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The selected codes have magnetic-support gaps two and three
Statement
For the two ordered code pairs in the cubic-moment lemma, define support to be the set of magnetic labels with nonzero coefficient. The spin-four union of supports is , with consecutive gaps ; the spin-five union is , with consecutive gaps . Their minimum distinct-label separations are therefore two and three. Their hosting spin blocks have dimensions nine and eleven, respectively.
Facts & Assumptions
Given: The finite objects, measure conventions and explicit hypotheses in the Statement.
The displayed coefficients and magnetic labels of both code pairs are explicit, nonzero and normalized. The selected spin-four and spin-five codes have nontrivial cubic moments
The spin- block is with orthonormal magnetic basis indexed by . Finite spin blocks, spherical tensors and Clebsch–Gordan phases
Proof
Given: The finite objects, measure conventions and explicit hypotheses in the Statement.
Goal: Establish the stated formula, convergence and qualifications.
In the spin-four pair the first column uses labels and the second uses . Sorting their union gives , whose consecutive differences are two, four and two. In the spin-five pair the first column uses and the second uses . Sorting gives , whose consecutive differences are three, four and three.
Any difference of two distinct ordered labels is a sum of one or more consecutive positive gaps, so the minimum distinct-label separation equals the smallest consecutive gap. It is therefore two for spin four and three for spin five. A spin-J magnetic basis has vectors, giving dimensions nine and eleven. This is a comparison of magnetic support and host dimension, not a claim of global optimality among codes.
Depends on
Dependency tree · 2 levels
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