Bourbaki

Exercise 23, § 5

Tag 037Y, permanent. Cite it as [Bourbaki, Tag 037Y].

Spectral Theories, IV, p. 361

We take up again the notation of the preceding exercise; in particular, we consider a sequence μ=(μn)n∈N\boldsymbol{\mu}= (\mu_n)_{n\in\mathbf{N}} of real numbers satisfying conditions (24) and such that the sesquilinear form bμb_{\boldsymbol{\mu}} is separating. We identify C[X]\mathbf{C}[X] with a dense subspace of EμE_{\boldsymbol{\mu}}.

a) There exists a unique sequence (pn)n∈N(p_n)_{n\in\mathbf{N}} of polynomials in C[X]\mathbf{C}[X] such that the following conditions are satisfied ("orthogonal polynomials of the first species associated with μ\boldsymbol{\mu}"):

(i) The family (pn)(p_n) is an orthonormal basis of EμE_{\boldsymbol{\mu}};

(ii) The polynomial pnp_n is of degree nn for every n∈Nn\in \mathbf{N};

(iii) The coefficient of XnX^n in pnp_n belongs to R+∗\mathbf{R}_+^*.

√ \surd

Moreover, one has pn∈R[X]p_n\in \mathbf{R}[X] for every n∈Nn\in \mathbf{N} and p0=1/μ0‾p_0= 1/\overline{\mu_0}. We also set p−1=0p_{-1}= 0.

b) There exist sequences (an)n⩾−1(a_n)_{n\geqslant-1} in R+∗\mathbf{R}^*_+ and (bn)n∈N(b_n)_{n\in\mathbf{N}} in R\mathbf{R} such that a−1=1a_{-1}= 1 and

uμ(pn)=anpn+1+bnpn+an−1pn−1 u_{\boldsymbol{\mu}}(p_n) =a_np_{n+1}+b_np_n+a_{n-1}p_{n-1}

for every n∈Nn\in \mathbf{N}. These sequences are unique.

c) For every n⩾1n\geqslant 1, the coefficient of XnX^n in the orthogonal polynomial pnp_n is equal to (a0⋯an−1)−1(a_0\cdots a_{n-1})^{-1}.

d) Let F\mathscr{F} be the complex vector space of sequences (zn)n⩾−1(z_n)_{n\geqslant-1} of complex numbers such that z−1=0z_{-1}= 0. We denote by v~μ\widetilde{v}_{\boldsymbol{\mu}} the linear mapping of F\mathscr{F} into itself such that v~μ(zn)=(wn)n∈N\widetilde{v}_{\boldsymbol{\mu}}(z_n) = (w_n)_{n\in\mathbf{N}} where w−1=0w_{-1}= 0 and

wn=anzn+1+bnzn+an−1zn−1 w_n=a_nz_{n+1}+b_nz_n+a_{n-1}z_{n-1}

for every n∈Nn\in \mathbf{N}.

For every s∈Cs\in \mathbf{C}, the sequence zs=(pn(s))n⩾−1z_s= (p_n(s))_{n\geqslant-1} is the unique sequence in F\mathscr{F} such that (zs)0=p0(z)(z_s)_0=p_0(z) and v~μ(zs)=szs\widetilde{v}_{\boldsymbol{\mu}}(z_s) =sz_s.

e) Let zz and ww be elements of F\mathscr{F}. We define the sequence W(z,w)=W(z, w) = (Wn(z,w))n∈N(W_n(z, w))_{n\in\mathbf{N}} by setting

Wn(z,w)=an(zn+1wn−znwn+1) W_n(z, w) =a_n(z_{n+1}w_n-z_nw_{n+1})

for n∈Nn\in \mathbf{N}. One has

Wn(z,w)=∑j=0n(v~μ(z)jwj−zjv~μ(w)j) W_n(z, w) =\sum_{j=0}^n(\widetilde{v}_{\boldsymbol{\mu}}(z)_jw_j-z_j\widetilde{v}_{\boldsymbol{\mu}}(w)_j)

for every n∈Nn\in \mathbf{N}.

f) Let P⊂ℓ2(N)P\subset \ell^2(\mathbf{N}) be the space of sequences with finite support. For every z∈Pz\in P, the sequence v~μ(z)\widetilde{v}_{\boldsymbol{\mu}}(z) belongs to ℓ2(N)\ell^2(\mathbf{N}).

We denote by vμv_{\boldsymbol{\mu}} the partial operator on ℓ2(N)\ell^2(\mathbf{N}) with domain P defined by z↦v~μ(z)z\mapsto \widetilde{v}_{\boldsymbol{\mu}}(z). It is symmetric.

g) The adjoint of vμv_{\boldsymbol{\mu}} is the partial operator with domain

dom(vμ∗v^*_{\boldsymbol{\mu}}) ={z∈ℓ2(N)∣v~μ(z)∈ℓ2(N)}=\{z\in \ell^2(\mathbf{N})|\widetilde{v}_{\boldsymbol{\mu}}(z)\in \ell^2(\mathbf{N})\}

such that vμ∗(z)=v~μ(z)v^*_{\boldsymbol{\mu}}(z) =\widetilde{v}_{\boldsymbol{\mu}}(z) for z∈z\in dom(vμ∗v_{\boldsymbol{\mu}}^*).

h) For all zz and ww in dom(vμ∗v_{\boldsymbol{\mu}}^*), the limit of Wn(z,w)W_n(z, w) as n→+∞n\rightarrow +\infty exists and is equal to ⟨w∣vμ∗(z)⟩−⟨vμ∗(w)∣z⟩\langle w|v^*_{\boldsymbol{\mu}}(z)\rangle - \langle v_{\boldsymbol{\mu}}^*(w)|z\rangle.

i) Let s∈Cs\in \mathbf{C}. The kernel of vμ∗−s⋅1ℓ2(N)v_{\boldsymbol{\mu}}^*-s\cdot 1_{\ell^2(\mathbf{N})} is of dimension ⩽1\leqslant 1; it is of dimension 1 if and only if zs∈ℓ2(N)z_s\in \ell^2(\mathbf{N}), and is then generated by zsz_s.

j) The closure of the partial operator vμv_{\boldsymbol{\mu}} (resp. of uμu_{\boldsymbol{\mu}}) has deficiency index (0,0)(0,0) or (1,1)(1,1); the former case holds if and only if there exists s∈C−Rs\in \mathbf{C}-\mathbf{R} such that zs∉ℓ2(N)z_s\notin\ell^2(\mathbf{N}). (For the case of uμu_{\boldsymbol{\mu}}, note that the mapping Xn↦enX^n\mapsto e_n, where (en)(e_n) is the canonical basis of ℓ2(N)\ell^2(\mathbf{N}), induces an isometric isomorphism of EμE_{\boldsymbol{\mu}} into ℓ2(N)\ell^2(\mathbf{N}) which permits one to identify uμu_{\boldsymbol{\mu}} with vμ.v_{\boldsymbol{\mu}}.)

k) Let s∈Cs\in \mathbf{C} and f∈f\in Ker(uμ∗−s⋅1Eμu^*_{\boldsymbol{\mu}}-s\cdot 1_{E_{\boldsymbol{\mu}}}). If ⟨f∣1⟩=0\langle f|1\rangle = 0, then f=0f= 0.

l) Let u1u_1 and u2u_2 be self-adjoint extensions of uμu_{\boldsymbol{\mu}} on EμE_{\boldsymbol{\mu}}. One has u1=u2u_1=u_2 if and only if there exists s∈C−Rs\in \mathbf{C}-\mathbf{R} such that ⟨R(u1,s)1∣1⟩=⟨R(u2,s)1∣1⟩\langle R(u_1, s)1|1\rangle =\langle R(u_2, s)1|1\rangle. (Suppose that such an equality holds; set f1=R(u1,s)1f_1= R(u_1, s)1, and now prove that f1f_1 does not belong to the domain of u‾μ\overline{u}_{\boldsymbol{\mu}}; deduce that u1u_1 coincides with the closure of the restriction of u1u_1 to dom(u‾μ\overline{u}_{\boldsymbol{\mu}})⊕Cf1\oplus \mathbf{C}f_1. Argue analogously with u2u_2 and f2=R(u2,s)1f_2= R(u_2, s)1, then prove that f1=f2f_1=f_2 to conclude that u1=u2.u_1=u_2.) m) Suppose that uμu_{\boldsymbol{\mu}} is not essentially self-adjoint. There then exist at least two measures ν∈Mm(R)\nu \in \mathscr{M}_m(\mathbf{R}) satisfying ν(xn)=μn\nu (x^n) =\mu_n for every n∈Nn\in \mathbf{N}. n) Suppose in the sequel that uμu_{\boldsymbol{\mu}} is essentially self-adjoint. For every s∈s\in C-R, there exists a sequence (rs,m)m∈N(r_{s,m})_{m\in\mathbf{N}} of polynomials such that (x−s)rs,m(x-s)r_{s,m} converges in EμE_\mu to the constant function 1 as m→+∞m\rightarrow +\infty.

o) Let ν∈Mm(R)\nu \in \mathscr{M}_m(\mathbf{R}) be a measure such that ν(xn)=μn\nu (x^n) =\mu_n for every n∈Nn\in \mathbf{N}. For every m∈Nm\in \mathbf{N}, the inequality

∣∫Rdν(t)t−s−∫Rrs,m(t)dν(t)∣⩽μ20∣I(s)2∣∥1−(x−s)rs,m∥Eμ |\int_{\mathbf{R}}\frac{d\nu(t)}{t-s}-\int_{\mathbf{R}}r_{s,m}(t)d\nu (t)|\leqslant \frac{\mu^{20}}{|\mathscr{I}(s)^2|}\|1-(x-s)r_{s,m}\|_{E_{\boldsymbol{\mu}}}

is valid.

p) The measure ν\nu is unique.

Solution

No solution has been written yet.

Cited by

Nothing.

Cites

Nothing.

Machine translation of the English, by gpt-5.4. Not checked by a person.