Bourbaki

Proposition 1

Tag 05YX, permanent. Cite it as [Bourbaki, Tag 05YX].

Algebra, chapter III, § 2. Examples of algebras

A quadratic algebra E is associative and commutative.

The fact that E is commutative follows from the equation e1e2=e2e1e_1 e_2 = e_2 e_1 in (2); similarly, to verify associativity, it suffices to see that x(yz)=(xy)zx(yz) = (xy)z when x,y,zx, y, z are each equal to e1e_1 or e2e_2. Now, this relation is obvious if at least one of the elements x,y,zx, y, z is equal to e1e_1; it is also true for x=y=z=e2x = y = z = e_2 since E is commutative; whence the proposition.

Let ee denote the unit element of a quadratic algebra E and let (e,i)(e, i) be a basis of E of type (α,β)(\alpha, \beta); every other basis of E containing ee is therefore of the form (e,j)(e, j) with j=γe+δij = \gamma e + \delta i (II, § 7, no. 2, Corollary to Proposition 3); moreover, for (e,j)(e, j) to be a basis of E, it is necessary and sufficient that δ\delta be invertible in A; the condition is obviously sufficient; conversely, if iˉ\bar{i} is the canonical image of ii in E/AeE/Ae, iˉ\bar{i} and jˉ=δiˉ\bar{j} = \delta \bar{i} must each form a basis of E/AeE/Ae, whence the necessity of the condition. Then

j2=(γ2+αδ2)e+(2γδ+βδ2)i=(αδ2−γ2−βγδ)e+(2γ+βδ)j; j^2 = (\gamma^2 + \alpha \delta^2)e + (2\gamma \delta + \beta \delta^2)i = (\alpha \delta^2 - \gamma^2 - \beta \gamma \delta)e + (2\gamma + \beta \delta)j;

thus it is seen that E is of type

(αδ2−γ2−βγδ,2γ+βδ) (\alpha \delta^2 - \gamma^2 - \beta \gamma \delta, 2\gamma + \beta \delta)

for all invertible δ∈A\delta \in A and all γ∈A\gamma \in A. In particular, if EE is of type (α,2β′)(\alpha, 2\beta'), ii is also of type (α+β′2,0)(\alpha + {\beta'}^2, 0) as is seen by taking γ=−β′\gamma = -\beta' and δ=1\delta = 1.

Bourbaki puts the proof directly after the statement, so what is above is the statement and its proof together.

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