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:
θ = 0⟹cos²(0) = 1(P(+_z | +_z) = 1,born_zPlus_zPlus);θ = π/2⟹cos²(π/4) = 1/2(the canonical 50/50 split,born_xPlus_zPlus).
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 #
- Malus 1809 (optical, classical analogue).
- The spin-1/2
cos²(θ/2)form: standard QM (Sakurai, Modern QM; the rotated-spin projection probability).
The θ-rotated spin state #
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.