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PhyslibAlpha.AlgebraicFramework.HilbertSpace.Unbounded.Flow.Stone

Stone generator of a domain-aware spectral theorem

This file is the operator-level hand-off from the real spectral integral to Stone's theorem. The scalar and Hilbert-space limit is proved in `Stone`; the theorem below uses the domain equality and self-adjoint uniqueness package from `SelfAdjointSpectralTheorem` to identify the maximal spectral integral with the given unbounded operator.

6 declarations

theorem

lim⁡t→0eitTx−xt=iTx\lim_{t \to 0} \frac{e^{itT}x - x}{t} = iTx for x∈D(T)x \in \mathcal{D}(T)

Let TT be a self-adjoint operator on a Hilbert space HH with domain D(T)\mathcal{D}(T). Let U(t)=eitTU(t) = e^{itT} be the strongly continuous one-parameter unitary group associated with TT via the spectral theorem, defined by the spectral integral U(t)=∫Reitλ dμS(λ)U(t) = \int_{\mathbb{R}} e^{it\lambda} \, d\mu_S(\lambda). For any vector x∈D(T)x \in \mathcal{D}(T), the limit of the difference quotient as t→0t \to 0 converges in the norm topology of HH to iTxiTx: lim⁡t→0eitTx−xt=iTx\lim_{t \to 0} \frac{e^{itT}x - x}{t} = iTx where ii is the imaginary unit.

theorem

The derivative of eitTxe^{itT}x at t=0t=0 is iTxiTx for x∈dom(T)x \in \text{dom}(T)

Let TT be a self-adjoint operator acting on a Hilbert space HH, and let μS\mu_S be its associated spectral measure. Let U(t)=eitTU(t) = e^{itT} be the strongly continuous one-parameter unitary group defined by the spectral integral U(t)=∫Reitλ dμS(λ)U(t) = \int_{\mathbb{R}} e^{it\lambda} \, d\mu_S(\lambda). For any vector xx in the domain of TT, the function t↦U(t)xt \mapsto U(t)x is differentiable at t=0t = 0, and its derivative is given by ddt(eitTx)∣t=0=iTx \left. \frac{d}{dt} (e^{itT}x) \right|_{t=0} = iTx where ii is the imaginary unit.

theorem

The derivative of eitTxe^{itT}x at any time ss is eisT(iTx)e^{isT}(iTx)

Let HH be a Hilbert space and TT a self-adjoint operator on HH with domain dom(T)\text{dom}(T). Let U(t)=eitTU(t) = e^{itT} be the strongly continuous one-parameter unitary group associated with TT via the spectral theorem, defined by U(t)=∫Reitλ dμS(λ)U(t) = \int_{\mathbb{R}} e^{it\lambda} \, d\mu_S(\lambda). For any vector x∈dom(T)x \in \text{dom}(T) and any time s∈Rs \in \mathbb{R}, the function t↦U(t)xt \mapsto U(t)x is differentiable at t=st = s with derivative ddt(eitTx)∣t=s=eisT(iTx) \frac{d}{dt} \left( e^{itT}x \right) \bigg|_{t=s} = e^{isT}(iTx) where ii is the imaginary unit.

theorem

x∈D(T)x \in \mathcal{D}(T) if and only if the limit of eitTx−xt\frac{e^{itT}x - x}{t} exists as t→0t \to 0

Let HH be a Hilbert space and TT be a self-adjoint operator with domain D(T)\mathcal{D}(T) and spectral measure μS\mu_S. Let U(t)=eitTU(t) = e^{itT} be the strongly continuous one-parameter unitary group associated with TT, defined by the spectral integral U(t)=∫Reitλ dμS(λ)U(t) = \int_{\mathbb{R}} e^{it\lambda} \, d\mu_S(\lambda). For any vector x∈Hx \in H, xx belongs to the domain of TT if and only if there exists a vector y∈Hy \in H such that the limit of the difference quotient converges as t→0t \to 0: lim⁡t→0U(t)x−xt=y \lim_{t \to 0} \frac{U(t)x - x}{t} = y

theorem

x∈dom(T)x \in \text{dom}(T) if and only if t↦eitTxt \mapsto e^{itT}x is differentiable at t=0t=0

Let HH be a Hilbert space and TT be a self-adjoint operator on HH with domain dom(T)\text{dom}(T). Let U(t)=eitTU(t) = e^{itT} be the strongly continuous one-parameter unitary group associated with TT via the spectral theorem. For any vector x∈Hx \in H, xx belongs to dom(T)\text{dom}(T) if and only if the vector-valued function t↦U(t)xt \mapsto U(t)x is differentiable at t=0t = 0, i.e., there exists a vector y∈Hy \in H such that ddt(U(t)x)∣t=0=y\frac{d}{dt}(U(t)x)|_{t=0} = y.

theorem

U(t)∗=U(−t)U(t)^* = U(-t) for the Stone unitary group

Let HH be a Hilbert space and TT a self-adjoint operator with associated spectral measure μS\mu_S. Let U(t)=eitTU(t) = e^{itT} be the strongly continuous one-parameter unitary group defined by the spectral integral U(t)=∫Reitλ dμS(λ)U(t) = \int_{\mathbb{R}} e^{it\lambda} \, d\mu_S(\lambda) For any t∈Rt \in \mathbb{R}, the adjoint of the unitary operator U(t)U(t) satisfies U(t)∗=U(−t)U(t)^* = U(-t).