Bourbaki

§ 1. Prehilbertian spaces and hilbertian spaces

1. Hermitian forms

We recall the following definition given in Algebra (A, IX, § 3, No. 1):

Definition 1

Let E be a vector space over the field K. A hermitian form (on the left) on E is a map f from E × E into K satisfying the following conditions (for x1,x2,x,y1,y2,yx_1, x_2, x, y_1, y_2, y in E and λ,μ\lambda, \mu in K):

(1)

{f(x1+x2,y)=f(x1,y)+f(x2,y)f(x,y1+y2)=f(x,y1)+f(x,y2) \begin{cases} f(x_1 + x_2, y) = f(x_1, y) + f(x_2, y) \\ f(x, y_1 + y_2) = f(x, y_1) + f(x, y_2) \end{cases}

(2)

{f(λx,y)=λ‾f(x,y)f(x,μy)=μf(x,y) \begin{cases} f(\lambda x, y) = \overline{\lambda} f(x, y) \\ f(x, \mu y) = \mu f(x, y) \end{cases}

(3)

f(x,y)=f(y,x)‾. f(x, y) = \overline{f(y, x)} .

When the field K is R, the notion of hermitian form on E reduces to that of symmetric bilinear form on E × E (A, III, § 6, No. 3).

We note that the second condition (1) and the second condition (2) follow from the other three.

¹ For the reader specially interested in hilbertian spaces, we point out that only No. 7 of § 1 and No. 8 of § 4 depend on results of chapters III and IV. For this the reader can consult « Summary of some important properties of Banach spaces » which appears at the end of this volume. The only references to chapters I and II concern the definition of a convex set and of a semi-norm (II, p. 1 and p. 7), that of a topological direct sum (I, p. 4), of a total family and a topologically independent family (I, p. 12).

From (1) and (2) we deduce immediately that

f(∑jλjxj,∑kμkyk)=∑j,kλ‾jμkf(xj,yk). f(\sum_j \lambda_j x_j, \sum_k \mu_k y_k) = \sum_{j,k} \overline{\lambda}_j \mu_k f(x_j, y_k).

In particular, if E is finite dimensional, and if (ej)1≤j≤n(e_j)_{1 \leq j \leq n} is a basis of E, then for x=∑j=1nξjejx = \sum_{j=1}^n \xi_j e_j and y=∑j=1nηjejy = \sum_{j=1}^n \eta_j e_j, we have,

f(x,y)=∑j,kαjkξ‾jηk f(x, y) = \sum_{j,k} \alpha_{jk} \overline{\xi}_j \eta_k

with the notation αjk=f(ej,ek)\alpha_{jk} = f(e_j, e_k); moreover, relation (3) amounts to αjk=α‾kj\alpha_{jk} = \overline{\alpha}_{kj} for every pair of indices j,kj, k; this implies in particular that the numbers αjj\alpha_{jj} are real.

From (3), the number Q(x)=f(x,x)Q(x) = f(x, x) is real for all x∈Ex \in E. Moreover, we immediately establish the following formulas, known as polarization formulas

(5)

4f(x,y)=∑ε2=1εQ(x+εy)if K is R, 4f(x, y) = \sum_{\varepsilon^2 = 1} \varepsilon Q(x + \varepsilon y) \quad \text{if } K \text{ is } \mathbf{R},
(6)
4f(x,y)=∑ε4=1,ε∈CεQ(x+ε‾y)if K is C. 4f(x, y) = \sum_{\varepsilon^4 = 1, \varepsilon \in \mathbf{C}} \varepsilon Q(x + \overline{\varepsilon} y) \quad \text{if } K \text{ is } \mathbf{C}.

Remark

— We observe that formula (6) is valid for every sesquilinear form on E×EE \times E (that is to say, for every function ff satisfying (1) and (2), but not necessarily (3)). This remark shows that, when K=CK = \mathbf{C}, a sesquilinear form ff such that f(x,x)f(x, x) is real for all x∈Ex \in E is necessarily hermitian: relation (6) then gives f(y,x)‾=f(x,y)\overline{f(y, x)} = f(x, y) since we have y+εx=ε(x+ε‾y)y + \varepsilon x = \varepsilon(x + \overline{\varepsilon} y) and Q(εz)=Q(z)Q(\varepsilon z) = Q(z) whenever ε4=1\varepsilon^4 = 1.

From the polarisation formulas, we have in particular,

Proposition 1

If ff is a hermitian form on EE, and MM a vector subspace of EE such that f(x,x)=0f(x, x) = 0 for all x∈Mx \in M, then we also have f(x,y)=0f(x, y) = 0 for every pair of points x,yx, y in MM.

Let ff be a hermitian form on EE; the set NN of all x∈Ex \in E such that f(x,y)=0f(x, y) = 0 for all y∈Ey \in E is a vector subspace of EE. It follows from (3) that, if x1≡x2x_1 \equiv x_2 (mod. NN) and y1≡y2y_1 \equiv y_2 (mod. NN), we have f(x1,y1)=f(x2,y2)f(x_1, y_1) = f(x_2, y_2); hence, on the quotient space E/NE/N we define a sesquilinear form ff by putting f(x˙,y˙)=f(x,y)f(\dot{x}, \dot{y}) = f(x, y) for all x∈x˙x \in \dot{x} and all y∈y˙y \in \dot{y}; it is clear that ff is hermitian and that the relation «f(x˙,y˙)=0f(\dot{x}, \dot{y}) = 0 for all y˙∈E/N\dot{y} \in E/N» implies x˙=0\dot{x} = 0 in E/NE/N, in other words (A, IX) ff is separating. We say that ff is the separating hermitian form associated with ff.

2. Positive hermitian forms

Definition 2

Let EE be a vector space over the field KK. A hermitian form ff on EE is said to be positive if f(x,x)≥0f(x, x) \geq 0 for all x∈Ex \in E.

It is clear that hermitian forms on a vector space EE form a vector space over the field R\mathbf{R} (but not over the field C\mathbf{C}, when KK is C\mathbf{C}) : in this space the positive hermitian forms constitute a pointed convex proper cone (II, p. 10) as a result of def. 2 and prop. 1.

Proposition 2

— *If f is a positive hermitian form, we have

∣f(x,y)∣2≤f(x,x) f(y,y) |f(x, y)|^2 \leq f(x, x) \ f(y, y)

for every x and y in E (Cauchy-Schwarz inequality).

First assume that we have f(y,y)≠0f(y, y) \neq 0. For every ξ∈K\xi \in \mathbf{K}, we have

f(y,y) f(x+ξy,x+ξy)≥0 f(y, y) \ f(x + \xi y, x + \xi y) \geq 0

which can be written as

f(x,x) f(y,y)−∣f(x,y)∣2+(ξf(y,y)+f(x,y)‾)(ξ‾f(y,y)+f(x,y))≥0. f(x, x) \ f(y, y) - |f(x, y)|^2 + (\xi f(y, y) + \overline{f(x, y)}) (\overline{\xi} f(y, y) + f(x, y)) \geq 0 .

Replacing ξ\xi by −f(x,y)‾/f(y,y)-\overline{f(x, y)}/f(y, y) in this inequality, we get (7). If f(x,x)≠0f(x, x) \neq 0, we argue similarly.

Finally, if f(x,x)=f(y,y)=0f(x, x) = f(y, y) = 0, we have f(x+ξy,x+ξy)≥0f(x + \xi y, x + \xi y) \geq 0 for all ξ∈K\xi \in \mathbf{K}, which can be written as

ξf(x,y)+ξ‾f(x,y)≥0. \xi f(x, y) + \overline{\xi} f(x, y) \geq 0 .

Replacing ξ\xi by −f(x,y)‾-\overline{f(x, y)} in this inequality, we get −2 ∣f(x,y)∣2≥0-2 \ |f(x, y)|^2 \geq 0, and therefore f(x,y)=0f(x, y) = 0; we again get (7) in this case.

Corollary 1

— *If f is a positive hermitian form, the set N of all x \in E such that f(x, x) = 0 coincides with the vector subspace of all x \in E such that f(x, y) = 0 for all y \in E.

Corollary 2

— *For a positive hermitian form to be separating, it is necessary and sufficient that the relation x \neq 0 implies f(x, x) > 0.

This follows immediately from cor. 1.

For every positive hermitian form f on E, the separating hermitian form associated with f (V, p. 2) is evidently a positive hermitian form on E/N.

Proposition 3

— *Let f be a positive hermitian form on E. Put

p(x)=f(x,x)1/2 p(x) = f(x, x)^{1/2}

for all x \in E. Then p is a semi-norm on E, and is a norm if and only if f is separating.

It is enough to prove the inequality p(x+y)≤p(x)+p(y)p(x + y) \leq p(x) + p(y). But we have

f(x+y,x+y)=f(x,x)+f(y,y)+f(x,y)+f(x,y)‾ f(x + y, x + y) = f(x, x) + f(y, y) + f(x, y) + \overline{f(x, y)}

and, by Cauchy-Schwarz inequality

f(x+y,x+y)≤f(x,x)+f(y,y)+2(f(x,x)f(y,y))1/2 f(x + y, x + y) \leq f(x, x) + f(y, y) + 2(f(x, x) f(y, y))^{1/2}
=(f(x,x)1/2+f(y,y)1/2)2. = (f(x, x)^{1/2} + f(y, y)^{1/2})^2 .

Remark

— 1) Suppose f is positive and separating, and let x, y be two vectors ≠0\neq 0. The proof of Cauchy-Schwarz inequality shows that, if the two members of (7) are equal, then there exists a scalar ξ\xi such that f(x+ξy,x+ξy)=0f(x + \xi y, x + \xi y) = 0, hence x+ξy=0x + \xi y = 0, in other words, xx and yy are linearly dependent; the converse is immediate. The proof of inequality (8) shows that the equality p(x+y)=p(x)+p(y)p(x + y) = p(x) + p(y) is possible only if xx and yy are linearly dependent; if y=λxy = \lambda x, the preceding equality can be written as ∣1+λ∣=1+∣λ∣|1 + \lambda| = 1 + |\lambda|, and implies that λ\lambda is real and positive.

2) Let ff be a positive hermitian form on EE, and let EE be assigned the semi-norm x↦f(x,x)1/2x \mapsto f(x, x)^{1/2}; if ff is the positive, separating hermitian form defined on E/NE/N associated with ff, then the normed space obtained by assigning the norm x↦f(x˙,x˙)1/2x \mapsto f(\dot{x}, \dot{x})^{1/2} to E/NE/N is the normed space associated with EE (II, p. 5).

Definition 3

Let EE be a vector space over the field KK. A semi-norm pp on EE is said to be prehilbertian if there exists a positive hermitian form ff on EE such that p(x)=f(x,x)1/2p(x) = f(x, x)^{1/2} for all x∈Ex \in E*.

Observe that for a semi-norm pp on EE, there exists at most one positive hermitian form ff such that p(x)=f(x,x)1/2p(x) = f(x, x)^{1/2} for all x∈Ex \in E; this follows from the polarization formulas (V, p. 2).

3. Prehilbertian spaces

Definition 4

A prehilbertian space is a set EE with the structure of a vector space over KK and with a positive hermitian form. We say that EE is a real (resp. complex) prehilbertian space when KK is R\mathbf{R} (resp. KK is C\mathbf{C}).

Example 1

The form (λ,μ)↦λ‾μ(\lambda, \mu) \mapsto \overline{\lambda} \mu defines a prehilbertian structure on KK, said to be canonical. When KK is considered as a prehilbertian space, we shall always mean, unless otherwise mentioned that it has this structure.

Example 2

Let II be an interval (bounded or not) in R\mathbf{R}, and let EE be the set of regulated functions (FVR, II, p. 4) defined on II with values in C\mathbf{C}, having compact support. It is clear that EE is a vector space over C\mathbf{C}; let ff be the sesquilinear form (x,y)↦∫11x(t)‾ y(t) dt(x, y) \mapsto \int_1^1 \overline{x(t)}\ y(t)\ dt; it is immediate that ff is a positive hermitian form on EE, and hence defines a prehilbertian structure on this space.

Example 3

Let n⩾0n \geqslant 0 be an integer. We define a prehilbertian space structure on the space KnK^n, by means of the hermitian form

(x,y)↦∑j=1nxj‾yj (x, y) \mapsto \sum_{j=1}^n \overline{x_j} y_j

(for x=(x1,...,xn)x = (x_1, ..., x_n) and y=(y1,...,yn)y = (y_1, ..., y_n)). When KK is R\mathbf{R}, we see that this is just the scalar product of two vectors of Rn\mathbf{R}^n (GT, VI, § 2, No. 2).

Example 4

Let ℓ2\ell^2 (or ℓ2(N)\ell^2(\mathbf{N})) be the set of sequences x=(xn)n∈Nx = (x_n)_{n \in \mathbf{N}} of elements of KK such that ∑n=0∞∣xn∣2\sum_{n=0}^\infty |x_n|^2 is finite. One can show that ℓ2\ell^2 is a vector subspace of KNK^\mathbf{N} and define a prehilbertian space structure on ℓ2\ell^2 by means of the hermitian form (x,y)↦∑n=0∞xn‾yn(x, y) \mapsto \sum_{n=0}^\infty \overline{x_n} y_n (cf. V, p. 18).

Example 5

Let EE be a real prehilbertian space, ff the corresponding symmetric bilinear form on EE. Let E(c)E_{(c)} be the vector space complexification of EE; we identify EE with a subset of E(c)E_{(c)} by the map x↦1⊗xx \mapsto 1 \otimes x, in such a way that every element of E(c)E_{(c)} can be written uniquely as x1+ix2x_1 + ix_2 with x1,x2x_1, x_2 in EE. The map ff extends uniquely to a hermitian form f(c)f_{(c)} on E(c)E_{(c)}; we have,

f(c)(x1+ix2,y1+iy2)=f(x1,y1)+f(x2,y2)+i(f(x1,y2)−f(x2,y1)). f_{(c)}(x_1 + ix_2, y_1 + iy_2) = f(x_1, y_1) + f(x_2, y_2) + i(f(x_1, y_2) - f(x_2, y_1)) .

In particular, we have

f(C)(x1+ix2,x1+ix2)=f(x1,x1)+f(x2,x2)⩾0, f_{(\mathbf{C})}(x_1 + ix_2, x_1 + ix_2) = f(x_1, x_1) + f(x_2, x_2) \geqslant 0,
hence f(C)f_{(\mathbf{C})} is positive. We say that E(C)E_{(\mathbf{C})}, with f(C)f_{(\mathbf{C})} is the prehilbertian space complexification of EE.

Whenever only one prehilbertian space structure on a vector space EE is under consideration, the value, for a pair (x,y)(x, y) of points of EE, of the hermitian form which defines the said structure is denoted by ⟨x∣y⟩E\langle x|y \rangle_E or simply ⟨x∣y⟩\langle x|y \rangle, if no confusion is likely to arise. This number is called the scalar product 1^1 of xx and yy (scalar square of xx if y=xy = x). Two vectors x,yx, y are said to be orthogonal if ⟨x∣y⟩=0\langle x|y \rangle = 0. The function x↦∥x∥=⟨x∣x⟩1/2x \mapsto \|x\| = \langle x|x \rangle^{1/2} is a semi-norm on the vector space EE (V, p. 3); a prehilbertian space is always considered with this semi-norm assigned to it (and consequently also with the corresponding topology and uniform structure).

With these notations, in a prehilbertian space EE, the Cauchy-Schwarz inequality can be written as

∣⟨x∣y⟩∣⩽∥x∥⋅∥y∥. |\langle x|y \rangle| \leqslant \|x\| \cdot \|y\|.

Consequently, the scalar product is a continuous sesquilinear form on E×EE \times E (II, p. 5, prop. 4).

In order that EE be Hausdorff, it is necessary and sufficient that x↦∥x∥x \mapsto \|x\| is a norm on EE; in other words, that the hermitian form (x,y)↦⟨x∣y⟩(x, y) \mapsto \langle x|y \rangle is positive and separating; this is equivalent to saying that 00 is the only vector of EE, which is orthogonal to itself.

According to general definitions (S, IV, § 1, No. 5), an isomorphism from a prehilbertian space EE onto a prehilbertian space FF is a bijective linear mapping uu from EE onto FF such that

⟨u(x)∣u(y)⟩=⟨x∣y⟩ \langle u(x)|u(y) \rangle = \langle x|y \rangle
for every xx and yy in EE. We deduce from this that ∥u(x)∥=∥x∥\|u(x)\| = \|x\| for all x∈Ex \in E, and uu is evidently an isomorphism for the topological vector space structures of EE and of FF; if EE and FF are Hausdorff, uu is an isometry from EE onto FF. Conversely, if uu is a bijective linear mapping from EE onto FF, such that ∥u(x)∥=∥x∥\|u(x)\| = \|x\| for all x∈Ex \in E, the polarization formulas (V, p. 2) show that uu is a prehilbertian space isomorphism from EE onto FF.

Let EE be a complex prehilbertian space, and ⟨x∣y⟩\langle x|y \rangle the scalar product in EE. On the set EE, we can define a second vector space structure with respect to C\mathbf{C}, taking the same law of the additive group and for the law of external composition (λ,x)↦λ‾x(\lambda, x) \mapsto \overline{\lambda} x (A, II, § 1, No. 13) for this vector space structure, (x,y)↦⟨y∣x⟩(x, y) \mapsto \langle y|x \rangle is a *positive hermitian

1 It may happen sometimes that we write (x∣y)(x|y) for ⟨y∣x⟩\langle y|x \rangle. Observe that the formula (4) of V, p. 2, takes the following equivalent forms:

⟨∑iλixi∣∑jμjyj⟩=∑i,jλ‾iμj⟨xi∣yj⟩.(∑iλixi∣∑jμjyj)=∑i,jλiμ‾j(xi∣yj). \begin{align*} \langle \sum_i \lambda_i x_i | \sum_j \mu_j y_j \rangle &= \sum_{i,j} \overline{\lambda}_i \mu_j \langle x_i|y_j \rangle. \\ (\sum_i \lambda_i x_i | \sum_j \mu_j y_j) &= \sum_{i,j} \lambda_i \overline{\mu}_j (x_i|y_j). \end{align*}

form. The prehilbertian space E‾\overline{E} obtained by assigning this new vector space structure and the new hermitian form to E, is said to be conjugate to E. An isomorphism uu from E onto E‾\overline{E} is a semi-linear mapping from E onto itself (with respect to the automorphism ξ↦ξ‾\xi \mapsto \overline{\xi} of C\mathbf{C}) such that ⟨u(y)∣u(x)⟩=⟨x∣y⟩\langle u(y)|u(x) \rangle = \langle x|y \rangle or ⟨u(x)∣u(y)⟩=⟨x∣y⟩‾\langle u(x)|u(y) \rangle = \overline{\langle x|y \rangle} (for x,yx, y in E); such a mapping is said to be a semi-automorphism of the prehilbertian space E.

If E is a prehilbertian space, M a vector subspace of E, the restriction of the scalar product ⟨x∣y⟩\langle x|y \rangle to M×MM \times M is a positive hermitian form on M, which then defines a prehilbertian space structure on M; we say that this structure is induced by the structure of E, or that M is a prehilbertian subspace of E.

4. Hilbertian spaces

Definition 5

A hilbertian space* (or Hilbert space) is a prehilbertian space which is Hausdorff and complete. We say that a norm on a vector space E (over K) is hilbertian if it is prehilbertian, and if the normed space E is complete.

If E is a hilbertian space and M a closed vector subspace of E, the prehilbertian space structure induced on M is in fact a hilbertian space structure. In this case we say that M, with the induced structure is a hilbertian subspace of E.

Example 1

The prehilbertian spaces defined in examples 1, 3, 4 of V, p. 4, are hilbertian spaces. On the other hand, the prehilbertian space defined in example 2 is neither Hausdorff, nor complete. The complexification of a hilbertian space is a hilbertian space.

Example 2

\* Let X be a Hausdorff topological space and let μ\mu be a positive measure on X. Let L2(X,μ)L^2(X, \mu) be the space consisting of equivalence classes, for μ\mu, of all square μ\mu-integrable functions on X with values in C\mathbf{C}. This is a complex hilbertian space, whose scalar product is given by

⟨f∣g⟩=∫Xf(x)‾ g(x) dμ(x). \langle f|g \rangle = \int_X \overline{f(x)}\ g(x)\ d\mu(x) .

Example 3

\* Let n⩾1n \geqslant 1 be an integer and let U be an open set in Rn\mathbf{R}^n. Let μ\mu be the measure on U induced by the Lebesgue measure on Rn\mathbf{R}^n, and put H0=L2(U,μ)\mathscr{H}^0 = L^2(U, \mu). Let H1\mathscr{H}^1 denote the space of all functions f∈H0f \in \mathscr{H}^0 with the following property; for 1⩽i⩽n1 \leqslant i \leqslant n, there exists a function gi∈H∘g_i \in \mathscr{H}^\circ such that

∫Ugi(x) h(x) dμ(x)=−∫Uf(x) Dih(x) dμ(x) \int_U g_i(x)\ h(x)\ d\mu(x) = - \int_U f(x)\ D_i h(x)\ d\mu(x)

for every function hh of class C1C^1 with compact support in U. The function gig_i is defined uniquely up to equivalence with respect to μ\mu, and is denoted by DifD_i f or ∂f/∂xi\partial f / \partial x_i (ith partial derivative). By induction on the integer s⩾1s \geqslant 1, we define Hs\mathscr{H}^s as the set of all functions f∈H1f \in \mathscr{H}^1 such that Dif∈Hs−1D_i f \in \mathscr{H}^{s-1} for 1⩽i⩽n1 \leqslant i \leqslant n. We define a scalar product on Hs\mathscr{H}^s by the formula

⟨f∣g⟩=∑k=0s∑1⩽i1⩽…⩽ik⩽n∫Di1…Dikf‾⋅Di1…Dikg dμ. \langle f|g \rangle = \sum_{k=0}^s \sum_{1 \leqslant i_1 \leqslant \ldots \leqslant i_k \leqslant n} \int \overline{D_{i_1} \ldots D_{i_k} f} \cdot D_{i_1} \ldots D_{i_k} g\ d\mu .

Then Hs\mathscr{H}^s is a complex hilbertian space, called Sobolev space of index s.

Example 4

\* Let X be a differential variety of class CrC^r (with r⩾1r \geqslant 1) pure of finite dimension nn.

In the vector fibre space ΛnT(X)\Lambda^n T(X), let L be the complement of the zero section. For every real number λ≠0\lambda \neq 0, the mapping u↦λuu \mapsto \lambda u from ΛnT(X)\Lambda^n T(X) into itself leaves L stable.

Let α\alpha be a complex number. A complex valued function ω\omega on L such that ω(λu)=∣λ∣αω(u)\omega(\lambda u) = |\lambda|^{\alpha} \omega(u) for u∈Lu \in L and any non-zero real number λ\lambda is called a density of order α\alpha on X. We say that a density ω\omega of order 1 is locally integrable if there exists an open cover (Ui)i∈I(U_i)_{i \in I} of X, and for every i∈Ii \in I a system of coordinates ξi=(ξi1,...,ξin)\xi_i = (\xi_i^1, ..., \xi_i^n) on UiU_i and a complex valued function fif_i on ξi(Ui)\xi_i(U_i) satisfying the following conditions:

a) The function fif_i is locally integrable on the open set ξi(Ui)\xi_i(U_i) of Rn\mathbf{R}^n with respect to the Lebesgue measure μ\mu;

b) Let x∈Uix \in U_i; if (∂1,i,x,...,∂n,i,x)(\partial_{1,i,x}, ..., \partial_{n,i,x}) is the basis of TxXT_x X associated to the system of coordinates (ξi′,...,ξin)(\xi_i', ..., \xi_i^n) in UiU_i we have

ω(∂1,i,x∧...∧∂n,i,x)=fi(ξi1(x),...,ξin(x)). \omega(\partial_{1,i,x} \wedge ... \wedge \partial_{n,i,x}) = f_i(\xi_i^1(x), ..., \xi_i^n(x)) .

Then, there exists one and only one measure ω~\tilde{\omega} on X such that for every i∈Ii \in I, the image under ξi\xi_i of the restriction of ω~\tilde{\omega} to UiU_i is equal to the measure fi⋅μf_i \cdot \mu (cf. VAR, R, 10.4.3).

Let V\mathscr{V} (resp. N\mathscr{N}) be the vector space of measurable densities ω\omega of order 1/2 such that the measure associated with the density ∣ω∣2|\omega|^2 of order 1 is bounded (resp. null). Let ω1\omega_1 and ω2\omega_2 be in V\mathscr{V}; then ω=ω1‾ω2\omega = \overline{\omega_1} \omega_2 is a density of order 1, and the measure ω~\tilde{\omega} associated with ω\omega is bounded; the number ∫Xω~\int_X \tilde{\omega} depends only on the classes ω˙1\dot{\omega}_1 and ω˙2\dot{\omega}_2 of ω1\omega_1 and ω2\omega_2 modulo N\mathscr{N} and is denoted by ⟨ω1∣ω2⟩\langle \omega_1 | \omega_2 \rangle or ⟨ω˙1∣ω˙2⟩\langle \dot{\omega}_1 | \dot{\omega}_2 \rangle. Then the mapping (ω˙1,ω˙2)↦⟨ω˙1∣ω˙2⟩(\dot{\omega}_1, \dot{\omega}_2) \mapsto \langle \dot{\omega}_1 | \dot{\omega}_2 \rangle assigns a complex hilbertian space structure to the vector space Ω1/2(X)=V/N\Omega_{1/2}(X) = \mathscr{V}/\mathscr{N}.

Example 5

\* Let D be the open disc with centre 0 and radius 1 in C\mathbf{C}. The Hardy space H2(D)H^2(D) consists of all holomorphic functions f:D→Cf : D \to \mathbf{C} for which

sup⁡0<R<1∫01∣f(R⋅e(θ))∣2dθ<+∞. \sup_{0 < R < 1} \int_0^1 |f(R \cdot e(\theta))|^2 d\theta < + \infty .
If f1f_1 and f2f_2 belong to H2(D)H^2(D), the limit
⟨f1∣f2⟩=lim⁡R→1∫01f1(R⋅e(θ))‾⋅f2(R⋅e(θ)) dθ \langle f_1 | f_2 \rangle = \lim_{R \to 1} \int_0^1 \overline{f_1(R \cdot e(\theta))} \cdot f_2(R \cdot e(\theta)) \, d\theta
exists; the mapping (f1,f2)↦⟨f1∣f2⟩(f_1, f_2) \mapsto \langle f_1 | f_2 \rangle assigns a complex hilbertian space structure to the vector space H2(D)H^2(D).

For a function f:D→Cf : D \to \mathbf{C} to belong to H2(D)H^2(D), it is necessary and sufficient that there exists a sequence (an)n∈N(a_n)_{n \in \mathbf{N}} of complex numbers such that ∑n=0∞∣an∣2<+∞\sum_{n=0}^\infty |a_n|^2 < + \infty and that

f(z)=∑n=0∞anzn f(z) = \sum_{n=0}^\infty a_n z^n
for all z∈Dz \in D. Then we have ∥f∥2=∑n=0∞∣an∣2\|f\|^2 = \sum_{n=0}^\infty |a_n|^2 which gives an isomorphism from H2(D)H^2(D) onto the hilbertian space ℓ2\ell^2 (V, p. 4).

Every Hausdorff prehilbertian space is isomorphic to an everywhere dense subspace of a hilbertian space determined up to an isomorphism. Precisely :

Proposition 4

— Let E be a Hausdorff prehilbertian space, E^\hat{E} the normed space completion of E(GT, IX, § 3, No. 3). The scalar product* (x,y)↦⟨x∣y⟩(x, y) \mapsto \langle x|y \rangle extends by continuity to a positive and separating hermitian form on* E^\hat{E}, and defines a hilbertian space structure on E^\hat{E}.

The existence of the extension of (x,y)↦⟨x∣y⟩(x, y) \mapsto \langle x|y \rangle to E^×E^\hat{E} \times \hat{E} follows from the continuity of this sesquilinear form an E×EE \times E (GT, III, § 6, No. 5, th. 1). Moreover, this extension, which will also be denoted by (x,y)↦⟨x∣y⟩(x, y) \mapsto \langle x|y \rangle is a hermitian form and satisfies the relation ⟨x∣x⟩=∥x∥2\langle x|x \rangle = \|x\|^2, by virtue of the principle of extension of identities (∥x∥\|x\| being the norm on E^\hat{E} obtained by extending the norm on E by continuity) ; this proves that the relation ⟨x∣x⟩=0\langle x|x \rangle = 0 implies x=0x = 0 in E^\hat{E}, hence that the form (x,y)↦⟨x∣y⟩(x, y) \mapsto \langle x|y \rangle is positive and separating, and consequently defines a hilbertian space structure on E^\hat{E}. Q.E.D.

This hilbertian space is said to be the completion of the Hausdorff prehilbertian space E.

\* Example 6. — Let U be an open subset of Rn\mathbf{R}^n (n⩾1n \geqslant 1). Let C01(U)\mathscr{C}_0^1(\mathrm{U}) be the vector space of all functions of class C1\mathrm{C}^1 with compact support in U. We define a Hausdorff prehilbertian space structure on C01(U)\mathscr{C}_0^1(\mathrm{U}) whose scalar product is given by

⟨f∣g⟩=∑i=1n∫UDif(x)‾.Dig(x) dx. \langle f|g \rangle = \sum_{i=1}^{n} \int_{\mathrm{U}} \overline{\mathrm{D}_i f(x)} . \mathrm{D}_i g(x) \, dx .

This prehilbertian space is not complete. Its completion is called the Dirichlet space associated with U. \*

Corollary

— Let V be a vector space over K and f a positive hermitian form on V. a) There exists a Hilbert space E and a linear mapping u:V→Eu : V \to E such that f(x,y)=⟨u(x)∣u(y)⟩f(x, y) = \langle u(x)|u(y) \rangle for x, y in V, and such that u(V) is dense in E. b) If two pairs (Ei,ui)(E_i, u_i) satisfy the conditions analogous to a), then there exists a unique isomorphism ϕ\phi from the Hilbert space E1E_1 onto the Hilbert space E2E_2 such that u2=ϕ∘u1u_2 = \phi \circ u_1.

Let N be the set of all x∈Vx \in V such that f(x,x)=0f(x, x) = 0. We define a positive and separating hermitian form on the space V/N by ⟨x˙∣y˙⟩=f(x,y)\langle \dot{x}|\dot{y} \rangle = f(x, y) for x∈x˙x \in \dot{x} and y∈y˙y \in \dot{y}. Let E be the hilbertian space completion of V/N and uu the mapping x↦x+Nx \mapsto x + N from V into E. Then the conditions of a) are satisfied.

Under the hypotheses of b), N is equal to the kernel of u1u_1 and to that of u2u_2. Hence there exists a bijective linear mapping ϕ0\phi_0 from u1(V)u_1(V) onto u2(V)u_2(V) such that u2(x)=ϕ0(u1(x))u_2(x) = \phi_0(u_1(x)) for all x∈Vx \in V. We verify immediately that ϕ0\phi_0 is an isomorphism of prehilbertian spaces, hence an isometry. Since ui(V)u_i(V) is dense in EiE_i for i=1,2i = 1, 2, ϕ0\phi_0 extends uniquely to an isometry ϕ\phi from E1E_1 onto E2E_2, and b) follows.

We say that the hilbertian space E is the separated completion of V (for the form f).

Example 7. — Let G be a group (with unit element 1) and π\pi a homomorphism from G into the group of automorphisms of a complex hilbertian space E ; we say that π\pi is a unitary representation of G in E. Let a∈Ea \in E ; we put

ϕ(x)=⟨a∣π(x).a⟩ \phi(x) = \langle a|\pi(x).a \rangle

for all x∈Gx \in G. Then ϕ:G→C\phi : G \to \mathbf{C} is positive definite, in other words satisfies the relation :

(PD) For every λ1,...,λn\lambda_1, ..., \lambda_n in C\mathbf{C} and x1,...,xnx_1, ..., x_n in GG, we have

∑i,j=1nλi‾λjϕ(xi−1xj)⩾0. \sum_{i,j=1}^n \overline{\lambda_i} \lambda_j \phi(x_i^{-1} x_j) \geqslant 0 .

In fact, the first member of (11) is precisely ∥∑i=1nλiπ(xi).a∥2\| \sum_{i=1}^n \lambda_i \pi(x_i) . a \| ^2.

Conversely, let ϕ\phi be a positive definite function on GG. Let C(G)C^{(G)} be the vector space of all functions with finite support on GG. We define a hermitian form Φ\Phi on GG by

Φ(u,v)=∑x,y∈Gu(x)‾ v(y) ϕ(x−1y) \Phi(u, v) = \sum_{x,y \in G} \overline{u(x)} \ v(y) \ \phi(x^{-1} y)

and the relation (PD) expresses the fact that Φ\Phi is positive. By the corollary of prop. 4, there exists a hilbertian space EE and a linear mapping ρ:C(G)→E\rho : C^{(G)} \to E, with a dense image, such that

Φ(u,v)=⟨ρ(u)∣ρ(v)⟩foru,vinC(G). \Phi(u, v) = \langle \rho(u)|\rho(v) \rangle \quad \text{for} \quad u, v \quad \text{in} \quad C^{(G)} .

For every x∈Gx \in G, let γx\gamma_x be the left translation by xx in C(G)C^{(G)} defined by γxu(y)=u(x−1y)\gamma_x u(y) = u(x^{-1} y) for u∈C(G)u \in C^{(G)} and y∈Gy \in G. We have Φ(γxu,γxv)=Φ(u,v)\Phi(\gamma_x u, \gamma_x v) = \Phi(u, v). Now apply assertion b) of the corollary of prop. 4 to ρ\rho and ρ∘γx\rho \circ \gamma_x: there exists a unique automorphism π(x)\pi(x) of the hilbertian space EE such that ρ∘γx=π(x)∘ρ\rho \circ \gamma_x = \pi(x) \circ \rho. We see immediately that π\pi is a homomorphism from GG into the group of automorphisms of EE.

Let δ\delta be the element of C(G)C^{(G)} defined by δ(1)=1,δ(x)=0\delta(1) = 1, \delta(x) = 0 for x≠1x \neq 1 in GG. We have u=∑x∈Gu(x).γxδu = \sum_{x \in G} u(x) . \gamma_x \delta for all u∈C(G)u \in C^{(G)}, and so ρ(u)=∑x∈Gu(x) π(x).a\rho(u) = \sum_{x \in G} u(x) \ \pi(x) . a by putting a=ρ(δ)a = \rho(\delta).

Formulas (12) and (13) imply that ϕ(x)=⟨a∣π(x).a⟩\phi(x) = \langle a|\pi(x).a \rangle for all x∈Gx \in G. We remark that the set of vectors π(x).a\pi(x).a for all x∈Gx \in G, is total in EE.

5. Convex subsets of a prehilbertian space

If we calculate ∥x−y∥2=⟨x−y∣x−y⟩\| x - y \| ^2 = \langle x - y|x - y \rangle and ∥x+y∥2=⟨x+y∣x+y⟩\| x + y \| ^2 = \langle x + y|x + y \rangle for any two points x,yx, y of a prehilbertian space EE, we immediately get the « identity of the median »

∥12(x+y)∥2+∥12(x−y)∥2=12(∥x∥2+∥y∥2). \| \frac{1}{2}(x + y) \| ^2 + \| \frac{1}{2}(x - y) \| ^2 = \frac{1}{2} (\| x \| ^2 + \| y \| ^2 ) .

From this identity we deduce the following proposition :

!Diagram showing sets B', B, and A, with x and y marked within A

Fig. 1.

Proposition 5

— Let EE be a prehilbertian space. Let dd be a real number >0> 0, δ\delta a real number such that 0⩽δ⩽d0 \leqslant \delta \leqslant d. Let BB and B′B' be subsets of EE defined by ∥x∥<d\| x \| < d,

∥x∥≤d+δ respectively, and let A be a convex set contained in B′−B. Then for every pair of points x,y of A, we have ∥x−y∥≤12dδ (fig. 1). \|x\| \leq d + \delta \text{ respectively, and let } A \text{ be a convex set contained in } B' - B. \text{ Then for every pair of points } x, y \text{ of } A, \text{ we have } \|x - y\| \leq \sqrt{12d\delta} \text{ (fig. 1).}
In fact, we have 12(x+y)∈A\frac{1}{2}(x + y) \in A, hence ∥12(x+y)∥≥d\left\| \frac{1}{2}(x + y) \right\| \geq d; hence from (14) we get the inequality
∥12(x−y)∥2=12(∥x∥2+∥y∥2)−∥12(x+y)∥2≤(d+δ)2−d2≤3dδ \left\| \frac{1}{2}(x - y) \right\|^2 = \frac{1}{2}(\|x\|^2 + \|y\|^2) - \left\| \frac{1}{2}(x + y) \right\|^2 \leq (d + \delta)^2 - d^2 \leq 3d\delta
from which the proposition follows.

Theorem 1

Let E be a prehilbertian space, and H a non-empty convex subset of E such that H is a Hausdorff and complete uniform subspace of E. For every x∈Ex \in E, there exists a unique point pH(x)p_H(x) in H such that ∥x−pH(x)∥=inf⁡y∈H∥x−y∥\|x - p_H(x)\| = \inf_{y \in H} \|x - y\|. The element pH(x)p_H(x) of H is also the unique element a of H satisfying the relation*

ℜ⟨x−a∣y−a⟩≤0 \Re \langle x - a | y - a \rangle \leq 0
for all y∈Hy \in H.

!Diagram showing a point x, a point y, and a line segment labeled a + λ(y − a)

Fig. 2.

Put d=inf⁡y∈H∥x−y∥d = \inf_{y \in H} \|x - y\|, and for every integer n>0n > 0, let HnH_n be the set of points yy of H such that ∥x−y∥≤d+n−1\|x - y\| \leq d + n^{-1}. The set HnH_n is closed in H, is convex and non-empty, and its diameter is bounded by 12dn\sqrt{12 \frac{d}{n}} for all large enough nn, by prop. 5. The sequence (Hn)n≥1(H_n)_{n \geq 1} being decreasing, and the set H being Hausdorff and complete it follows that the base of the Cauchy filter (Hn)n≥1(H_n)_{n \geq 1} converges to a point pH(x)p_H(x) of H; we have {pH(x)}=⋂n≥1Hn\{ p_H(x) \} = \bigcap_{n \geq 1} H_n, hence pH(x)p_H(x) is the unique point aa of H such that ∥x−a∥=d\|x - a\| = d.

1 We recall (GT, VIII, § 1, No. 1) that ℜ(z)\Re(z) denotes the real part of the complex number z; we have ℜ(z)=z\Re(z) = z if z is real.

Let y∈Hy \in \mathbf{H}; since H\mathbf{H} is convex, the point z(λ)=pH(x)+λ(y−pH(x))z(\lambda) = p_{\mathbf{H}}(x) + \lambda(y - p_{\mathbf{H}}(x)) of E belongs to H\mathbf{H} for every real number λ\lambda such that 0<λ<10 < \lambda < 1. Hence we have

∥x−z(λ)∥2≥∥x−pH(x)∥2for0<λ<1, \| x - z(\lambda) \|^{2} \geq \| x - p_{\mathbf{H}}(x) \|^{2} \quad \text{for} \quad 0 < \lambda < 1 ,
which gives
R⟨x−pH(x)∣y−pH(x)⟩=lim⁡λ→012λ{∥x−pH(x)∥2−∥x−z(λ)∥2}≤0. \mathscr{R} \langle x - p_{\mathbf{H}}(x)|y - p_{\mathbf{H}}(x) \rangle = \lim_{\lambda \to 0} \frac{1}{2\lambda} \left\{ \| x - p_{\mathbf{H}}(x) \|^{2} - \| x - z(\lambda) \|^{2} \right\} \leq 0 .
Conversely, let aa be a point of H\mathbf{H} such that R⟨x−a∣y−a⟩≤0\mathscr{R} \langle x - a|y - a \rangle \leq 0 for all y∈Hy \in \mathbf{H}. For every y∈Hy \in \mathbf{H}, we have
∥x−y∥2=∥x−a∥2+∥y−a∥2−2R⟨x−a∣y−a⟩≥∥x−a∥2, \| x - y \|^{2} = \| x - a \|^{2} + \| y - a \|^{2} - 2 \mathscr{R} \langle x - a|y - a \rangle \geq \| x - a \|^{2} ,
and so ∥x−a∥=d\| x - a \| = d and finally that a=pH(x)a = p_{\mathbf{H}}(x) follows from the first part of the proof. Q.E.D.

In what follows the mapping pHp_{\mathbf{H}} of E in H\mathbf{H} will be called the projection from E onto H\mathbf{H}. We remark that pH(x)=xp_{\mathbf{H}}(x) = x for all x∈Hx \in \mathbf{H}.

The first part of th. 1 is valid under more general hypotheses on the space E (V, p. 67, exerc. 31).

The proof of th. 1 establishes, among others, the following property :

Corollary 1

Let I be a set directed by a filter F\mathfrak{F} and let (yi)i∈I(y_{i})_{i \in I} be a family of points of H\mathbf{H}. Let x∈Ex \in \mathbf{E}. Suppose that we have*

lim⁡i,F∥x−yi∥=inf⁡z∈H∥x−z∥. \lim_{i, \mathfrak{F}} \| x - y_{i} \| = \inf_{z \in \mathbf{H}} \| x - z \| .
*Then yiy_{i} tends to pH(x)p_{\mathbf{H}}(x) with respect to the filter F\mathfrak{F}.

Corollary 2

For every x,yx, y in E\mathbf{E}, we have*

∥pH(x)−pH(y)∥≤∥x−y∥. \| p_{\mathbf{H}}(x) - p_{\mathbf{H}}(y) \| \leq \| x - y \| .
*In particular, the mapping pHp_{\mathbf{H}} from E\mathbf{E} into H\mathbf{H} is continuous.

Let x,yx, y be two points of E\mathbf{E}. Put a=pH(x)−x,b=pH(y)−pH(x),c=y−pH(y)a = p_{\mathbf{H}}(x) - x, b = p_{\mathbf{H}}(y) - p_{\mathbf{H}}(x), c = y - p_{\mathbf{H}}(y). By formula (15) (V, p. 10) we have R⟨a∣b⟩≥0\mathscr{R} \langle a|b \rangle \geq 0 and R⟨c∣b⟩≥0\mathscr{R} \langle c|b \rangle \geq 0. We also have a+b+c=y−xa + b + c = y - x, which gives,

∥x−y∥2=∥a+b+c∥2=∥b∥2+∥a+c∥2+2R⟨a∣b⟩+2R⟨c∣b⟩ \| x - y \|^{2} = \| a + b + c \|^{2} = \| b \|^{2} + \| a + c \|^{2} + 2 \mathscr{R} \langle a|b \rangle + 2 \mathscr{R} \langle c|b \rangle
≥∥b∥2=∥pH(x)−pH(y)∥2. \geq \| b \|^{2} = \| p_{\mathbf{H}}(x) - p_{\mathbf{H}}(y) \|^{2} .
This proves corollary 2.

Proposition 6

Let E\mathbf{E} be a prehilbertian space and let Φ\Phi be a non-empty, directed decreasing set of non-empty Hausdorff and complete convex subsets of E\mathbf{E}. For every x∈Ex \in \mathbf{E} and every subset H\mathbf{H} of E\mathbf{E}, put d(x,H)=inf⁡z∈H∥x−z∥d(x, \mathbf{H}) = \inf_{z \in \mathbf{H}} \| x - z \|. In order that the intersection M of the sets H belonging to Φ\Phi be non-empty, it is necessary and sufficient that there exists x0x_0 in E such that sup⁡H∈Φd(x0,H)\sup_{H \in \Phi} d(x_0, H) is finite. For every x∈Ex \in E we then have

pM(x)=lim⁡H∈ΦpH(x) p_M(x) = \lim_{H \in \Phi} p_H(x)
(limit with respect to the directed set Φ\Phi).

If M is non-empty, d(x,H)≤d(x,M)d(x, H) \leq d(x, M) for all H∈ΦH \in \Phi and all x∈Ex \in E.

Conversely, suppose that there exists a point x0x_0 in E and a real number C≥0C \geq 0 such that d(x0,H)≤Cd(x_0, H) \leq C for all H∈ΦH \in \Phi. Let x∈Ex \in E; then

d(x,H)≤∥x−x0∥+Cfor all H∈Φ, d(x, H) \leq \|x - x_0\| + C \quad \text{for all } H \in \Phi,
hence the number d=sup⁡H∈Φd(x,H)d = \sup_{H \in \Phi} d(x, H) is finite. Let B be the set of all z∈Ez \in E such that ∥x−z∥≤d\|x - z\| \leq d. Since B is convex and closed in E, the sets H∩BH \cap B, for H ranging over Φ\Phi, are convex, Hausdorff and complete. Let ε>0\varepsilon > 0; there exists a set H∈ΦH \in \Phi such that d(x,H)≥d−εd(x, H) \geq d - \varepsilon, and if ε<d/2\varepsilon < d/2, the diameter of H∩BH \cap B is bounded by 12ε(d−ε)\sqrt{12 \varepsilon (d - \varepsilon)} by prop. 5 (V, p. 9). In other words, for all H0∈ΦH_0 \in \Phi, the closed sets H∩BH \cap B, for H∈ΦH \in \Phi and H⊂H0H \subset H_0, form a base of the Cauchy filter on the Hausdorff and complete space H0H_0. Hence the intersection of the sets H∩BH \cap B (for H∈ΦH \in \Phi) reduces to a point y. We get y∈My \in M and ∥x−y∥=d=d(x,M)\|x - y\| = d = d(x, M). Since M is closed in H0H_0, it is a Hausdorff, convex and complete set in E, and so y=pM(x)y = p_M(x). For every H∈ΦH \in \Phi, we have pH(x)∈H∩Bp_H(x) \in H \cap B, from which we get that pM(x)=lim⁡H∈ΦpH(x)p_M(x) = \lim_{H \in \Phi} p_H(x).

Proposition 7

Let E be a Hausdorff prehilbertian space and let Ψ\Psi be a non-empty directed increasing set of non-empty, convex, complete subsets of E. Put A=⋃H∈ΨHA = \bigcup_{H \in \Psi} H and suppose that the closure N of A is complete. Then N is convex and we have*

pN(x)=lim⁡H∈ΨpH(x) for all x∈E. p_N(x) = \lim_{H \in \Psi} p_H(x) \text{ for all } x \in E.

It is clear that A is convex, hence its closure N is convex (II, p. 13). With the notations of prop. 6, d(x,N)=inf⁡H∈Ψd(x,H)d(x, N) = \inf_{H \in \Psi} d(x, H), and consequently d(x,N)d(x, N) is the limit of d(x,H)d(x, H) with respect to the section filter of Ψ\Psi. Since pH(x)∈Hp_H(x) \in H and

lim⁡H∈Ψ∥x−pH(x)∥=lim⁡H∈Ψd(x,H)=d(x,N), \lim_{H \in \Psi} \|x - p_H(x)\| = \lim_{H \in \Psi} d(x, H) = d(x, N),
it follows from cor. 1 of V, p. 11 that pH(x)p_H(x) tends to the projection pN(x)p_N(x) of xx onto N with respect to the section filter of Ψ\Psi.

6. Vector subspaces and orthoprojectors

Let E be a prehilbertian space. Recall that two vectors xx and yy of E are said to be orthogonal if ⟨x∣y⟩=0\langle x | y \rangle = 0; then

∥x+y∥2=∥x∥2+∥y∥2 \|x + y\|^2 = \|x\|^2 + \|y\|^2
(« Pythagoras’ theorem »).

Let A be a subset of E. We say that a vector x in E is orthogonal to A if it is orthogonal to every vector of A. The set of all vectors orthogonal to A is a closed vector subspace of A, denoted by A∘A^\circ and called (by abuse of language) the orthogonal of A.

Let A and B be two subsets of E. We say that A and B are orthogonal if every vector of A is orthogonal to every vector of B. This is equivalent to saying that A⊂B∘A \subset B^\circ, or that B⊂A∘B \subset A^\circ. If E is Hausdorff and if A and B are orthogonal then A∩BA \cap B is empty or reduces to 0 since 0 is the only vector of E orthogonal to itself.

Theorem 2

Let E be a prehilbertian space and M a vector subspace of E, which is Hausdorff and complete. Then E is the topological direct sum of M and of M∘M^\circ the subspace orthogonal to M. The projector from E onto M associated with the decomposition E=M⊕M∘E = M \oplus M^\circ is the projection pMp_M from E onto M defined in th. 1 (V, p. 10).

We first show that x−pM(x)x - p_M(x) belongs to M∘M^\circ for all x∈Ex \in E. Let y∈My \in M. For every scalar λ∈K\lambda \in K, the vector pM(x)+λyp_M(x) + \lambda y belongs to M; hence by formula 15 (V, p. 10) we have,

R(λ⟨x−pM(x)∣y⟩)≤0 \mathscr{R}(\lambda \langle x - p_M(x)|y \rangle) \leq 0

for all λ∈K\lambda \in K. If, in particular we take λ=⟨x−pM(x)∣y⟩‾\lambda = \overline{\langle x - p_M(x)|y \rangle} we conclude that ⟨x−pM(x)∣y⟩=0\langle x - p_M(x)|y \rangle = 0, hence our assertion.

Since M is Hausdorff, 0 is the only vector of M, orthogonal to itself, hence M∩M∘={0}M \cap M^\circ = \{0\}. For every x∈Ex \in E, we have pM(x)∈Mp_M(x) \in M and x−pM(x)∈M∘x - p_M(x) \in M^\circ. Consequently, E is the direct sum of M and M∘M^\circ, and pMp_M is the projector from E onto M with kernel M∘M^\circ. Since pMp_M is a continuous mapping from E into M (V, p. 11, cor. 2), if follows from GT, III, § 6, No. 2 that E is the topological direct sum of M and M∘M^\circ.

Corollary

Let E be a Hausdorff prehilbertian space and M a finite dimensional vector subspace of E. Then E is the direct sum of M and M∘M^\circ.

Since E is Hausdorff, so is M; since M is finite dimensional, it is complete (I, p. 13). It is therefore enough to apply th. 2.

With the notations of th. 2, we say that M∘M^\circ is the orthogonal complement of M and that pMp_M is the orthoprojector (or the orthogonal projector, or by abuse of language, the projector) from E onto M; if x is a vector of E, the vector pM(x)p_M(x) of M is also called the orthogonal projection of x on M. Note that pMp_M is a continuous linear mapping from E onto M and that we have ∥pM∥=1\|p_M\| = 1 by cor. 2 of V, p. 11, except in the case when M={0}M = \{0\} in which case pM=0p_M = 0.

It follows immediately from Pythagoras theorem that the canonical mapping ψ\psi from E/ME/M onto M∘M^\circ deduced from the direct sum decomposition E=M⊕M∘E = M \oplus M^\circ is isometric if E/ME/M is assigned the quotient semi-norm from that of E (II, p. 4). We shall always assign that prehilbertian structure to E/ME/M for which ψ\psi is an isomorphism of prehilbertian spaces; the quotient semi-norm on E/ME/M is then deduced from this prehilbertian structure.

We shall often use the preceding results when E is a hilbertian space and M a closed vector subspace of E. In this case, M∘M^\circ is a closed vector subspace of E, and pM∘=1−pMp_{M^\circ} = 1 - p_M, and (M∘)∘=M(M^\circ)^\circ = M.

Proposition 8

— Let E be a hilbertian space, M a closed vector subspace of E, I a non-empty ordered directed set and (Mi)i∈I(M_i)_{i \in I} a family of closed vector subspaces of E. We assume that either the mapping i↦Mii \mapsto M_i is increasing and that M is the closure of ⋃i∈IMi\bigcup_{i \in I} M_i or that the mapping i↦Mii \mapsto M_i is decreasing and that M=⋂i∈IMiM = \bigcap_{i \in I} M_i. Then pM(x)=lim⁡i∈IpMi(x)p_M(x) = \lim_{i \in I} p_{M_i}(x) for all x∈Ex \in E.

Prop. 8 follows immediately from props. 6 (V, p. 11) and 7 (V, p. 12).

Proposition 9

— Let E be a hilbertian space and M, N two closed vector subspaces of E.

a) The following conditions are equivalent : (i) pMpN=pNpMp_M p_N = p_N p_M; (ii) if x∈Mx \in M is orthogonal to M∩NM \cap N and if y∈Ny \in N is orthogonal to M∩NM \cap N, then x and y are orthogonal; (iii) every vector of M orthogonal to M∩NM \cap N is orthogonal to N; (iv) M=(M∩N)+(M∩N∘)M = (M \cap N) + (M \cap N^\circ).

b) If the equivalent conditions of a) are satisfied, we have pM∩N=pMpNp_{M \cap N} = p_M p_N, the vector subspace M+NM + N of E is closed and we have pM+N=pM+pN−pMpNp_{M+N} = p_M + p_N - p_M p_N.

c) We have pMpN=0p_M p_N = 0 if and only if M is orthogonal to N. If this is so, then the vector subspace M+NM + N of E is closed, and pM+N=pM+pNp_{M+N} = p_M + p_N.

Put L=M∩NL = M \cap N, M1=M∩L∘M_1 = M \cap L^\circ and N1=N∩L∘N_1 = N \cap L^\circ. Condition (ii) implies that M1M_1 and N1N_1 are orthogonal, and (iii) implies that M1M_1 and N are orthogonal. Since we have N=N1+LN = N_1 + L and M1M_1 is orthogonal to L, we have proved the equivalence of (ii) and (iii). If condition (iii) is satisfied, we have M1=M∩N∘M_1 = M \cap N^\circ and since M=L+M1M = L + M_1, condition (iv) is satisfied. Conversely, from (iv) we conclude that M1=M∩N∘M_1 = M \cap N^\circ since the subspaces M∩NM \cap N and M∩N∘M \cap N^\circ of M are orthogonal, and so M1⊂N∘M_1 \subset N^\circ, that is, the relation (iii).

Assume that condition (iv) is satisfied. It is immediate that pN(y)=pL(y)p_N(y) = p_L(y) for all y∈My \in M and hence pNpM(x)=pLpM(x)p_N p_M(x) = p_L p_M(x) for all x∈Ex \in E. But, for every x∈Ex \in E, the vector pLpM(x)p_L p_M(x) belongs to L, and the vector

x−pLpM(x)=(x−pM(x))+(pM(x)−pL(pM(x))) x - p_L p_M(x) = (x - p_M(x)) + (p_M(x) - p_L(p_M(x)))
belongs to M∘+L∘=L∘M^\circ + L^\circ = L^\circ; hence we have pLpM(x)=pL(x)p_L p_M(x) = p_L(x). Finally, pNpM=pLpM=pLp_N p_M = p_L p_M = p_L. Since condition (ii) is equivalent to (iv) and is symmetric in M and N, we also have pMpN=pLp_M p_N = p_L. Finally we get pMpN=pNpM=pM∩Np_M p_N = p_N p_M = p_{M \cap N} which gives (i).

Conversely, suppose condition (i) is satisfied. Let x∈Mx \in M; we have

pM(pN(x))=pN(pM(x))=pN(x) p_M(p_N(x)) = p_N(p_M(x)) = p_N(x)
and so pN(x)∈Mp_N(x) \in M. We conclude that x−pN(x)∈Mx - p_N(x) \in M, hence xx is the sum of an element pN(x)p_N(x) of M∩NM \cap N and an element x−pN(x)x - p_N(x) of M∩N∘M \cap N^\circ, which gives (iv).

We have proved a) and the first part of b). Assume now that pMp_M and pNp_N commute and put q=pM+pN−pMpNq = p_M + p_N - p_M p_N; since pMp_M and pNp_N are idempotents in the algebra L(E)\mathscr{L}(E), so is q; hence (GT, III, § 6, No. 2) the image of q is a closed vector subspace of E.

It is clear that the image of qq is contained in M+NM + N; however, we have pN(x)=xp_N(x) = x, hence q(x)=xq(x) = x for all x∈Nx \in N; since we also have q=pM+pN−pNpMq = p_M + p_N - p_N p_M, we get q(x)=xq(x) = x for all x∈Mx \in M. We conclude that the image of qq is equal to M+NM + N. The orthogonal of M+NM + N is equal to M∘∩N∘M^\circ \cap N^\circ, and the kernel of qq obviously contains M∘∩N∘M^\circ \cap N^\circ, hence q=pM+Nq = p_{M+N}. This proves b).

We have pMpN=0p_M p_N = 0 if and only if the image NN of pNp_N is contained in the kernel M∘M^\circ of pMp_M, that is, if and only if MM is orthogonal to NN. The rest of the assertion c) is then a particular case of b).

Remark

— Let EE be a hilbertian space and M,NM, N two closed vector subspaces of EE. The relation M⊂NM \subset N is equivalent to the orthogonality of MM and N∘N^\circ, that is to say, to the relation pMpN∘=0p_M p_{N^\circ} = 0 by prop. 9, c). Since we have pN∘=1−pNp_{N^\circ} = 1 - p_N, we conclude that the relations M⊂NM \subset N and pM=pMpNp_M = p_M p_N are equivalent (« the three perpendicular theorem », cf. fig. 3).

!Diagram showing subspaces M, N, and projections p_M(x), p_N(x)

Fig. 3.

7. Dual of a hilbertian space

Theorem 3

Let EE be a hilbertian space. For every x∈Ex \in E, let x∗x^* be the continuous linear form y↦⟨x∣y⟩y \mapsto \langle x | y \rangle on EE; the mapping x↦x∗x \mapsto x^* is a bijective, semi-linear (for the automorphism ξ↦ξˉ\xi \mapsto \bar{\xi}) mapping from EE onto its dual E′E', and an isometry from the normed space EE onto the normed space E′E'.

The mapping x↦x∗x \mapsto x^* is semi-linear by (2) (V, p. 1) and by virtue of the Cauchy-Schwarz inequality, we have ∥x∗∥=sup⁡∥y∥≤1∣⟨x∣y⟩∣=∥x∥\|x^*\| = \sup_{\|y\| \leq 1} |\langle x | y \rangle| = \|x\|, hence x↦x∗x \mapsto x^* is an isometry from EE into E′E', and in particular, is injective. To complete the proof, we need to prove that for all x′≠0x' \neq 0 in E′E', there exists x∈Ex \in E such that x′=x∗x' = x^*. But the hyperplane H=Ker x′H = \mathrm{Ker}\, x' is closed in EE; its orthogonal is a line DD. Let bb be a non-zero element of DD; the kernel of the linear form b∗b^* is equal to HH and hence there exists a scalar λ≠0\lambda \neq 0 such that x′=λ⋅b∗=(λ‾⋅b)∗x' = \lambda \cdot b^* = (\overline{\lambda} \cdot b)^*. Q.E.D.

The mapping x↦x∗x \mapsto x^* from EE onto its dual E′E' is said to be canonical. The inverse mapping from E′E' onto EE is also called canonical and is denoted by x′↦x′∗x' \mapsto {x'}^*. We have

⟨x∣y⟩=⟨y,x∗⟩,⟨x,x′⟩=⟨x′∗∣x⟩ \langle x | y \rangle = \langle y, x^* \rangle, \quad \langle x, x' \rangle = \langle {x'}^* | x \rangle

for x,yx, y in EE and x′x' in E′E'. Also (x∗)∗=x(x^*)^* = x for x∈Ex \in E.

When K is R\mathbf{R}, the mapping x↦x∗x \mapsto x^* is linear. We shall transfer the scalar product of E to E' by this mapping. When K=CK = \mathbf{C}, we can consider the mapping x↦x∗x \mapsto x^* as an isomorphism from the vector space E‾\overline{E}, the conjugate of E onto E' (V, p. 6). We shall transfer the scalar product of E‾\overline{E} to E' by this mapping.

In the two cases considered, E' is a hilbertian space and we have the formulae

⟨x∗∣y∗⟩=⟨x∣y⟩‾,⟨x′∣x′⟩=∥x′∥2 \langle x^*|y^* \rangle = \overline{\langle x|y \rangle}, \quad \langle x'|x' \rangle = \|x'\|^2

for x,yx, y in E and x′x' in E'.

To say that the vector x∈Ex \in E is orthogonal to a vector y∈Ey \in E is equivalent to saying that the linear form x∗∈E′x^* \in E' is orthogonal to yy in the sense defined in II, p. 41 (this justifies the use of the word « orthogonal » in the two cases). If M is a closed vector subspace of E, the subspace M∘M^\circ orthogonal to M in E' (II, p. 44) is the image under x↦x∗x \mapsto x^* of the orthogonal of M in E, defined in V, p. 13 (this justifies the use of the notation M∘M^\circ in the two cases).

Corollary 1

In order that the family (xi)i∈I(x_i)_{i \in I} of points of a hilbertian space E be total, it is necessary and sufficient that the relations ⟨xi∣y⟩=0\langle x_i|y \rangle = 0 for y∈Ey \in E and for all indices i∈Ii \in I imply that y=0y = 0.

In fact, this says that 0 is the only vector of E' which is orthogonal to all the xix_i (II, p. 43 and IV, p. 1).

Corollary 2

Let E and F be two hilbertian spaces. For u∈L(E;F)u \in \mathscr{L}(E; F), x∈Ex \in E and y∈Fy \in F, put

Φu(y,x)=⟨y∣u(x)⟩. \Phi_u(y, x) = \langle y|u(x) \rangle .

The mapping u↦Φuu \mapsto \Phi_u is an isomorphism from the Banach space L(E;F)\mathscr{L}(E; F) onto the space of all continuous sesquilinear 1^1 forms on F×EF \times E, endowed with the norm

∥f∥=sup⁡x∈E,y∈F∥x∥≤1,∥y∥≤1∣f(y,x)∣. \|f\| = \sup_{\substack{x \in E, y \in F \\ \|x\| \leq 1, \|y\| \leq 1}} |f(y, x)| .

It is clear that Φu\Phi_u is sesquilinear and continuous for all u∈L(E;F)u \in \mathscr{L}(E; F). Conversely, let ff be a continuous sesquilinear form on F×EF \times E. For every x∈Ex \in E, the mapping y↦f(y,x)y \mapsto f(y, x) is a continuous linear form on the hilbertian space F. By th. 3, for every x∈Ex \in E, there exists a unique element u(x)u(x) in F such that f(y,x)=⟨u(x)∣y⟩f(y, x) = \langle u(x)|y \rangle for all y∈Fy \in F. The mapping u:x↦u(x)u : x \mapsto u(x) from E into F is linear and we have

∥f∥=sup⁡∥x∥≤1sup⁡∥y∥≤1∣f(y,x)∣=sup⁡∥x∥≤1sup⁡∥y∥≤1∣⟨y∣u(x)⟩∣=sup⁡∥x∥≤1∥u(x)∥; \begin{align*} \|f\| &= \sup_{\|x\| \leq 1} \sup_{\|y\| \leq 1} |f(y, x)| = \sup_{\|x\| \leq 1} \sup_{\|y\| \leq 1} |\langle y|u(x) \rangle| \\ &= \sup_{\|x\| \leq 1} \|u(x)\| ; \end{align*}

hence uu belongs to L(E;F)\mathscr{L}(E; F), f=Φuf = \Phi_u and ∥u∥=∥f∥\|u\| = \|f\|. This proves cor. 2.

1^1 Recall (A, IX, § 1, No. 5) that a sesquilinear form (on the left) ff on F×EF \times E is a mapping from F×EF \times E into K which satisfies relations (1) and (2) of V, p. 1.

The canonical mapping from E into its bidual E'' (IV, p. 14) maps E onto E'', in other words (IV, p. 16), E is a reflexive Banach space. In fact, if E is a real (resp. complex) hilbertian space, the canonical mapping φ from E' onto E is an isomorphism from the normed space E' onto E (resp. onto the conjugate space E‾\overline{E} of E); applying th. 3 to E (resp. E), we see that every continuous linear form on the normed space E' is of the form x′↦⟨ϕ(x′)∣x⟩=⟨x,x′⟩x' \mapsto \langle \phi(x')|x \rangle = \langle x, x' \rangle with x∈Ex \in E, hence our assertion follows.

As a consequence (IV, p. 17, prop. 6):

Theorem 4

In a hilbertian space E, the unit ball is weakly compact.

Proposition 10

If, in a hilbertian space E, a filter F\mathfrak{F} converges weakly to x0x_0, and if moreover lim⁡F∥x∥=∥x0∥\lim_{\mathfrak{F}} \|x\| = \|x_0\|, then F\mathfrak{F} converges to x0x_0 for the initial topology of E.

In fact, ∥x−x0∥2=∥x∥2−2ℜ⟨x∣x0⟩+∥x0∥2\|x - x_0\|^2 = \|x\|^2 - 2\Re \langle x|x_0 \rangle + \|x_0\|^2. Since ⟨x∣x0⟩\langle x|x_0 \rangle tends to ∥x0∥2\|x_0\|^2 with respect to F\mathfrak{F} by hypothesis, and ∥x∥\|x\| tends to ∥x0∥\|x_0\| with respect to F\mathfrak{F}, ∥x−x0∥\|x - x_0\| tends to 0 with respect to F\mathfrak{F}, hence the proposition.

Remark

— If E is a Hausdorff prehilbertian space and E^\hat{E} the hilbertian space completion of E, we know (III, p. 16) that the dual E' of E can be identified with the dual of E^\hat{E}; it then follows from th. 3 (V, p. 15) that every continuous linear form on E can be written in a unique way as x↦⟨a∣x⟩x \mapsto \langle a|x \rangle, where a∈E^a \in \hat{E}.

Exercises

See the exercises for § 1.

Transcribed from the printed volume. Not translated.