Alphabeta Math
DefinitionDefinition: AI-adaptedProof: Not applicablePipeline-generatedaudited 2026-09-22
How statement and proof provenance work

The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.

  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.

These labels describe origin, not correctness: citations and verification chips remain separate evidence.

Strongly continuous one-parameter unitary group

Definition

A strongly continuous one-parameter unitary group on the complex Hilbert space H is a map U:R→B(H) such that U(0)=I, U(s+t)=U(s)U(t) for all s,t∈R, each U(t) is unitary (that is, onto and norm preserving, equivalently U(t)∗U(t)=U(t)U(t)∗=I, A bounded linear operator between normed spaces, The operator norm as the least bound and as the unit-sphere or unit-ball supremum), and the orbit maps t↦U(t)x are continuous at every t for every x∈H, from the usual metric on R to the norm metric of H (Continuity of a map between metric spaces, at a point and globally, in the ε-δ form).

Continuity at the origin suffices, and weak continuity is equivalent to strong continuity. These two clauses are part of the definition's content and are proved here. If t↦U(t)x is continuous at t=0 and t0∈R, then U(t)x−U(t0)x=U(t0)(U(t−t0)x−x) and U(t0) is isometric, so ∥U(t)x−U(t0)x∥=∥U(t−t0)x−x∥→0 as t→t0; the group law and isometry turn continuity at one point into continuity everywhere. Likewise, if t↦U(t)x is merely weakly continuous at 0, then for x∈H the expansion ∥U(t)x−x∥2=2∥x∥2−2Re⁡⟨U(t)x,x⟩ shows that norm convergence at t=0 follows from ⟨U(t)x,x⟩→⟨x,x⟩; and at an arbitrary t0 one has U(t)y−U(t0)y=U(t0)(U(t−t0)y−y), so weak continuity at t0 for every y follows from the case t=0. Conversely, norm continuity of an orbit implies its weak continuity, since for each fixed y∈H, Cauchy--Schwarz gives ∣⟨U(t)x−U(t0)x,y⟩∣≤∥U(t)x−U(t0)x∥ ∥y∥⟶0. Finally, a group with U(0)=I is automatically invertible with U(t)−1=U(−t), so the unitarity and group clauses are symmetric in t.

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