Bourbaki

§ 8. Types of quadratic forms

In this paragraph we suppose that A is a commutative field.

1. Types of quadratic forms.

Given a quadratic form Q (§3,n°4§ 3, n° 4) on a vector space E over A, we shall say that E is the space of defini-

(*) These results (unpublished) were communicated to us by I. Kaplansky.

tion of Q and that dim(E) is the dimension of Q. Given two quadratic forms Q, Q' on vector spaces E, E' over A, we shall denote by Q ⊕ Q' their direct sum (§ 3, no 4). Recall that the direct sum of two neutral forms is neutral (§ 4, no 2).

Let us introduce the following relation:

« Q and Q' are non-degenerate quadratic forms of finite dimensions over A, and there exist neutral quadratic forms N, N' such that Q ⊕ N is equivalent to Q' ⊕ N' ».

This relation, which we shall denote by Q ~ Q', is manifestly reflexive and symmetric. It is also transitive: indeed, if Q, Q', Q'' are quadratic forms such that Q ~ Q' and Q' ~ Q'', there exist neutral quadratic forms M, M', N, N' such that Q ⊕ M is equivalent to Q' ⊕ M' and Q' ⊕ N to Q'' ⊕ N' ; then Q ⊕ (M ⊕ N) is equivalent to (Q ⊕ M) ⊕ N, hence to (Q' ⊕ M') ⊕ N, and also to (Q' ⊕ N) ⊕ M', hence again to (Q'' ⊕ N') ⊕ M' and to Q'' ⊕ (N' ⊕ M') ; since M ⊕ N and N' ⊕ M' are neutral, we indeed have Q ~ Q''. The relation Q ~ Q' is therefore an equivalence relation between Q and Q'. It is clear that, if Q and Q' are two non-degenerate quadratic forms of finite dimensions and equivalent, we have Q ~ Q'.

For every quadratic form Q over A, non-degenerate and of finite dimension, we shall put

(1)

θ(Q)=τx(X∼Q), \theta(Q) = \tau_x(X \sim Q),
and we shall say that θ(Q)\theta(Q) is the type of Q. If Q and Q' are two quadratic forms over A, non-degenerate and of finite dimensions, the relations Q ~ Q' and θ(Q)=θ(Q′)\theta(Q) = \theta(Q') are equivalent.

Proposition 1

Let Q and Q' be two quadratic forms over A, non-degenerate and of finite dimensions. In order that Q and Q' be equivalent, it is necessary and sufficient that they have the same dimension and the same type.

The condition is obviously necessary. Suppose that it is satisfied. There then exist neutral forms N, N' such that Q ⊕ N and Q' ⊕ N' are equivalent. Since these two forms have the same dimension, the same is true of N and N', which are consequently equivalent (§ 4, no 2, cor. 2 of prop. 2). Hence Q and Q' are equivalent by virtue of Witt's theorem (§ 4, no 3, cor. 1 of th. 1).

Proposition 2

The relation « there exists a quadratic form Q over A, non-degenerate and of finite dimension, such that X = θ(Q) » is collectivizing in X (Ens., chap. II, § 1, n° 4).

Indeed, let V be an infinite-dimensional vector space over A, S\mathfrak{S} the set of non-degenerate quadratic forms defined on the finite-dimensional subspaces of V, and W\mathfrak{W} the set of the θ(Q)\theta(Q) for Q∈SQ \in \mathfrak{S}. It is clear that every non-degenerate quadratic form Q′Q' of finite dimension over A is equivalent to at least one element of S\mathfrak{S}; whence θ(Q′)∈W\theta(Q') \in \mathfrak{W}, which proves our assertion.

2. Group of types of quadratic forms.

We shall endow the set W\mathfrak{W} of the types of non-degenerate quadratic forms of finite dimensions over A with a commutative group structure. We shall define an addition in W\mathfrak{W} by the formula

T+T′=θ(TτT′)(2) T + T' = \theta(T \tau T') \tag{2}

This addition is commutative since T′τTT' \tau T is equivalent to TτT′T \tau T'. It is associative because, if T,T′T, T' and T′′T'' are elements of W\mathfrak{W}, we have

(T+T′)+T′′∼(T+T′)τT′′∼(TτT′)τT′′ (T + T') + T'' \sim (T + T') \tau T'' \sim (T \tau T') \tau T''
∼Tτ(T′τT′′)∼Tτ(T′+T′′)∼T+(T′+T′′), \sim T \tau (T' \tau T'') \sim T \tau (T' + T'') \sim T + (T' + T''),
whence (T+T′)+T′′=T+(T′+T′′)(T + T') + T'' = T + (T' + T'') since two elements of W\mathfrak{W} which have the same type are equal. Moreover the addition which we have just defined possesses an identity element: it is clear indeed that all neutral forms have the same type T0T_0, namely that of the zero form of zero dimension; we see at once that T0T_0 is the identity element sought. Finally the existence, for every T∈WT \in \mathfrak{W}, of an element opposite to T follows at once from the following proposition:

Proposition 3

Let Q be a non-degenerate quadratic form of finite dimension on a vector space V over A. Let – Q denote the quadratic form on V defined by (−Q)(x)=−Q(x)(-Q)(x) = -Q(x) (x∈Vx \in V). Then the form Qτ(−Q)Q \tau (-Q) is neutral.

Indeed the restriction of Qτ(−Q)Q \tau (-Q) to the diagonal D of V×VV \times V is zero. The index of this form is therefore ⩾12dim⁡(V×V)\geqslant \frac{1}{2} \dim (V \times V) (§ 4, no 2, déf. 2), and consequently is equal to 12dim⁡(V×V)\frac{1}{2} \dim (V \times V) (ibid., formula (4)). It follows that Qτ(−Q)Q \tau (-Q) is neutral (ibid.).

This permits us to give the following definition:

Definition 1

The set of types of non-degenerate quadratic forms of finite dimensions over AA, endowed with the addition defined by (2), is called the group of types of quadratic forms, or Witt group, of AA.

Remarks. — 1) Every non-degenerate quadratic form QQ of finite dimension whose type is zero (i.e. such that θ(Q)=T0\theta(Q) = T_0 with the above notation) is a neutral form. There indeed exist neutral forms N,N′N, N' such that QτNQ \tau N is equivalent to N′N'. This shows that QQ is of even dimension, and hence that there exists a neutral form N1N_1 having the same dimension as QQ. Since QQ and N1N_1 have the same type, it follows from prop. 1 that they are equivalent, and hence that QQ is neutral.

2) For every finite-dimensional quadratic form QQ over AA, let δ(Q)\delta(Q) denote the class modulo 2 of the dimension of QQ. We have

δ(QτQ′)=δ(Q)+δ(Q′). \delta(Q \tau Q') = \delta(Q) + \delta(Q').
Since every neutral form NN is of even dimension, we have δ(N)=0\delta(N) = 0; the relation Q∼Q′Q \sim Q' therefore entails δ(Q)=δ(Q′)\delta(Q) = \delta(Q'). Thus the restriction of δ\delta to the group W\mathfrak{W} of types of quadratic forms over AA is a homomorphism of W\mathfrak{W} into the group Z/(2)\mathbf{Z}/(2). This homomorphism is surjective when AA is of characteristic ≠2\neq 2, but is not so if AA is of characteristic 2, since a quadratic form of odd dimension is then degenerate, its associated bilinear form being alternating (cf. § 5).

3) Let aa be an element ≠0\neq 0 of AA. If NN is a neutral form, then so is aNaN. It follows that the relation Q∼Q′Q \sim Q' entails aQ∼aQ′aQ \sim aQ'. For every element TT of the group W\mathfrak{W}, we shall put

a.T=θ(aT). a.T = \theta(aT).
We thus obtain an external composition law between the group A∗A^* of the non-zero elements of AA and the group W\mathfrak{W}. The following formulas result immediately from the definition:
a.(T+T′)=a.T+a.T′,ab.T=a.(b.T) a.(T + T') = a.T + a.T', \quad ab.T = a.(b.T)
(a,b in A∗,T,T′ in W). (a, b \text{ in } A^*, \quad T, T' \text{ in } \mathfrak{W}).

On the other hand, if a,ba, b and a+ba + b are in A∗A^*, one does not in general have (a+b).T=a.T+b.T(a + b).T = a.T + b.T (T∈WT \in \mathfrak{W}).

Proposition 4

Let Q be a non-degenerate quadratic form on a finite-dimensional vector space E over A. Suppose that A is of characteristic ≠2\neq 2, and let (x1,…,xn)(x_1, \ldots, x_n) be an orthogonal basis of V. Let T1T_1 be the type of the quadratic form Q1Q_1 defined on the vector space A and such that Q1(1)=1Q_1(1) = 1. The type of Q is then ∑i=1nQ(xi)⋅T1\sum_{i=1}^n Q(x_i) \cdot T_1.

Indeed the form Q is equivalent to

(Q(x1)Q1)τ…τ(Q(xn)Q1)(Q(x_1)Q_1) \tau \ldots \tau (Q(x_n)Q_1)

Corollary

The hypotheses and notation being those of prop. 3, the elements a.T1a.T_1 (a∈A∗a \in A^*) form a set of generators of the group of types of quadratic forms over A.

To seek the structure of the group of types of quadratic forms over A is therefore to seek the Z\mathbf{Z}-linear relations which exist between the elements of the form a.T1a.T_1. If b∈A∗b \in A^*, the form Q1Q_1 defined in prop. 4 is manifestly equivalent to b2Q1b^2Q_1; hence a.T1=ab2.T1a.T_1 = ab^2.T_1, which shows that a.T1a.T_1 depends only on the class of aa modulo the subgroup (A∗)2(A^*)^2 of squares of elements of A∗A^*. Moreover, it follows from prop. 3 that we have (−a).T1=−a.T1(-a).T_1 = -a.T_1. However, in general there are other Z\mathbf{Z}-linear relations between the a.T1a.T_1 than those which follow from the relations we have just indicated.

Proposition 5

We suppose that A is a maximal ordered field. Let Q be a non-degenerate quadratic form of finite dimension over A, and (s,t)(s, t) its signature (§7§ 7, no 2, def. 2). Then the type of Q is (s−t).T1(s - t).T_1, and the group W\mathfrak{W} of types of quadratic forms over A is an infinite monogenic group generated by T1T_1.

Indeed, since A∗/(A∗)2A^*/(A^*)^2 is of order 2 and (−1).T1=−T1(-1).T_1 = -T_1, W\mathfrak{W} is generated by T1T_1 and is therefore monogenic. For every n>0n > 0, n.T1n.T_1 is the type of the positive non-degenerate quadratic forms of dimension nn; since these forms are not neutral, we have n.T1≠0n.T_1 \neq 0, which shows that W\mathfrak{W} is infinite. Finally, a form of signature (s,t)(s, t) is isomorphic, with the notation of prop. 4, to the direct sum of ss forms Q1Q_1 and of tt forms −Q1- Q_1 (§ 7, n° 2, th. 1); it follows that its type is (s−t).T1(s - t). T_1.

3. Ring of types of quadratic forms.

We shall suppose, in this no., that AA is a field of characteristic ≠2\neq 2.

Given two quadratic forms Q,Q′Q, Q' on vector spaces V,V′V, V' over AA, we shall call tensor product of QQ and Q′Q', and denote by Q⊗Q′Q \otimes Q' the quadratic form on V⊗V′V \otimes V' whose associated bilinear form is the tensor product (§ 1, n° 9, def. 11) of the bilinear forms associated with QQ and Q′Q'. It is readily seen that Q⊗Q′Q \otimes Q' satisfies the relation

(5)(5)
(Q⊗Q′)(x⊗x′)=Q(x)Q′(x′)(x∈V,x′∈V′).(Q \otimes Q')(x \otimes x') = Q(x)Q'(x') \quad (x \in V, x' \in V').

If QQ and Q′Q' are non-degenerate and of finite dimensions, the same is true of Q⊗Q′Q \otimes Q' (§ 1, n° 9, prop. 9).

Let Q,Q′,Q′′Q, Q', Q'' be quadratic forms on the vector spaces V,V′,V′′V, V', V''. Using the canonical isomorphism of V⊗V′V \otimes V' onto V′⊗VV' \otimes V (resp. of (V⊗V′)⊗V′′(V \otimes V') \otimes V'' onto V⊗(V′⊗V′′)V \otimes (V' \otimes V'')), of (V×V′)⊗V′′(V \times V') \otimes V'' onto (V⊗V′′)×(V′⊗V′′)(V \otimes V'') \times (V' \otimes V'')), one sees at once that Q⊗Q′Q \otimes Q' is equivalent to Q′⊗QQ' \otimes Q (resp. (Q⊗Q′)⊗Q′′(Q \otimes Q') \otimes Q'' to Q⊗(Q′⊗Q′′)Q \otimes (Q' \otimes Q''), (QτQ′)⊗Q′′(Q \tau Q') \otimes Q'' to (Q⊗Q′′)τ(Q′⊗Q′′)(Q \otimes Q'') \tau (Q' \otimes Q'')).

Let QQ and Q′Q' be two non-degenerate quadratic forms of finite dimensions. If QQ is neutral, then so is Q⊗Q′Q \otimes Q'. Indeed, let V,V′V, V' be the spaces on which Q,Q′Q, Q' are defined, 2n2n and n′n' their dimensions, and let WW be a totally singular subspace of dimension nn of VV (§ 4, No. 2); then, W⊗V′W \otimes V' is a totally singular subspace, and its dimension is half that of V⊗V′V \otimes V'; it follows, as in prop. 3, that Q⊗Q′Q \otimes Q' is neutral. Analogously Q⊗Q′Q \otimes Q' is neutral whenever Q′Q' is neutral.

It follows from this that, if Q,Q′,Q1,Q1′Q, Q', Q_1, Q'_1 are non-degenerate quadratic forms of finite dimensions over AA, and if one assumes that θ(Q1)=θ(Q)\theta(Q_1) = \theta(Q) and θ(Q1′)=θ(Q′)\theta(Q'_1) = \theta(Q'), then θ(Q1⊗Q1′)=θ(Q⊗Q′)\theta(Q_1 \otimes Q'_1) = \theta(Q \otimes Q'). It is enough in fact to verify this in the case where Q1=QτNQ_1 = Q \tau N and Q1′=Q′τN′Q'_1 = Q' \tau N', NN and N′N' being neutral forms; in this case Q1⊗Q1′Q_1 \otimes Q'_1 is equivalent to

(Q⊗Q′)τ(Q⊗N′τQ′⊗NτN⊗N′) (Q \otimes Q') \tau (Q \otimes N' \tau Q' \otimes N \tau N \otimes N')

and the second parenthesis denotes a neutral form; this proves our assertion.

Let now B\mathfrak{B} be the group of types of quadratic forms over AA. Define, on the set B\mathfrak{B}, a second law of composition, denoted multiplicatively, by the formula

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TT′=θ(T⊗T′)(T,T′ dans B). TT' = \theta(T \otimes T') \qquad (T, T' \text{ dans } \mathfrak{B}).

It follows at once from what we have just seen that this law of composition is commutative, associative and distributive with respect to addition. It has a unit element, namely the type T1T_1 of the quadratic form Q1Q_1 defined on the vector space AA and such that Q1(1)=1Q_1(1) = 1: indeed, according to (5), Q1⊗Q=QQ_1 \otimes Q = Q for every quadratic form QQ. The additive group B\mathfrak{B}, endowed with the multiplication which we have just defined, is therefore a commutative ring with unit element; it is called the ring of types of quadratic forms of AA (or the Witt ring of AA, when there is no danger of confusion).

Remark 1

It is clear that, if aa is an element of A∗A^*, one has

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a.(TT′)=(a.T)T′=T(a.T′) a . (TT') = (a . T)T' = T(a . T')

whatever the elements T,T′T, T' of B\mathfrak{B} may be. It will moreover be observed that one has a.T=TaTa . T = T_a T, denoting by TaT_a the type of the quadratic form aQ1aQ_1 over AA.

Remark 2

Since AA is of characteristic ≠2\neq 2, every element TT of B\mathfrak{B} can be written in the form ∑i=1nai.T1\sum_{i=1}^n a_i . T_1 where ai∈A∗a_i \in A^* (No. 2, prop. 4). One has

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(∑i=1nai.T1)(∑j=1qbj.T1)=∑i,jaibj.T1(ai,bj dans A∗). (\sum_{i=1}^n a_i . T_1)(\sum_{j=1}^q b_j . T_1) = \sum_{i,j} a_i b_j . T_1 \qquad (a_i, b_j \text{ dans } A^*).

Remark 3

Suppose that AA is a maximal ordered field. Then the ring B\mathfrak{B} is isomorphic to Z\mathbf{Z} (prop. 5), the integer corresponding to the type of a form of signature (s, t)(s,\ t) being s−ts - t (ibid.). Since the tensor product of two forms QQ, Q′Q' of signatures (s, t)(s,\ t), (s′, t′)(s',\ t') is a form of dimension (s+t) (s′+t′)(s + t)\,(s' + t'), it follows, by means of an elementary calculus, that the signature of Q⊗Q′Q \otimes Q' is (ss′+tt′, st′+ts′)(ss' + tt',\ st' + ts').

Machine translation of the English, by gpt-5-6-mini, against glossary version 34. Not checked by a person. That model is a cut down version of the one the rest of this language was written by.