PhyslibAlpha.AlgebraicFramework.Dynamics.OneParameterGroup
One-parameter groups acting on a bare carrier
i. Overview
The most primitive notion of time evolution is a group action `α : G → E → E`. This file specializes only the group to `G = (ℝ, +)` — nothing about *what `α` preserves* (linearity, order, a Jordan product, a `⋆`-structure, ...) and nothing about *continuity* belongs here. Those are independent axes:
- structure preservation is a predicate about `α t` for each fixed `t` (see e.g. `Algebra/Derivation.lean`'s companion notion for the infinitesimal picture, or state directly `∀ t a b, α t (a * b) = α t a * α t b` at the point of use — no dedicated class is introduced here since the right notion of "automorphism" depends on which structure `E` carries); - continuity, and the existence of a generator, is `Dynamics/Generator.lean`, requiring a topology `E` need not have at all to be a one-parameter group in the sense below.
This mirrors the point that an Archimedean order-unit space's topology (`OrderUnit/Norm.lean`) is not "AOU has dynamics" — it only supplies enough structure that a generic dynamical construction can later be instantiated there. Likewise here: `E` need not be an order-unit space, a Jordan algebra, or carry any topology for `IsOneParameterGroup` to be meaningful.
ii. Key definitions and results
- `IsOneParameterGroup`
iii. Table of contents
- A. The group law
A. The group law
3 declarations
is the left inverse of for one-parameter groups
For a one-parameter group acting on a carrier set , any time , and any element , the transformation at time acts as the left inverse of the transformation at time . That is, .
Right inverse property of a one-parameter group:
Let be a set and be a one-parameter group. For any and any , the application of the group element to returns the original element, i.e., .
Each in a one-parameter group is a bijection
Let be a one-parameter group acting on a carrier . For any real number , the transformation is a bijective function.
