The Schrödinger flow is a Kähler symplectomorphism #
Category: 3-Local (The Schrödinger flow is a Kähler symplectomorphism).
This ties the pointwise Kähler form (Mathlib/Analysis/InnerProductSpace/KahlerForm.lean) to the
Schrödinger pillar (schrodingerUnitary, LF4/ProjectedDynamics.lean): the deterministic quantum
evolution exp(-itH) preserves the Fubini–Study Kähler structure — the metric g = re⟪·,·⟫ and
the fundamental form ω = im⟪·,·⟫. So Schrödinger evolution is a symplectic isometry (a
symplectomorphism) of the projective phase space — the Kibble / Ashtekar–Schilling picture of quantum
mechanics as classical Hamiltonian mechanics on the Kähler manifold ℂℙ^{N-1}, at the
pointwise/linear level.
The mechanism is elementary: exp(-itH) is unitary (schrodingerUnitary,
expNegITH_unitary_group), so it preserves the Hermitian inner product
(inner_toEuclideanLin_unitary), hence its real and imaginary parts g and ω.
Why this matters (and its honest scope) #
This is the first rung of the geometric-QM statement "Schrödinger evolution is Hamiltonian flow on the
Fubini–Study phase space" — the dynamics-preserves-the-form half. It connects, in one theorem, the
Kähler form, the Schrödinger flow, and the geometric (Kibble/Ashtekar–Schilling) formulation. It is the
form-level companion to the geometric phase / action (Aharonov–Anandan), whose primitive is the
symplectic potential of ω.
It does NOT derive the flow FROM the form (the Hamiltonian-vector-field statement X_H = ω⁻¹dH,
KG-2) — that needs the symplectic-gradient / manifold-differential API Mathlib lacks and stays
blocked. This module proves the invariance (a symmetry of ω), not the generation. It is at the
Hilbert-vector level; the descent to the ray-level FS form rides on the tangent-space J-invariance
(Kahler.tangent_complexStructure_invariant).
The Schrödinger flow on the state vector. exp(-itH) acting on ψ ∈ ℂ^N, i.e. the
deterministic unitary evolution schrodingerUnitary hH t applied as a linear map.
Equations
- CSD.LF4.schrodingerVectorFlow hH t v = (Matrix.toEuclideanLin ↑(CSD.LF4.schrodingerUnitary hH t)) v
Instances For
Schrödinger evolution preserves the metric g. g (U_t u) (U_t v) = g u v for
U_t = exp(-itH) — the flow is a g-isometry (it preserves the Fubini–Study Riemannian metric).
Schrödinger evolution preserves the fundamental form ω. ω (U_t u) (U_t v) = ω u v for
U_t = exp(-itH) — the flow is a symplectomorphism (it preserves the Fubini–Study symplectic form).
Schrödinger evolution is a Kähler symplectomorphism. The deterministic flow exp(-itH)
preserves BOTH the Fubini–Study metric g and the symplectic form ω:
g (U_t u)(U_t v) = g u v and ω (U_t u)(U_t v) = ω u v. So quantum evolution is a symplectic isometry
of the Kähler geometry of ℂℙ^{N-1} — the Kibble / Ashtekar–Schilling geometric picture (QM as
Hamiltonian mechanics on the Fubini–Study phase space), at the pointwise/linear level. Ties the Kähler
form to the Schrödinger pillar; the converse (flow generated BY the form, X_H = ω⁻¹dH, KG-2) needs
the manifold symplectic-gradient API Mathlib lacks and stays blocked.