Bourbaki

Exercise 31, § 3

Tag 032G, permanent. Cite it as [Bourbaki, Tag 032G].

Spectral Theories, IV, p. 343

Let LL denote the differential operator

L=−i∂1+∂2−2(x1+ix2)∂3 L =-i\partial_1+\partial_2-2(x_1+ix_2)\partial_3

of order 1 on R3\mathbf{R}^3, where (x1,x2,x3)(x_1, x_2, x_3) is the dual basis of the canonical basis of R3\mathbf{R}^3, the xix_i being regarded as polynomials on R3\mathbf{R}^3 (“Lewy operator”).

a) Let U be an open neighbourhood of 0 in R3\mathbf{R}^3. There exists a function φ∈D(U)\varphi \in \mathscr{D}(U) such that φ(0)=1\varphi (0) = 1 and such that L(φ)L(\varphi ) is zero in a neighbourhood V of 0 contained in U. (Use the Cauchy–Kowalewski theorem.)

b) Let u∈C∞(U)u\in \mathscr{C}^{\infty}(U) be a function such that L(u)=0L(u) = 0 and u(0)=0u(0) = 0. Suppose that there exists δ>0\delta >0 such that R(u(x))<−2δ\mathscr{R}(u(x))<-2\delta for x∈Ux\in U - V. Put vt=φv_t=\varphi exp(t(u+δ)t(u+\delta )). Then vt∈C∞(U)v_t\in \mathscr{C}^{\infty}(U) and L(vt)L(v_t) tends to 0 in D(U)\mathscr{D}(U) when t→+∞t\rightarrow +\infty.

c) Let F be the space of functions f∈C∞(U)f\in \mathscr{C}^{\infty}(U) such that ∂αf\partial^{\alpha}f is bounded on U for every α∈N3\alpha \in \mathbf{N}^3. The space F endowed with the seminorms qα(f)=q_{\alpha}(f) = supx∈U∣∂αf∣_{x\in U}|\partial^{\alpha}f| is a Fréchet space.

d) Let ψ∈D(R3)\psi \in \mathscr{D}(\mathbf{R}^3). Denote by ftf_t the restriction to U of the function x↦t3ψ(tx)x\mapsto t^3\psi (tx). Then ft∈Ff_t\in F for t⩾1t\geqslant 1, and there exists a real number c⩾0c\geqslant 0 such that qα(ft)⩽ct∣α∣+3q_{\alpha}(f_t)\leqslant ct^{|\alpha|+3} for every α∈N3\alpha \in \mathbf{N}^3 and every t⩾1t\geqslant 1.

e) For every t⩾1t\geqslant 1, let λt\lambda_t denote the linear form f↦∫Ufvtf\mapsto \int_Uf v_t on F. It is continuous and, for tt sufficiently large, one has

λt(ft)=eδt(∫Uψ(x)\lambda_t(f_t) =e^{\delta t}(\int_U\psi (x) exp(∑j=13ξjxj)dx1dx2dx3+ε(t))(\sum_{j=1}^3\xi_jx_j)dx_1dx_2dx_3+\varepsilon (t))

where ξj=∂ju(0)\xi_j=\partial_ju(0) and ε(t)→0\varepsilon (t)\rightarrow 0 when t→+∞t\rightarrow +\infty.

f ) Suppose that (ξj)≠0(\xi_j)\not = 0; there exists f∈Ff\in F such that the integrals ∫Ufvt\int_Uf v_t are not bounded when t→+∞t\rightarrow +\infty. (If the assertion were false, obtain a contradiction by using the preceding question and the Banach– Steinhaus theorem.)

g) The functions vtv_t do not converge to 0 in D′(U)\mathscr{D}'(U) when t→+∞t\rightarrow +\infty. h) Let ξ=(0,0,ξ3)∈R3\xi = (0,0, \xi_3)\in \mathbf{R}^3 be such that ξ3<0\xi_3<0. There exists a neighbourhood U of 0 in R3\mathbf{R}^3 and a function u∈C∞(U)u\in \mathscr{C}^{\infty}(U) such that L(u)=0L(u) = 0 and u(0)=0u(0) = 0, and satisfying the conditions of questions b) and f). (Use the Cauchy–Kowalewski theorem.)

i) Let (vt)(v_t) be functions in D(U)\mathscr{D}(U) such that L(vt)→0L(v_t)\rightarrow 0, and let f∈D(U)f\in \mathscr{D}(U) be such that ∫Ufvt\int_Uf v_t is not bounded when t→+∞t\rightarrow +\infty (question g)) ; the equation Lv=fLv=f has no solution v∈D′(U)v\in \mathscr{D}'(U) ("Lewy's theorem"). (Note that the formal adjoint of L coincides with L.)

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