Bourbaki

Appendix 2 determinants over a noncommutative field

In this appendix, D is a field, and Dab∗D^*_{ab} is the quotient of the multiplicative group D∗D^* of D by its derived group (I, §6, No. 2, p. 70). The group Dab∗D^*_{ab} is commutative, and Dab∗D^*_{ab} can be identified with D∗D^* if the field D is commutative. We denote the canonical homomorphism from D∗D^* to Dab∗D^*_{ab} by π\pi.

1. A Generalization of Alternating Multilinear Forms

Let V be a right vector space over the field D, of finite dimension n⩾0n\geqslant 0. We denote by B(V) the set of bases of V and by Ω(V) the set of mappings ω\omega from B(V) to Dab∗D^*_{ab} that satisfy the following two conditions:

a) If λ1,...,λn\lambda_1, . . . , \lambda_n are the elements of D∗D^*, then we have

ω(v1λ1,...,vnλn)=π(λ1⋯λn)ω(v1,...,vn)(1) \omega (v_1\lambda_1, . . . , v_n\lambda_n) =\pi (\lambda_1\cdots \lambda_n)\omega (v_1, . . . , v_n) \tag{1}

for every basis (v1,...,vn)(v_1, . . . , v_n) of V.

b) If ii and jj are two distinct integers in the interval [1,n][1, n], then we have

ω(v1,...,vi−1,vi+vj,vi+1,...,vn)=ω(v1,...,vn)(2) \omega (v_1, . . . , v_{i-1}, v_i+v_j, v_{i+1}, . . . , v_n) =\omega (v_1, . . . , v_n) \tag{2}

for every basis (v1,...,vn)(v_1, . . . , v_n) of V.

Let ω\omega be an element of Ω(V). Let (v1,...,vn)(v_1, . . . , v_n) be a basis of V and ii an integer in the interval [1,n−1][1, n-1]; by property b), we have

ω(v1,...,vi,vi+1,...,vn)=ω(v1,...,vi+vi+1,vi+1,...,vn) \omega (v_1, . . . , v_i, v_{i+1}, . . . , v_n) =\omega (v_1, . . . , v_i+v_{i+1}, v_{i+1}, . . . , v_n)
=ω(v1,...,vi+vi+1,vi+1−(vi+vi+1),...,vn) =\omega (v_1, . . . , v_i+v_{i+1}, v_{i+1}-(v_i+v_{i+1}), . . . , v_n)
=ω(v1,...,vi+vi+1,−vi,...,vn) =\omega (v_1, . . . , v_i+v_{i+1},-v_i, . . . , v_n)
=ω(v1,...,(vi+vi+1)−vi,−vi,...,vn) =\omega (v_1, . . . ,(v_i+v_{i+1})-v_i,-v_i, . . . , v_n)

and therefore

ω(v1,...,vi,vi+1,...,vn)=π(−1)ω(v1,...,vi+1,vi,...,vn)(3) \omega (v_1, . . . , v_i, v_{i+1}, . . . , v_n) =\pi (-1)\omega (v_1, . . . , v_{i+1}, v_i, . . . , v_n) \tag{3}

Since the symmetric group Sn\mathfrak{S}_n is generated by the transpositions of two consecutive elements of the interval [1,n][1, n] (I, §5, No. 7, p. 63, Proposition 9), formula (3) generalizes to

ω(vσ(1),...,vσ(n))=π(ε(σ))ω(v1,...,vn)(4) \omega (v_{\sigma(1)}, . . . , v_{\sigma(n)}) =\pi (\varepsilon (\sigma ))\omega (v_1, . . . , v_n) \tag{4}

where σ\sigma belongs to Sn\mathfrak{S}_n and ε(σ)\varepsilon (\sigma ) is its signature (I, §5, No. 7, p. 64).

Formula (2) generalizes as follows. First, for every λ\lambda in D∗D^*, we have

ω(v1,...,vn)=π(λ)ω(v1,...,viλ−1,...,vn) \omega (v_1, . . . , v_n) =\pi (\lambda )\omega (v_1, . . . , v_i\lambda^{-1}, . . . , v_n)
=π(λ)ω(v1,...,viλ−1+vj,...,vn) =\pi (\lambda )\omega (v_1, . . . , v_i\lambda^{-1}+v_j, . . . , v_n)
=ω(v1,...,(viλ−1+vj)λ,...,vn) =\omega (v_1, . . . ,(v_i\lambda^{-1}+v_j)\lambda , . . . , v_n)

that is,

ω(v1,...,vn)=ω(v1,...,vi+vjλ,...,vn)(5) \omega (v_1, . . . , v_n) =\omega (v_1, . . . , v_i+v_j\lambda , . . . , v_n) \tag{5}

By an immediate induction, we deduce

ω(v1,...,vn)=ω(v1,...,vi+w,...,vn)(6) \omega (v_1, . . . , v_n) =\omega (v_1, . . . , v_i+w, . . . , v_n) \tag{6}

for every linear combination w=∑j≠ivjλjw=\sum_{j\not=i}v_j\lambda_j of the vectors vjv_j for jj different from ii in the interval [1,n][1, n].

2. A Uniqueness Theorem

In this subsection, for any strictly positive integer mm, any integer ii in the interval [1,m][1, m], and any sequence (v1,...,vm)(v_1, . . . , v_m) in VmV^m, we write (v1,...,v^i,...,vm)(v_1, . . . ,\widehat{v}_i, . . . , v_m) for the sequence (v1,...,vi−1,vi+1,...,vm)(v_1, . . . , v_{i-1}, v_{i+1}, . . . , v_m) in Vm−1V^{m-1}.

Proposition 1 00Q1

Let W be a hyperplane in V and ee be a vector in V- W. Let φ\varphi be an element of Ω(W). There exists a unique element ω\omega of Ω(V) such that we have

ω(w1,...,wn−1,e)=φ(w1,...,wn−1)(7) \omega (w_1, . . . , w_{n-1}, e) =\varphi (w_1, . . . , w_{n-1}) \tag{7}

for every basis (w1,...,wn−1)(w_1, . . . , w_{n-1}) of W.

Cites 1 · Cited by 2

Cites App. 2. Determinants over a Noncommutative Field

Cited by Exercise 2, Appendix 2, Corollary 1

A) Uniqueness of ω:\omega : Let ω\omega be an element of Ω(V). Let (v1,...,vn)(v_1, . . . , v_n) be a basis of V, and let μ1,...,μn\mu_1, . . . , \mu_n be the coordinates of ee in this basis. Denote by I the set of integers from 1 to nn (inclusive) such that μi≠0\mu_i\not= 0; it is not empty. Let ii be an element of I. The sequence (v1,...,v^i,...,vn,e)(v_1, . . . ,\widehat{v}_i, . . . , v_n, e) is a basis of V, and since e−viμie-v_i\mu_i is a linear combination of the sequence (v1,...,v^i,...,vn)(v_1, . . . ,\widehat{v}_i, . . . , v_n), formula (6) implies

ω(v1,...,v^i,...,vn,viμi)=ω(v1,...,v^i,...,vn,e)(8) \omega (v_1, . . . ,\widehat{v}_i, . . . , v_n, v_i\mu_i) =\omega (v_1, . . . ,\widehat{v}_i, . . . , v_n, e) \tag{8}

It follows from formulas (1) and (3) that the left-hand side of this equality is equal to π(−1)n−iπ(μi)ω(v1,...,vn)\pi (-1)^{n-i}\pi (\mu_i)\omega (v_1, . . . , v_n). Denote by pp the projector of V with image W and kernel eDeD. The vectors vj−p(vj)v_j-p(v_j) are proportional to ee, and repeatedly applying formula (6) shows that the right-hand side of formula (8) is equal to ω(p(v1),...,p^(vi),...,p(vn),e)\omega (p(v_1), . . . ,\widehat{p}(v_i), . . . , p(v_n), e).

It follows from this that if ω\omega satisfies relation (7), then we have

ω(v1,...,vn)=π(−1)n−iπ(μi)−1φ(p(v1),...,p^(vi),...,p(vn))(9) \omega (v_1, . . . , v_n) =\pi (-1)^{n-i}\pi (\mu_i)^{-1}\varphi (p(v_1), . . . ,\widehat{p}(v_i), . . . , p(v_n)) \tag{9}

for every ii in I, which proves the uniqueness of ω\omega.

B) Construction of ω:\omega : Let (v1,...,vn)(v_1, . . . , v_n) be a basis of V; we define μ1,...,μn\mu_1, . . . , \mu_n and I as above. For every ii in I, the assumption μi≠0\mu_i\not= 0 implies that the sequence (v1,...,v^i,...,vn,e)(v_1, . . . ,\widehat{v}_i, . . . , v_n, e) generates the space V, so the sequence (p(v1),...,p^(vi),...,p(vn))(p(v_1), . . . ,\widehat{p}(v_i), . . . , p(v_n)) generates the space W=p(V)W =p(V). In other words, this last sequence is a basis of W, and

ti=π(−1)n−iπ(μi)−1φ(p(v1),...,p^(vi),...,p(vn))(10) t_i=\pi (-1)^{n-i}\pi (\mu_i)^{-1}\varphi (p(v_1), . . . ,\widehat{p}(v_i), . . . , p(v_n)) \tag{10}

defines an element of Dab∗D^*_{ab}.

Let ii and jj be two elements of I such that i<ji < j; let us prove the equality ti=tjt_i=t_j. By definition, the vector viμi+vjμj−ev_i\mu_i+v_j\mu_j-e is a linear combination of the vectors p(vk)p(v_k) for kk different from ii and jj. Consequently, p(vi)μi+p(vj)μjp(v_i)\mu_i+p(v_j)\mu_j is a linear combination of the vectors p(vk)p(v_k) for kk different from ii and jj. By formula (6), we therefore have

φ(p(v1),...,p(v^i),...,p(v^j),...,p(vn),p(vi)μi) \varphi (p(v_1), . . . ,p(\widehat{v}_i), . . . ,p(\widehat{v}_j), . . . , p(v_n), p(v_i)\mu_i)
=φ(p(v1),...,p(v^i),...,p(v^j),...,p(vn),−p(vj)μj) =\varphi (p(v_1), . . . ,p(\widehat{v}_i), . . . ,p(\widehat{v}_j), . . . , p(v_n),-p(v_j)\mu_j)

By applying formulas (1) and (3), we deduce

φ(p(v1),...,p(v^j),...,p(vn))π(μi)π(−1)n−i−1 \varphi (p(v_1), . . . ,p(\widehat{v}_j), . . . , p(v_n))\pi (\mu_i)\pi (-1)^{n-i-1}
=φ(p(v1),...,p^(vi),...,p(vn))π(−μj)π(−1)n−j =\varphi (p(v_1), . . . ,\widehat{p}(v_i), . . . , p(v_n))\pi (-\mu_j)\pi (-1)^{n-j}

and therefore ti=tjt_i=t_j.

Having proved this, we define ω(v1,...,vn)\omega (v_1, . . . , v_n) as the common value of the tit_i for ii in I. We have thus constructed a mapping ω\omega from B(V) to Dab∗D^*_{ab} that satisfies relation (9). Let (w1,...,wn−1)(w_1, . . . , w_{n-1}) be a basis of W; if we set vi=wiv_i=w_i for 1⩽i⩽n−11\leqslant i\leqslant n-1 and vn=ev_n=e, then we have I={n}I =\{n\} and μn=1\mu_n= 1. We moreover have p(vi)=wip(v_i) =w_i for 1⩽i⩽n−11\leqslant i\leqslant n-1, and the formula ω(w1,...,wn−1,e)=φ(w1,...,wn−1)\omega (w_1, . . . , w_{n-1}, e) =\varphi (w_1, . . . , w_{n-1}) is a specific case of (9).

We must now prove that ω\omega belongs to Ω(V).

C) Proof of formula (1): Let λ1,...,λn\lambda_1, . . . , \lambda_n be elements of D∗D^* and (v1,...,vn)(v_1, . . . , v_n) be a basis of V. We define μ1,...,μn\mu_1, . . . , \mu_n and I as above. Choose an ii in I. Since we have e=∑j=1n(vjλj)(λj−1μj)e=\sum^n_{j=1}(v_j\lambda_j)(\lambda^{-1}_j\mu_j), formula (9) implies

ω(v1λ1,...,vnλn)(11) \omega (v_1\lambda_1, . . . , v_n\lambda_n) \tag{11}
=π(−1)n−iπ(λi−1μi)−1φ(p(v1)λ1,...,p(vi)λi^,...,p(vn)λn) =\pi (-1)^{n-i}\pi (\lambda^{-1}_i\mu_i)^{-1}\varphi (p(v_1)\lambda_1, . . . ,\widehat{p(v_i)\lambda_i}, . . . , p(v_n)\lambda_n)

But we have π(λi−1μi)−1=π(μi)−1π(λi)\pi (\lambda^{-1}_i\mu_i)^{-1}=\pi (\mu_i)^{-1}\pi (\lambda_i) and

φ(p(v1)λ1,...,p(vi)λi^,...,p(vn)λn) \varphi (p(v_1)\lambda_1, . . . ,\widehat{p(v_i)\lambda_i}, . . . , p(v_n)\lambda_n)
=φ(p(v1),...,p(vi)^,...,p(vn))π(λ1...λ^i...λn) =\varphi (p(v_1), . . . ,\widehat{p(v_i)}, . . . , p(v_n))\pi (\lambda_1. . .\widehat{\lambda}_i. . . \lambda_n)

Comparing formulas (9) and (11) leads to the desired relation

ω(v1λ1,...,vnλn)=ω(v1,...,vn)π(λ1...λn) \omega (v_1\lambda_1, . . . , v_n\lambda_n) =\omega (v_1, . . . , v_n)\pi (\lambda_1. . . \lambda_n)

D) Proof of the formula (2): Let (v1,...,vn)(v_1, . . . , v_n) be a basis of V and i,ji, j be two distinct integer in the interval [1,n][1, n]; we define μ1,...,μn\mu_1, . . . , \mu_n as before. Consider the basis (v1′,...,vn′)(v'_1, . . . , v'_n) of V defined by vi′=vi+vjv'_i=v_i+v_j and vk′=vkv'_k=v_k for k≠ik\not=i, and let us introduce the coordinates μ1′,...,μn′\mu'_1, . . . , \mu'_n of ee with respect to this basis; they satisfy μj′=μj−μi\mu'_j=\mu_j-\mu_i and μk′=μk\mu'_k=\mu_k for k≠jk\not=j. We set t=ω(v1,...,vn)t=\omega (v_1, . . . , v_n) and t′=ω(v1′,...,vn′)t'=\omega (v'_1, . . . , v'_n). We must prove that tt and t′t' are equal.

Let us first note that, by the definition of ω\omega, we have

t=π(−1)n−kπ(μk)−1φ(p(v1),...,p(vk)^,...,p(vn))(12) t=\pi (-1)^{n-k}\pi (\mu_k)^{-1}\varphi (p(v_1), . . . ,\widehat{p(v_k)}, . . . , p(v_n)) \tag{12}
t′=π(−1)n−kπ(μk′)−1φ(p(v1′),...,p(vk′)^,...,p(vn′))(13) t'=\pi (-1)^{n-k}\pi (\mu'_k)^{-1}\varphi (p(v'_1), . . . ,\widehat{p(v'_k)}, . . . , p(v'_n)) \tag{13}

for every kk such that μk\mu_k and μk′\mu'_k are nonzero.

a) If μi≠0\mu_i\not=0, then the sequences (p(v1),...,p(vk)^,...,p(vn))(p(v_1), . . . ,\widehat{p(v_k)}, . . . , p(v_n)) and (p(v1′),...,p(vk′)^,...,p(vn′))(p(v'_1), . . . ,\widehat{p(v'_k)}, . . . , p(v'_n)) are equal, and we have μi\mu_i = μi′\mu'_i, and therefore t=t′t=t'.

b) If there exists an index kk different from ii and jj such that μk≠0\mu_k\not= 0, then we have p(vl′)=p(vl)p(v'_l) =p(v_l) for l≠il\not=i and p(vi′)=p(vi)+p(vj)p(v'_i) =p(v_i) +p(v_j). The elements p(vi)p(v_i) and p(vj)p(v_j) both belong to the sequence (p(v1),...,p(v^k),...,p(vn))(p(v_1), . . . ,p(\widehat{v}_k), . . . , p(v_n)). Since φ\varphi belongs to Ω(W), formula (2) of VIII, p. 447 applies; it gives

φ(p(v1),...,p(v^k),...,p(vn))=φ(p(v1′),...,p(v^k′),...,p(vn′)) \varphi (p(v_1), . . . ,p(\widehat{v}_k), . . . , p(v_n)) =\varphi (p(v'_1), . . . ,p(\widehat{v}'_k), . . . , p(v'_n))

But we also have μk=μk′\mu_k=\mu'_k, and therefore t=t′t=t'.

c) It remains to examine the case when the only index kk such that μk≠0\mu_k\not= 0 is jj. We then have μj′=μj,e=vjμj\mu'_j=\mu_j,e=v_j\mu_j, and p(vj)=0p(v_j) = 0. Set k=jk=j in formulas (12) and (13). Since the sequences (p(v1),...,p(v^j),...,p(vn))(p(v_1), . . . ,p(\widehat{v}_j), . . . , p(v_n)) and (p(v1′),...,p(v^j′),...,p(vn′))(p(v'_1), . . . ,p(\widehat{v}'_j), . . . , p(v'_n)) are equal, we have t=t′t=t'.

Corollary 1 00Q2

Let (e1,...,en)(e_1, . . . , e_n) be a basis of V and tt an element of Dab∗D^*_{ab}. There exists a unique element ω\omega of Ω(V) such that ω(e1,...,en)=t\omega (e_1, . . . , e_n) =t.

Cites 1 · Cited by 1

Cites Proposition 1

Cited by Remark

Let us prove the corollary by induction on nn. If n=0n= 0, then the only basis of V is the empty one, so the assertion is true. Now suppose n⩾1n\geqslant 1; denote by W the subspace of V generated by e1,...,en−1e_1, . . . , e_{n-1}. By Proposition 1, there exists a bijection Λ from Ω(V) to Ω(W) satisfying

(Λ(ω))(w1,...,wn−1)=ω(w1,...,wn−1,en) (\Lambda (\omega ))(w_1, . . . , w_{n-1}) =\omega (w_1, . . . , w_{n-1}, e_n)

for every basis (w1,...,wn−1)(w_1, . . . , w_{n-1}) of W and every ω\omega in Ω(V). By the induction hypothesis, there exists a unique element φ\varphi of Ω(W) such that φ(e1,...,en−1)=t\varphi (e_1, . . . , e_{n-1}) =t. The relation ω(e1,...,en)=t\omega (e_1, . . . , e_n) =t, for ω\omega in Ω(V), is equivalent to Λ(ω)=φ\Lambda (\omega ) =\varphi. Corollary 1 follows.

Corollary 2 00Q3

Let ω\omega and ω′\omega ' be two elements of Ω(V). There exists a unique element tt of Dab∗D^*_{ab} such that ω′=tω\omega '=t\omega.

Cited by 2

Cited by App. 2. Determinants over a Noncommutative Field, Proposition 2

Remark 00Q4

Suppose that the field D is commutative. By definition, B(V) is a subset of VnV^n. It is clear that the restriction to B(V) of a nonzero alternating nn-linear form f:Vn→Df: V^n\rightarrow D belongs to Ω(V). Moreover, if (e1,...,en)(e_1, . . . , e_n) is a basis of V and tt is a nonzero element of D, then there exists a unique alternating nn-linear form ff such that f(e1,...,en)=tf(e_1, . . . , e_n) =t (III, §7, No. 4, p. 511 and III, §7, No. 8, p. 518). By Corollary 1, the set Ω(V) consists of the restrictions to B(V) of the nonzero alternating nn-linear forms.

Cites 2

Cites III § 7. Exterior algebras, Corollary 1

3. Determinant of an Automorphism

We first suppose that the field D is commutative. In view of the remark above, the determinant of an automorphism uu of V is the unique element det uu of D∗D^* such that we have

(14) ω(u(v1),...,u(vn))=\omega (u(v_1), . . . , u(v_n)) = (det uu)ω(v1,...,vn)\omega (v_1, . . . , v_n)

for every basis (v1,...,vn)(v_1, . . . , v_n) of V and every element ω\omega of Ω(V).

Let us return to the case when D is no longer supposed to be commutative.

Proposition 2 00Q5

a) Let uu be an automorphism of V. There exists a unique element of Dab∗D^*_{ab}, denoted by det uu and called the determinant of uu, such that we have

Cites 1 · Cited by 1

Cites Corollary 2

Cited by Proposition 9, VIII § 17

(15) ω(u(v1),...,u(vn))=\omega (u(v_1), . . . , u(v_n)) = (det uu)ω(v1,...,vn)\omega (v_1, . . . , v_n)

for every basis (v1,...,vn)(v_1, . . . , v_n) of V and every ω\omega in Ω(V).

b) The mapping u↦u\mapsto det uu from GL(V)\mathbf{G}\mathbf{L}(V) to Dab∗D^*_{ab} is a group homomorphism.

Let ω0\omega_0 be an element of Ω(V). The mapping (v1,...,vn)↦(v_1, . . . , v_n)\mapsto ω0(u(v1),...,u(vn))\omega_0(u(v_1), . . . , u(v_n)) from B(V) to Dab∗D^*_{ab} belongs to Ω(V). By Corollary 2 of VIII, p. 451, there exists a unique element tt of Dab∗D^*_{ab} such that we have

ω0(u(v1),...,u(vn))=tω0(v1,...,vn) \omega_0(u(v_1), . . . , u(v_n)) =t\omega_0(v_1, . . . , v_n)

for (v1,...,vn)(v_1, . . . , v_n) in B(V). If ω\omega is another element of Ω(V), then there exists an element ss of Dab∗D^*_{ab} such that

ω(v1,...,vn)=sω0(v1,...,vn) \omega (v_1, . . . , v_n) =s\omega_0(v_1, . . . , v_n)

for every basis (v1,...,vn)(v_1, . . . , v_n) of V (loc. cit.). We immediately deduce the relation

ω(u(v1),...,u(vn))=tω(v1,...,vn) \omega (u(v_1), . . . , u(v_n)) =t\omega (v_1, . . . , v_n)

This proves a); assertion b) is an immediate consequence of a).

4. Determinant of a Square Matrix

Let nn be a positive integer. Let us apply the above to the right vector space DdnD^n_d over the field D; the elements of DdnD^n_d are viewed as matrices with nn rows and one column. Let (ε1,...,εn)(\varepsilon_1, . . . , \varepsilon_n) be the canonical basis of DdnD^n_d. By Corollary 2 of VIII, p. 451, there exists a unique element ω0\omega_0 of Ω(Ddn)\Omega (D^n_d) such that ω0(ε1,...,εn)=1\omega_0(\varepsilon_1, . . . , \varepsilon_n) = 1. If A is an element of GLn\mathbf{G}\mathbf{L}_n(D), then its columns a1,...,ana_1, . . . , a_n form a basis of DdnD^n_d; the element ω0(a1,...,an)\omega_0(a_1, . . . , a_n) of Dab∗D^*_{ab} is called the determinant of A and denoted by det(A). Since we have ai=Aεia_i=A\varepsilon_i for 1⩽i⩽n1\leqslant i\leqslant n, the determinant of A is simply the determinant of the automorphism x↦Axx\mapsto Ax of DdnD^n_d. In particular, if the field D is commutative, then the determinant of A coincides with that defined in III, §8, No. 3, p. 524.

Let V be a right vector space of finite dimension nn over the field D, and let (e1,...,en)(e_1, . . . , e_n) be a basis of V. If uu is an automorphism of V and A is the matrix of uu with respect to the basis (e1,...,en)(e_1, . . . , e_n), then we have det(uu) == det(A).

We denote by (EijE_{ij}) the family of matrix units of Mn(D)\mathbf{M}_n(D) (II, §10, No. 3, p. 341). For every element λ\lambda of D and every pair (i,j)(i, j) of distinct integers in [1,n][1, n], we set (II, §10, No. 13, p. 361)

Bij(λ)=In+λEij B_{ij}(\lambda ) =I_n+\lambda E_{ij}

it is an element of GLn(D)\mathbf{G}\mathbf{L}_n(D). If λ1,...,λn\lambda_1, . . . , \lambda_n are elements of D∗D^*, then the diagonal matrix diag(λ1,...,λn\lambda_1, . . . , \lambda_n) also belongs to GLn(D)\mathbf{G}\mathbf{L}_n(D).

Proposition 3 00Q6

The mapping det is the unique homomorphism from GLn(D)\mathbf{G}\mathbf{L}_n(D) to Dab∗D^*_{ab} that satisfies the relations

Cited by 3

Cited by Example 3, Example 5, Proposition 9, VIII § 17

(16) det(Bij(1)B_{ij}(1)) =1= 1

for i≠ji\not=j and

(17) det(diag(λ1,...,λn\lambda_1, . . . , \lambda_n)) =π(λ1⋯λn)=\pi (\lambda_1\cdots \lambda_n),

for λ1,...,λn∈D∗\lambda_1, . . . , \lambda_n\in D^*

Let A be an element of GLn(D)\mathbf{G}\mathbf{L}_n(D) and a1,...,ana_1, . . . , a_n be its columns. We have

det(A) =ω0(a1,...,an)=\omega_0(a_1, . . . , a_n).

Now, the columns of the matrix A diag(λ1,...,λn\lambda_1, . . . , \lambda_n) are a1λ1,...,anλna_1\lambda_1, . . . , a_n\lambda_n, and those of the matrix ABij(1)_{ij}(1) are therefore a1,...,aj+ai,aj+1,...,ana_1, . . . , a_j+a_i, a_{j+1}, . . . , a_n. Since ω0\omega_0 is the unique element of Ω(Ddn)\Omega (D^n_d) such that ω0(ε1,...,εn)=1\omega_0(\varepsilon_1, . . . , \varepsilon_n) = 1, we see that the determinant is the unique mapping φ:GLn(D)→Dab∗\varphi :\mathbf{G}\mathbf{L}_n(D)\rightarrow D^*_{ab} that satisfies the relations

(18) φ(\varphi (A diag(λ1,...,λn\lambda_1, . . . , \lambda_n)) =φ(=\varphi (A)π(λ1⋯λn))\pi (\lambda_1\cdots \lambda_n),

(19) φ(\varphi (ABij(1))=φ(_{ij}(1)) =\varphi (A) for i≠ji\not=j,

φ(In)=1(20) \varphi (I_n) = 1 \tag{20}

This proves, to begin with, that the determinant mapping satisfies relations (16) and (17). We already know that this mapping is a homomorphism from GLn(D)\mathbf{G}\mathbf{L}_n(D) to Dab∗D^*_{ab}. Conversely, if φ\varphi is a homomorphism from GLn(D)\mathbf{G}\mathbf{L}_n(D) to Dab∗D^*_{ab} such that φ(Bij(1))=1\varphi (B_{ij}(1)) = 1 for i≠ji\not=j and φ\varphi(diag(λ1,...,λn\lambda_1, . . . , \lambda_n)) =π(λ1⋯λn)=\pi (\lambda_1\cdots \lambda_n), then φ\varphi satisfies relations (18) through (20) and is therefore equal to det.

Example 1 00Q7

The columns of the matrix Bij(λ)B_{ij}(\lambda ) are ε1,...,εj\varepsilon_1, . . . , \varepsilon_j + εiλ,εi+1,...,εn\varepsilon_i\lambda , \varepsilon_{i+1}, . . . , \varepsilon_n. By formula (5) of VIII, p. 448, we have

(21) det(Bij(λ)B_{ij}(\lambda )) =1= 1.

Cites 1 · Cited by 2

Cites App. 2. Determinants over a Noncommutative Field

Cited by Example 3, Theorem 1

Example 2 00Q8

Let σ\sigma be a permutation of the interval [1,n][1, n] in N\mathbf{N}, with signature ε(σ)\varepsilon (\sigma ). Let M(σ)(\sigma ) be the matrix of the permutation σ\sigma (II, §10, No. 7, p. 351). The columns of the matrix M(σ)(\sigma ) are εσ(1),...,εσ(n)\varepsilon_{\sigma(1)}, . . . , \varepsilon_{\sigma(n)}. Applying formula (4) of VIII, p. 448, we therefore have

(22) det(M(σ)(\sigma )) =π(ε(σ))=\pi (\varepsilon (\sigma )).

Cites 2 · Cited by 1

Cites II § 10. Matrices, App. 2. Determinants over a Noncommutative Field

Cited by Example 6

Example 3 00Q9

Suppose n⩾1n\geqslant 1. For every invertible diagonal matrix of the form Δ = diag(d1,...,dnd_1, . . . , d_n), we have ΔBij(λB_{ij}(\lambda)Δ−1=Bij(diλdj−1)^{-1}=B_{ij}(d_i\lambda d^{-1}_j). Let A be an element of GLn(D)\mathbf{G}\mathbf{L}_n(D). By Corollary 1 of II, §10, No. 13, p. 362 and the previous formula, there exist matrices P and Δ in GLn(D)\mathbf{G}\mathbf{L}_n(D) such that A = PΔ, that P is the product of matrices of the form Bij(λ)B_{ij}(\lambda ), and that Δ is a diagonal matrix of the form diag(1,...,1,d, . . . ,1, d). We have det(P) = 1 by Example 1, and therefore det(A) = det(Δ) =π(d)=\pi (d) by Proposition 3.

Cites 3 · Cited by 2

Cites Corollary 1, II § 10, Example 1, Proposition 3

Cited by Example 4, Example 7

Example 4 00QA

Let D′D' be a field, and let uu be a homomorphism from D to D′D'. When passing to the quotients, uu defines a group homomorphism uabu_{ab} from Dab∗D^*_{ab} to Dab′∗D^{'*}_{ab}. Let unu_n be the homomorphism from GLn(D)\mathbf{G}\mathbf{L}_n(D) to GLn(D′)\mathbf{G}\mathbf{L}_n(D') that transforms a matrix A =(aij)= (a_{ij}) into the matrix (u(aij))(u(a_{ij})). The formula

(23) det(un(u_n(A)) =uab=u_{ab}(det(A))

for A∈GLn(D)A\in \mathbf{G}\mathbf{L}_n(D) follows immediately from Example 3.

Cites 1

Cites Example 3

Example 5 00QB

We have GL1(D)=D∗\mathbf{G}\mathbf{L}_1(D) = D^*, and Proposition 3 shows that we have det(aa) =π(a)=\pi (a) for aa in GL1(D)\mathbf{G}\mathbf{L}_1(D).

Cites 1

Cites Proposition 3

Example 6 00QC

Suppose n=2n= 2. Let A=(abcd)A = \begin{pmatrix} a & b \\ c & d \end{pmatrix} be an element of GL2(D)\mathbf{G}\mathbf{L}_2(D). The elements aa and cc of D are not both zero. We will give the determinant of A explicitly.

If aa is not zero, then we have

(24) A=(10ca−11)(a00d−ca−1b)(1a−1b01)A = \begin{pmatrix} 1 & 0 \\ ca^{-1} & 1 \end{pmatrix}\begin{pmatrix} a & 0 \\ 0 & d-ca^{-1}b \end{pmatrix}\begin{pmatrix} 1 & a^{-1}b \\ 0 & 1 \end{pmatrix}.

Consequently, ad−aca−1b≠0ad-aca^{-1}b\not= 0 and

(25) det(A) =π(ad−aca−1b)=\pi (ad-aca^{-1}b).

b) If aa is zero, then we have c≠0c\not= 0 and

(26) A=(0bcd)=(0110)(cd0b)A = \begin{pmatrix} 0 & b \\ c & d \end{pmatrix} = \begin{pmatrix} 0 & 1 \\ 1 & 0 \end{pmatrix}\begin{pmatrix} c & d \\ 0 & b \end{pmatrix}.

Consequently, by a) and Example 2, we have cb≠0cb\not= 0 and

(27) det(A) =π(−cb)=\pi (-cb).

Cites 1 · Cited by 1

Cites Example 2

Cited by Example 7

Example 7 00QD

Let DoD^o be the opposite field of D. The mapping A↦tAA\mapsto^tA from Mn(D)\mathbf{M}_n(D) to Mn(Do)\mathbf{M}_n(D^o) satisfies t(^t(AB)=tBtA) =^tB^tA. Therefore, for every matrix A in GLn\mathbf{G}\mathbf{L}_n(D), the transposed matrix tA^tA is invertible in Mn(Do)\mathbf{M}_n(D^o), but it is not necessarily invertible in Mn(D)\mathbf{M}_n(D). It follows from Example 3 that if A belongs to GLn\mathbf{G}\mathbf{L}_n(D), then the elements A of GLn(D)\mathbf{G}\mathbf{L}_n(D) and tA^tA of GLn(Do)\mathbf{G}\mathbf{L}_n(D^o) have the same determinant. On the other hand, even if the matrix tA^tA belongs to GLn\mathbf{G}\mathbf{L}_n(D), its determinant in GLn(D)_n(D) is not necessarily equal to that of A (cf. Example 6).

Cites 2 · Cited by 1

Cites Example 3, Example 6

Cited by Remark 1

Remark 1 00QE

Let V be a right vector space over the field D, of finite dimension nn. We view the dual space V∗=V^*= HomD(V,D)_D(V,D) as a right vector space over the opposite field DoD^o of D. Let uu be an automorphism of V, and let tu^tu be the automorphism of V∗V^* that is the transpose of uu. If uu is represented by a matrix A in Mn(D)\mathbf{M}_n(D) with respect to a basis (e1,...,en)(e_1, . . . , e_n) of V, then the automorphism tu^tu is represented by the matrix tA^tA in Mn(Do)\mathbf{M}_n(D^o) with respect to the basis (e1∗,...,en∗)(e^*_1, . . . , e^*_n) of V∗V^* dual to (e1,...,en)(e_1, . . . , e_n) (II, §10, No. 4, p. 344, Proposition 3). By Example 7, the determinant of tu^tu is equal to that of uu.

Cites 2

Cites Proposition 3, II § 10, Example 7

Remark 2 00QF

The results of Subsections 1 through 4 generalize to the case when D is a local ring (VIII, p. 459, Exercise 2).

Cites 1

Cites Exercise 2, Appendix 2

5. The Unimodular Group

Let nn be a positive integer. We denote by SLn(D)\mathbf{S}\mathbf{L}_n(D) the kernel of the group homomorphism det:GLn(D)→Dab∗:\mathbf{G}\mathbf{L}_n(D)\rightarrow D^*_{ab}, and we call it the unimodular group or special linear group (cf. III, §8, No. 9, p. 537 when the field D is commutative).

Theorem 1 00QG

Suppose n⩾2n\geqslant 2.

Cites 1 · Cited by 1

Cites Example 1

Cited by Remark

a) The subgroup SLn(D)\mathbf{S}\mathbf{L}_n(D) of GLn(D)\mathbf{G}\mathbf{L}_n(D) is generated by the matrices Bij(λ)B_{ij}(\lambda ), where ii and jj are distinct integers in the interval [1,n][1, n] and λ\lambda runs through D.

b) Suppose n⩾3n\geqslant 3 or Card(D) ⩾3\geqslant 3. The derived group of GLn(D)\mathbf{G}\mathbf{L}_n(D) is equal to SLn(D)\mathbf{S}\mathbf{L}_n(D).

c) Suppose n⩾3n\geqslant 3 or Card(D) ⩾4\geqslant 4. The derived group of SLn(D)\mathbf{S}\mathbf{L}_n(D) is equal to SLn(D)\mathbf{S}\mathbf{L}_n(D).

A) Denote by T the subgroup of GLn(D)\mathbf{G}\mathbf{L}_n(D) generated by the matrices Bij(λ)B_{ij}(\lambda ). By Example 1 of VIII, p. 454, we have det(Bij(λ)B_{ij}(\lambda )) =1= 1, and therefore T⊂SLn(D)T\subset \mathbf{S}\mathbf{L}_n(D). To prove that these two groups are equal, it then suffices, by Example 3 of loc. cit., to prove that every matrix of the form diag(1,...,1,d, . . . ,1, d) with π(d)=1\pi (d) = 1 belongs to T. The matrix diag(1,...,1,d, . . . ,1, d) belongs to the image of the homomorphism U↦(In−200U)U\mapsto \begin{pmatrix} I_{n-2} & 0 \\ 0 & U \end{pmatrix} from GL2(D)\mathbf{G}\mathbf{L}_2(D) to GLn(D)\mathbf{G}\mathbf{L}_n(D); it therefore suffices to consider the case n=2n= 2. Since the kernel of π\pi is the derived group of D∗D^*, we may assume d=uvu−1v−1d=uvu^{-1}v^{-1} with u,vu, v in D∗D^*. Our assertion then follows from the equalities

(28) (100d)=(u−100u)(v−100v)(vu00u−1v−1)\begin{pmatrix} 1 & 0 \\ 0 & d \end{pmatrix} = \begin{pmatrix} u^{-1} & 0 \\ 0 & u \end{pmatrix}\begin{pmatrix} v^{-1} & 0 \\ 0 & v \end{pmatrix}\begin{pmatrix} vu & 0 \\ 0 & u^{-1}v^{-1} \end{pmatrix}

and

(29) (s00s−1)=(1s01)(101−s−11)(1−101)(101−s1)\begin{pmatrix} s & 0 \\ 0 & s^{-1} \end{pmatrix} = \begin{pmatrix} 1 & s \\ 0 & 1 \end{pmatrix}\begin{pmatrix} 1 & 0 \\ 1-s^{-1} & 1 \end{pmatrix}\begin{pmatrix} 1 & -1 \\ 0 & 1 \end{pmatrix}\begin{pmatrix} 1 & 0 \\ 1-s & 1 \end{pmatrix}

for s∈D∗s\in D^*.

B) By construction, SLn(D)\mathbf{S}\mathbf{L}_n(D) is the kernel of a homomorphism from GLn(D)\mathbf{G}\mathbf{L}_n(D) to a commutative group, so it contains the derived group (GLn(D),GLn(D))(\mathbf{G}\mathbf{L}_n(D),\mathbf{G}\mathbf{L}_n(D)) of GLn(D)\mathbf{G}\mathbf{L}_n(D). By the above, we have

SLn(D)⊃(GLn(D),GLn(D))⊃(SLn(D),SLn(D)) \mathbf{S}\mathbf{L}_n(D)\supset (\mathbf{G}\mathbf{L}_n(D),\mathbf{G}\mathbf{L}_n(D))\supset (\mathbf{S}\mathbf{L}_n(D),\mathbf{S}\mathbf{L}_n(D))

To prove c), it suffices to prove that the matrices Bij(λ)B_{ij}(\lambda ) are commutators in SLn(D)\mathbf{S}\mathbf{L}_n(D).

Suppose n⩾3n\geqslant 3. If i,j,ki,j,k are distinct integers in the interval [1,n][1, n] and μ,ν\mu, \nu are elements of D, then we have

Bij(μν)=Bik(μ)−1Bkj(ν)−1Bik(μ)Bkj(ν)(30) B_{ij}(\mu\nu ) =B_{ik}(\mu)^{-1}B_{kj}(\nu )^{-1}B_{ik}(\mu)B_{kj}(\nu ) \tag{30}

By taking μ=1\mu= 1 and ν=λ\nu =\lambda, we see that the matrix Bij(λ)B_{ij}(\lambda ) is a commutator of elements of SLn(D)\mathbf{S}\mathbf{L}_n(D).

Now suppose n=2n= 2. Let uu and vv be elements of D with u≠0u\not= 0. We have the relations

(31) (1v−uvu01)=(u00u−1)(1−v01)(u−100u)(1v01)\begin{pmatrix} 1 & v-uvu \\ 0 & 1 \end{pmatrix} = \begin{pmatrix} u & 0 \\ 0 & u^{-1} \end{pmatrix}\begin{pmatrix} 1 & -v \\ 0 & 1 \end{pmatrix}\begin{pmatrix} u^{-1} & 0 \\ 0 & u \end{pmatrix}\begin{pmatrix} 1 & v \\ 0 & 1 \end{pmatrix} and

(32) (10v−uvu1)=(u−100u)(10−v1)(u00u−1)(10v1)\begin{pmatrix} 1 & 0 \\ v-uvu & 1 \end{pmatrix} = \begin{pmatrix} u^{-1} & 0 \\ 0 & u \end{pmatrix}\begin{pmatrix} 1 & 0 \\ -v & 1 \end{pmatrix}\begin{pmatrix} u & 0 \\ 0 & u^{-1} \end{pmatrix}\begin{pmatrix} 1 & 0 \\ v & 1 \end{pmatrix}.

We have det (u00u−1)\begin{pmatrix} u & 0 \\ 0 & u^{-1} \end{pmatrix} = 1, so the matrices B12(v−uvu)B_{12}(v-uvu) and B21(v−uvu)B_{21}(v-uvu) are commutators of elements of SLn(D)\mathbf{S}\mathbf{L}_n(D).

Suppose that the field D has at least four elements. Let λ\lambda be an element of D. If λ\lambda is equal to 0, 1, or −1-1, choose an arbitrary element uu in D−{0,1,−1}D-\{0,1,-1\}; otherwise, set u=λu=\lambda. In both cases, uu is a nonzero element of D, it commutes with λ\lambda, and we have u2≠1u^2\not= 1. Set v=λ(1−u2)−1v=\lambda (1-u^2)^{-1}. We have uv=vuuv=vu and therefore v−uvu=v(1−u2)=λv-uvu=v(1-u^2) =\lambda. It then follows from relations (31) and (32) that the matrices B12(λ)B_{12}(\lambda ) and B21(λ)B_{21}(\lambda ) are commutators in SLn(D)\mathbf{S}\mathbf{L}_n(D). This completes the proof of c).

C) It remains to prove that SL2(D)\mathbf{S}\mathbf{L}_2(D) is the derived group of GL2(D)\mathbf{G}\mathbf{L}_2(D) when D has three elements. By A), the group SL2(D)\mathbf{S}\mathbf{L}_2(D) is generated by the matrices B12(1)=(1101)B_{12}(1) = \begin{pmatrix} 1 & 1 \\ 0 & 1 \end{pmatrix} and B21(1)=(1011)B_{21}(1) = \begin{pmatrix} 1 & 0 \\ 1 & 1 \end{pmatrix}, and these matrices are commutators of elements of GL2(D)\mathbf{G}\mathbf{L}_2(D) because we have B21(1)=tB12(1)B_{21}(1) =^tB_{12}(1) and

(33) (1101)=(−1001)(1101)(−1001)−1(1101)−1\begin{pmatrix} 1 & 1 \\ 0 & 1 \end{pmatrix} = \begin{pmatrix} -1 & 0 \\ 0 & 1 \end{pmatrix}\begin{pmatrix} 1 & 1 \\ 0 & 1 \end{pmatrix}\begin{pmatrix} -1 & 0 \\ 0 & 1 \end{pmatrix}^{-1}\begin{pmatrix} 1 & 1 \\ 0 & 1 \end{pmatrix}^{-1}.

Remark 00QH

If D is a field with two elements, then GL2(D)\mathbf{G}\mathbf{L}_2(D) is equal to SL2\mathbf{S}\mathbf{L}_2(D), and it is a group of order 6 whose derived group has order 3. If D is a field with three elements, then the group SL2(D)\mathbf{S}\mathbf{L}_2(D) has order 24, and its derived group has order 8. Suppose n⩾2n\geqslant 2; except in the two previous cases, every normal subgroup of SLn(D)\mathbf{S}\mathbf{L}_n(D) distinct from SLn(D)\mathbf{S}\mathbf{L}_n(D) is contained in the center Z(SLn(D))Z(\mathbf{S}\mathbf{L}_n(D)) of SLn(D)\mathbf{S}\mathbf{L}_n(D) (II, §10, p. 421, Exercises 13 and 14). The group SLn(D)/Z(SLn(D))\mathbf{S}\mathbf{L}_n(D)/Z(\mathbf{S}\mathbf{L}_n(D)) is then simple.

Let V be a right vector space over the field D, of finite dimension nn. We denote by SL(V), and call unimodular group of V, the kernel of the homomorphism det:GL(V)→Dab∗:\mathbf{G}\mathbf{L}(V)\rightarrow D^*_{ab}. Choosing a basis of V allows one to identify this group with SLn(D)\mathbf{S}\mathbf{L}_n(D).

We say that an automorphism uu of V is a transvection if there exist a vector vv of V and a linear form φ\varphi on V such that φ(v)=0\varphi (v) = 0 and u(x)=x+vφ(x)u(x) =x+v\varphi (x) for every xx in V. When n⩾2,un\geqslant 2,u is a transvection if and only if there exists a basis of V with respect to which the matrix of uu is of the form Bij(λ)B_{ij}(\lambda ). Theorem 1 implies the following corollary.

Cites 2

Cites II § 10. Matrices, Theorem 1

Corollary 00RU

Let V be a right vector space over the field D, of finite dimension n⩾2n\geqslant 2.

a) The subgroup SL(V)\mathbf{S}\mathbf{L}(V) of GL(V)\mathbf{G}\mathbf{L}(V) is generated by the transvections.

b) The subgroup SL(V)\mathbf{S}\mathbf{L}(V) is the derived group of GL(V)\mathbf{G}\mathbf{L}(V) unless we have n=2n= 2 and D has two elements.

c) The group SL(V)\mathbf{S}\mathbf{L}(V) is equal to its derived group unless we have n=2n= 2 and D has two or three elements.

Exercises

See the exercises for Appendix 2.

Transcribed from the printed edition, 2023, Springer Nature. Not translated.