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CsdLean4.Empirical.QM.Malus

Empirical: Malus's law (spin-1/2 Born probability) #

Category: 3-Local. QM-validity layer (pure inner-product geometry, no CSD ontology). The QM-side companion to Empirical/CSD/MalusVolume.lean: the same cos²(θ/2) value, here as a textbook Born identity rather than a derived Fubini-Study volume.

What this file proves #

For a spin-1/2 prepared in the +-eigenstate of spin along the polar angle θ, ψ_θ = cos(θ/2)|0⟩ + sin(θ/2)|1⟩, and measured along +z:

P(+_z | θ) = |⟨0|ψ_θ⟩|² = cos²(θ/2)        (Malus's law)
P(−_z | θ) = |⟨1|ψ_θ⟩|² = sin²(θ/2)

plus the basis-completeness identity cos²(θ/2) + sin²(θ/2) = 1.

Malus's law subsumes the two Stern-Gerlach values:

The angular law cos²(θ/2) is the spin-1/2 analogue of the classical optical Malus law I = I₀ cos²θ (Malus 1809); the half-angle reflects the spin-1/2 double cover. It reuses the Stern-Gerlach bornProb (the doubly-normalised |⟨state|prep⟩|²), so the result is invariant under (un)normalisation.

Source #

The θ-rotated spin state #

noncomputable def CSD.Empirical.Malus.malus (θ : ) :
Fin 2

The spin-θ +-eigenstate ψ_θ = cos(θ/2)|0⟩ + sin(θ/2)|1⟩ (in the unnormalised Fin 2 → ℂ convention; it is in fact a unit vector).

Equations
Instances For

    Malus's law #

    Malus's law P(+_z | θ) = cos²(θ/2). The Born probability that a spin prepared at polar angle θ is measured + along z.

    Complementary outcome P(−_z | θ) = sin²(θ/2).

    Basis completeness: the two z-outcome probabilities sum to 1.

    Recovery of the Stern-Gerlach values #

    θ = 0 recovers P(+_z | +_z) = 1: at zero angle the prep is |0⟩.

    θ = π/2 recovers the canonical 50/50 split P = 1/2.