Original text: CC0 1.0. Prerequisite proofs and component terms.

Banach holomorphy, generators, and resolvent limits

OA-MOD-SG-04 — Stone's theorem with the derivative domain

Theorem. Let U:R→B(H)U:\mathbb R\to B(H) be a strongly continuous unitary group. There is a unique self-adjoint operator AA such that

Ut=eitA(t∈R).(SG.8) U_t=e^{itA}\qquad(t\in\mathbb R). \tag{SG.8}

Its domain and action are exactly

D(A)={x:lim⁡h→0Uhx−xh exists in H},iAx=lim⁡h→0Uhx−xh.(SG.9) \begin{aligned} D(A)&=\left\{x:\lim_{h\to0}\frac{U_hx-x}{h} \text{ exists in }H\right\},\\ iAx&=\lim_{h\to0}\frac{U_hx-x}{h}. \end{aligned} \tag{SG.9}

Conversely, the spectral group of every self-adjoint AA is strongly continuous and has (SG.9) as its derivative domain.

Proof. Define AA by (SG.9). For ε>0\varepsilon>0, set

Tεx=1ε∫0εUtx dt.(SG.10) T_\varepsilon x=\frac1\varepsilon\int_0^\varepsilon U_t x\,dt. \tag{SG.10}

A difference quotient and translation of the integral give

TεH⊆D(A),iATε=Uε−Iε.(SG.11) T_\varepsilon H\subseteq D(A),\qquad iAT_\varepsilon=\frac{U_\varepsilon-I}{\varepsilon}. \tag{SG.11}

Strong continuity gives Tεx→xT_\varepsilon x\to x, so D(A)D(A) is dense. For x∈D(A)x\in D(A), the group law gives

ddtUtx=iUtAx=iAUtx.(SG.12) \frac d{dt}U_tx=iU_tAx=iAU_tx. \tag{SG.12}

If xj→xx_j\to x and Axj→yAx_j\to y, integrate (SG.12) and pass to the limit:

Utx−x=i∫0tUsy ds. U_tx-x=i\int_0^tU_sy\,ds.

The derivative at zero puts x∈D(A)x\in D(A) and gives Ax=yAx=y. Thus AA is closed. Differentiating ⟨Utx,Uty⟩\langle U_tx,U_ty\rangle at zero shows

⟨Ax,y⟩=⟨x,Ay⟩(x,y∈D(A)), \langle Ax,y\rangle=\langle x,Ay\rangle \quad(x,y\in D(A)),

so AA is symmetric.

The two norm integrals

B+x=i∫0∞e−tU−tx dt,B−x=−i∫0∞e−tUtx dt(SG.13) B_+x=i\int_0^\infty e^{-t}U_{-t}x\,dt, \qquad B_-x=-i\int_0^\infty e^{-t}U_tx\,dt \tag{SG.13}

exist and have norm at most one. Changing variables in the difference quotients gives

UhB+x−B+xh⟶−B+x+ix,UhB−x−B−xh⟶B−x+ix. \frac{U_hB_+x-B_+x}{h}\longrightarrow-B_+x+ix, \qquad \frac{U_hB_-x-B_-x}{h}\longrightarrow B_-x+ix.

Therefore

(A−i)B+=I,(A+i)B−=I.(SG.14) (A-i)B_+=I,\qquad (A+i)B_-=I. \tag{SG.14}

Both A−iA-i and A+iA+i are onto. If y∈D(A∗)y\in D(A^*), choose x∈D(A)x\in D(A) with (A−i)x=(A∗−i)y(A-i)x=(A^*-i)y. Then y−x∈ker⁡(A∗−i)=ran⁡(A+i)⊥=0y-x\in\ker(A^*-i)=\operatorname{ran}(A+i)^\perp=0. Hence D(A∗)⊆D(A)D(A^*)\subseteq D(A), and symmetry gives A=A∗A=A^*.

Let Vt=eitAV_t=e^{itA}, using the spectral calculus. Both UtU_t and VtV_t preserve D(A)D(A), commute there with AA, and have derivative iAiA. For x∈D(A)x\in D(A), differentiation of Ut−sVsxU_{t-s}V_sx with respect to ss gives zero. Thus Utx=VtxU_tx=V_tx; density proves (SG.8) on all of HH.

Conversely, scalar dominated convergence proves strong continuity of eitAe^{itA}. It also gives the derivative iAxiAx for x∈D(A)x\in D(A). If the difference quotient converges for an arbitrary xx, its norms are bounded along a sequence h→0h\to0. Fatou's lemma applied to

∣eihλ−1h∣2⟶λ2 \left|\frac{e^{ih\lambda}-1}{h}\right|^2 \longrightarrow\lambda^2

puts xx in the spectral domain of AA. This proves the converse domain in (SG.9). Uniqueness follows from that formula. □\square

Editable source · Proof dependencies and component terms