Stabilizer label spaces imply the operational computational distribution #
This file joins finite-dimensional symplectic algebra to the explicit complex amplitude Pauli action. The public state premises are normalization, actual Pauli eigenvector equations, isotropy, and maximal label-space dimension. Uniform measurement distributions are conclusions, not premises.
Every label in L represents an actual Pauli eigenvector equation for ψ.
Equations
- LeanPool.SingleCopyStabilizer.HasEigenlabels ψ L = ∀ a ∈ L, ∃ (ζ : ℂ), LeanPool.SingleCopyStabilizer.Measurement.IsPauliEigenvector ψ a.1 a.2 ζ
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A normalized amplitude together with its maximal isotropic eigenlabel space. Eigenvalue phases remain existential and are not discarded from the underlying quantum equations.
- amplitude : Measurement.Amplitude ι
The actual pure-state amplitudes.
- normalized : Measurement.IsNormalized self.amplitude
The maximal isotropic space of actual Pauli eigenlabels.
- isotropic : IsIsotropic self.labels
- eigenlabels : HasEigenlabels self.amplitude self.labels
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Supported outcome differences annihilate diagonal labels for any eigenlabel space, without a maximality or stabilizer-state promise.
For maximal isotropic eigenlabels the geometric X-projection theorem turns every supported difference into an actual stabilizer X direction.
The paper's affine uniform-support theorem, now derived from actual amplitude eigenvector equations and maximal isotropic label-space dimension.
Full diagonal dimension forces any two supported outcomes to coincide.
The termination readout is a point mass when diagonal rank is full. This theorem needs neither isotropy nor maximality beyond the stated full diagonal-rank condition.
Full diagonal rank identifies the amplitude with a basis vector times a unit-modulus scalar, making the global-phase qualification explicit.
Two independent fresh computational measurements followed by subtraction. The second distribution is constant in the first outcome, so this is an independent product experiment expressed with mathlib's PMF bind/map.
Equations
- One or more equations did not get rendered due to their size.
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The PMF subtraction pushforward equals the usual finite convolution formula, derived from bind and map rather than assumed.
Finite convolution of one uniform affine distribution removes its affine offset and gives the uniform distribution on its direction subgroup.
Actual independent Born-measurement differences of a stabilizer state have the uniform PMF on its X projection. The only assumptions are the quantum eigenvector equations and maximal isotropic label-space structure.