Bourbaki

§ 4. Partial operators

1. Partial operators

In this number, K is a commutative field.

We recall (E, II, §3, p. 9–10) that a graph[^1] is a set all of whose elements are pairs. If A and B are sets, a correspondence between A and B is a triplet (Γ,A,B)(\Gamma ,A,B), where Γ is a graph contained in A×BA\times B; its set of definition (also called its domain) is pr1_1(Γ), and the set of its values is pr2(Γ)_2(\Gamma ). A correspondence is a function (E, II, p. 13, def. 9) if its graph is functional and if its initial set coincides with its set of definition. Every subset of a functional graph is a functional graph.

Definition 1 032J

Let E and F be vector spaces over K. A partial operator uu from E into F is a correspondence (Γ,E,F)(\Gamma ,E,F) between E and F satisfying the following conditions:

(i) The graph Γ is a vector subspace of E×FE\times F;

(ii) The graph Γ is functional.

If E = F, one says that uu is a partial operator on E.

Let uu be a partial operator from E into F. The graph Γ of the correspondence uu is called the graph of the partial operator uu, and is also denoted by Γu\Gamma_u. We denote by P(E;F)\mathscr{P}(E; F) the set of partial operators from E into F; we write simply P(E)=P(E;E)\mathscr{P}(E) =\mathscr{P}(E; E).

To give a partial operator from E into F amounts to giving a vector subspace D of E and a linear mapping uu from D into F, the associated partial operator being the correspondence (Γ,E,F)(\Gamma ,E,F) where Γ⊂D×F\Gamma \subset D\times F is the graph of uu.

The domain of definition of a partial operator uu is called simply the domain of uu, and denoted by dom(uu).

Every linear mapping uu from E into F is a partial operator from E into F.

If D⊂ED\subset E is a vector subspace, we shall denote by 1D1_D the partial operator with domain D which is the identity mapping on D, that is, the correspondence (ΔD,E,E)(\Delta_D,E,E) where ΔD\Delta_D is the diagonal of D×DD\times D (E, II, p. 13, def. 8). We shall denote by 0D0_D the partial operator with domain D which is zero on D, that is, the correspondence (D×{0},E,F)(D\times \{0\},E,F).

Two partial operators u=(Γ,E,F)u= (\Gamma ,E,F) and u′=(Γ′,E,F)u'= (\Gamma ',E,F) from E into F are equal if and only if dom(uu) == dom(u′u') and if the linear mappings uu and u′u' from dom(uu) into F coincide.

Following E, II, §3, the following notions are defined:

(i) Let uu be a partial operator from E into F; let D be its domain and u:D→Fu: D\rightarrow F the associated linear mapping. The image of a subset A of E by uu is the subset u(A∩D)u(A\cap D) of F; it is denoted simply by u(A)u(A). The inverse image by uu of a subset B of F by uu is the subset u−1(B)\overset{-1}{u}(B) of D.

If A (resp. B) is a vector subspace of E (resp. of F), then its image by uu (resp. its inverse image) is a vector subspace of F (resp. of E).

The image of uu is the vector subspace u(D)u(D) of F, also denoted by Im(uu). One says that uu is a surjective partial operator if Im(uu) =F= F. The kernel of uu is the vector subspace u−1({0})\overset{-1}{u}(\{0\}) of E, also denoted by Ker(uu). The kernel of uu is reduced to 0 if and only if the linear mapping uu from dom(uu) into F is injective. One then says that uu is injective. If uu is injective and surjective, one says that it is bijective.

(ii) If E, F and G are K-vector spaces and u=(Γ,E,F)u= (\Gamma ,E,F), v=(Γ′,F,G)v= (\Gamma ',F,G) are partial operators from E into F and from F into G, respectively, the composite correspondence v∘u=(Γ′∘Γ,E,G)v\circ u= (\Gamma '\circ \Gamma ,E,G) is a partial operator from E into G. Its domain is u−1\overset{-1}{u}(dom(vv)). If H is a K-vector space and w=(Γ′′,G,H)w= (\Gamma '',G,H) a partial operator from G into H, one has w∘(v∘u)=(w∘v)∘uw\circ (v\circ u) = (w\circ v)\circ u. One will sometimes write vuvu instead of v∘uv\circ u.

(iii) In particular, for every partial operator uu from E into F and every a∈Ka\in K, the partial operators au=(a1F)∘uau= (a1_F)\circ u and ua=u∘(a1E)ua=u\circ (a1_E) are defined. They are equal if a≠0a\not = 0, or if the domain of uu is equal to E; one has u0=0Eu0 = 0_E and 0u=0dom(u)0u= 0_{dom(u)}.

Let E be a vector space. From what precedes, the set P\mathscr{P}(E), endowed with the law of composition defined by (u,v)↦u∘v(u, v)\mapsto u\circ v, is a unital associative magma (A, I, p. 4, Def. 5 and A, I, p. 12, Def. 2) with identity element 1E1_E. For every n∈Nn\in \mathbf{N}, one denotes by unu^n the composite ∘nu\overset{n}{\circ}u (A, I, p. 13).

Moreover, one defines the following notions:

(i) If u=(Γ,E,F)u= (\Gamma ,E,F) is a partial operator from E into F, and if G is a subspace of E, the reduction of uu to G is the partial operator (Γ∩(G×F),E,F)(\Gamma \cap (G\times F),E,F) from E into F. Its domain is dom(uu)∩G\cap G; one will sometimes denote it by u∣Gu|G, when no confusion with the restriction of uu to the subspace G is to be feared.

(ii) Let vv be an injective partial operator from F into E. Then the inverse correspondence v−1=(Γ−1,E,F)v^{-1}= (\Gamma^{-1},E,F) of vv is a partial operator such that dom(v−1v^{-1}) == Im(vv). One says that v−1v^{-1} is the inverse partial operator of vv. One has the equalities v∘v−1=1dom(v−1)v\circ v^{-1}= 1_{dom(v^{-1})} in P(E)\mathscr{P}(E) and v−1∘v=1dom(v)v^{-1}\circ v= 1_{dom(v)} in P(F)\mathscr{P}(F). The partial operator v−1v^{-1} is injective and one has (v−1)−1=v(v^{-1})^{-1}=v.

(iii) Let E, F and G be vector spaces. Let uu (resp. vv) be an injective partial operator from E into F (resp. from F into G). Then the partial operator v∘uv\circ u is injective and (v∘u)−1=u−1∘v−1(v\circ u)^{-1}=u^{-1}\circ v^{-1}.

(iv) If uu and vv are partial operators from E into F, one says that vv is an extension of uu, and one writes u⊂vu\subset v, if the graph of uu is contained in the graph of vv. This implies that dom(uu)⊂\subset dom(vv) and that uu is the restriction of vv to dom(uu). The relation “ u⊂vu\subset v ” is an order relation in P(E;F)\mathscr{P}(E; F). For example, one has au⊂uaau\subset ua for every a∈Ka\in K and every u∈P(E;F)u\in \mathscr{P}(E; F).

(v) Let E be a vector space over K and (Fi)i∈I(F_i)_{i\in I} a family of vector spaces over K. For i∈Ii\in I, let uiu_i be a partial operator from E into FiF_i. The product partial operator of the uiu_i is the partial operator from E into the product vector space of the spaces FiF_i whose domain is the intersection D of the spaces dom(uiu_i) and which associates to x∈Dx\in D the family (ui(x))i∈I(u_i(x))_{i\in I}. It is denoted by (ui)i∈I(u_i)_{i\in I}.

(vi) Let A:F×F→FA : F\times F\rightarrow F be the linear mapping (x,y)↦x+y(x, y)\mapsto x+y. Let uu and vv be partial operators from E into F. The sum u+vu+v is the partial operator A∘(u,v)A\circ (u, v) from E into F. Its domain is dom(uu)∩\cap dom(vv). For u,v,wu,v,w in P(E;F)\mathscr{P}(E; F), one has (u+v)+w=u+(v+w)(u+v) +w=u+ (v+w).

Let G be a vector space over K. For every uu and vv in P(E;F)\mathscr{P}(E; F) and every w∈P(F;G)w\in \mathscr{P}(F; G), one has w∘u+w∘v⊂w∘(u+v)w\circ u+w\circ v\subset w\circ (u+v). In general, there is no equality in this formula (exercise 1 of IV, p. 344), but this is the case when the domain of ww is equal to F. For w∈P(G;E)w\in \mathscr{P}(G; E), one has u∘w+v∘w=(u+v)∘wu\circ w+v\circ w= (u+v)\circ w.

(vii) Let L be an extension of the field K. Let E and F be vector spaces over K and E(L)=L⊗KE,F(L)=L⊗KFE_{(L)}= L\otimes_KE, F_{(L)}= L\otimes_KF the L-vector spaces obtained by extension of scalars from K to L (A, II, p. 82). For every partial operator uu from E into F, let u(L)u_{(L)} denote the partial operator from E(L)E_{(L)} into F(L)F_{(L)} whose graph is the vector subspace L⊗KΓuL\otimes_K\Gamma_u of E(L)×F(L)E_{(L)}\times F_{(L)}; its domain is L⊗KL\otimes_K dom(uu), and it coincides on this with the unique linear mapping sending 1⊗x1\otimes x to 1⊗u(x)1\otimes u(x) for every x∈x\in dom(uu).

Let vv be a partial operator from E into F. One has u⊂vu\subset v if and only if u(L)⊂v(L)u_{(L)}\subset v_{(L)}.

(viii) Let E1,F1,E2,F2E_1, F_1, E_2, F_2 be K-vector spaces. Let uu (resp. vv) be a partial operator from E1E_1 into F1F_1 (resp. from E2E_2 into F2F_2). Let u⊗vu\otimes v denote the partial operator from E1⊗F1E_1\otimes F_1 into E2⊗F2E_2\otimes F_2 with domain dom(uu)⊗\otimesdom(vv) such that (u⊗v)(x⊗y)=u(x)⊗v(y)(u\otimes v)(x\otimes y) =u(x)\otimes v(y) for every (x,y)∈E1×E2(x, y)\in E_1\times E_2.

2. Closed operators, closable operators, and operators with dense domain

In this No., K denotes a commutative topological field (TG, III, p. 54).

Definition 2 032K

Let E and F be topological vector spaces over K (EVT, I, p. 1, def. 1). Let u∈P(E;F)u\in \mathscr{P}(E; F) be a partial operator from E into F.

One says that uu is an operator with dense domain if the domain of uu is dense in E.

One says that uu is closed if the graph of uu is closed in the topological vector space E×FE\times F. One says that uu is closable if it possesses a closed extension.

Let E, F and G be topological vector spaces over K. Every extension of an operator u∈P(E;F)u\in \mathscr{P}(E; F) with dense domain has dense domain. Moreover, if v∈L(E;F)v\in \mathscr{L}(E; F), then u+vu+v is an operator with dense domain. If v:F→Gv: F\rightarrow G (resp. w:G→Ew: G\rightarrow E) is an isomorphism of topological vector spaces, then v∘uv\circ u (resp u∘wu\circ w) is an operator with dense domain.

Example 032L

Let E and F be topological vector spaces over K.

1) Suppose the space F separated. Let uu be a linear mapping from E into F. If uu is continuous, then the partial operator uu is closed (TG, I, p. 53, Corollary 2). Suppose moreover that K is a non-discrete valued field and that E and F are metrisable complete topological vector spaces over K. By the closed graph theorem (EVT, I, p. 19, Corollary 5), the partial operator defined by uu is then closed if and only if uu is continuous.

2) Suppose the space E separated. Let vv be an injective continuous linear mapping from F into E. The partial operator v−1∈P(E;F)(v^{-1}\in \mathscr{P}(E; F) (cf. IV, p. 226) is then closed, since its graph is the image of the graph of vv, which is closed, under the isomorphism of topological vector spaces from F×EF\times E onto E×FE\times F defined by (y,x)↦(x,y)(y, x)\mapsto (x, y).

Proposition 1 032M

Let E and F be topological vector spaces over K. A partial operator uu of E into F is closable if and only if the closure of the graph Γu\Gamma_u of uu in E×FE\times F is a functional graph. There then exists a unique partial operator vv of E into F whose graph is Γ‾u\overline{\Gamma}_u, and it is the smallest closed extension of uu.

If the closure of the graph of uu in E×FE\times F is a functional graph, it is the graph of a partial operator, and this is a closed extension of uu, so that uu is closable. Conversely, suppose that u⊂wu\subset w with ww closed. The closure Γ‾u\overline{\Gamma}_u of the graph of uu in E×FE\times F is contained in Γw\Gamma_w, hence Γu\Gamma_u is a functional graph.

The last assertion follows from the fact that if ww is a closed extension of uu, then the graph of ww contains Γ‾u\overline{\Gamma}_u.

Definition 3 032N

Let E and F be topological vector spaces over K. Let uu be a closable operator of E into F. The closed operator whose graph is Γu\Gamma_u is called the closure of uu. It is denoted by u‾\overline{u}.

Remark 032O

Let E and F be topological vector spaces over K. Let uu be a closable operator of E into F. The domain of the closure of uu is contained in the closure of the domain of uu in E. In general, it is distinct from it (exercise 1 of IV, p. 344, b)).

If u∈P(E;F)u\in \mathscr{P}(E; F) is closable and dom(uu) =E= E, then u=u‾u=\overline{u} is closed, since then dom(u‾\overline{u}) == dom(uu).

Proposition 2 032P

Let K=RK =\mathbf{R} and let E and F be topological vector spaces over R\mathbf{R}. Let uu be a partial operator of E into F. Then uu has dense domain (resp. is closed, is closable) if and only if u(C)u_{(\mathbf{C})} has dense domain (resp. is closed, is closable).

Suppose that the domain of uu is dense in E. Every neighbourhood of 0 in E(C)E_{(\mathbf{C})} contains a neighbourhood of the form V+iVV +iV (TVS, II, p. 65), where V is a neighbourhood of 0 in E, and therefore contains an element of the domain of u(C)u_{(\mathbf{C})}; this partial operator therefore has dense domain. The converse is also true since the mapping of E(C)E_{(\mathbf{C})} into E which associates xx to x+iyx+iy for every (x,y)∈E×E(x, y)\in E\times E is continuous and surjective.

The graph of u(C)u_{(\mathbf{C})} identifies with the complexified topological vector space of the graph of uu. It is therefore closed in E(C)×E(C)E_{(\mathbf{C})}\times E_{(\mathbf{C})} if the graph of uu is closed in E×EE\times E. Conversely, one has Γu=Γu(C)∩(E×E)\Gamma_u= \Gamma_{u_{(\mathbf{C})}}\cap (E\times E) in E(C)×E(C)E_{(\mathbf{C})}\times E_{(\mathbf{C})}; since E×EE\times E is closed in E(C)×E(C)E_{(\mathbf{C})}\times E_{(\mathbf{C})}, the partial operator uu is closed when u(C)u_{(\mathbf{C})} is.

A partial operator vv from E into F is an extension of uu if and only if v(C)v_{(\mathbf{C})} is an extension of u(C)u_{(\mathbf{C})}, hence the partial operator u(C)u_{(\mathbf{C})} is closable if uu is closable. Conversely, if u(C)u_{(\mathbf{C})} is closable, the partial operator uu is also, since Γu=Γu(C)∩(E×E)\Gamma_u= \Gamma_{u_{(\mathbf{C})}}\cap (E\times E), which is then a functional graph (prop. 1).

Lemma 1 032Q

Let E, F and G be topological vector spaces over K. Let uu be a closed operator from E into F.

a) For every v∈L(E;F)v\in \mathscr{L}(E; F), the partial operator u+vu+v is closed.

b) For every v∈L(G;E)v\in \mathscr{L}(G; E), the partial operator u∘vu\circ v is closed.

Let us prove a). Let γ\gamma be the mapping (x,y)↦(x,y−v(x))(x, y)\mapsto (x, y-v(x)) of E×FE\times F into itself; it is continuous. For every (x,y)∈E×F(x, y)\in E\times F, one has γ(x,y)∈Γu\gamma (x, y)\in \Gamma_u if and only if x∈x\in dom(uu) and y=u(x)+v(x)y=u(x) +v(x), that is to say that γ−1(Γu)=Γu+v\overset{-1}{\gamma}(\Gamma_u) = \Gamma_{u+v}. The assertion follows.

Let us prove b). The mapping η=(v,1F)\eta = (v,1_F) of G×FG\times F into E×FE\times F is continuous; for every (z,y)∈G×F(z, y)\in G\times F, one has η(z,y)=(v(z),y)\eta (z, y) = (v(z), y), hence η−1(Γu)=Γu∘v\overset{-1}{\eta}(\Gamma_u) = \Gamma_{u\circ v}. The assertion follows.

Let E and F be topological vector spaces over K, F being separated. Let a∈Ka\in K. If u∈P(E;F)u\in \mathscr{P}(E; F) is closable, the same is true of auau. If a≠0a\not = 0, one has au‾=au\overline{au}=au, and uu is closed if and only if auau is. If a=0a= 0, the closure of auau is 0dom(u)‾0_{\overline{dom(u)}}, and auau is equal to 0dom(u‾)0_{dom(\overline{u})}; it may therefore happen that uu is closed but that auau is not.

Proposition 3 032R

Let E and F be topological vector spaces over K, F being separated. Let uu be a closed partial operator from E into F. The kernel of uu is a closed subspace of E.

In fact, the kernel of uu is the inverse image of the closed subspace Γu∩(E×{0})\Gamma_u\cap (E\times \{0\}) of E×FE\times F by the continuous linear mapping x↦(x,0)x\mapsto (x,0) of E into E×FE\times F.

In the rest of this No., it is assumed that K is a non-discrete valued field.

Definition 4 032S

Let E and F be normed spaces over K and let uu be a partial operator from E into F. For xx in dom(uu), one writes

∥x∥u=(∥x∥E2+∥u(x)∥F2)1/2 \|x\|_u= (\|x\|^2_E+\|u(x)\|^2_F)^{1/2}

The mapping x↦∥x∥ux\mapsto \|x\|_u resulting is a norm on dom(uu). The normed space thus obtained is denoted by EuE_u.

Remark 032T

Let E and F be normed spaces over K and let uu be a partial operator from E into F.

1) The canonical injection of EuE_u into E is continuous since one has ∥x∥⩽∥x∥u\|x\|\leqslant \|x\|_u for every x∈Ex\in E. In particular, every subspace of dom(uu) which is closed in E is closed in EuE_u.

2) If E and F are Hilbert spaces, then the space EuE_u is a prehilbertian space, since the norm on EuE_u arises from the positive Hermitian form

(x,y)↦(x∣y)u=⟨x∣y⟩+⟨u(x)∣u(y)⟩ (x, y)\mapsto (x|y)_u=\langle x|y\rangle +\langle u(x)|u(y)\rangle

on dom(uu).

Proposition 4 032U

Let E and F be Banach spaces (resp. Hilbert spaces), and let uu be a partial operator from E into F. Then uu is closed if and only if the normed space EuE_u is a Banach space (resp. a Hilbert space).

It is enough to treat the case of Banach spaces. The norm of EuE_u is obtained, by transport of structure by means of the bijective linear mapping (x,y)↦x(x, y)\mapsto x of Γu\Gamma_u onto dom(uu), from the norm obtained by restriction to the subspace Γu\Gamma_u of the norm (x,y)↦(∥x∥E2+∥y∥F2)1/2(x, y)\mapsto (\|x\|^2_E+\|y\|^2_F)^{1/2} on the Banach space E⊕FE\oplus F. Thus the space EuE_u is a Banach space if and only if the subspace Γu\Gamma_u of E⊕FE\oplus F is closed.

If uu and vv are partial operators from E into F and from F into G, respectively, and if uu is closed, then the partial operator v∘uv\circ u is not closed in general, even if vv is continuous (exercise 1 of IV, p. 344, c)). One nevertheless has the following sufficient condition:

Lemma 2 032V

Let E, F and G be normed spaces over K, F being a Banach space. Let uu be a closed partial operator from E into F and let v∈L(F;G)v\in \mathscr{L}(F; G). If there exists C∈R+C\in \mathbf{R}_+ such that

∥u(x)∥⩽C(∥x∥+∥(v∘u)(x)∥) \|u(x)\|\leqslant C(\|x\|+\|(v\circ u)(x)\|)

for every x∈x\in dom(v∘uv\circ u) == dom(uu), that is to say, if the linear mapping x↦u(x)x\mapsto u(x) from Ev∘uE_{v\circ u} into F is continuous, then v∘uv\circ u is closed.

Let us write w=v∘uw=v\circ u. Let (xn,w(xn))n∈N(x_n, w(x_n))_{n\in\mathbf{N}} be a sequence in the graph of ww which converges in E×GE\times G. Let xx be the limit of the sequence (xn)(x_n). The hypothesis implies that the sequence (u(xn))n∈N(u(x_n))_{n\in\mathbf{N}} is then a Cauchy sequence in F; it converges to an element yy of F. Since uu is closed, one has therefore x∈x\in dom(uu) and y=u(x)y=u(x). Then w(xn)=v(u(xn))w(x_n) =v(u(x_n)) tends to v(y)=v(y) = v(u(x))v(u(x)) since vv is continuous, hence the graph of ww is closed.

Let uu be a closed partial operator on a Banach space E and F a subspace of dom(uu). If F is dense in the Banach space EuE_u, then the restriction of uu to F is closable, and its closure is equal to uu. One then says that F is a core for uu.

3. Examples of partial operators

In this No., K=RK =\mathbf{R} or C\mathbf{C}.

Example 1 032W

Let X be a locally compact topological space and let μ\mu be a positive measure on X. Let p1p_1 and p2p_2 be fixed elements of [1,+∞[[1,+\infty [.

Let gg be a μ\mu-measurable function on X with values in K. Let D denote the subspace of LKp1(X,μ)\mathscr{L}_K^{p_1}(X, \mu) formed by the functions ff in LKp1(X,μ)\mathscr{L}_K^{p_1}(X, \mu) such that gf∈LKp2(X,μ)gf\in \mathscr{L}_K^{p_2}(X, \mu). The linear mapping from D into LKp2(X,μ)\mathscr{L}_K^{p_2}(X, \mu) defined by f↦gff\mapsto gf determines a partial operator from LKp1(X,μ)\mathscr{L}_K^{p_1}(X, \mu) into LKp2(X,μ)\mathscr{L}_K^{p_2}(X, \mu), which is denoted by mgm_g.

The vector subspace of μ\mu-negligible functions in LKp1(X,μ)\mathscr{L}_K^{p_1}(X, \mu) is contained in D, and the image under mgm_g of a μ\mu-negligible function is again μ\mu-negligible. We shall denote by m~g\widetilde{m}_g the partial operator from LKp1(X,μ)L^{p_1}_K(X, \mu) into LKp2(X,μ)L^{p_2}_K(X, \mu) deduced from mgm_g by passing to quotients. It is said to be the multiplication operator by gg from LKp1(X,μ)L^{p_1}_K(X, \mu) into LKp2(X,μ)L^{p_2}_K(X, \mu). Functions g1g_1 and g2g_2 which are locally equal μ\mu-almost everywhere define the same multiplication operator.

Proposition 5 032X

The multiplication operator m~g\widetilde{m}_g from LKp1(X,μ)L^{p_1}_K(X, \mu) into LKp2(X,μ)L^{p_2}_K(X, \mu) is a closed operator with dense domain.

Let us first prove that the partial operator m~g\widetilde{m}_g is closed. Let (fn,hn)n∈N(f_n, h_n)_{n\in\mathbf{N}} be a sequence in LKp1(X,μ)×LKp2(X,μ)\mathscr{L}_K^{p_1}(X, \mu)\times \mathscr{L}_K^{p_2}(X, \mu) such that the sequence (fn~,h~n)(f_{\widetilde{n}},\widetilde{h}_n) of the classes of fnf_n and hnh_n belongs to the graph of m~g\widetilde{m}_g and converges in LKp1(X,μ)×LKp2(X,μ)L^{p_1}_K(X, \mu)\times L^{p_2}_K(X, \mu) when nn tends to infinity. Let (f,h)(f, h) be a pair in LKp1(X,μ)×LKp2(X,μ)\mathscr{L}_K^{p_1}(X, \mu)\times \mathscr{L}_K^{p_2}(X, \mu) such that the pair (f~,h~)(\widetilde{f} ,\widetilde{h}) of their classes is the limit of (f~n,h~n)(\widetilde{f}_n,\widetilde{h}_n).

There exists a sequence (fnk)k∈N(f_{n_k})_{k\in\mathbf{N}} extracted from the sequence (fn)n(f_n)_n such that fnk(x)f_{n_k}(x) converges to f(x)f(x) for μ\mu-almost every xx (INT, IV, p. 131, § 3, no4^o4, th. 3). This implies that hnk(x)=g(x)fnk(x)h_{n_k}(x) =g(x)f_{n_k}(x) converges μ\mu-almost everywhere to g(x)f(x)g(x)f(x). Moreover the sequence (hnk)(h_{n_k}) converges to hh in the space LKp2(X,μ)\mathscr{L}_K^{p_2}(X, \mu). The functions hh and gfgf are therefore equal μ\mu-almost everywhere (loc. cit.). Thus f~\widetilde{f} belong to the domain of m~g\widetilde{m}_g and h~=m~g(f~)\widetilde{h}=\widetilde{m}_g(\widetilde{f}). This proves that m~g\widetilde{m}_g is closed.

Let us prove that the domain of m~g\widetilde{m}_g is dense in LKp1(X,μ)L^{p_1}_K(X, \mu). It is enough to verify that the classes of functions f∈K(X;K)f\in \mathscr{K}(X; K) belong to the closure of the domain of m~g\widetilde{m}_g in LKp1(X,μ)L^{p_1}_K(X, \mu). Let f∈K(X;K)f\in \mathscr{K}(X; K) and let f~\widetilde{f} be its class in LKp1(X,μ)L^{p_1}_K(X, \mu). For every integer n∈Nn\in \mathbf{N}, let φn\varphi_n denote the characteristic function of the set of elements x∈Xx\in X such that ∣g(x)∣⩽n|g(x)|\leqslant n, and put fn=fφnf_n=f \varphi_n. Then ∣gfn∣⩽n∣f∣|gf_n|\leqslant n|f|, which belong to LKp2(X,μ)\mathscr{L}_K^{p_2}(X, \mu), hence fnf_n belong to the domain of m~g\widetilde{m}_g. For every element xx of X, the sequence (fn(x))n∈N(f_n(x))_{n\in\mathbf{N}} converges to f(x)f(x) when n→+∞n\rightarrow +\infty; moreover, one has ∣fn∣⩽∣f∣|f_n|\leqslant |f|, which belong to LKp1(X,μ)\mathscr{L}_K^{p_1}(X, \mu). By Lebesgue's theorem (INT, IV, p. 137, § 3, no7^o7, th. 6), the sequence of classes of fnf_n converges to f~\widetilde{f} in LKp1(X,μ)L^{p_1}_K(X, \mu). Thus, the class of ff belong to the closure of the domain of m~g\widetilde{m}_g.

In the following proposition, it is supposed that p1=p2=2p_1=p_2= 2.

Proposition 6 032Y

a) Let g′g' be a μ\mu-measurable function on X such that ∣g∣⩽∣g′∣|g|\leqslant |g'|. One has dom(m~g′\widetilde{m}_{g'})⊂\subset dom(m~g\widetilde{m}_g) and dom(m~g′\widetilde{m}_{g'}) is a core of the partial operator m~g\widetilde{m}_g;

b) Let F be a subspace of LK2(X,μ)\mathscr{L}_K^2(X, \mu) whose intersection with K(X;K)\mathscr{K}(X; K) is dense in K(X;K)\mathscr{K}(X; K) and whose image G in LK2(X,μ)L^2_K(X, \mu) is contained in dom(m~g\widetilde{m}_g). If ∣g∣2|g|^2 is locally μ\mu-integrable, then K(X;K)\mathscr{K}(X; K) is contained in the domain of m~g\widetilde{m}_g and G is a core of mgm_g.

Let us prove a). If f∈LK2(X,μ)f\in \mathscr{L}_K^2(X, \mu) belong to the domain of mg′m_{g'}, so that fg′∈LK2(X,μ)f g'\in \mathscr{L}_K^2(X, \mu), the assumption implies that fg∈LK2(X,μ)f g\in \mathscr{L}_K^2(X, \mu), whence the result.

Let us prove that dom(m~g′\widetilde{m}_{g'}) is a core of m~g\widetilde{m}_g, that is to say that the domain of m~g′\widetilde{m}_{g'} is dense in the Hilbert space Em~gE_{\widetilde{m}_g}. Let h∈LK2(X,μ)h\in \mathscr{L}_K^2(X, \mu)

whose class h~\widetilde{h} belong to Em~gE_{\widetilde{m}_g} and is orthogonal to dom(m~g′\widetilde{m}_{g'}). This means that

(h~∣h~′)m~g=∫Xhh′(1+∣g∣2)dμ=0 (\widetilde{h}|\widetilde{h}')_{\widetilde{m}_g}=\int_Xh h'(1 +|g|^2)d\mu= 0

for every function h′∈LK2(X,μ)h'\in \mathscr{L}_K^2(X, \mu) whose class h~′\widetilde{h}' belongs to dom(m~g′\widetilde{m}_{g'}).

Let C be a compact subset of X and let φ\varphi be its characteristic function. Let n∈Nn\in \mathbf{N}. Denote by φn\varphi_n the characteristic function of the μ\mu-integrable set CnC_n of the x∈Cx\in C such that ∣h(x)∣⩽n|h(x)|\leqslant n and put hn′=φnhh'_n=\varphi_nh. The class of hn′h'_n belongs to the domain of m~g′\widetilde{m}_{g'} since ∣g′hn′∣⩽nφ|g'h'_n|\leqslant n\varphi; hence

0=∫Xh‾hn′(1+∣g∣2)dμ=∫X∣h∣2φn(1+∣g∣2)dμ 0 =\int_X\overline{h}h'_n(1 +|g|^2)d\mu=\int_X|h|^2\varphi_n(1 +|g|^2)d\mu

This implies that hh is zero for μ\mu-almost every x∈Cnx\in C_n and therefore, since nn is arbitrary, that hh is zero for μ\mu-almost every x∈Cx\in C. It follows finally that hh is zero μ\mu-almost everywhere, since C is arbitrary and hh is moderate (INT, V, p. 9, § 1, no3^o3, cor.).

Let us now consider assertion b). Since ∣g∣2|g|^2 is locally μ\mu-integrable, the function fgf g belongs to LK2(X,μ)\mathscr{L}_K^2(X, \mu) if f∈K(X;K)f\in \mathscr{K}(X; K), hence K(X;K)\mathscr{K}(X; K) is contained in the domain of m~g\widetilde{m}_g.

Let h∈LK2(X,μ)h\in \mathscr{L}_K^2(X, \mu) whose class h~\widetilde{h} belongs to EmgE_{m_g} and is orthogonal to G. One then has

0=(h~∣h~′)m~g=∫Xhh‾′(1+∣g∣2)dμ 0 = (\widetilde{h}|\widetilde{h}')_{\widetilde{m}_g}=\int_Xh\overline{h}'(1 +|g|^2)d\mu

for every h′∈Fh'\in F of class h~′\widetilde{h}'. In view of the assumption on F, this means that the measure h(1+∣g∣2)⋅μh(1 +|g|^2)\cdot \mu is zero, hence that hh is zero μ\mu-almost everywhere since hh is moderate.

Let pp be a real number ⩾1\geqslant 1. Let hh be an element of LK∞(X,μ)\mathscr{L}_K^{\infty}(X, \mu). The multiplication operator m~h\widetilde{m}_h by hh is an endomorphism of LKp(X,μ)L^p_K(X, \mu)(IV, p. 186, No.o5^o5). Suppose that the set Y of the x∈Xx\in X such that h(x)=0h(x) = 0 is locally μ\mu-negligible. Then the endomorphism m~h\widetilde{m}_h is injective (Lemma 7 of IV, p. 186). Let us denote by h−1h^{-1} the function on X equal to 0 on Y and to x↦1/h(x)x\mapsto 1/h(x) on X- Y. The reciprocal partial operator m~h−1\widetilde{m}^{-1}_h is the multiplication operator by h−1h^{-1} from LKp(X,μ)L^p_K(X, \mu) into LKp(X,μ)L^p_K(X, \mu), that is to say, m~h−1=m~h−1\widetilde{m}^{-1}_h=\widetilde{m}_{h^{-1}}. In fact, the image of m~h\widetilde{m}_h is the space of classes of functions g∈LKp(X,μ)g\in \mathscr{L}_K^p(X, \mu) of the form g=hfg=hf for f∈LKp(X,μ)f\in \mathscr{L}_K^p(X, \mu). This condition is equivalent to g(x)/h(x)=f(x)g(x)/h(x) =f(x) for every x∈Xx\in X- Y and g(x)=0g(x) = 0 if x∈Yx\in Y. This implies that the domain of m~h−1\widetilde{m}^{-1}_h in LKp(X,μ)L^p_K(X, \mu) is the domain of m~h−1\widetilde{m}_{h^{-1}}, and that the equality m~h−1=m~h−1\widetilde{m}^{-1}_h=\widetilde{m}_{h^{-1}} is valid.

In what follows, we shall sometimes denote simply by mhm_h the partial multiplication operator by hh from LKp1(X,μ)L^{p^1}_K(X, \mu) into LKp2(X,μ)L^{p_2}_K(X, \mu).

Example 2 032Z

Let E be a Hilbert space over K and B=(ei)i∈IB = (e_i)_{i\in I} an orthonormal basis of E. Let (λi)i∈I(\lambda_i)_{i\in I} be a family of elements of K. Let D be the vector subspace of E consisting of the elements x∈Ex\in E such that the family (λi⟨ei∣x⟩)i∈I(\lambda_i\langle e_i|x\rangle )_{i\in I} is square-summable in K. The space D is dense in E since it contains the vector eie_i for every i∈Ii\in I. The partial operator uu with domain D given by

x↦∑i∈Iλi⟨ei∣x⟩ei x\mapsto \sum_{i\in I}\lambda_i\langle e_i|x\rangle e_i

is called a diagonal partial operator in the basis B, and (λi)i∈I(\lambda_i)_{i\in I} is called the family of eigenvalues of uu.

The operator uu is closed. In fact, let (xn,u(xn))n∈N(x_n, u(x_n))_{n\in\mathbf{N}} be a sequence of elements of the graph of uu which converges in E×EE\times E, and let (x,y)(x, y) be its limit. Then ⟨ei∣xn⟩→⟨ei∣x⟩\langle e_i|x_n\rangle \rightarrow \langle e_i|x\rangle for every i∈Ii\in I and

⟨ei∣u(xn)⟩=λi⟨ei∣xn⟩→⟨ei∣y⟩ \langle e_i|u(x_n)\rangle =\lambda_i\langle e_i|x_n\rangle \rightarrow \langle e_i|y\rangle

for every i∈Ii\in I. Consequently, λi⟨ei∣x⟩=⟨ei∣y⟩\lambda_i\langle e_i|x\rangle =\langle e_i|y\rangle for every i∈Ii\in I, which proves that x∈Dx\in D and u(x)=yu(x) =y, that is to say that uu is closed.

This example is in fact a particular case of the preceding one, applied to the topological space X = I endowed with the discrete topology and the counting measure μ\mu, since E identifies with the space ℓ2(I)=L2(I,μ)\ell^2(I) = L^2(I, \mu) by the mapping x↦(⟨ei∣x⟩)i∈Ix\mapsto (\langle e_i|x\rangle )_{i\in I} (EVT, V, p. 23, cor. 2) and uu then identifies with the multiplication operator mλm_{\lambda}, where λ\lambda is the function i↦λii\mapsto \lambda_i.

Example 3 0330

The set NR=N∪{∞,ω}\mathbf{N}_{\mathbf{R}}=\mathbf{N}\cup \{\infty , \omega \} is endowed with the total ordering described in VAR, R2, p. 10, such that n<∞<ωn <\infty < \omega for every n∈Nn\in \mathbf{N}. Let r∈NRr\in \mathbf{N}_{\mathbf{R}}. Let n∈Nn\in \mathbf{N} and let U be an open subset of Rn\mathbf{R}^n. Let k∈Nk\in \mathbf{N} be such that k⩽rk\leqslant r. Let (nα)∣α∣⩽k(n_{\alpha})_{|\alpha|\leqslant k} be a family of elements of Cr\mathscr{C}^r(U), where the multi-indices considered belong to Nn\mathbf{N}^n. The family (nα)(n_{\alpha}) defines a scalar differential operator D of order ⩽k\leqslant k on U (cf. VAR, R2, 14.1.6, 14.1.4). For every integer mm such that k⩽m⩽rk\leqslant m\leqslant r, the differential operator D defines a linear mapping of Cm(U)C^m(U) into Cm−k(U)C^{m-k}(U) which sends f∈Cm(U)f\in C^m(U) to

D(f)=∑∣α∣⩽knα∂α(f) D(f) =\sum_{|\alpha|\leqslant k}n_{\alpha}\partial^{\alpha}(f)

The same formula defines a continuous linear mapping of D(U)\mathscr{D}(U) into D′(U)\mathscr{D}'(U) (def. 2 of IV, p. 208).

Definition 5 0331

Let E be a vector subspace of D′(U)\mathscr{D}'(U) containing D(U)\mathscr{D}(U). A differential operator associated with D on E is any partial operator on E which is an extension of the partial operator with domain D(U)\mathscr{D}(U) defined by φ↦D(φ)\varphi \mapsto D(\varphi ).

Suppose for example that the coefficients nαn_{\alpha} are bounded functions on U. Let μ\mu be the Lebesgue measure on U. If pp is an element of [1,+∞[[1,+\infty [, one can then define on Lp(U)L^p(U) a differential operator associated with D whose domain is the Sobolev space Wk,p(U)W^{k,p}(U) (No. 14 of IV, p. 221), since in this case one has nα∂α(f)∈Lp(U)n_{\alpha}\partial^{\alpha}(f)\in L^p(U) for every f∈Wk,p(U)f\in W^{k,p}(U) and every ∣α∣⩽k|\alpha |\leqslant k.

4. Adjoint

In this No., K is one of the fields R\mathbf{R} or C\mathbf{C}, and E and F denote Hilbert spaces over K.

Let uu be an operator with dense domain from E into F. Let D denote the domain of uu. For y∈Fy\in F, let λy\lambda_y be the linear form on D such that λy(x)=⟨y∣u(x)⟩\lambda_y(x) =\langle y|u(x)\rangle for every x∈Dx\in D. We denote by D∗D^* the set of vectors y∈Fy\in F such that λy\lambda_y is continuous on D. It is a vector subspace of F. Let y∈D∗y\in D^*; since D is dense in E, the linear form λy\lambda_y extends in a unique way to a continuous linear form on E, which we again denote by λy\lambda_y. By EVT, V, p. 15, Theorem 3, there exists a unique element u∗(y)u^*(y) in E such that λy(x)=⟨u∗(y)∣x⟩\lambda_y(x) =\langle u^*(y)|x\rangle for every x∈Ex\in E. The mapping y↦u∗(y)y\mapsto u^*(y) is linear from D∗D^* into E.

Definition 6 0332

The partial operator from F into E with domain D∗D^* defined by y↦u∗(y)y\mapsto u^*(y) is called the adjoint of uu. It is denoted by u∗u^*.

Remark 0333

Thus y∈D∗y\in D^* if and only if there exists c∈R+c\in \mathbf{R}_+ such that ∣⟨y∣u(x)⟩∣⩽c∥x∥|\langle y|u(x)\rangle |\leqslant c\|x\| for every x∈Dx\in D. The element u∗(y)u^*(y) is then characterised by the relation

⟨y∣u(x)⟩=⟨u∗(y)∣x⟩(1) \langle y|u(x)\rangle =\langle u^*(y)|x\rangle \tag{1}

for every x∈Dx\in D. We then have ∣⟨y∣u(x)⟩∣⩽∥u∗(y)∥∥x∥|\langle y|u(x)\rangle |\leqslant \|u^*(y)\| \|x\| for every x∈Dx\in D.

In the case where uu is a continuous linear mapping from E into F, its adjoint in the sense of the preceding definition coincides with the adjoint defined in EVT, V, p. 38, Definition 1, since D∗D^* is equal to F in this case.

Let v∈P(E;F)v\in \mathscr{P}(E; F) be such that u⊂vu\subset v. Then v∗⊂u∗v^*\subset u^*.

Let v∈P(E;F)v\in \mathscr{P}(E; F) be such that u+vu+v has dense domain. Then the partial operator vv has dense domain and we have u∗+v∗⊂(u+v)∗u^*+v^*\subset (u+v)^*. In general, there is no equality (exercise 9 of IV, p. 347). If v∈L(E;F)v\in \mathscr{L}(E; F), then u+vu+v has dense domain and (u+v)∗=u∗+v∗(u+v)^*=u^*+v^*. This is so, for example, if F = E and if v=λ1Ev=\lambda 1_E where λ∈K\lambda \in K.

Let G be a Hilbert space over K and let v∈P(F;G)v\in \mathscr{P}(F; G) be an operator with dense domain. If v∘uv\circ u has dense domain, then u∗∘v∗⊂(v∘u)∗u^*\circ v^*\subset (v\circ u)^*. In general, there is no equality (loc. cit.). If uu (resp. vv) is an isomorphism, then v∘uv\circ u has dense domain and we have (v∘u)∗=u∗∘v∗(v\circ u)^*=u^*\circ v^*. This is so, for example, if E = F (resp. F = G) and u=λ1Eu=\lambda 1_E (resp. v=λ1Fv=\lambda 1_F) where λ∈K∗\lambda \in K^*.

Let ss denote the isometric isomorphism of Hilbert spaces from E⊕FE\oplus F into F⊕EF\oplus E defined by s(x,y)=(−y,x)s(x, y) = (-y, x) for every (x,y)∈E⊕F(x, y)\in E\oplus F.

Proposition 7 0334

Let uu be a partial operator with dense domain from E into F.

a) The graph of u∗u^* is equal to s(Γu∘)=s(Γu)∘s(\Gamma^{\circ}_u) =s(\Gamma_u)^{\circ};

b) The partial operator u∗u^* is closed;

c) The kernel of u∗u^* is the orthogonal of the image of uu.

Let us put W=s(Γu)∘W =s(\Gamma_u)^{\circ}. Since the linear mapping ss is unitary, we have W=s(Γu∘)W =s(\Gamma^{\circ}_u).

We have (y,x)∈W(y, x)\in W if and only if

⟨(y,x)∣(−u(x′),x′)⟩=0 \langle (y, x)|(-u(x'), x')\rangle = 0

for all x′∈x'\in dom(uu), that is to say, if

⟨y∣u(x′)⟩=⟨x∣x′⟩ \langle y|u(x')\rangle =\langle x|x'\rangle

for all x′∈x'\in dom(uu). When y∈y\in dom(u∗u^*) and x=u∗(y)x=u^*(y), this property holds (cf. formula (1), p. 236). Conversely, if this condition is satisfied, it follows that ∣⟨y∣u(x′)⟩∣⩽∥x∥∥x′∥|\langle y|u(x')\rangle |\leqslant \|x\| \|x'\| for all x′∈x'\in dom(uu), whence it follows that yy belong to dom(u∗u^*); one then has u∗(y)=xu^*(y) =x. Hence W=Γu∗W = \Gamma_{u^*}.

The operator u∗u^* is closed, because the space s(Γu)∘s(\Gamma_u)^{\circ} is closed in F⊕EF\oplus E.

Let us prove assertion c). If yy is orthogonal to the image of uu, the linear form λy:x↦⟨y∣u(x)⟩\lambda_y:x\mapsto \langle y|u(x)\rangle on D is zero, hence y∈y\in dom(u∗u^*) and u∗(y)=0u^*(y) = 0. Conversely, let y∈y\in dom(u∗u^*). Then u∗(y)=0u^*(y) = 0 if and only if yy is orthogonal to u(x)u(x) for all x∈Dx\in D (formula (1), p. 236).

Proposition 8 0335

Let uu be an operator with dense domain from E into F. Then u∗u^* has dense domain if and only if uu is closable. When this is so, the closure u‾\overline{u} of uu is equal to u∗∗u^{**}, and the adjoint of u‾\overline{u} is equal to u∗u^*.

By Prop. 7, the partial operator u∗u^* is closed. Suppose that the domain D∗D^* of u∗u^* is dense in F. Let u∗∗u^{**} be the adjoint of u∗u^*; it is a closed partial operator from E into F. Let us prove that u⊂u∗∗u\subset u^{**}, which will imply that uu is closable. Let x∈x\in dom(uu). By definition of u∗u^*, the linear forms on D∗D^* given by y↦⟨x∣u∗(y)⟩y\mapsto \langle x|u^*(y)\rangle and y↦⟨u(x)∣y⟩y\mapsto \langle u(x)|y\rangle are equal; hence x∈x\in dom(u∗∗u^{**}) and u∗∗(x)=u(x)u^{**}(x) =u(x), whence the assertion.

Conversely, suppose that uu is closable; one has Γu‾=Γ‾u\Gamma_{\overline{u}}=\overline{\Gamma}_u (Prop. 1 of IV, p. 228). Let y∈Fy\in F be a vector orthogonal to dom(u∗u^*). The element (y,0)(y,0) of F⊕EF\oplus E then belongs to the orthogonal complement of the graph of u∗u^*. But, by Prop. 7, a), one has

Γu∗∘=(s(Γu)∘)∘=s(Γu)=s(Γu) \Gamma^{\circ}_{u^*}= (s(\Gamma_u)^{\circ})^{\circ}=s(\Gamma_u) =s(\Gamma_u)

It follows therefore that (0,y)∈Γu‾(0, y)\in \Gamma_{\overline{u}}, whence y=u‾(0)=0y=\overline{u}(0) = 0. Since the orthogonal complement of dom(u∗u^*) is reduced to 0, the space dom(u∗u^*) is dense in F.

Finally, Prop. 7, applied to u∗u^*, implies that

Γu∗∗=s−1(Γu∗∘)=s−1(s(Γu∘∘))=Γ‾u \Gamma_{u^{**}}=s^{-1}(\Gamma^{\circ}_{u^*}) =s^{-1}(s(\Gamma^{\circ \circ}_u)) =\overline{\Gamma}_u

hence u∗∗=u‾u^{**}=\overline{u}, then u‾∗=(u∗)∗∗=u∗‾=u∗\overline{u}^*= (u^*)^{**}=\overline{u^*}=u^* since u∗u^* is closed.

Corollary 0336

If uu is a closed partial operator with dense domain from E into F, then u∗u^* has dense domain and one has u∗∗=uu^{**}=u.

Definition 7 0337

Let uu be a partial operator on E. One says that uu is symmetric if uu has dense domain and if u∗u^* is an extension of uu. One says that uu is self-adjoint if uu has dense domain and u∗=uu^*=u. One says that uu is essentially self-adjoint if it is closable and if the closure u‾\overline{u} of uu is self-adjoint.

One says that uu is a partial operator bounded below if uu is symmetric and if there exists a real number cc such that ⟨x∣u(x)⟩⩾c∥x∥2\langle x|u(x)\rangle \geqslant c\|x\|^2 for every xx belonging to the domain of uu. One then says that cc is a lower bound of uu. If c=0c= 0, one also says that uu is a positive partial operator.

We denote by A(E)\mathscr{A}(E) the set of self-adjoint partial operators on E.

Remark 1 0338

For an operator uu with dense domain on E to be symmetric, it is necessary and sufficient that one have

⟨x∣u(y)⟩=⟨u(x)∣y⟩(2) \langle x|u(y)\rangle =\langle u(x)|y\rangle \tag{2}

for every (x,y)∈(x, y)\in dom(uu)2^2. This formula in fact shows that the domain of uu is contained in that of u∗u^*, and then that u∗u^* and uu coincide on the domain of uu. In particular, it follows that ⟨x∣u(x)⟩∈R\langle x|u(x)\rangle \in \mathbf{R} for every x∈x\in dom(uu).

As will be seen in different examples, formula (2) can often be verified by a straightforward calculus. On the other hand, the exact determination of the domain of the adjoint, which alone makes it possible to know whether or not a symmetric operator is self-adjoint, may be very delicate.

Remark 2 0339

A self-adjoint partial operator uu is essentially self-adjoint (cf. prop. 8).

Remark 3 033A

Let uu be a symmetric partial operator on E. The operator uu is closable (prop. 7, b)). It satisfies dom(uu)⊂\subset dom(u∗u^*), and uu is self-adjoint if and only if dom(uu) == dom(u∗u^*). Moreover, the closure u‾\overline{u} of uu is symmetric since u‾⊂u∗=u‾∗\overline{u}\subset u^*=\overline{u}^* (prop. 8).

Remark 4 033B

Suppose K=CK =\mathbf{C}. Let u∈P(E;E)u\in \mathscr{P}(E; E) be a partial operator with dense domain. The condition ⟨x∣u(x)⟩∈R\langle x|u(x)\rangle \in \mathbf{R} for every x∈x\in dom(uu) implies that uu is symmetric (EVT, V, p. 2, remark); in particular, if ⟨x∣u(x)⟩∈R+\langle x|u(x)\rangle \in \mathbf{R}_+ for every x∈x\in dom(uu), then uu is positive.

Remark 5 033C

Let uu and vv be symmetric partial operators on E. If uu is self-adjoint and if u⊂vu\subset v, then v⊂v∗⊂u∗=uv\subset v^*\subset u^*=u, hence u=vu=v.

Remark 6 033D

An essentially self-adjoint partial operator uu is symmetric, since u⊂u‾u\subset \overline{u} implies u‾=u‾∗⊂u∗\overline{u}=\overline{u}^*\subset u^*, hence u⊂u∗u\subset u^*.

Remark 7 033E

Let uu and vv be symmetric partial operators on E. If u+vu+v has dense domain, for example if uu or vv belong to L\mathscr{L} (E), then u+vu+v is symmetric. In general, the partial operator u+vu+v is not self-adjoint, even if uu and vv are (exercise 9 of IV, p. 347).

Remark 8 033F

Let uu be a symmetric partial operator on E. A real number cc is a lower bound of uu if and only if the operator u−c⋅1Eu-c\cdot 1_E is positive.

Lemma 3 033G

Suppose that K=RK =\mathbf{R}. Let uu be a partial operator with dense domain from E into F.

a) The adjoint of u(C)u_{(\mathbf{C})} is (u∗)(C)(u^*)_{(\mathbf{C})};

b) Suppose that E = F; the partial operator uu is symmetric (resp. self-adjoint) if and only if the partial operator u(C)u_{(\mathbf{C})} is symmetric (resp. self-adjoint).

Let us prove a). Let y∈F(C)y\in F_{(\mathbf{C})} and write y=y1+iy2y=y_1+iy_2 with y1,y2∈Fy_1,y_2\in F. For all (x1,x2)∈E×E(x_1, x_2)\in E\times E, we have

⟨u(C)(x1+ix2)∣y⟩=⟨u(x1)∣y1⟩+i⟨u(x1)∣y2⟩ \langle u_{(\mathbf{C})}(x_1+ix_2)|y\rangle =\langle u(x_1)|y_1\rangle +i\langle u(x_1)|y_2\rangle
−i⟨u(x2)∣y1⟩+⟨u(x2)∣y2⟩ -i\langle u(x_2)|y_1\rangle +\langle u(x_2)|y_2\rangle

If y∈y\in dom(u∗u^*)(C)_{(\mathbf{C})}, it follows that y∈y\in dom((u(C)u_{(\mathbf{C})})∗^*) and that u(C)∗(y)=(u(C))∗(y)u^*_{(\mathbf{C})}(y) = (u_{(\mathbf{C})})^*(y), hence u(C)∗⊂(u(C))∗u^*_{(\mathbf{C})}\subset (u_{(\mathbf{C})})^*.

Conversely, suppose that yy belongs to dom((u(C)u_{(\mathbf{C})})∗^*). Taking x2=0x_2= 0 (resp. x1=0x_1= 0) in the above formula, we verify that y1∈y_1\in dom(u∗u^*) (resp. that y2∈y_2\in dom(u∗u^*)), whence y∈y\in dom(u∗u^*)(C)_{(\mathbf{C})}.

Assertion a) implies that u(C)u_{(\mathbf{C})} is symmetric (resp. self-adjoint) if uu is.

Conversely, suppose that u(C)u_{(\mathbf{C})} is symmetric. The relation ⟨u(x)∣y⟩=⟨x∣u(y)⟩\langle u(x)|y\rangle =\langle x|u(y)\rangle for all (x,y)∈(x, y)\in dom(u(C)u_{(\mathbf{C})})×\times dom(u(C)u_{(\mathbf{C})}) implies that uu is symmetric on taking xx and yy in the subspace dom(uu) of dom(u(C)u_{(\mathbf{C})}). If u(C)u_{(\mathbf{C})} is self-adjoint, what precedes proves that uu is symmetric; since dom(u∗u^*) == dom(u(C)∗u^*_{(\mathbf{C})})∩F\cap F, assertion a) implies that dom(u∗u^*) == dom(u(C)u_{(\mathbf{C})})∩F=\cap F = dom(uu), therefore uu is self-adjoint.

5. Elementary Criteria for Self-Adjoint Operators

Proposition 9 033H

Let v∈L(F;E)v\in \mathscr{L}(F; E) be an injective continuous linear mapping of F into E whose image is dense in E. The adjoint of vv is an injective continuous linear mapping of E into F and one has (v∗)−1=(v−1)∗(v^*)^{-1}= (v^{-1})^*. In particular, if E = F, the endomorphism vv is hermitian if and only if the partial operator v−1v^{-1} is self-adjoint.

The partial operator v−1v^{-1} is a closed operator with dense domain from E into F (Example 2 of IV, p. 228), and the adjoint v∗v^* of vv is a continuous linear mapping from E into F; it is injective, since the image of vv is dense in E (EVT, V, p. 41, prop. 4). Let ss (resp. s′s') be the isometric isomorphism (x,y)↦(−y,x)(x, y)\mapsto (-y, x) of E⊕FE\oplus F onto F⊕EF\oplus E (resp. the isometric isomorphism (y,x)↦(−x,y)(y, x)\mapsto (-x, y) of F⊕EF\oplus E onto E⊕FE\oplus F), and let ι\iota (resp. ι′\iota ') be the isometric isomorphism (y,x)↦(x,y)(y, x)\mapsto (x, y) of F⊕EF\oplus E onto E⊕FE\oplus F (resp. the isometric isomorphism (x,y)↦(y,x)(x, y)\mapsto (y, x) of E⊕FE\oplus F onto F⊕EF\oplus E). Then s∘ι=−ι′∘s′s\circ \iota =-\iota '\circ s', whence

Γ(v−1)∗=s(Γv−1)∘=s(ι(Γv))∘=−ι′(s′(Γv))∘=−ι′(Γv∗)=Γ(v∗)−1 \Gamma_{(v^{-1})^*}=s(\Gamma_{v^{-1}})^{\circ}=s(\iota (\Gamma_v))^{\circ}=-\iota '(s'(\Gamma_v))^{\circ}=-\iota '(\Gamma_{v^*}) = \Gamma_{(v^*)^{-1}}

by prop. 7 of IV, p. 236. The proposition follows.

Proposition 10 (Hellinger–Toeplitz) 033I

Let uu be a symmetric partial operator on the Hilbert space E. If the domain of uu is equal to E, then u∈L(E)u\in \mathscr{L}(E) and uu is hermitian.

In fact, the partial operator uu is closable (prop. 8 of IV, p. 237), and therefore closed since its domain is E (IV, p. 228, Remark). We then conclude by invoking EVT, I, p. 19, cor. 5.

Corollary 033J

Let uu be a symmetric partial operator on E. If the partial operator uu induces a bijective linear mapping of dom(uu) onto E, then uu is self-adjoint.

In fact, the inverse partial operator u−1u^{-1} of uu is symmetric with domain E (prop. 9), hence u−1u^{-1} is a self-adjoint element of L(E)\mathscr{L}(E) (prop. 10), and uu is therefore hermitian (prop. 9).

Proposition 11 033K

Let uu be a symmetric partial operator on E, and let λ∈C\lambda \in \mathbf{C}. If u+λ1Eu+\lambda 1_E and u+λ1Eu+\lambda 1_E are surjective, then uu is self-adjoint.

It is enough to prove that dom(u∗u^*)⊂\subset dom(uu). Let x∈x\in dom(u∗u^*). By hypothesis there exists y∈y\in dom(uu) such that u(y)+λy=u∗(x)+λxu(y) +\lambda y=u^*(x) +\lambda x. Let us prove that y=xy=x. For every z∈z\in dom(uu), we have

⟨(u+λ1E)(z)∣x⟩=⟨z∣(u∗+λ‾1E)(x)⟩ \langle (u+\lambda 1_E)(z)|x\rangle =\langle z|(u^*+\overline{\lambda}1_E)(x)\rangle
=⟨z∣(u+λ‾1E)(y)⟩=⟨(u+λ1E)(z)∣y⟩ =\langle z|(u+\overline{\lambda}1_E)(y)\rangle =\langle (u+\lambda 1_E)(z)|y\rangle

since uu is symmetric. Since the operator u+λ1Eu+\lambda 1_E is surjective, we indeed have y=xy=x, hence x∈x\in dom(uu).

We shall see later (cf. prop. 17 of IV, p. 248) that if λ∈C−R\lambda \in \mathbf{C}-\mathbf{R}, then the converse is true.

Proposition 12 033L

Let uu be a closed operator with dense domain from E into F. The partial operator u∗∘uu^*\circ u on E is self-adjoint and positive. Its domain is a core for uu.

Let us denote by vv the partial operator 1E+u∗∘u1_E+u^*\circ u. Its domain is dom(u∗∘uu^*\circ u), which is contained in dom(uu). For all x∈x\in dom(uu) and y∈y\in dom(vv), one has u(y)∈u(y)\in dom(u∗u^*) and

⟨x∣v(y)⟩=⟨x∣y⟩+⟨x∣(u∗∘u)(y)⟩=⟨x∣y⟩+⟨u(x)∣u(y)⟩(3) \langle x|v(y)\rangle =\langle x|y\rangle +\langle x|(u^*\circ u)(y)\rangle =\langle x|y\rangle +\langle u(x)|u(y)\rangle \tag{3}
⟨y∣v(y)⟩=∥y∥2+∥u(y)∥2(4) \langle y|v(y)\rangle =\|y\|^2+\|u(y)\|^2 \tag{4}

Formula (4) implies that the partial operator vv is injective. Moreover, by prop. 7 of IV, p. 236, a), one has F⊕E=Γu∗⊕s(Γu)F\oplus E = \Gamma_{u^*}\oplus s(\Gamma_u). Let x∈Ex\in E. There exist y′∈y'\in dom(u∗u^*) and x′∈x'\in dom(uu) such that

(0,x)=(y′,u∗(y′))+(−u(x′),x′)=(y′−u(x′),x′+u∗(y′)) (0, x) = (y', u^*(y')) + (-u(x'), x') = (y'-u(x'), x'+u^*(y'))

Hence one has y′=u(x′)y'=u(x'), whence x′∈x'\in dom(u∗∘uu^*\circ u) == dom(vv) and

x=x′+u∗(y′)=x′+(u∗∘u)(x′)=v(x′) x=x'+u^*(y') =x'+ (u^*\circ u)(x') =v(x')

The partial operator vv on E is therefore surjective, and induces a bijective linear mapping of dom(vv) onto E.

Let x∈Ex\in E be orthogonal to dom(vv). Write x=v(x′)x=v(x') where x′∈x'\in dom(vv). By formula (4), one obtains

0=⟨x′∣x⟩=⟨x′∣v(x′)⟩=∥x′∥2+∥u(x′)∥2 0 =\langle x'|x\rangle =\langle x'|v(x')\rangle =\|x'\|^2+\|u(x')\|^2

whence x′=0x'= 0, and then x=0x= 0. The domain of vv is therefore dense in E.

The partial operator vv has dense domain; it is bijective and formula (3) shows that it is symmetric. One concludes that vv is self-adjoint by applying the corollary to proposition 10. Consequently, u∗∘u=v−1Eu^*\circ u=v-1_E is self-adjoint. Moreover, the formula

⟨x∣(u∗∘u)(x)⟩=∥u(x)∥2 \langle x|(u^*\circ u)(x)\rangle =\|u(x)\|^2

for all x∈x\in dom(u∗∘uu^*\circ u) implies that u∗∘uu^*\circ u is positive.

Finally, let y∈Euy\in E_u be orthogonal to dom(u∗∘uu^*\circ u). There exists an element xx in the domain of u∗∘uu^*\circ u such that y=v(x)=x+(u∗∘u)(x)y=v(x) =x+ (u^*\circ u)(x). One then has 0=(x∣y)u=⟨y∣y⟩0 = (x|y)_u=\langle y|y\rangle, whence y=0y= 0.

6. Differential operators

Let n∈Nn\in \mathbf{N} and U be an open set in Rn\mathbf{R}^n. We endow Rn\mathbf{R}^n and U with the Lebesgue measure denoted by μ\mu.

Let k∈Nk\in \mathbf{N} and h∈Nh\in \mathbf{N} be such that h⩾kh\geqslant k. Let D be a scalar differential operator on U of order ⩽k\leqslant k, with coefficients (nα)∣α∣⩽k(n_{\alpha})_{|\alpha|\leqslant k} of class ChC^h on U. Suppose that for every α\alpha such that ∣α∣⩽k|\alpha |\leqslant k and every β\beta such that 0⩽β⩽α0\leqslant \beta \leqslant \alpha, the function ∂βnα\partial^{\beta}n_{\alpha} is bounded on U.

Let tD^tD be the scalar differential operator on U transpose of D (VAR, R2, 14.3.2); it is of order ⩽k\leqslant k and of class Ch−kC^{h-k}; for φ∈D\varphi \in \mathscr{D}(U), one has

tD(φ)=∑∣α∣⩽k(−1)∣α∣∂α(n‾αφ) ^tD(\varphi ) =\sum_{|\alpha|\leqslant k}(-1)^{|\alpha|}\partial^{\alpha}(\overline{n}_{\alpha}\varphi )

(loc. cit.); in particular, the coefficients of tD^tD are bounded on U.

We denote by D−D_- the partial operator on L2(U)L^2(U) with domain D(U)\mathscr{D}(U) defined by

φ↦D(φ)=∑∣α∣⩽knα∂αφ(5) \varphi \mapsto D(\varphi ) =\sum_{|\alpha|\leqslant k}n_{\alpha}\partial^{\alpha}\varphi \tag{5}

Let HDH_D be the space of f∈L2(U)f\in L^2(U) such that the distribution

D(f)=∑∣α∣⩽knα∂αf D(f) =\sum_{|\alpha|\leqslant k}n_{\alpha}\partial^{\alpha}f

belongs to L2(U)L^2(U); we denote by D+D_+ the partial operator with domain HDH_D defined by f↦D(f)f\mapsto D(f).

Since one has ∂αf∈L2(U)\partial^{\alpha}f\in L^2(U) if f∈Hk(U)f\in H^k(U) and ∣α∣⩽k|\alpha |\leqslant k, the Sobolev space Hk(U)H^k(U) is contained in HDH_D; in general, these spaces are distinct.

One has D−⊂D+D_-\subset D_+, and these are differential operators associated with D on L2(U)L^2(U) (def. 5 of IV, p. 235).

Proposition 13 033M

Let uu be a partial operator on L2(U)L^2(U). If D−⊂u⊂D+D_-\subset u\subset D_+, then uu is closable and (tD)−⊂u∗⊂(tD)+(^tD)_-\subset u^*\subset (^tD)_+.

Let φ\varphi and ψ\psi belong to D(U)\mathscr{D}(U). Then one has

⟨φ∣D(ψ)⟩=∑∣α∣⩽∫kUnαφ∂αψdμ \langle \varphi |D(\psi )\rangle =\sum_{|\alpha|\leqslant}\int_{kU}n_{\alpha}\varphi \partial^{\alpha}\psi d\mu
=∑∣α∣⩽k(−1)∣α∣⟨∂α(n‾αφ)∣ψ⟩=⟨tD(φ)∣ψ⟩ =\sum_{|\alpha|\leqslant k}(-1)^{|\alpha|}\langle \partial^{\alpha}(\overline{n}_{\alpha}\varphi )|\psi \rangle =\langle^tD(\varphi )|\psi \rangle

(cf. VAR, R2, 14.3.8). Since D(U)\mathscr{D}(U) is dense in L2(U)L^2(U) (prop. 4 of IV, p. 202), this implies that φ∈\varphi \in dom(u∗u^*) and u∗(φ)=tD(φ)u^*(\varphi ) =^tD(\varphi ). Hence one has (tD)−⊂u∗(^tD)_-\subset u^*; in particular, u∗u^* has dense domain and uu is closable (prop. 8 of IV, p. 237).

Let f∈f\in dom(u∗u^*) and φ∈D(U)\varphi \in \mathscr{D}(U). Since D(U)⊂\mathscr{D}(U)\subset dom(uu), the distribution associated with u∗(f)u^*(f) satisfies

⟨u∗(f),φ⟩=⟨φ‾∣u∗(f)⟩=⟨u(φ‾)∣f⟩ \langle u^*(f), \varphi \rangle =\langle \overline{\varphi}|u^*(f)\rangle =\langle u(\overline{\varphi})|f\rangle

Since D−⊂uD_-\subset u, u(φ‾)u(\overline{\varphi}) is calculated by formula (5), whence

⟨u∗(f),φ⟩=∑α⟨nα∂αφ‾∣f⟩=∑α⟨∂αφ‾∣n‾αf⟩ \langle u^*(f), \varphi \rangle =\sum_{\alpha}\langle n_{\alpha}\partial^{\alpha}\overline{\varphi}|f\rangle =\sum_{\alpha}\langle \partial^{\alpha}\overline{\varphi}|\overline{n}_{\alpha}f\rangle
=∑α⟨n‾αf,∂αφ⟩=∑α(−1)∣α∣⟨∂α(n‾αf),φ⟩=⟨tD(f),φ⟩ =\sum_{\alpha}\langle \overline{n}_{\alpha}f, \partial^{\alpha}\varphi \rangle =\sum_{\alpha}(-1)^{|\alpha|}\langle \partial^{\alpha}(\overline{n}_{\alpha}f), \varphi \rangle =\langle^tD(f), \varphi \rangle

The distributions u∗(f)u^*(f) and tD(f)^tD(f) are therefore equal; the distribution ff therefore belongs to HtDH_{_tD} and u∗(f)=tD(f)u^*(f) =^tD(f), whence u∗⊂(tD)+u^*\subset (^tD)_+.

Remark 033N

The proposition means that the adjoint of a partial operator uu such that D−⊂u⊂D+D_-\subset u\subset D_+ can always be calculated in the sense of distributions: the elements ff of the domain of u∗u^* are elements of L2(U)L^2(U) such that the distribution tD(f)^tD(f) belongs to L2L^2(U), and one has u∗(f)=tD(f)u^*(f) =^tD(f).

One says that D is formally symmetric if tD=D^tD = D as a scalar differential operator. If this is the case, the partial operator D−D_- is symmetric.

Consider the particular case of the scalar differential operator of order 2 defined by

Δ=−∑i=1n∂i2 \Delta =-\sum_{i=1}^n\partial_i^2

A Laplacian on U is any partial operator uu, self-adjoint on L2L^2(U), such that Δ−⊂u(\Delta_-\subset u(cf. VAR, R2, 14.4.3, p. 83). We shall see later (IV, p. 261, example) that there always exists at least one Laplacian on L2(U)L^2(U); there may exist more than one (exercise 17 of IV, p. 358).

7. Spectrum and Resolvent

Lemma 4 033O

Let E be a complex Banach space and let uu be a closed injective partial operator on E such that u−1∈L(E)u^{-1}\in \mathscr{L}(E). Let v∈L(E)v\in \mathscr{L}(E) be such that ∥v∥<∥u−1∥−1\|v\|<\|u^{-1}\|^{-1}. Then the partial operator u+vu+v is injective, one has (u+v)−1∈L(E)(u+v)^{-1}\in \mathscr{L}(E), and

(u+v)−1=u−1∘∑k=0+∞(−vu−1)k(6) (u+v)^{-1}=u^{-1}\circ \sum_{k=0}^{+\infty}(-vu^{-1})^k \tag{6}

where the series is absolutely convergent in L(E)\mathscr{L}(E). Moreover, one has

∥(u+v)−1∥⩽∥u−1∥−1 \|(u+v)^{-1}\|\leqslant \|u^{-1}\|_{-1}
1−∥v∥∥u∥ 1- \|v\| \|u\|

Since ∥v∥∥u−1∥<1\|v\| \|u^{-1}\|<1, the series with general term (−vu−1)k(-vu^{-1})^k is absolutely convergent in L\mathscr{L} (E), and its sum is the inverse of the endomorphism 1E+vu−11_E+vu^{-1} (prop. 2 of I, p. 22). Consequently, the partial operator (1E+vu−1)∘u=u+v((1_E+vu^{-1})\circ u=u+v(IV, p. 226, rem. vi) is injective and the reciprocal partial operator (u+v)−1=u−1∘(1E+vu−1)−1((u+v)^{-1}=u^{-1}\circ (1_E+vu^{-1})^{-1}(IV, p. 226, rem. iii) belongs to L(E)\mathscr{L}(E). Since

∥(1E+vu−1)−1∥⩽∑+∞(∥v∥∥u−1∥)k=\|(1_E+vu^{-1})^{-1}\|\leqslant \sum^{+\infty}(\|v\| \|u^{-1}\|)^k= 1 −1_{-1},

1−∥v∥∥u∥ 1- \|v\| \|u\|
k=0k=0

the lemma is proved.

Definition 8 033P

Let uu be a closed operator with dense domain on a complex Banach space E. The resolvent set of uu is the set of complex numbers λ\lambda such that the partial operator λ1E−u\lambda 1_E-u is injective and its inverse (λ1E−u)−1(\lambda 1_E-u)^{-1} belongs to L(E)\mathscr{L}(E).

The spectrum of uu, denoted by Sp(uu), is the complement of the resolvent set in C\mathbf{C}.

If λ∈C−\lambda \in \mathbf{C}- Sp(uu), we denote by R(u,λ)∈L(E)R(u, \lambda )\in \mathscr{L}(E) the inverse of λ1E−u\lambda 1_E-u. The mapping of C−\mathbf{C}- Sp(uu) into L(E)\mathscr{L}(E) which associates R(u,λ)R(u, \lambda ) to λ\lambda is called the resolvent of uu.

Remark 033Q

Let E be a complex Banach space and let uu be a closed operator with dense domain on E.

1) If u∈Lu\in \mathscr{L} (E), its spectrum coincides with the spectrum of the element uu of the algebra L(E)\mathscr{L}(E)(I, p. 2, Definition 1).

2) Let D be the domain of uu. For every λ∈C−\lambda \in \mathbf{C}- Sp(uu), one has

1E=(λ1E−u)∘R(u,λ),1D=R(u,λ)∘(λ1E−u)(7) 1_E= (\lambda 1_E-u)\circ R(u, \lambda ),1_D= R(u, \lambda )\circ (\lambda 1_E-u) \tag{7}

Moreover, for λ1\lambda_1 and λ2\lambda_2 in the resolvent set of uu, one has

R(u,λ1)−R(u,λ2)=(λ2−λ1)R(u,λ2)∘R(u,λ1)(8) R(u, \lambda_1)-R(u, \lambda_2) = (\lambda_2-\lambda_1)R(u, \lambda_2)\circ R(u, \lambda_1) \tag{8}
R(u,λ1)∘R(u,λ2)=R(u,λ2)∘R(u,λ1)(9) R(u, \lambda_1)\circ R(u, \lambda_2) = R(u, \lambda_2)\circ R(u, \lambda_1) \tag{9}

In fact, one has

R(u,λ1)−R(u,λ2)=R(u,λ1)∘1E−1D∘R(u,λ2) R(u, \lambda_1)-R(u, \lambda_2) = R(u, \lambda_1)\circ 1_E-1_D\circ R(u, \lambda_2)

Since 1E=(λ21E−u)∘R(u,λ2)1_E= (\lambda_21_E-u)\circ R(u, \lambda_2) and 1D=R(u,λ1)∘(λ11E−u)1_D= R(u, \lambda_1)\circ (\lambda_11_E-u), one obtains

R(u,λ1)−R(u,λ2)=λ2R(u,λ1)∘R(u,λ2) R(u, \lambda_1)-R(u, \lambda_2) =\lambda_2R(u, \lambda_1)\circ R(u, \lambda_2)
−R(u,λ1)∘u∘R(u,λ2)−λ1R(u,λ1)∘R(u,λ2) -R(u, \lambda_1)\circ u\circ R(u, \lambda_2)-\lambda_1R(u, \lambda_1)\circ R(u, \lambda_2)
+R(u,λ1)∘u∘R(u,λ2) + R(u, \lambda_1)\circ u\circ R(u, \lambda_2)

whence the first formula. By interchanging the roles of λ1\lambda_1 and λ2\lambda_2, one deduces the second formula.

3) Let λ∈C\lambda \in \mathbf{C}. By the closed graph theorem (EVT, I, p. 19, Corollary 5), if the linear mapping of dom(uu) into E defined by x↦(λ1E−u)(x)x\mapsto (\lambda 1_E-u)(x) is bijective, then its inverse, whose graph is closed, is continuous from E into E. Therefore λ\lambda belongs to the resolvent set of uu if and only if the mapping x↦(λ1E−u)(x)x\mapsto (\lambda 1_E-u)(x) of dom(uu) into E is bijective.

4) If λ\lambda belongs to the spectrum of uu, one of the following properties holds:

(i) The kernel of λ1E−u\lambda 1_E-u is not reduced to 0; one then says that λ\lambda is an eigenvalue of uu, and that the dimension of Ker(λ1E−u\lambda 1_E-u) is its multiplicity;

(ii) The partial operator λ1E−u\lambda 1_E-u is injective and its image is not dense in E; one then says that λ\lambda belongs to the residual spectrum of uu;

(iii) The partial operator λ1E−u\lambda 1_E-u is injective, its image is dense in E, but λ1E−u\lambda 1_E-u is not surjective; one then says that λ\lambda belongs to the continuous spectrum of uu.

5) Let λ\lambda be a complex number belonging to the resolvent set of uu. The resolvent R(u,λ)R(u, \lambda ) is an injective linear mapping of E into E; its image is the domain of uu and u=λ1E−R(u,λ)−1(u=\lambda 1_E-R(u, \lambda )^{-1}(cf. IV, p. 226). Conversely, this property characterizes the resolvent set and the resolvent. Precisely, let λ∈C\lambda \in \mathbf{C}; if there exists a continuous injective linear mapping ww of E into E such that u=λ1E−w−1u=\lambda 1_E-w^{-1}, then λ\lambda belongs to the resolvent set of uu and w=R(u,λ)w= R(u, \lambda ).

In particular, if vv is a closed operator with dense domain on E, and if λ∈C\lambda \in \mathbf{C} is a complex number not belonging to Sp(uu)∪\cup Sp(vv), then the equality R(u,λ)=R(v,λ)R(u, \lambda ) = R(v, \lambda ) implies that u=vu=v.

6) The spectrum of a closable partial operator uu is defined as the spectrum of its closure.

There exist closed operators whose spectrum is empty, or whose spectrum is equal to C\mathbf{C} (exercise 12 of IV, p. 347).

Let E be a complex Banach space and uu a closed operator with dense domain on E. If F is a complex Banach space and if v:E→Fv: E\rightarrow F is an isomorphism, then one has Sp(v∘u∘v−1v\circ u\circ v^{-1}) == Sp(uu) and R(v∘u∘v−1,λ)=v∘R(u,λ)∘v−1R(v\circ u\circ v^{-1}, \lambda ) =v\circ R(u, \lambda )\circ v^{-1} for every λ∉\lambda \notin Sp(uu).

Proposition 14 033R

Let E be a complex Banach space. Let uu be a closed operator with dense domain on E and U its resolvent set.

a) For every λ∈U\lambda \in U, the open disc in C\mathbf{C} with center λ\lambda and radius ∥R(u,λ)∥−1\|R(u, \lambda )\|^{-1} is contained in U;

b) The set U is open in C\mathbf{C};

c) Suppose that Sp(uu) is not empty. Let λ∈U\lambda \in U and denote by δ\delta the distance in C\mathbf{C} from λ\lambda to the spectrum of uu. One has δ>0\delta >0 and ∥R(u,λ)∥⩾1/δ\|R(u, \lambda )\|\geqslant 1/\delta;

d) The mapping λ↦R(u,λ)\lambda \mapsto R(u, \lambda ) is a holomorphic mapping of U into L(E)\mathscr{L}(E). For every integer k∈Nk\in \mathbf{N} and every λ∈U\lambda \in U, one has

∂k∂λkR(u,λ)=(−1)kk\frac{\partial^k}{\partial \lambda^k}R(u, \lambda ) = (-1)^kk!R(u,λu, \lambda )k+1^{k+1}.

Let λ∈U\lambda \in U. For every μ∈C\mu\in \mathbf{C} such that ∥(μ−λ)1E∥<∥R(u,λ)∥−1\|(\mu-\lambda )1_E\|<\|R(u, \lambda )\|^{-1}, lemma 4 applied to the injective partial operator λ1E−u\lambda 1_E-u and to v=(μ−λ)1Ev= (\mu-\lambda )1_E implies that the partial operator μ1E−u=λ1E−u+v\mu1_E-u=\lambda 1_E-u+v is injective and has a continuous inverse. This implies a). According to loc. cit., one also has the formula

R(u,μ)=R(u,λ)∘∑k∈N(λ−μ)kR(u,λ)k R(u, \mu) = R(u, \lambda )\circ \sum_{k\in\mathbf{N}}(\lambda -\mu)^kR(u, \lambda )^k

which implies that the resolvent of uu is holomorphic in U.

Assertion b) results at once from a). If Sp(uu) is nonempty, the distance from λ\lambda to Sp(uu) is strictly positive (TG, IX, p. 13, Prop. 2), whence c).

The last part of assertion d) is proved by induction on kk, the case k=1k= 1 being a consequence of formula (8), p. 245.

Proposition 15 033S

Let uu be a closed operator with dense domain on a complex Banach space E and λ\lambda a complex number belonging to the resolvent set of uu.

a) The subset Sp(R(u,λu, \lambda ))−{0}-\{0\} of C\mathbf{C} is the image of the spectrum of uu under the mapping μ↦(λ−μ)−1\mu\mapsto (\lambda -\mu)^{-1} of C−{λ}\mathbf{C}-\{\lambda \} into C∗\mathbf{C}^*;

b) For every μ≠λ\mu\not =\lambda in C\mathbf{C}, one has

Ker(μ1E−u\mu1_E-u) == Ker((λ−μ\lambda -\mu)−11E−R(u,λ)^{-1}1_E-R(u, \lambda )).

Let us prove assertion a). For every μ≠λ\mu\not =\lambda, we compute

μ1E−u=(λ−μ)((λ−μ)−11E−R(u,λ))(λ1E−u) \mu1_E-u= (\lambda -\mu) ((\lambda -\mu)^{-1}1_E-R(u, \lambda )) (\lambda 1_E-u)

Since λ∉\lambda \notin Sp(uu) and μ≠λ\mu\not =\lambda, the linear mapping (λ−μ)(λ1E−u)(\lambda -\mu)(\lambda 1_E-u) is a bijection of dom(uu) onto E. Consequently, this formula implies that μ1E−u\mu1_E-u is a bijection of dom(uu) onto E if and only if (λ−μ)−11E−R(u,λ)(\lambda -\mu)^{-1}1_E-R(u, \lambda ) is a bijection of E onto E, which implies the assertion.

Let us prove b). If μ≠λ\mu\not =\lambda and x∈x\in Ker((λ−μ\lambda -\mu)−11E−R(u,λ)^{-1}1_E-R(u, \lambda )), then x∈x\in dom(uu) and the formula 1E=(λ1E−u)∘R(u,λ)1_E= (\lambda 1_E-u)\circ R(u, \lambda ) implies that x∈x\in Ker(μ1E−u\mu1_E-u). Conversely, if x∈x\in Ker(μ1E−u\mu1_E-u) and μ≠λ\mu\not =\lambda, the formula 1dom(u)=R(u,λ)∘(λ1E−u)1_{dom(u)}= R(u, \lambda )\circ (\lambda 1_E-u) implies R(u,λ)(x)=(λ−μ)−1xR(u, \lambda )(x) = (\lambda -\mu)^{-1}x.

Proposition 16 033T

Let uu be a closed operator with dense domain on a complex Hilbert space E. The spectrum of u∗u^* is the image of the spectrum of uu under complex conjugation and, for every element λ\lambda of the resolvent set of uu, one has R(u,λ)∗=R(u∗,λ)R(u, \lambda )^*= R(u^*, \lambda ). In particular, if uu is self-adjoint, the endomorphism R(u,λ)R(u, \lambda ) is normal for every λ∉\lambda \notin Sp(uu).

Let λ∈C−\lambda \in \mathbf{C}- Sp(uu) be an element of the resolvent set of uu. One has u=λ1E−R(u,λ)−1u=\lambda 1_E-R(u, \lambda )^{-1}, hence

u∗=λ‾1E−(R(u,λ)−1)∗=λ‾1E−(R(u,λ)∗)−1 u^*=\overline{\lambda}1_E-(R(u, \lambda )^{-1})^*=\overline{\lambda}1_E-(R(u, \lambda )^*)^{-1}

(IV, p. 236 and prop. 9 of IV, p. 239). Applying remark 5, we deduce that λ‾∈C−\overline{\lambda}\in \mathbf{C}- Sp(u∗u^*) and that R(u,λ)∗=R(u∗,λ)R(u, \lambda )^*= R(u^*, \lambda ). Consequently, the spectrum of u∗u^* is contained in the image of Sp(uu) under complex conjugation. We obtain equality by applying this property to u∗u^*, since u∗∗=uu^{**}=u (cor. to prop. 8 of IV, p. 237). The last assertion then results from formula (9), p. 245.

Corollary 033U

Let uu be a self-adjoint partial operator on a complex Hilbert space E. If E is not zero, then the spectrum of uu is not empty.

Suppose that Sp(uu) is empty. Then uu is injective and u−1=−R(u,0)u^{-1}=-R(u,0) is an injective endomorphism of E such that Sp(u−1u^{-1})⊂{0}\subset \{0\} (prop. 15, a)), hence Sp(u−1u^{-1}) ={0}(=\{0\}(I, p. 26, cor. 1). Since u−1u^{-1} is normal (prop. 16), this implies that u−1u^{-1} is zero (I, p. 110, example 1), which is a contradiction.

Lemma 5 033V

Let E be a complex Hilbert space and let uu be a closed partial operator with dense domain on E. Let λ∈C\lambda \in \mathbf{C}. Suppose that there exists a real number c>0c >0 such that

(10) ∥u(x)−λx∥⩾c∥x∥\|u(x)-\lambda x\|\geqslant c\|x\| for every x∈x\in dom(uu),

(11) ∥u∗(x)−λx∥⩾c∥x∥\|u^*(x)-\lambda x\|\geqslant c\|x\| for every x∈x\in dom(u∗u^*).

Then λ\lambda belongs to the resolvent set of uu and ∥R(u,λ)∥⩽c−1\|R(u, \lambda )\|\leqslant c^{-1}.

The assumption implies that u−λ1Eu-\lambda 1_E and u∗−λ‾1Eu^*-\overline{\lambda}1_E are injective. Let F be the image of u−λ1Eu-\lambda 1_E. The space F is dense in E, since its orthogonal is equal to Ker(u∗−λ‾1Eu^*-\overline{\lambda}1_E) (prop. 7, c) of IV, p. 236), which is zero.

Let us prove that the space F is closed. Let (xn)n∈N(x_n)_{n\in\mathbf{N}} be a sequence in dom(uu) such that the sequence (u(xn)−λxn)n∈N(u(x_n)-\lambda x_n)_{n\in\mathbf{N}} converges to y∈Fy\in F. Inequality (10) implies that the sequence (xn)n∈N(x_n)_{n\in\mathbf{N}} is a Cauchy sequence in E. Let x∈Ex\in E be its limit. The sequence (xn,u(xn))(x_n, u(x_n)) converges to (x,y+λx)(x, y+\lambda x) in E×EE\times E; since the graph of uu is closed, we therefore have x∈x\in dom(uu) and u(x)=y+λxu(x) =y+\lambda x, which proves that y∈Fy\in F.

We conclude that F = E. Thus, the partial operator u−λ1Eu-\lambda 1_E is bijective, whence λ∉\lambda \notin Sp(uu) (remark 3). Inequality (10) then implies that ∥R(u,λ)∥⩽c−1\|R(u, \lambda )\|\leqslant c^{-1}.

Proposition 17 033W

Let E be a complex Hilbert space and let uu be a self-adjoint partial operator on E.

a) The spectrum of uu is contained in R\mathbf{R};

b) If uu is positive, then the spectrum of uu is contained in R+\mathbf{R}_+;

c) Suppose that E is nonzero. Let λ∉\lambda \notin Sp(uu) and let δ>0\delta >0 be the distance from λ\lambda to the spectrum of uu. One has ∥R(u,λ)∥=δ−1\|R(u, \lambda )\|=\delta^{-1}.

Let (a,b)∈R×R(a, b)\in \mathbf{R}\times \mathbf{R} and λ=a+ib\lambda =a+ib. Let x∈x\in dom(uu). Since uu is self-adjoint, one has ⟨x∣u(x)⟩∈R\langle x|u(x)\rangle \in \mathbf{R}, whence

∥u(x)−λx∥2=∥u(x)∥2−2a⟨x∣u(x)⟩+(a2+b2)∥x∥2 \|u(x)-\lambda x\|^2=\|u(x)\|^2-2a\langle x|u(x)\rangle + (a^2+b^2)\|x\|^2
=∥u(x)−λx∥2 =\|u(x)-\lambda x\|^2

Suppose that b≠0b\not = 0. One then obtains

∥u(x)−λx∥2=∥u(x)−λx∥2⩾(∥u(x)∥−a∥x∥)2+b2∥x∥2 \|u(x)-\lambda x\|^2=\|u(x)-\lambda x\|^2\geqslant (\|u(x)\| -a\|x\|)^2+b^2\|x\|^2
⩾b2∥x∥2 \geqslant b^2\|x\|^2

By Lemma 5, one therefore has λ∉\lambda \notin Sp(uu), whence assertion a).

Suppose that uu is also positive. If b=0b= 0 and a<0a <0, one analogously obtains for x∈x\in dom(uu) the inequality

∥u(x)−λx∥2=∥u(x)−λx∥2⩾(∥u(x)∥−a∥x∥)2⩾a2∥x∥2 \|u(x)-\lambda x\|^2=\|u(x)-\lambda x\|^2\geqslant (\|u(x)\| -a\|x\|)^2\geqslant a^2\|x\|^2

therefore λ∉\lambda \notin Sp(uu) ((loc. cit.)), which proves b).

Finally, let us prove c). By Prop. 16, the resolvent R(u,λ)R(u, \lambda ) is a normal endomorphism of E. Its norm is therefore equal to its spectral radius (Cor. 1 of I, p. 108), whence

∥R(u,λ)∥=\|R(u, \lambda )\|= supμ∈Sp(R(u,λ))∣μ∣_{\mu\in Sp(R(u,\lambda))}|\mu|

(Th. 1 of I, p. 24). The spectrum of R(u,λ)R(u, \lambda ) cannot be reduced to {0}\{0\}, for in that case one would have ∥R(u,λ)∥=0\|R(u, \lambda )\|= 0, hence the image dom(uu) of R(u,λ)R(u, \lambda ) would be zero, and E likewise. Prop. 15 therefore implies that

∥R(u,λ)∥=\|R(u, \lambda )\|= supμ∈Sp(u)1∣λ−μ∣=1δ_{\mu\in Sp(u)}\frac{1}{|\lambda-\mu|}=\frac{1}{\delta}.

Corollary 033X

Let uu be a self-adjoint operator on E.

a) The residual spectrum of uu is empty;

b) For all λ≠μ\lambda \not =\mu in C\mathbf{C}, the eigenspaces of uu corresponding to λ\lambda and μ\mu are orthogonal.

Let us prove a). Let λ\lambda belong to the spectrum of uu; it is a real number (Prop. 17). One has Ker(λ1E−u\lambda 1_E-u) == Im(λ1E−u\lambda 1_E-u)∘^{\circ} (Prop. 7 of IV, p. 236), therefore λ\lambda is not an eigenvalue of uu if the partial operator λ1E−u\lambda 1_E-u has dense image. By definition this implies that the residual spectrum of uu is empty.

Let us prove b). By the proposition, we may suppose that λ\lambda and μ\mu are real. Let x∈x\in dom(uu) be such that u(x)=λxu(x) =\lambda x and y∈y\in dom(uu) be such that u(y)=μyu(y) =\mu y. We then have

λ⟨x∣y⟩=⟨u(x)∣y⟩=⟨x∣u(y)⟩=μ⟨x∣y⟩ \lambda \langle x|y\rangle =\langle u(x)|y\rangle =\langle x|u(y)\rangle =\mu\langle x|y\rangle

whence ⟨x∣y⟩=0\langle x|y\rangle = 0.

Remark 033Y

If uu is a closed symmetric non-self-adjoint operator, its spectrum is not contained in R(\mathbf{R}(cf. cor. 10 of IV, p. 257 below), and it is possible that the eigenspaces of uu relative to λ\lambda and λ‾\overline{\lambda} are not orthogonal (exercise 11 of IV, p. 347).

8. Pseudospectrum

Definition 9 033Z

Let E be a complex Banach space and let uu be a closed partial operator on E. Let ε\varepsilon be a strictly positive real number. The ε\varepsilon-pseudospectrum of uu is by definition the union of the spectrum of uu and of the set of complex numbers λ\lambda belonging to the resolvent set of uu such that ∥R(u,λ)∥>ε−1\|R(u, \lambda )\|> \varepsilon^{-1}. This set is denoted by PSpε(u)_{\varepsilon}(u).

Some authors define the ε\varepsilon-pseudospectrum of uu as the set Tε(u)T_{\varepsilon}(u) equal to the union of Sp(uu) and of the set of λ∈C−\lambda \in \mathbf{C}- Sp(uu) such that ∥R(u,λ)∥⩾ε−1\|R(u, \lambda )\|\geqslant \varepsilon^{-1}. The closure of PSpε(u)_{\varepsilon}(u) is contained in Tε(u)T_{\varepsilon}(u), but this inclusion may be strict, even if E is a Hilbert space (cf. exercises 18 of IV, p. 348 and 19 of IV, p. 349).

Proposition 18 0340

Let E be a complex Banach space and uu a closed partial operator on E. Let ε∈R+∗\varepsilon \in \mathbf{R}^*_+. The set PSpε(u)_{\varepsilon}(u) is an open subset of C\mathbf{C}. It is nonempty if E is nonzero.

If E is zero, then PSpε(u)_{\varepsilon}(u) is empty. Suppose that E is nonzero. By prop. 14 of IV, p. 246, the set PSpε(u)_{\varepsilon}(u) is an open subset of C\mathbf{C}.

The set PSpε(u)_{\varepsilon}(u) is nonempty if the spectrum of uu is nonempty. If Sp(uu) is empty, then Liouville's theorem (VAR, R1, p. 29, 3.3.6) implies that the holomorphic function on C\mathbf{C} defined by λ↦R(u,λ)\lambda \mapsto R(u, \lambda ) is not bounded, hence there exists λ\lambda in C\mathbf{C} such that ∥R(u,λ)∥>ε−1\|R(u, \lambda )\|> \varepsilon^{-1}.

Proposition 19 0341

Let E be a complex Banach space and uu a closed partial operator on E. One has PSpε(u)⊂_{\varepsilon}(u)\subset PSpδ(u)_{\delta}(u) if 0<ε<δ0< \varepsilon < \delta and

⋂ε∈R+∗\bigcap_{\varepsilon\in\mathbf{R}^*_+} PSpε(u)=_{\varepsilon}(u) = Sp(uu).

The first assertion results from the definition. For the second, the spectrum of uu is contained in PSpε(u)_{\varepsilon}(u) for every ε>0\varepsilon >0 by definition, and if λ∉\lambda \notin Sp(uu), then λ∉\lambda \notin PSpε(u)_{\varepsilon}(u) when ε<∥R(u,λ)∥−1\varepsilon <\|R(u, \lambda )\|^{-1}.

Proposition 20 0342

Let E be a complex Banach space and uu a closed partial operator on E. Let ε∈R+∗\varepsilon \in \mathbf{R}^*_+. For every λ∈C\lambda \in \mathbf{C}, the following conditions are equivalent:

(i) One has λ∈\lambda \in PSpε(u)_{\varepsilon}(u);

(ii) Either λ∈\lambda \in Sp(uu), or there exists x∈x\in dom(uu) such that ∥x∥=1\|x\|= 1 and ∥(λ1E−u)(x)∥<ε\|(\lambda 1_E-u)(x)\|< \varepsilon;

(iii) There exists v∈L(E)v\in \mathscr{L}(E) such that ∥v∥<ε\|v\|< \varepsilon and λ∈\lambda \in Sp(u+vu+v).

One may suppose that E is nonzero. Condition (ii) is a reformulation of the definition, and hence of condition (i).

Suppose that condition (i) is satisfied and let us prove (iii). If λ\lambda belongs to the spectrum of uu, one can take v=0v= 0 in (iii).

Suppose therefore that λ∉\lambda \notin Sp(uu). By definition of PSpε(u)_{\varepsilon}(u), there exists y∈Ey\in E such that ∥y∥=1\|y\|= 1 and ∥R(u,λ)y∥>ε−1\|R(u, \lambda )y\|> \varepsilon^{-1}. Put x=R(u,λ)yx= R(u, \lambda )y. One has x≠0x\not = 0. By the Hahn–Banach theorem (EVT, II, p. 67, cor. 2), the linear form ℓ\ell on Cx\mathbf{C}x such that ℓ(x)=1\ell (x) = 1 admits a continuous extension ℓ1∈E′\ell_1\in E' such that ∥ℓ1∥=∥ℓ∥\|\ell_1\|=\|\ell \|; hence ∥ℓ1∥=∥x∥−1<ε\|\ell_1\|=\|x\|^{-1}< \varepsilon. For every e∈Ee\in E, put v(e)=ℓ1(e)yv(e) =\ell_1(e)y. One has v∈L(E)v\in \mathscr{L}(E) and v(x)=yv(x) =y. It follows that (u+v)x=u(x)+y=λx(u+v)x=u(x) +y=\lambda x, therefore λ∈\lambda \in Sp(u+vu+v). Since moreover ∥v∥=∥ℓ1∥<ε\|v\|=\|\ell_1\|< \varepsilon, condition (iii) is satisfied.

Conversely, let v∈L(E)v\in \mathscr{L}(E) such that ∥v∥<ε\|v\|< \varepsilon and λ∈\lambda \in Sp(u+vu+v). The partial operator λ1E−(u+v)\lambda 1_E-(u+v) is therefore not injective with a continuous inverse; by Lemma 4 of IV, p. 243, applied to the injective partial operator λ1E−u\lambda 1_E-u and to −v-v, one therefore has ∥v∥⩾∥R(u,λ)∥−1\|v\|\geqslant \|R(u, \lambda )\|^{-1}. It follows that condition (iii) implies (i).

Corollary 0343

Let E be a complex Banach space and uu a closed partial operator on E. Let ε>0\varepsilon >0.

a) For every v∈L(E)v\in \mathscr{L}(E), one has PSpε(u)⊂_{\varepsilon}(u)\subset PSpε+∥v∥(u+v)_{\varepsilon+\|v\|}(u+v);

b) Let δ>0\delta >0 and let DδD_{\delta} be the open disk with center 0 and radius δ\delta in C\mathbf{C}. One has PSpε(u)+Dδ⊂_{\varepsilon}(u) + D_{\delta}\subset PSpε+δ(u)_{\varepsilon+\delta}(u).

Let λ∈\lambda \in PSpε(u)_{\varepsilon}(u). There exists an endomorphism w∈L(E)w\in \mathscr{L}(E) such that ∥w∥<ε\|w\|< \varepsilon and λ∈\lambda \in Sp(u+wu+w) (Prop. 20). Since u+w=(u+v)+(w−v)u+w= (u+v)+(w-v) and ∥w−v∥<ε+∥v∥\|w-v\|< \varepsilon +\|v\|, one has λ∈\lambda \in PSpε+∥v∥(u+v)(_{\varepsilon+\|v\|}(u+v) (loc. cit.).

Let μ∈Dδ\mu\in D_{\delta}; one has λ+μ∈\lambda +\mu\in Sp(u+(w+μ1E)u+ (w+\mu1_E)) and ∥w+μ1E∥<ε+δ\|w+\mu1_E\|< \varepsilon +\delta, hence λ+μ∈\lambda +\mu\in PSpε+δ(u)(_{\varepsilon+\delta}(u) (loc. cit.).

Proposition 21 0344

Let E be a complex Banach space and uu a closed partial operator on E. Let ε∈R+∗\varepsilon \in \mathbf{R}^*_+. Every bounded connected component of PSpε(u)_{\varepsilon}(u) meets the spectrum of uu.

Let U be a connected component of PSpε(u)_{\varepsilon}(u) which does not meet Sp(uu). The set U is open and closed in PSpε(u)_{\varepsilon}(u), and its closure U in C\mathbf{C} therefore satisfies U∩U\cap PSpε(u)=U_{\varepsilon}(u) = U.

Since Sp(uu) is contained in PSpε(u)_{\varepsilon}(u) and U does not meet Sp(uu), this equality proves that the set U is disjoint from Sp(uu), hence contained in the resolvent set of uu. Moreover, it implies that the set U‾−\overline{U}- U does not meet PSpε(u)_{\varepsilon}(u).

One therefore has ∥R(u,λ)∥⩽ε−1\|R(u, \lambda )\|\leqslant \varepsilon^{-1} for every λ\lambda in U‾−\overline{U}- U, whereas ∥R(u,λ)∥>ε−1\|R(u, \lambda )\|> \varepsilon^{-1} for λ∈U\lambda \in U. If the set U is bounded, its closure U‾\overline{U} is compact and there exists λ0∈U‾\lambda_0\in \overline{U} such that ∥R(u,λ)∥⩽∥R(u,λ0)∥\|R(u, \lambda )\|\leqslant \|R(u, \lambda_0)\| for λ∈U\lambda \in U. The foregoing implies that λ0∈U\lambda_0\in U, which contradicts the maximum principle (VAR, R1, p. 29, 3.3.7) since the resolvent of uu is holomorphic in the resolvent set of uu (Prop. 14 of IV, p. 246).

9. Multiplication operators

Let X be a locally compact space and μ\mu a positive measure on X. We consider the multiplication operators on L2(X,μ)L^2(X, \mu); these are closed operators with dense domain (Prop. 5 of IV, p. 232). For every μ\mu-measurable function gg on X, we shall denote by mgm_g the partial operator of multiplication by gg on L2(X,μ)L^2(X, \mu).

Proposition 22 0345

Let gg be a μ\mu-measurable function on X.

a) The spectrum of mgm_g is the essential μ\mu-image S of gg;

b) Let λ∈C−\lambda \in \mathbf{C}- Sp(mgm_g). The resolvent R(mg,λ)R(m_g, \lambda ) is the multiplication operator mhm_h, where hh is the function on X defined by h(x)=0h(x) = 0 if g(x)=λg(x) =\lambda and h(x)=(λ−g(x))−1h(x) = (\lambda -g(x))^{-1} otherwise.

Let us prove that C−\mathbf{C}- S is contained in the resolvent set of mgm_g. Let λ∈C−\lambda \in \mathbf{C}- S. There exists an open neighbourhood U of λ\lambda such that the subset Y=g−1(U)Y =\overset{-1}{g}(U) of X is locally μ\mu-negligible. The function kk defined on X by k(x)=(λ−g(x))−1k(x) = (\lambda -g(x))^{-1} if x∉Yx \notin Y and k(x)=0k(x) = 0 if x∈Yx\in Y then belong to L∞(X,μ)\mathscr{L}^{\infty}(X, \mu) (Lemma 5 of IV, p. 184); the multiplication operator by kk is therefore an endomorphism of L2(X,μ)L^2(X, \mu).

Since ∣gk∣⩽1+∣λk∣|gk|\leqslant 1 +|\lambda k|, we have

∣gkf∣⩽∣f∣+∣λkf∣ |gkf|\leqslant |f|+|\lambda kf|

for f∈L2(X,μ)f\in \mathscr{L}^2(X, \mu), which implies that the image of mkm_k is contained in the domain of mgm_g. Conversely, let f∈L2(X,μ)f\in \mathscr{L}^2(X, \mu) whose class f~\widetilde{f} belongs to the domain of mgm_g. Outside the locally μ\mu-negligible set Y, we have f(x)=k(x)(λ−g(x))f(x)f(x) =k(x)(\lambda -g(x))f(x), hence f~\widetilde{f} is in the image of mkm_k. The same formula proves that λ\lambda belongs to the resolvent set of mgm_g and that R(mg,λ)=mkR(m_g, \lambda ) =m_k. Since the set Y is locally μ\mu-negligible, the multiplication operator mkm_k coincides with the operator mhm_h described in assertion b).

Let us prove conversely that C−\mathbf{C}- Sp(mgm_g) is contained in C−\mathbf{C}- S. Let λ∈C−\lambda \in \mathbf{C}- Sp(mgm_g). Let M>∥R(mg,λ)∥M>\|R(m_g, \lambda )\| be a real number. Let us denote by Y the set of x∈Xx\in X such that ∣λ−g(x)∣<M−1|\lambda -g(x)|<M^{-1}. Let us prove that Y is locally μ\mu-negligible, which will imply that λ\lambda does not belong to S, and will complete the proof.

Let K be a compact subset of X. Let φ\varphi be the characteristic function of Y∩KY\cap K; it is an element of L2(X,μ)\mathscr{L}^2(X, \mu), and we denote by φ~\widetilde{\varphi} its class in L2(X,μ)L^2(X, \mu). Let ψ\psi be a function in L2(X,μ)\mathscr{L}^2(X, \mu) whose class in L2(X,μ)L^2(X, \mu) is R(mg,λ)(φ~)R(m_g, \lambda )(\widetilde{\varphi}). We have R(mg,λ)(φ~)∈R(m_g, \lambda )(\widetilde{\varphi})\in dom(mgm_g) and (λ−mg)(R(mg,λ)(φ~))=φ~(\lambda -m_g)(R(m_g, \lambda )(\widetilde{\varphi})) =\widetilde{\varphi}, hence (λ−g(x))ψ(x)=1(\lambda -g(x))\psi (x) = 1 for μ\mu-almost all x∈Y∩Kx\in Y\cap K. This implies

∥R(mg,λ)∥2∥φ~∥2⩾∥R(mg,λ)(φ~)∥2⩾M2μ(Y∩K)=M2∥φ~∥2 \|R(m_g, \lambda )\|^2\|\widetilde{\varphi}\|^2\geqslant \|R(m_g, \lambda )(\widetilde{\varphi})\|^2\geqslant M^2\mu(Y\cap K) = M^2\|\widetilde{\varphi}\|^2

In view of the choice of M, this means that φ\varphi is zero μ\mu-almost everywhere. Thus, the set Y∩KY\cap K is μ\mu-negligible. Therefore the set Y is locally μ\mu-negligible (INT, IV, p. 172, § 5, no2^o2, Prop. 5).

Proposition 23 0346

Let gg be a μ\mu-measurable function on X. The adjoint of the multiplication operator mgm_g is mg‾m_{\overline{g}}.

For every integer n⩾n\geqslant 1, let φn\varphi_n be the characteristic function of the set of elements x∈x\in X such that ∣g(x)∣⩽n|g(x)|\leqslant n, and let φ~n\widetilde{\varphi}_n be its class in L2(X,μ)L^2(X, \mu). Let f∈L2(X,μ)f\in \mathscr{L}^2(X, \mu) be such that its class f~\widetilde{f} belongs to dom(mg∗m^*_g), and let ψ\psi be a function whose class is mg∗(f~)m^*_g(\widetilde{f}).

For every h∈L2(X,μ)h\in \mathscr{L}^2(X, \mu) whose class h~\widetilde{h} belongs to dom(mgm_g), we have also h~φ~n∈\widetilde{h}\widetilde{\varphi}_n\in dom(mgm_g), and therefore ⟨f~∣mg(h~φ~n)⟩=⟨mg∗(f~)∣h~φ~n⟩\langle \widetilde{f}|m_g(\widetilde{h}\widetilde{\varphi}_n)\rangle =\langle m^*_g(\widetilde{f})|\widetilde{h}\widetilde{\varphi}_n\rangle. This yields the equality

∫X(fg−ψ)‾φnhdμ=0 \int_X\overline{(f g-\psi)}\varphi_nh d\mu= 0

Since the domain of mgm_g is dense in L2(X,μ)L^2(X, \mu), it follows that (fg−ψ)φn(f g-\psi )\varphi_n is zero μ\mu-almost everywhere. Since nn is arbitrary, this means that mg∗(f~)m^*_g(\widetilde{f}) is the class in L2(X,μ)L^2(X, \mu) of fgf g. In particular, since mg∗(f~)∈L2(X,μ)m^*_g(\widetilde{f})\in L^2(X, \mu), one concludes that ff belongs to the domain of mg‾m_{\overline{g}} and that mg∗(f~)=mg‾(f~)m^*_g(\widetilde{f}) =m_{\overline{g}}(\widetilde{f}).

The adjoint of mgm_g is therefore an extension of mg‾m_{\overline{g}}. Moreover, one has

⟨f∣mg(h)⟩=∫Xf‾⋅(gh)dμ=∫Xfg‾hdμ \langle f|m_g(h)\rangle =\int_X\overline{f}\cdot (gh)d\mu=\int_Xf\overline{g}h d\mu

for every f∈L2(X,μ)f\in L^2(X, \mu) and h∈h\in dom(mgm_g), which proves that the linear form h↦⟨f∣mg(h)⟩h\mapsto \langle f|m_g(h)\rangle is continuous whenever mg‾(f)gm_{\overline{g}}(f)g belongs to L2(X,μ)L^2(X, \mu). Consequently the domain of mg‾m_{\overline{g}} is contained in that of mg∗m^*_g, which concludes the proof.

Corollary 0347

Let gg be a μ\mu-measurable function on X. The multiplication operator mgm_g on L2(X,μ)L^2(X, \mu) is self-adjoint (resp. positive ) if and only if the function gg is locally μ\mu-almost everywhere real-valued (resp. locally μ\mu-almost everywhere positive).

The first assertion results from the proposition. If gg is locally μ\mu-almost everywhere positive, one has ⟨f∣mg(f)⟩=∫Xg∣f∣2dμ⩾0\langle f|m_g(f)\rangle =\int_Xg|f|^2d\mu\geqslant 0 for every f∈L2(X,μ)f\in L^2(X, \mu), hence the partial operator mgm_g is positive.

Conversely, if mgm_g is positive, then its spectrum is contained in R+\mathbf{R}_+ (prop. 17 of IV, p. 248); since this is the μ\mu-essential image of gg (prop. 22, a)), this means that gg is locally μ\mu-almost everywhere positive.

Lemma 6 0348

Let g1g_1 and g2g_2 be μ\mu-measurable functions on X.

a) The partial operator mg1+mg2m_{g_1}+m_{g_2} is closable and its closure is the multiplication operator mg1+g2m_{g_1+g_2};

b) One has mg1∘mg2⊂mg1g2m_{g_1}\circ m_{g_2}\subset m_{g_1g_2};

c) Suppose that g1g_1 is bounded. Then one has mg2∘mg1=mg1g2m_{g_2}\circ m_{g_1}=m_{g_1g_2}. Moreover, the domain of mg2m_{g_2} is contained in the domain of mg1g2m_{g_1g_2}, and mg1∘mg2m_{g_1}\circ m_{g_2} is the restriction of mg1g2m_{g_1g_2} to dom(mg2m_{g_2}).

It is elementary that mg1+g2m_{g_1+g_2} is an extension of mg1+mg2m_{g_1}+m_{g_2}; the latter operator is therefore closable, and mg1+mg2‾⊂mg1+g2\overline{m_{g_1} + m_{g_2}}\subset m_{g_1+g_2}.

Let f∈L2(X,μ)f\in \mathscr{L}^2(X, \mu) be such that the function h=(g1+g2)fh= (g_1+g_2)f belongs to L2(X,μ)\mathscr{L}^2(X, \mu). For every integer n⩾1n\geqslant 1, let XnX_n denote the set of x∈Xx\in X such that ∣g1(x)∣+∣g2(x)∣⩽n|g_1(x)|+|g_2(x)|\leqslant n, and let φn\varphi_n be the characteristic function of XnX_n. We have φnf∈\varphi_nf\in dom(mg1+mg2m_{g_1}+m_{g_2}). Since (φnf)(x)(\varphi_nf)(x) tends to f(x)f(x) for every x∈Xx\in X, and since for every n∈Nn\in \mathbf{N} one has ∣φnf∣⩽∣f∣|\varphi_nf|\leqslant |f| and ∣(g1+g2)φnf∣⩽|(g_1+g_2)\varphi_nf|\leqslant ∣(g1+g2)f∣=∣h∣|(g_1+g_2)f|=|h|, with h∈L2(X,μ)h\in \mathscr{L}^2(X, \mu) by hypothesis, Lebesgue's theorem (INT, IV, p. 137, § 3, No.o7^o7, Theorem 6) implies that the sequence of pairs of classes in L2(X,μ)×L2(X,μ)L^2(X, \mu)\times L^2(X, \mu) of (φnf,(g1+g2)φnf)(\varphi_nf,(g_1+g_2)\varphi_nf), which belong to the graph of mg1+mg2m_{g_1}+m_{g_2}, tends to the pair of classes of (f,h)(f, h) in L2(X,μ)L^2(X, \mu). The closure of mg1+mg2m_{g_1}+m_{g_2} is therefore indeed equal to mg1+g2m_{g_1+g_2}.

It is elementary that mg1∘mg2⊂mg1g2m_{g_1}\circ m_{g_2}\subset m_{g_1g_2}. Suppose that g1g_1 is bounded, so that mg1m_{g_1} is a continuous linear mapping on L2(X,μ)L^2(X, \mu). Then the domain of mg2∘mg1m_{g_2}\circ m_{g_1} is the set of classes of functions f∈L2(X,μ)f\in \mathscr{L}^2(X, \mu) such that g2(g1f)∈L2(X,μ)g_2(g_1f)\in \mathscr{L}^2(X, \mu), that is to say the domain of mg1g2m_{g_1g_2}. Hence mg2∘mg1=mg1g2m_{g_2}\circ m_{g_1}=m_{g_1g_2}.

It is likewise elementary that dom(mg1∘mg2m_{g_1}\circ m_{g_2}) == dom(mg2m_{g_2}) is contained in dom(mg1g2m_{g_1g_2}), and that the restriction of mg1g2m_{g_1g_2} to this space is equal to mg1∘mg2m_{g_1}\circ m_{g_2}.

One must beware of believing that mg1∘mg2=mg1g2m_{g_1}\circ m_{g_2}=m_{g_1g_2} in general (exercise 10 of IV, p. 347). Nevertheless, one has the following partial result:

Proposition 24 0349

Let gg be a μ\mu-measurable function on X.

a) One has mg‾∘mg=m∣g∣2m_{\overline{g}}\circ m_g=m_{|g|^2};

b) For all integers k,ℓ∈Nk, \ell \in \mathbf{N}, one has mgkg‾ℓ=mgkmg‾ℓm_{g^k\overline{g}^{\ell}}=m^k_gm^{\ell}_{\overline{g}}.

One has mg‾∘mg⊂m∣g∣2m_{\overline{g}}\circ m_g\subset m_{|g|^2} by Lemma 6. Conversely, one deduces from the inequality ∣g∣⩽1+∣g∣2|g|\leqslant 1 +|g|^2 that dom(m∣g∣2m_{|g|^2}) == dom(mg‾∘mgm_{\overline{g}}\circ m_g), whence the first assertion.

Let k,ℓ∈Nk, \ell \in \mathbf{N}. We have mgkmg‾ℓ⊂mgkg‾ℓ(m^k_gm^{\ell}_{\overline{g}}\subset m_{g^k\overline{g}^{\ell}}(loc. cit.). The domain of mgkmg‾ℓm^k_gm^{\ell}_{\overline{g}} is the set of classes in L2(X,μ)L^2(X, \mu) of functions h∈L2(X,μ)h\in \mathscr{L}^2(X, \mu) such that ∣g∣jh|g|^jh belong to L2(X,μ)\mathscr{L}^2(X, \mu) for every integer jj such that 0⩽j⩽k+ℓ0\leqslant j\leqslant k+\ell. The inequalities

∣gjh∣⩽∣h∣+∣gk+ℓh∣ |g^jh|\leqslant |h|+|g^{k+\ell}h|

valid for 0⩽j⩽k+ℓ0\leqslant j\leqslant k+\ell, show that dom(mgkmg‾ℓm^k_gm^{\ell}_{\overline{g}}) is equal to dom(mgkg‾ℓm_{g^k\overline{g}^{\ell}}), whence assertion b).

10. Self-adjoint extensions of a symmetric operator

In this No., we shall classify the self-adjoint extensions of symmetric operators on a complex Hilbert space, and in particular determine conditions ensuring the existence of a self-adjoint extension of such an operator.

Let E be a complex Hilbert space. For every partial operator uu on E, in this No. we shall write u+iu+i and u−iu-i instead of u+i1Eu+i1_E and u−i1Eu-i1_E.

Let uu be a closed operator with dense domain on E. We recall (cf. definition 4 of IV, p. 230 and proposition 4 of IV, p. 230) that EuE_u denotes the Hilbert space dom(uu) endowed with the Hermitian form

(x∣y)u=⟨x∣y⟩+⟨u(x)∣u(y)⟩ (x|y)_u=\langle x|y\rangle +\langle u(x)|u(y)\rangle

We denote by ∥x∥u\|x\|_u the norm of an element xx of the Hilbert space EuE_u. Every subspace of dom(uu) which is closed in E is closed in Eu(E_u(IV, p. 230, remark 1).

Definition 10 034A

Let uu be a closed symmetric operator on a complex Hilbert space E. Let E+=E_+= Ker(u∗−iu^*-i) and E−=E_-= Ker(u∗+iu^*+i). The pair (E+,E−)(E_+,E_-) of subspaces of dom(u∗u^*) is called the deficiency pair of uu. The subspaces E+E_+ and E−E_- are closed subspaces of E (prop. 3 of IV, p. 229). The pair (dim(E+_+), dim(E−_-)) of the Hilbert dimensions of these subspaces is called the deficiency index of uu.

Proposition 25 034B

Let uu be a closed symmetric operator on a complex Hilbert space E. We have

Ker(u∗−iu^*-i)∘=^{\circ}= Im(u+iu+i),

Ker(u∗+iu^*+i)∘=^{\circ}= Im(u−iu-i).

By prop. 7, c) of IV, p. 236, it is enough to prove that the image of u+iu+i (resp. of u−iu-i) is closed in E. Since uu is symmetric, we have ⟨(u+i)(x)∣(u+i)(y)⟩=(x∣y)u\langle (u+i)(x)|(u+i)(y)\rangle = (x|y)_u for all xx and yy in dom(uu). The mapping x↦u(x)+ixx\mapsto u(x) +ix of EuE_u into E is therefore isometric. Its image is closed in E (lemma 8 of I, p. 107). Since this is also the image of u+iu+i, the latter is closed in E. Analogously, the image of u−iu-i is closed in E.

Lemma 7 034C

Let uu be a closed symmetric operator on a complex Hilbert space E and vv a closed symmetric extension of uu. The domain of uu is a closed subspace of the Hilbert space EvE_v.

Since vv is an extension of uu, we have (x∣y)v=(x∣y)u(x|y)_v= (x|y)_u for xx and yy in dom(uu). The canonical injection of EuE_u into EvE_v is therefore isometric, and the conclusion follows (lemma 8 of I, p. 107).

Proposition 26 034D

Let uu be a closed symmetric operator on a complex Hilbert space E. Let (E+,E−)(E_+,E_-) be the deficiency pair of uu. The spaces E+,E−E_+,E_- and dom(uu) are closed mutually orthogonal subspaces of Eu∗E_{u^*} whose Hilbert sum is equal to Eu∗E_{u^*}.

Since uu is symmetric, we have u⊂u∗u\subset u^*, hence the space dom(uu) is closed in Eu∗E_{u^*} (lemma 7). The subspaces E+E_+ and E−E_- are closed in E and contained in dom(u∗u^*), hence closed in Eu∗E_{u^*}.

Let x∈E+x\in E_+. We have u∗(x)=ixu^*(x) =ix, whence ⟨x∣u(y)⟩=−i⟨x∣y⟩\langle x|u(y)\rangle =-i\langle x|y\rangle for every y∈y\in dom(uu). Consequently, for every y∈y\in dom(uu), we have

(x∣y)u∗=⟨x∣y⟩+⟨u∗(x)∣u∗(y)⟩=i(⟨x∣u(y)⟩−⟨x∣u∗(y)⟩)=0 (x|y)_{u^*}=\langle x|y\rangle +\langle u^*(x)|u^*(y)\rangle =i(\langle x|u(y)\rangle - \langle x|u^*(y)\rangle )= 0

since uu is symmetric. The spaces E+E_+ and dom(uu) are therefore orthogonal in Eu∗E_{u^*}. Analogously, E−E_- and dom(uu) are orthogonal in Eu∗E_{u^*}.

Let x∈E+x\in E_+ and y∈E−y\in E_-. Then

(x∣y)u∗=⟨x∣y⟩+⟨u∗(x)∣u∗(y)⟩=⟨x∣y⟩−⟨x∣y⟩=0 (x|y)_{u^*}=\langle x|y\rangle +\langle u^*(x)|u^*(y)\rangle =\langle x|y\rangle - \langle x|y\rangle = 0

therefore E+E_+ and E−E_- are orthogonal in Eu∗E_{u^*}.

Let x∈Eu∗x\in E_{u^*} be orthogonal to the closed subspace dom(uu)⊕E+⊕E−\oplus E_+\oplus E_-. For every y∈y\in dom(uu), we have u∗(y)=u(y)u^*(y) =u(y) since u⊂u∗u\subset u^*, whence

0=(x∣y)u∗=⟨x∣y⟩+⟨u∗(x)∣u∗(y)⟩=⟨x∣y⟩+⟨u∗(x)∣u(y)⟩ 0 = (x|y)_{u^*}=\langle x|y\rangle +\langle u^*(x)|u^*(y)\rangle =\langle x|y\rangle +\langle u^*(x)|u(y)\rangle

This implies that z=u∗(x)z=u^*(x) belongs to the domain of u∗u^* and satisfies u∗(z)=−xu^*(z) =-x. Let x−=z−ixx_-=z-ix. This is an element of dom(u∗u^*) satisfying u∗(x−)=−x−iz=−ix−u^*(x_-) =-x-iz=-ix_-. Hence x−x_- belongs to E−E_-. But, for every w∈E−w\in E_-, we have

−i⟨x−∣w⟩=−i⟨z∣w⟩+⟨x∣w⟩ -i\langle x_-|w\rangle =-i\langle z|w\rangle +\langle x|w\rangle
=⟨u∗(x)∣u∗(w)⟩+⟨x∣w⟩=(x∣w)u∗=0 =\langle u^*(x)|u^*(w)\rangle +\langle x|w\rangle = (x|w)_{u^*}= 0

Taking w=x−w=x_-, we deduce that x−=0x_-= 0, that is to say z=ixz=ix; since z=u∗(x)z=u^*(x), we therefore have x∈E+x\in E_+, whence xx = 0 since xx is orthogonal to E+E_+ in Eu∗E_{u^*}. This completes the proof that the direct sum dom(uu)⊕E+⊕E−\oplus E_+\oplus E_- is equal to Eu∗E_{u^*}.

Corollary 034E

Let uu be a closed symmetric operator on E. Then uu is self-adjoint if and only if the deficiency index of uu is equal to (0,0)(0,0).

In fact, the symmetric operator uu is self-adjoint if and only if dom(u∗u^*) == dom(uu); now the proposition proves that dom(u∗u^*) is the Hilbert sum of dom(uu) and of the deficiency subspaces of uu.

Let uu be a closed symmetric partial operator. The spectrum of uu is contained in R\mathbf{R} if and only if uu is self-adjoint. In fact, it is known that Sp(uu)⊂R\subset \mathbf{R} if uu is self-adjoint (Prop. 17 of IV, p. 248); if uu is not self-adjoint, one of the subspaces Ker(u∗+iu^*+i) or Ker(u∗−iu^*-i) is nonzero, hence the image of u+iu+i or of u−iu-i is a proper subspace of E (Prop. 25 of IV, p. 256), so that ii or −i-i belongs to Sp(uu).

Definition 11 034F

Let uu be a closed symmetric operator on a complex Hilbert space E. A boundary condition for uu is a partially isometric linear mapping (TVS, V, p. 41, Def. 3) of Ker(u∗−iu^*-i) into Ker(u∗+iu^*+i).

Let uu be a closed symmetric operator on a complex Hilbert space E and bb a boundary condition for uu. Let I = Ker(bb)∘^{\circ} be the initial subspace of bb. We denote by ubu_b the reduction of u∗u^* to the subspace of dom(u∗u^*) which is the direct sum of dom(uu) and of the graph in E+⊕E−E_+\oplus E_- of the restriction of bb to I. Since Eu∗=E_{u^*}= dom(uu)⊕E+⊕E−\oplus E_+\oplus E_- (Prop. 26), the partial operator ubu_b is well defined.

In other words, the domain of ubu_b is the space of elements x∈Ex\in E of the form x=x0+y+b(y)x=x_0+y+b(y), where x0∈x_0\in dom(uu) and yy belongs to the initial subspace of bb. One then has ub(x0+y+b(y))=u(x0)+iy−ib(y)u_b(x_0+y+b(y)) =u(x_0) +iy-ib(y).

Theorem 1 (von Neumann) 034G

Let uu be a closed symmetric operator on a complex Hilbert space E and (E+,E−)(E_+,E_-) its deficiency pair.

a) For every boundary condition bb for uu, the partial operator ubu_b is a closed symmetric extension of uu;

b) The mapping b↦ubb\mapsto u_b is a bijection of the set of boundary conditions for uu onto the set of closed symmetric extensions of uu;

c) For every boundary condition bb for uu, one has

Im(ub+iu_b+i) == Im(u+iu+i)⊕\oplus Im(bb)

Im(ub−iu_b-i) == Im(u−iu-i)⊕\oplus Ker(bb)∘^{\circ};

d) For every boundary condition bb for uu, the deficiency pair of ubu_b is (Ker(bb), Ker(b∗b^*)).

Let bb be a boundary condition for uu and I⊂E+I\subset E_+ its initial subspace. The restriction of u∗u^* to Γb∣I⊂E+⊕E−\Gamma_{b|I}\subset E_+\oplus E_- is the continuous linear mapping defined by x+b(x)↦ix−ib(x)x+b(x)\mapsto ix-ib(x) for x∈Ix\in I. The graph of ubu_b is the direct sum of the graph of uu and the graph of this linear mapping; it is therefore closed. The closed operator ubu_b is an extension of uu such that ub⊂u∗u_b\subset u^*.

Let γ1\gamma_1 and η1\eta_1 be elements of I. Consider the elements

γ=γ1+b(γ1),η=η1+b(η1) \gamma =\gamma_1+b(\gamma_1),\eta =\eta_1+b(\eta_1)

of the graph Γb∣I\Gamma_{b|I}. We calculate

⟨γ∣u∗(η)⟩=i(⟨b(γ1)∣η1⟩−⟨γ1∣b(η1)⟩)+i(⟨γ1∣η1⟩−⟨b(γ1)∣b(η1)⟩) \langle \gamma |u^*(\eta )\rangle =i(\langle b(\gamma_1)|\eta_1\rangle - \langle \gamma_1|b(\eta_1)\rangle )+i(\langle \gamma_1|\eta_1\rangle - \langle b(\gamma_1)|b(\eta_1)\rangle )
=i(⟨b(γ1)∣η1⟩−⟨γ1∣b(η1)⟩) =i(\langle b(\gamma_1)|\eta_1\rangle - \langle \gamma_1|b(\eta_1)\rangle )

since bb is isometric on I. It follows that one has

⟨u∗(γ)∣η⟩=⟨γ∣u∗(η)⟩(12) \langle u^*(\gamma )|\eta \rangle =\langle \gamma |u^*(\eta )\rangle \tag{12}

for all γ\gamma and η\eta in Γb∣I\Gamma_{b|I}.

Let xx and yy be elements of dom(uu),γ,\gamma and η\eta elements of Γb∣I\Gamma_{b|I}. Then

⟨x+γ∣ub(y+η)⟩=⟨x∣u(y)⟩+⟨x∣u∗(η)⟩+⟨γ∣u(y)⟩+⟨γ∣u∗(η)⟩ \langle x+\gamma |u_b(y+\eta )\rangle =\langle x|u(y)\rangle +\langle x|u^*(\eta )\rangle +\langle \gamma |u(y)\rangle +\langle \gamma |u^*(\eta )\rangle
=⟨u(x)∣y⟩+⟨u(x)∣η⟩+⟨u∗(γ)∣y⟩+⟨u∗(γ)∣η⟩ =\langle u(x)|y\rangle +\langle u(x)|\eta \rangle +\langle u^*(\gamma )|y\rangle +\langle u^*(\gamma )|\eta \rangle
=⟨ub(x+γ)∣y+η⟩ =\langle u_b(x+\gamma )|y+\eta \rangle

where we have used the fact that uu is symmetric and that γ\gamma and η\eta belong to the domain of u∗u^*, as well as formula (12). The operator ubu_b is therefore a closed symmetric extension of uu. Assertion a) is proved.

The mapping b↦ubb\mapsto u_b is injective. In fact, a partially isometric mapping of E+E_+ into E−E_- is uniquely determined by its initial subspace and by its restriction to the latter. Now the domain of ubu_b determines the initial subspace I of bb and the graph of the restriction of bb to I.

Let us prove that the mapping b↦ubb\mapsto u_b is surjective. Let ww be a closed symmetric extension of uu. One has w⊂w∗⊂u∗w\subset w^*\subset u^*. The domain of ww is therefore a subspace of dom(u∗u^*) containing dom(uu), and ww is the restriction of u∗u^* to this subspace. Let G be the intersection of the domain of ww and of E+⊕E−E_+\oplus E_-. It is a closed subspace of Eu∗E_{u^*} (lemma 7) and one has dom(ww) == dom(uu)⊕G\oplus G by proposition 26.

Let x∈E+x\in E_+ and y∈E−y\in E_- be such that x+y∈Gx+y\in G. Since ww is symmetric, and is the restriction of u∗u^* to dom(ww), we have

⟨x+y∣u∗(x+y)⟩=⟨u∗(x+y)∣x+y⟩ \langle x+y|u^*(x+y)\rangle =\langle u^*(x+y)|x+y\rangle

This equality is equivalent to

⟨x∣ix⟩+⟨x∣−iy⟩+⟨y∣ix⟩+⟨y∣−iy⟩ \langle x|ix\rangle +\langle x| -iy\rangle +\langle y|ix\rangle +\langle y| -iy\rangle
=⟨ix∣x⟩+⟨ix∣y⟩+⟨−iy∣x⟩+⟨−iy∣y⟩ =\langle ix|x\rangle +\langle ix|y\rangle +\langle -iy|x\rangle +\langle -iy|y\rangle

that is, to ∥x∥2=∥y∥2\|x\|^2=\|y\|^2. In particular, the canonical projection p+:G→E+p_+: G\rightarrow E_+ is injective and, if I denotes its image, the space G is the graph of an isometric mapping b0b_0 of I into E−E_-. For xx in I and yy in E−E_- such that x+y∈Gx+y\in G, we have

∥x+y∥u∗2=∥x∥u∗2+∥y∥u∗2=2(∥x∥2+∥y∥2) \|x+y\|^2_{u^*}=\|x\|^2_{u^*}+\|y\|^2_{u^*}= 2(\|x\|^2+\|y\|^2)
=4∥x∥2=4∥p+(x+y)∥2 = 4\|x\|^2= 4\|p_+(x+y)\|^2

Thus, considering G as a closed subspace of the Hilbert space Eu∗E_{u^*}, the mapping x↦12p+(x)x\mapsto \frac{1}{2}p_+(x) of G into I is an isometry. In particular, I is closed in E+E_+ (lemma 8 of I, p. 107). There then exists a unique boundary condition bb for uu whose initial space is I and which coincides with b0b_0 on I. We have dom(ww) == dom(ubu_b), whence w=ubw=u_b. This establishes assertion b).

Let us prove assertions c) and d). Let bb be a boundary condition for uu and I its initial subspace. For x0∈x_0\in dom(uu) and y∈Iy\in I, we have

ub(x0+y+b(y))−i(x0+y+b(y))=(u−i)(x0)−2ib(y) u_b(x_0+y+b(y))-i(x_0+y+b(y)) = (u-i)(x_0)-2ib(y)

We have Im(u−iu-i) =E−∘= E^{\circ}_- (prop. 25). Since the image of bb is contained in E−E_-, this formula shows that Im(ub−iu_b-i) == Im(u−iu-i)⊕\oplus Im(bb). By loc. cit., we thus have Ker(ub∗+iu^*_b+i) =E−∩= E_-\cap Im(bb)∘=^{\circ}= Ker(b∗b^*).

Analogously, one verifies that Im(ub+iu_b+i) == Im(u+iu+i)⊕I\oplus I and hence (loc. cit.) that Ker(ub∗−iu^*_b-i) =I∘∩E+== I^{\circ}\cap E_+= Ker(bb).

Corollary 1 034H

Let uu be a closed symmetric operator on a complex Hilbert space E. The mapping b↦ubb\mapsto u_b induces a bijection of the set of isometries of Ker(u∗−iu^*-i) onto Ker(u∗+iu^*+i) onto the set of self-adjoint extensions of uu. In particular, there exists a self-adjoint extension of uu if and only if the two components of the deficiency index of uu are equal.

This follows from the corollary of proposition 26 and the theorem, together with EVT, V, p. 25, cor. 2.

Corollary 2 034I

Let E be a real Hilbert space. Let uu be a closed symmetric operator on E. The partial operator u(C)u_{(\mathbf{C})} on E(C)E_{(\mathbf{C})} is symmetric and closed, and admits at least one self-adjoint extension.

The partial operator u(C)u_{(\mathbf{C})} is closed and symmetric by prop. 2 of IV, p. 228 and lemma 3 of IV, p. 239. The R\mathbf{R}-linear isomorphism jj of E(C)E_{(\mathbf{C})} onto E(C)E_{(\mathbf{C})} such that j(z⊗x)=z‾⊗xj(z\otimes x) =\overline{z}\otimes x for every z∈Cz\in \mathbf{C} and every x∈Ex\in E induces an isomorphism of Hilbert spaces of Ker(u(C)∗−iu^*_{(\mathbf{C})}-i) onto Ker(u(C)∗+iu^*_{(\mathbf{C})}+i), and one can apply corollary 1.

Corollary 3 034J

Let uu be a symmetric operator on E. The following conditions are equivalent:

(i) The operator uu is essentially self-adjoint;

(ii) The spaces Ker(u∗+iu^*+i) and Ker(u∗−iu^*-i) are zero;

(iii) The spaces Im(u+iu+i) and Im(u−iu-i) are dense in E;

(iv) The partial symmetric operator uu has a unique self-adjoint extension.

Conditions (ii) and (iii) are equivalent by prop. 7, c) of IV, p. 236.

The partial operator uu is essentially self-adjoint if and only if u‾\overline{u} is self-adjoint, that is to say if Ker(u‾∗−i\overline{u}^*-i) == Ker(u‾∗+i\overline{u}^*+i) ={0}=\{0\} (cor. of prop. 26). Since u‾∗=u∗\overline{u}^*=u^* (prop. 8 of IV, p. 237), condition (i) is therefore equivalent to condition (ii). Moreover, the preceding corollary shows that (ii) implies that uu has a unique self-adjoint extension, which is condition (iv).

Finally, suppose that uu has a unique self-adjoint extension vv. Then the same is true of u‾\overline{u}, since every self-adjoint extension of u‾\overline{u} is one of uu, hence is equal to vv. By the preceding corollary, the spaces Ker(u‾∗+i\overline{u}^*+i) and Ker(u‾∗−i\overline{u}^*-i) must be zero, whence condition (ii), using again u‾∗=u∗\overline{u}^*=u^*.

Example 034K

Let U be an open set of Rn\mathbf{R}^n endowed with the Lebesgue measure μ\mu. Let Δ be the scalar differential operator

Δ=−∑i=1n∂i2 \Delta =-\sum_{i=1}^n\partial_i^2

on U. Let us denote by uu the partial operator on the real Hilbert space LR2(U,μ)L^2_{\mathbf{R}}(U, \mu) with domain DR(U)(\mathscr{D}_{\mathbf{R}}(U) (IV, p. 201, remark) defined by φ↦−∑i=1n∂i2φ\varphi \mapsto -\sum^n_{i=1}\partial_i^2\varphi. One has u(C)=Δ−u_{(\mathbf{C})}= \Delta_-, which is a closable partial operator (prop. 13 of IV, p. 242) and symmetric (since Δ is formally symmetric), hence uu is closable and symmetric (proposition 2 of IV, p. 228 and lemma 3 of IV, p. 239). By the above corollary, there therefore exists a self-adjoint extension of u(C)u_{(\mathbf{C})}. It is a Laplacian on U (IV, p. 243).

Exercises

Unless otherwise stated, the Banach spaces and Hilbert spaces below are assumed to be complex.

See the exercises for § 4.

[^1]: Care should be taken not to confuse the notion of graph considered here with that introduced in TA, II, p. 155, def. 1.

Machine translation of the English, by gpt-5.4, against glossary version 34. Not checked by a person.