Alphabeta Math
LemmaStatement: AI-generatedProof: AI-generated
How statement and proof provenance work

The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.

  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.

These labels describe origin, not correctness: citations and verification chips remain separate evidence.

Low-rank tensor families are spin polynomials

Statement

Fix J∈{4,5}. Let Pd denote the complex span of I and all products of at most d members of {Jx,Jy,Jz} on VJ. For r=0,1,2,3, the nonzero highest component Hr=J+r extends by normalized lowering commutators to a rank-r spherical tensor family, all of whose components lie in Pr. Every rank-r family from VJ to itself is a scalar multiple of this family. In particular all rank-zero, rank-one and rank-two tensor components lie in P2.

For any finite set S of spin labels containing J and satisfying ∣J′−J∣≤1 for every J′∈S, let H=⨁J′∈SVJ′, with one labelled copy of each block. Let ιJ:VJ→H be the input-block inclusion, let πJ:H→VJ be its orthogonal coordinate projection, and let ES⊆L(H) be the selected order-one absorption–emission tensor error span. Then ιJJaπJ∈ES for a=x,y,z.

Facts & Assumptions

Given: The finite objects, measure conventions and explicit hypotheses in the Statement.

[F1]

Finite spin generators, their adjoints, commutators and tensor-family equations are fixed. Finite spin blocks, spherical tensors and Clebsch–Gordan phases

[F2]

For fixed input and output blocks, every rank-r tensor family has one common reduced scalar multiplying the same coupled coefficients. Wigner–Eckart with explicit magnetic-label contract

[F3]

Finite self-adjoint angular-momentum triples decompose into spin blocks with the stated normalized highest-weight ladders. Finite spin-block decomposition

[F4]

For the selected blocks specified in the Statement, ES is a complex linear span in L(H) containing IH and every embedded component ιJTqπJ of every rank-one tensor family from VJ to itself. Order-one absorption–emission tensor error span

Proof

Given: The finite objects, measure conventions and explicit hypotheses in the Statement.

Goal: Establish the stated formula, convergence and qualifications.

1.1F1F3algebra

On the matrix space End⁡(VJ) use the coordinate inner product ⟨A,B⟩=∑m,nAmnBmn‾. For a self-adjoint matrix Ja, the commutator map KaA=[Ja,A] is self-adjoint for this inner product: expansion of the two finite matrix sums moves left multiplication and right multiplication to their corresponding adjoints. The identity [Kx,Ky]A=[ [Jx,Jy],A]=iKzA and its cyclic versions follow by expansion. Hence [F3] applies to this finite-dimensional matrix space.

2.1F1F3step 1.1algebra

For 0≤r≤3, J+r is nonzero since r≤2J. It has Kz weight r and is killed by K+. In the spin-block decomposition of step 1.1, a weight-r vector killed by the raising map has components only in blocks with highest weight r. Its cyclic ladder span is therefore one copy of spin r, even if the full matrix space has other copies: on each contributing block the same normalized lowering coefficients apply. Consequently Hq=(ad⁡J−)r−qJ+r/(r−q)!(2r)(2r−1)⋯(r+q+1) is a tensor family, using the empty product at q=r. The commutator derivation rule and the generator commutators show each component belongs to Pr.

3.1F1F2F4step 2.1algebra∎

By [F2], all rank-r families between the fixed spin-J copies are common scalars times one fixed coefficient family. The constructed nonzero family therefore spans every such family, proving the claimed polynomial inclusion. For r=1 its three components are H1=J+, H0=−2Jz, H−1=−J−. Since J∈S, [F4] puts Gq=ιJHqπJ in ES for q=1,0,−1. The identities ιJJxπJ=(G1−G−1)/2, ιJJyπJ=(G1+G−1)/(2i) and ιJJzπJ=−G0/2 then give the three asserted memberships by linearity.

Depends on

Used by · 3

Dependency tree · 2 levels

Each result is drawn at its shortest distance from this item. Arrows run from prerequisites to the items that use them; this item has a heavier outline. External source nodes link directly to the cited text. The view shows up to two dependency steps; open a prerequisite to continue.