Bourbaki

§ 3. Actions

1. Actions

Definition 1

Let Ω\Omega and E be two sets. A mapping of Ω\Omega into the set EEE^E of mappings of E into itself is called an action of Ω\Omega on E.

Cites 1

Cites Proposition 3, E II § 5

Let α↦fα\alpha \mapsto f_\alpha be an action of Ω\Omega on E. The mapping (α,x)↦fα(x)(\alpha, x) \mapsto f_\alpha(x) (resp. (x,α)↦fα(x)(x, \alpha) \mapsto f_\alpha(x)) is called the law of left (resp. right) action of Ω\Omega on E† associated with the given action of Ω\Omega on E. Given a mapping gg of Ω×E\Omega \times E (resp. E×ΩE \times \Omega) into E, there exists one and only one action α↦fα\alpha \mapsto f_\alpha of Ω\Omega on E such that the associated law of left (resp. right) action is gg (Set Theory, II, § 5, no. 2, Proposition 3).

In this chapter we shall say, for the sake of abbreviation, "law of action"

† Or sometimes the external law of composition on E with Ω\Omega as operating set.

instead of "law of left action". The element fα(x)f_\alpha(x) of E (for α∈Ω\alpha \in \Omega and x∈Ex \in E) is sometimes called the transform of xx under α\alpha or the composition of α\alpha and xx. It is often denoted by left (resp. right) multiplicative notation α.x\alpha . x (resp. x.αx . \alpha), the dot may be omitted; the composition of α\alpha and xx is then called the product of α\alpha and xx (resp. xx and α\alpha). The exponential notation xαx^\alpha is also used. In the arguments of the following paragraphs we shall generally use the notation α⊥x\alpha \perp x. The elements of Ω\Omega are often called operators.

Example

(1) Let E be an associative magma written multiplicatively. The mapping which associates with a strictly positive integer nn the mapping x↦xnx \mapsto x^n of E into itself is an action of N∗\mathbf{N}^* on E. If E is a group, the mapping which associates with a rational integer aa the mapping x↦xax \mapsto x^a of E into E is an action of Z\mathbf{Z} on E.

(2) Let E be a magma with law denoted by ⊤\top. The mapping which associates with x∈Ex \in E the mapping A↦x⊤AA \mapsto x \top A of the set of subsets of E into itself is an action of E on P(E)\mathscr{P}(E).

(3) Let E be a set. The identity mapping of EEE^E is an action of EEE^E on E, called the canonical action. The corresponding law of action is the mapping (f,x)↦f(x)(f, x) \mapsto f(x) of EE×EE^E \times E into E.

(4) Let (Ωi)i∈I(\Omega_i)_{i \in I} be a family of sets. For all i∈Ii \in I, let fi:Ωi→EEf_i : \Omega_i \to E^E be an action of Ωi\Omega_i on E. Let Ω\Omega be the sum of the Ωi\Omega_i (Set Theory, II, § 4, no. 8). The mapping ff of Ω\Omega onto EEE^E, extending the fif_i, is an action of Ω\Omega on E. This allows us to reduce the study of a family of actions to that of a single action.

(5) Given an action of Ω\Omega on E with law denoted by ⊥\perp, a subset Ξ\Xi of Ω\Omega and a subset X of E, Ξ⊥X\Xi \perp X denotes the set of α⊥x\alpha \perp x with α∈Ξ\alpha \in \Xi and x∈Xx \in X; when Ξ\Xi consists of a single element α\alpha, we generally write α⊥X\alpha \perp X instead of {α}⊥X\{\alpha\} \perp X. The mapping which associates with α∈Ω\alpha \in \Omega the mapping X↦α⊥XX \mapsto \alpha \perp X is an action of Ω\Omega on P(E)\mathscr{P}(E), which is said to be derived from the given action by extension to the set of subsets.

(6) Let α↦fα\alpha \mapsto f_\alpha be an action of Ω\Omega on E. Let g be a mapping of Ω′\Omega' into Ω\Omega. Then the mapping β↦fg(β)\beta \mapsto f_{g(\beta)} is an action of Ω′\Omega' on E.

(7) Let f:E×E→Ef : E \times E \to E be a law of composition on a set E. The mapping γ:x↦γx\gamma : x \mapsto \gamma_x (resp. δ:x↦δx\delta : x \mapsto \delta_x) (§ 2, no. 2) which associates with the element x∈Ex \in E left (resp. right) translation by xx is an action of E on itself; it is called the left (resp. right) action of E on itself derived from the given law. When ff is commutative, these two actions coincide.

The law of left (resp. right) action associated with γ\gamma is ff (resp. the opposite law to ff). The law of right (resp. left) action associated with δ\delta is ff (resp. the opposite law to ff).

Let Ω,E,F\Omega, E, F be sets, α↦fα\alpha \mapsto f_\alpha an action of Ω\Omega on E and α↦gα\alpha \mapsto g_\alpha an action of Ω\Omega on F. An Ω\Omega-*morphism of E into F*, or mapping of E into F compatible with the action of Ω\Omega, is a mapping hh of E into F such that

gα(h(x))=h(fα(x)) g_\alpha(h(x)) = h(f_\alpha(x))

for all α∈Ω\alpha \in \Omega and x∈Ex \in E. The composition of two Ω\Omega-morphisms is an Ω\Omega-morphism.

Let Ω,Ξ,E,F\Omega, \Xi, E, F be sets, α↦fα\alpha \mapsto f_\alpha an action of Ω\Omega on EE, β↦gβ\beta \mapsto g_\beta an action of Ξ\Xi on FF and ϕ\phi a mapping of Ω\Omega into Ω′\Omega'. A ϕ\phi-morphism of EE into FF is a mapping hh of EE into FF such that

gϕ(α)(h(x))=h(fα(x)) g_{\phi(\alpha)}(h(x)) = h(f_\alpha(x))
for all α∈Ω\alpha \in \Omega and x∈Ex \in E.

Cites 2

Cites E II § 4. Union and intersection of a family of sets, I § 2. Identity element; cancellable elements; invertible elements

2. Subsets stable under an action. Induced action

Definition 2

A subset AA of a set EE is called stable under an action α↦fα\alpha \mapsto f_\alpha of Ω\Omega on EE if fα(A)⊂Af_\alpha(A) \subset A for all α∈Ω\alpha \in \Omega. An element xx of EE is called invariant under an element α\alpha of Ω\Omega if fα(x)=xf_\alpha(x) = x.

The intersection of a family of stable subsets of EE under a given action is stable. There therefore exists a smallest stable subset of EE containing a given subset XX of EE; it is said to be generated by XX; it consists of the elements (fα1∘fα2∘⋯∘fαn)(x)(f_{\alpha_1} \circ f_{\alpha_2} \circ \cdots \circ f_{\alpha_n})(x), where x∈X,n≥0,αi∈Ωx \in X, n \geq 0, \alpha_i \in \Omega for all ii.

Remark

Let EE be a magma with law denoted by τ\tau. It should be noted that a subset AA of EE which is stable under the left action on EE on itself is not necessarily stable under the right action of EE on itself; a subset AA of EE stable under the left (resp. right) action of EE on itself is stable under the law on EE but the converse is not in general true. More precisely, AA is stable under the law on EE if and only if AτA⊂AA \tau A \subset A whereas AA is stable under the left (resp. right) action on EE on itself if and only if EτA⊂AE \tau A \subset A (resp. AτE⊂AA \tau E \subset A).

Example

Take the magma EE to be the set N\mathbf{N} with multiplication. The set {1}\{1\} is stable under the internal law of N\mathbf{N}, but the stable subset under the action of N\mathbf{N} on itself generated by {1}\{1\} is the whole of N\mathbf{N}.

Definition 3

Let α↦fα\alpha \mapsto f_\alpha be an action of Ω\Omega on EE and AA a stable subset of EE. The mapping which associates with an element α∈Ω\alpha \in \Omega the restriction of fαf_\alpha to AA (considered as a mapping of AA into itself) is an action of Ω\Omega on AA said to be induced by the given action.

3. Quotient action

Definition 4

Let α↦fα\alpha \mapsto f_\alpha be an action of a set Ω\Omega on a set EE. An equivalence relation RR on EE is said to be compatible with the given action if, for all elements xx and yy of EE such that x≡y(modR)x \equiv y \pmod{R} and all α∈Ω,fα(x)≡fα(y)(modR)\alpha \in \Omega, f_\alpha(x) \equiv f_\alpha(y) \pmod{R}. The mapping which associates with an element α∈Ω\alpha \in \Omega the mapping of E/RE/R into itself derived from fαf_\alpha by passing to the quotients is an action of Ω\Omega on E/RE/R called the quotient of the action of Ω\Omega on EE.

Cites 1

Cites I § 1. Laws of composition; associativity; commutativity

Let EE be a magma and RR an equivalence relation on EE. RR is said to be left (resp. right) compatible with the law on EE if it is compatible with the left (resp.

right) action of E on itself derived from the law on E. For R to be compatible with the law on E it is necessary and sufficient that it be left and right compatible with the law on E.

We leave to the reader the statement and proof of the analogues of Propositions 6, 7 and 8 of § 1, no. 6.

4. Distributivity

Definition 5

Let E1,…,EnE_1, \ldots, E_n and F be sets and u a mapping of E1×⋯×EnE_1 \times \cdots \times E_n into F. Let i∈{1,n}i \in \{1, n\}. Suppose EiE_i and F are given the structures of magmas. u is said to be distributive relative to the index variable i if the partial mapping

xi↦u(a1,…,ai−1,xi,ai+1,…,an) x_i \mapsto u(a_1, \ldots, a_{i-1}, x_i, a_{i+1}, \ldots, a_n)

is a homomorphism of EiE_i into F for all fixed aja_j in EjE_j and j≠ij \neq i.

Cited by 1

Cited by Remark

If ⊤\top denotes the internal laws on EiE_i and F, the distributivity of u is given by the equations

(1)

u(a1,…,ai−1,xi⊤xi′,ai+1,an)=u(a1,…,ai−1,xi,ai+1,…,an)⊤u(a1,…,ai−1,xi′,ai+1,…,an) u(a_1, \ldots, a_{i-1}, x_i \top x'_i, a_{i+1}, a_n) \\ = u(a_1, \ldots, a_{i-1}, x_i, a_{i+1}, \ldots, a_n) \top u(a_1, \ldots, a_{i-1}, x'_i, a_{i+1}, \ldots, a_n)

for i=1,2,…,n,a1∈E1,…,ai−1∈Ei−1,xi∈Ei,xi′∈Ei,ai+1∈Ei+1,…,an∈Eni = 1, 2, \ldots, n, a_1 \in E_1, \ldots, a_{i-1} \in E_{i-1}, x_i \in E_i, x'_i \in E_i, a_{i+1} \in E_{i+1}, \ldots, a_n \in E_n.

Example

Let E be a monoid (resp. group) written multiplicatively. The mapping (n,x)↦xn(n, x) \mapsto x^n of N×E\mathbf{N} \times E (resp. Z×E\mathbf{Z} \times E) into E is distributive with respect to the first variable by the equation xm+n=xmxnx^{m+n} = x^m x^n (with addition as law on N\mathbf{N}). If E is commutative, this mapping is distributive with respect to the second variable by the equation (xy)n=xnyn(xy)^n = x^n y^n.

Proposition 1

Let E1,E2,…,EnE_1, E_2, \ldots, E_n and F be commutative monoids written additively and let u be a mapping of E1×⋯×EnE_1 \times \cdots \times E_n into F, which is distributive with respect to all the variables. For i=1,2,…,ni = 1, 2, \ldots, n, let LiL_i be a non-empty finite set and (xi,λ)λ∈Li(x_{i,\lambda})_{\lambda \in L_i} a family of elements of EiE_i. Let yi=∑λ∈Lixi,λy_i = \sum_{\lambda \in L_i} x_{i,\lambda} for i=1,2,…,ni = 1, 2, \ldots, n. Then

Cites 1 · Cited by 2

Cites I § 1. Laws of composition; associativity; commutativity

Cited by Proposition 2, I § 4, I § 8. Rings

(2)

u(y1,…,yn)=∑αu(x1,α1,…,xn,αn) u(y_1, \ldots, y_n) = \sum_\alpha u(x_1, \alpha_1, \ldots, x_n, \alpha_n)

the sum being taken over all sequences α=(α1,…,αn)\alpha = (\alpha_1, \ldots, \alpha_n) belonging to L1×⋯×LnL_1 \times \cdots \times L_n.

We argue by induction on n, the case n=1n = 1 following from formula (2) of § 1, no. 2. From the same reference

(3)

u(y1,…,yn−1,yn)=∑αn∈Lnu(y1,…,yn−1,xn,αn) u(y_1, \ldots, y_{n-1}, y_n) = \sum_{\alpha_n \in L_n} u(y_1, \ldots, y_{n-1}, x_n, \alpha_n)

for yn=∑αn∈Lnxn,αny_n = \sum_{\alpha_n \in L_n} x_{n,\alpha_n} and the mapping z↦u(y1,…,yn−1,z)z \mapsto u(y_1, \ldots, y_{n-1}, z) of EnE_n into FF is a magma homomorphism. By the induction hypothesis applied to the distributive mappings (z1,…,zn−1)↦u(z1,…,zn−1,xn,αn)(z_1, \ldots, z_{n-1}) \mapsto u(z_1, \ldots, z_{n-1}, x_n, \alpha_n) from E1×⋯×En−1E_1 \times \cdots \times E_{n-1} to FF,

(4)

u(y1,…,yn−1,xn,αn)=∑α1,…,αn−1u(x1,α1,…,xn−1,αn−1,xn,αn), u(y_1, \ldots, y_{n-1}, x_n, \alpha_n) = \sum_{\alpha_1, \ldots, \alpha_{n-1}} u(x_1, \alpha_1, \ldots, x_{n-1}, \alpha_{n-1}, x_n, \alpha_n),
the sum being taken over the sequences (α1,…,αn−1)(\alpha_1, \ldots, \alpha_{n-1}) belonging to M=L1×⋯×Ln−1M = L_1 \times \cdots \times L_{n-1}. Now L1×⋯×Ln=M×LnL_1 \times \cdots \times L_n = M \times L_n; writing
tα1,…,αn=u(x1,α1,…,xn,αn), t_{\alpha_1, \ldots, \alpha_n} = u(x_1, \alpha_1, \ldots, x_n, \alpha_n),
we have (5)
∑α1,…,αntα1,…,αn=∑αn(∑α1,…,αn−1tα1,…,αn−1,αn) \sum_{\alpha_1, \ldots, \alpha_n} t_{\alpha_1, \ldots, \alpha_n} = \sum_{\alpha_n} \left( \sum_{\alpha_1, \ldots, \alpha_{n-1}} t_{\alpha_1, \ldots, \alpha_{n-1}, \alpha_n} \right)
by formula (7) of § 1, no. 5. (2) follows immediately from (3), (4) and (5).

Remark

If u(a1,…,ai−1,0,ai+1,…,an)=0u(a_1, \ldots, a_{i-1}, 0, a_{i+1}, \ldots, a_n) = 0 for i=1,2,…,ni = 1, 2, \ldots, n and aj∈Eja_j \in E_j (j≠ij \neq i), then formula (2) remains true for families (xi,λ)λ∈Li(x_i, \lambda)_{\lambda \in L_i} of finite support.

A special case of Definition 5 is that where uu is the law of action associated with the action of a set Ω\Omega on a magma EE. If uu is distributive with respect to the second variable, it is also said that the action of Ω\Omega on the magma EE is distributive. In other words:

Cites 1

Cites Definition 5

Definition 6

An action* α↦fα\alpha \mapsto f_\alpha of a set Ω\Omega on a magma EE is said to be distributive if, for all α∈Ω\alpha \in \Omega, the mapping fαf_\alpha is an endomorphism of the magma EE.

Cites 1

Cites I § 1. Laws of composition; associativity; commutativity

If ⊤\top denotes the law of the magma EE and ⊥\perp the law of action associated with the action of Ω\Omega on EE, the distributivity of the latter is then expressed by the formula (6)

α⊥(x⊤y)=(α⊥x)⊤(α⊥y)(for α∈Ω and x,y∈E). \alpha \perp (x \top y) = (\alpha \perp x) \top (\alpha \perp y) \quad \text{(for } \alpha \in \Omega \text{ and } x, y \in E\text{)}.

By an abuse of language, it is also said that the law ⊥\perp is distributive (or right distributive) with respect to the law ⊤\top.

Formula (2) of § 1, no. 2 shows that then, for every ordered sequence (xλ)λ∈L(x_\lambda)_{\lambda \in L} of elements of EE and every α∈Ω\alpha \in \Omega, (7)

α⊥(⋀λ∈Lxλ)=⋀λ∈L(α⊥xλ). \alpha \perp \left( \bigwedge_{\lambda \in L} x_\lambda \right) = \bigwedge_{\lambda \in L} (\alpha \perp x_\lambda).

If an action α↦fα\alpha \mapsto f_\alpha is distributive and an equivalence relation RR on EE is compatible with the law of composition of EE and the action α↦fα\alpha \mapsto f_\alpha, the quotient action on E/RE/R is distributive.

When the law on EE is written multiplicatively, we often use the exponential notation xαx^\alpha for a law of action which is distributive with respect to this multiplication, so that distributivity is expressed by the identity (xy)α=xαyα(xy)^\alpha = x^\alpha y^\alpha. If the law on E is written additively, we often use left (resp. right) multiplicative notation α.x\alpha . x (resp. x.αx . \alpha) for a law of action which is distributive with respect to this addition, the distributivity being expressed by the identity

α(x+y)=αx+αy(resp. (x+y)α=xα+yα). \alpha(x + y) = \alpha x + \alpha y \quad (\text{resp. } (x + y)\alpha = x\alpha + y\alpha).

We may also consider the case where Ω\Omega has an internal law, denoted by T‾\overline{T}, and the law of action is distributive with respect to the first variable, which means that

(8)

(αT‾β)⊥x=(α⊥x)T(β⊥x) (\alpha \overline{T} \beta) \perp x = (\alpha \perp x) T (\beta \perp x)
for all α,β∈Ω\alpha, \beta \in \Omega and x∈Ex \in E. Then, by formula (2) of § 1, no. 2

(9)

(T‾λ∈Lαλ)⊥x=T‾λ∈L(αλ⊥x) \left( \overline{T}_{\lambda \in L} \alpha_{\lambda} \right) \perp x = \overline{T}_{\lambda \in L} (\alpha_{\lambda} \perp x)
for every ordered sequence (αλ)λ∈L(\alpha_{\lambda})_{\lambda \in L} of elements of Ω\Omega and all x∈Ex \in E.

5. Distributivity of one internal law with respect to another

Definition 7

Let TT and ⊥\perp be two internal laws on a set E. The law ⊥\perp is said to be distributive with respect to the law TT if

(10)

x⊥(yTz)=(x⊥y)T(x⊥z) x \perp (y T z) = (x \perp y) T (x \perp z)
(11)
(xTy)⊥z=(x⊥z)T(y⊥z) (x T y) \perp z = (x \perp z) T (y \perp z)
for all x,y,zx, y, z in E.

Note that (10) and (11) are equivalent if the law ⊥\perp is commutative. In general, one of the laws is written additively and the other multiplicatively; if multiplication is distributive with respect to addition, then:

(12)

x.(y+z)=x.y+x.z x . (y + z) = x . y + x . z
(13)
(x+y).z=x.z+y.z (x + y) . z = x . z + y . z

Example

(1) In the set P(E)\mathscr{P}(E) of subsets of a set E, each of the internal laws ∩\cap and ∪\cup is distributive with respect to itself and the other. This follows from formulae of the form

A∩(B∪C)=(A∩B)∪(A∩C) A \cap (B \cup C) = (A \cap B) \cup (A \cap C)
A∪(B∩C)=(A∪B)∩(A∪C). A \cup (B \cap C) = (A \cup B) \cap (A \cup C).

(2) In Z\mathbf{Z} (and more generally, in any totally ordered set) each of laws sup and inf is distributive with respect to the other and with respect to itself.

(3) In Z\mathbf{Z}(and more generally in any ring) multiplication is distributive with respect to addition.

(4) In N\mathbf{N} addition and multiplication are distributive with respect to the laws sup and inf.

Exercises

See the exercises for § 3.

Transcribed from the printed edition, 1998, Springer. Not translated.