1

Taking P=InP=I_n proves reflexivity. If B=P1APB=P^{-1}AP, then A=(P1)1BP1A=(P^{-1})^{-1}BP^{-1}, proving symmetry. If also C=Q1BQC=Q^{-1}BQ, then associativity in [L4] gives C=(PQ)1A(PQ)C=(PQ)^{-1}A(PQ), proving transitivity. Thus similarity is an equivalence relation.

givenL1L4
2.1

If AA and BB represent the same endomorphism in bases B\mathcal B and C\mathcal C, [L2] gives B=P1APB=P^{-1}AP with P=PBCP=P_{\mathcal B\leftarrow\mathcal C}, so they are similar.

step 1.1L1L2
3.1

Conversely, suppose B=P1APB=P^{-1}AP. On V=Mn×1(F)V=M_{n\times1}(F) let T=LAT=L_A, which is linear by [L4], and let E=(Ei0)i<n\mathcal E=(E_{i0})_{i<n}. By [L3], every column yy has the unique expansion y=i<nyiEi0y=\sum_{i<n}y_iE_{i0}, so [L5] makes E\mathcal E the standard ordered basis. The columns of invertible PP form an ordered basis C\mathcal C: independence follows by multiplying Px=0Px=0 by P1P^{-1}, and every column vector yy equals P(P1y)P(P^{-1}y), so [L5] applies. Moreover, [T]EE=A[T]_{\mathcal E}^{\mathcal E}=A because T(Ej0)T(E_{j0}) is the jj-th column of AA. The change matrix PECP_{\mathcal E\leftarrow\mathcal C} is PP, so [L2] gives [T]CC=P1AP=B[T]_{\mathcal C}^{\mathcal C}=P^{-1}AP=B.

step 2.1L1L2L3L4L5
4.1

Steps 2.1 and 3.1 prove both directions of the characterisation, including n=0n=0, where the unique empty matrix represents the unique endomorphism of the zero space.

step 2.1step 3.1L1L2L3L4L5
DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-08-11Open item page →

The trace tr(A)\operatorname{tr}(A) as the sum of the diagonal entries

Definition

For a square matrix A=(aij)Mn(F)A=(a_{ij})\in M_n(F), its trace is the sum of its diagonal entries,

tr(A):=inaii.\operatorname{tr}(A):=\sum_{i\in n}a_{ii}.

For n=0n=0, this is the empty sum, so the unique empty matrix has trace 00.

PropositionStatement: Literature-sourcedProof: AI-generatedprecheck passaudited 2026-08-11Open item page →

Trace is a linear functional on Mn(F)M_n(F)

Statement

For every natural nn, the map tr:Mn(F)F\operatorname{tr}:M_n(F)\to F is linear:

tr(A+B)=tr(A)+tr(B),tr(λA)=λtr(A).\operatorname{tr}(A+B)=\operatorname{tr}(A)+\operatorname{tr}(B),\qquad \operatorname{tr}(\lambda A)=\lambda\operatorname{tr}(A).

Facts & Assumptions

Given: Matrices A,BMn(F)A,B\in M_n(F) and a scalar λF\lambda\in F.

[L1]

The trace is the finite sum of the diagonal entries (The trace tr(A)\operatorname{tr}(A) as the sum of the diagonal entries).

Proof

technique · direct
1.1

Entrywise addition and the finite-sum law give tr(A+B)=i<n(aii+bii)=i<naii+i<nbii=tr(A)+tr(B)\operatorname{tr}(A+B)=\sum_{i<n}(a_{ii}+b_{ii})=\sum_{i<n}a_{ii}+\sum_{i<n}b_{ii}=\operatorname{tr}(A)+\operatorname{tr}(B).

givenL1
2.1

Likewise, tr(λA)=i<nλaii=λi<naii=λtr(A)\operatorname{tr}(\lambda A)=\sum_{i<n}\lambda a_{ii}=\lambda\sum_{i<n}a_{ii}=\lambda\operatorname{tr}(A).

step 1.1L1
3.1

If n=0n=0, every displayed sum is empty and has value 00, so trace is the zero linear functional on the zero matrix space.

step 2.1L1
TheoremStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-08-11Open item page →

For AMm×n(F)A\in M_{m\times n}(F) and BMn×m(F)B\in M_{n\times m}(F), tr(AB)=tr(BA)\operatorname{tr}(AB)=\operatorname{tr}(BA)

Statement

For AMm×n(F)A\in M_{m\times n}(F) and BMn×m(F)B\in M_{n\times m}(F),

tr(AB)=tr(BA).\operatorname{tr}(AB)=\operatorname{tr}(BA).

The two products may have different sizes, and the equality includes m=0m=0 or n=0n=0.

Facts & Assumptions

Given: A field FF and the rectangular matrices in the Statement.

Proof

technique · direct
1.1

Expanding by [L1] gives tr(AB)=i<mj<naijbji\operatorname{tr}(AB)=\sum_{i<m}\sum_{j<n}a_{ij}b_{ji}.

givenL1
2.1

By [L2] and commutativity of multiplication in FF, this equals j<ni<mbjiaij\sum_{j<n}\sum_{i<m}b_{ji}a_{ij}.

step 1.1L1L2
3.1

The final double sum is tr(BA)\operatorname{tr}(BA) by [L1]. If m=0m=0 or n=0n=0, both sides are empty double sums and equal 00.

step 2.1L1L2
CorollaryStatement: Literature-sourcedProof: AI-adaptedprecheck passaudited 2026-08-11Open item page →

Similar matrices have the same trace

Statement

If square matrices AA and BB over FF are similar, then tr(A)=tr(B)\operatorname{tr}(A)=\operatorname{tr}(B).

Facts & Assumptions

Given: Similar matrices A,BMn(F)A,B\in M_n(F).

[L1]

Similarity means B=P1APB=P^{-1}AP for an invertible matrix PP (Similar matrices: B=P1APB=P^{-1}AP for an invertible PP).

[L2]

For conformable rectangular matrices X,YX,Y, one has tr(XY)=tr(YX)\operatorname{tr}(XY)=\operatorname{tr}(YX) (For AMm×n(F)A\in M_{m\times n}(F) and BMn×m(F)B\in M_{n\times m}(F), tr(AB)=tr(BA)\operatorname{tr}(AB)=\operatorname{tr}(BA)).

Proof

technique · direct
1.1

Choose invertible PP with B=P1APB=P^{-1}AP as in [L1].

givenL1
2.1

Apply [L2] to X=P1AX=P^{-1}A and Y=PY=P to obtain tr(B)=tr(P(P1A))\operatorname{tr}(B)=\operatorname{tr}(P(P^{-1}A)).

step 1.1L1L2
3.1

By associativity and unitality from [L3], P(P1A)=(PP1)A=InA=AP(P^{-1}A)=(PP^{-1})A=I_nA=A, so tr(B)=tr(A)\operatorname{tr}(B)=\operatorname{tr}(A).

step 2.1L1L2L3
DefinitionDefinition: Literature-sourcedProof: Not applicableaudited 2026-08-11Open item page →

The basis-independent trace of an endomorphism of a finite-dimensional vector space

Definition

Let VV be a finite-dimensional vector space over FF and let T:VVT:V\to V be linear. Choose any ordered basis B\mathcal B of VV and define the trace of the endomorphism TT by

tr(T):=tr([T]BB).\operatorname{tr}(T):=\operatorname{tr}([T]_{\mathcal B}^{\mathcal B}).

This is independent of the chosen basis: matrices of the same endomorphism in two ordered bases are similar, and similar matrices have equal trace. When VV is the zero space, the empty basis gives trace 00.

5 · Examples, counterexamples and false statements

None yet.

Sources

Standard references

Recommended treatments; not extraction sources.