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The quantum Serre sums vanish in the shuffle algebra, and the opposite Serre ideal annihilates the shuffle half

Statement

Let Sh(V), ⟨V⟩ and Uℏn+ be as in The formal quantum shuffle Borel and its Cartan crossed product.

(i) In ⟨V⟩⊆Sh(V) the Serre sums vanish: for all i≠j, ∑s=01−aij(−1)s(1−aijs)qi[vi]∗(1−aij−s)∗[vj]∗[vi]∗s=0, where ∗ is the shuffle product of The formal quantum shuffle Borel and its Cartan crossed product.

(ii) Let V∗=⨁iCξi be the dual space with ⟨ξi,vj⟩=di−1δij, let T(V∗)=⨁k≥0(V∗)⊗k⟦ℏ⟧ be the tensor algebra on V∗ with concatenation product, graded by deg⁡ξi=−ϵi, and let Δ:T(V∗)→T(V∗)⊗RT(V∗) be the braided coproduct with Δ(ξi)=ξi⊗1+1⊗ξi, the target carrying the braided product (u⊗v)(u′⊗v′)=q−⟨deg⁡u′,deg⁡v⟩uu′⊗vv′. Let J−⊴T(V∗) be the two-sided ideal generated by the negative Serre elements ∑s=01−aij(−1)s(1−aijs)qiξi1−aij−sξjξis, i≠j. Let ⟨⋅,⋅⟩Sh(V)×T(V∗):Sh(V)×T(V∗)→C((ℏ)),⟨[vi1∣⋯∣vik],ξj1⋯ξjl⟩=δkl ℏ−k∏t=1k⟨vit,ξjt⟩, be the wordwise pairing, extended bilinearly from the tensor-word bases. Then J− annihilates the shuffle half ⟨V⟩: ⟨x,y⟩=0for every x∈⟨V⟩, y∈J−, equivalently the wordwise pairing descends to a bilinear pairing ⟨V⟩×(T(V∗)/J−)→C((ℏ)). The twisted product on T(V∗)⊗RT(V∗) is used only in the definition of the braided coproduct, and no claim is made about the radical of the pairing on all of Sh(V) (see the note after the proof).

Facts & Assumptions

Given: The formal shuffle Borel of a finite symmetrizable Cartan datum and the wordwise pairing stated in part (ii).

[F1]

For i≠j, aij≤0, aii=2, di>0, and diaij=djaji, so ⟨ϵi,ϵj⟩=diaij is a symmetric bilinear form (Symmetrizable Cartan data for quantum groups).

[F2]

qi=qdi, [m]i! is the product of the symmetric qi-integers, and Cm,r=(mr)i=[m]i!/([r]i![m−r]i!) with Cm,0=1 (Quantum integers, factorials, Gaussian binomials and divided powers at qi).

[F3]

Bm,r(t)=[m]t!/([r]t![m−r]t!) are the coefficients in the q-binomial expansion when yx=txy, and Cm,r=Cm,m−r (The quantum binomial expansion for q-commuting elements, The quantum Pascal recurrences, the Gauss product formula and Gaussian integrality).

[F4]

The symmetric Gaussian coefficients are Laurent polynomials in qi and satisfy the q-Pascal and Gauss product identities (The quantum Pascal recurrences, the Gauss product formula and Gaussian integrality).

[F5]

The wordwise quantum shuffle product on Sh(V) uses inversion weight q−⟨deg⁡zi,deg⁡zj⟩ with ⟨ϵi,ϵj⟩=diaij; one-letter words are elements of V (The formal quantum shuffle Borel and its Cartan crossed product).

[F6]

The pairing of part (ii) is diagonal in the tensor-word bases: for tensor words u=[vi1∣⋯∣vik] and v=ξj1⋯ξjl it equals δklδi1j1⋯δikjkℏ−k∏tdit−1; in particular it carries no sign and it is invariant under the interchange i↔j of letters. The letter weights w(i,i)=2di and w(i,j)=diaij=w(j,i) are symmetric.

[F7]

The proof uses only finite word shuffles, coefficient identities, explicit word comparisons and the finitely many permutations of N+1 letters; no axiom of choice is used.

Proof

technique · Write $*$ for the shuffle product and expand the positive Serre expression one word at a time. Then compute the pairing of a shuffle product with the negative Serre element by an explicit permutation count, and compare it with the vanishing alternating sum just obtained
1.1F1F2F3F5givenalgebra

Put N=1−aij, x=[vi], y=[vj], t=qi−2, and Bm,r(t)=0 outside 0≤r≤m. Let Wm=[vi∣⋯∣vi] (with m letters), and let wp be the word with p copies of vi, then vj, then N−p copies of vi (omitting a zero-length block). Repeatedly shuffling one x into a block of m equal x-letters gives x∗m=AmWm, where Am=qi−m(m−1)/2[m]i!: the insertion weights sum to 1+qi−2+⋯+qi−2m=qi−m[m+1]i. In a three-block shuffle Wa∗y∗Wb, with a+b=N, fix wp, and let u (respectively v) count the b-block letters before (respectively after) y, so u+v=b. The prefix interleavings contribute Bp,u(t), the suffix interleavings contribute BN−p,v(t), the u letters before y cross y and the N−p−v letters after it, and each of those u letters crosses those N−p−v suffix x-letters; therefore coeff⁡wp(Wa∗y∗Wb)=∑u+v=bBp,u(t)BN−p,v(t)qi−aij(u+N−p−v)−2u(N−p−v).

1.2F5F6givenalgebra

The pairing is diagonal in the tensor-word bases: for tensor words u=[vi1∣⋯∣vik] and v=ξj1⋯ξjl the defining formula gives ⟨u,v⟩=δklδi1j1⋯δikjkℏ−k∏tdit−1, and ∏tdit−1 depends only on u. Consequently, for x=∑wxw[w] and tensor words y,y′ with letter-sequences u,u′, both sides of ⟨x,yy′⟩=∑k≥0⟨x≤k,y⟩⟨x>k,y′⟩ equal xuu′ℏ−(∣u∣+∣u′∣)(∏s∈uds−1)(∏s∈u′ds−1): the left side because only the word uu′ has nonzero pairing with yy′, the right side because only the cut k=∣u∣ contributes, the product in T(V∗) being concatenation and the cut coproduct of the word [u] being Δ([u])=∑k[u≤k]⊗[u>k]. Extending by bilinearity, this adjunction rule holds for all x∈Sh(V) and all y,y′∈T(V∗).

1.3F5givenalgebra

For homogeneous one-letter words [x1],…,[xm]∈V put w(a,b):=⟨deg⁡xa,deg⁡xb⟩. Then [x1]∗⋯∗[xm]=∑σ∈Smq−∑a<b, σ(a)>σ(b)w(a,b)[xσ−1(1)∣⋯∣xσ−1(m)]. Here σ maps each original letter position to its output position, consistently with [F5]. For m=1 this is the identity. If it holds for m−1, write the product as ([x1]∗⋯∗[xm−1])∗[xm]; inserting [xm] into the k-th position of a word [xσ−1(1)∣⋯∣xσ−1(m−1)] multiplies its coefficient by q−∑a<m, σ(a)≥kw(a,m), exactly the sum of the weights of the pairs (a,m) inverted by the resulting permutation, so the block formula reproduces the displayed expansion; the map (σ,k)↦ the resulting permutation is a bijection onto Sm.

2.1F1F2F3F4F5step 1.1algebra

In the coefficient of wp in ∑s=0N(−1)sCN,sx∗(N−s)∗y∗x∗s, set Q=N−p, write u+v=s, and use AN−sAsCN,s=qi−((N−s)(N−s−1)+s(s−1))/2[N]i! and −aij=N−1. The coefficient simplifies to [N]i!qi−N(N−1)/2+(N−1)Q(∑u=0p(−1)uBp,u(t)qiu(2p−1)−u2)(∑v=0Q(−1)vBQ,v(t)qiv−v2). The quotient definition gives Bm,r(t)=Bm−1,r(t)+tm−rBm−1,r−1(t); induction then yields ∑r=0m(−1)rtr(r−1)/2Bm,r(t)zr=∏j=0m−1(1−ztj). Thus the first factor in parentheses is ∏j=0p−1(1−qi2p−2−2j) and vanishes when p>0; the second is ∏j=0Q−1(1−qi−2j) and vanishes when Q>0. Since p+Q=N≥1, at least one factor vanishes for every p=0,…,N. These words exhaust the color degree Nϵi+ϵj, proving part (i).

2.2F5F6step 1.3algebra

Fix i≠j and N=1−aij, and put w(i,i)=2di, w(i,j)=w(j,i)=diaij; these are the values ⟨deg⁡va,deg⁡vb⟩, and w is symmetric by [F1]. Let z:=∑p=0N(−1)pCN,pξipξjξiN−p; since CN,N−p=CN,p, the element z differs from the printed Serre generator ∑s(−1)sCN,sξiN−sξjξis by the global sign (−1)N, so the two generate the same two-sided ideal. For t∈{0,…,N} let ζt:=[vi]∗t∗[vj]∗[vi]∗(N−t), and for p∈{0,…,N} let wp be the tensor word with p letters vi, then vj, then N−p letters vi. By [F6] and steps 1.2 and 1.3, ⟨ζt,z⟩=ℏ−(N+1)di−Ndj−1∑p=0N(−1)pCN,pM(t,p), where M(t,p):=∑σ∈SN+1, σ(t+1)=p+1q−∑a<b, σ(a)>σ(b)W(a,b) and W(a,b) is the weight w of the letters at positions a,b of the sequence (it,j,iN−t). Then M(t,p)=M(p,t): the map σ↦σ−1 is a bijection from the permutations with σ(t+1)=p+1 onto those with τ(p+1)=t+1, and it preserves the exponent, because the inversion pairs of σ correspond to those of τ=σ−1 with the same pair of letters: if c=σ(b)<d=σ(a) for an inverted pair a<b, then τ(c)=b>a=τ(d), and the weight of the pair {a,b} equals the weight of the letter pair at the positions d,c of the transposed sequence (ip,j,iN−p), since σ carries the position t+1 of j onto the position p+1, so the letter at position σ(x) of the transposed sequence is the letter at position x of the original sequence for every x.

2.3F5step 1.2algebra

The cut coproduct is an algebra map from Sh(V) to its tensor square with product (u⊗v)(u′⊗v′)=q−⟨deg⁡u′,deg⁡v⟩(u∗u′)⊗(v∗v′). Indeed a shuffle followed by a cut consists uniquely of shuffles of the two prefixes and two suffixes; its cross-cut inversions contribute q−⟨deg⁡u−,deg⁡v+⟩, exactly the scalar in this tensor product. On a letter the coproduct is primitive, so it sends every product of letters into ⟨V⟩⊗R⟨V⟩. Write this finite sum as Δ(x)=∑axa′⊗xa′′ with xa′,xa′′∈⟨V⟩; individual prefixes of ambient tensor words need not themselves belong to the generated half. If y annihilates ⟨V⟩, step 1.2 gives ⟨x,yu⟩=∑a⟨xa′,y⟩⟨xa′′,u⟩=0 and likewise ⟨x,uy⟩=0. Thus ⟨V⟩⊥ is a two-sided ideal.

3.1F3step 1.3step 2.2algebra

By part (i) the element ζ:=∑s=0N(−1)sCN,sζN−s is zero in ⟨V⟩⊆Sh(V), so all of its tensor-word coefficients vanish. By step 1.3 the coefficient of wp in ζN−s is M(N−s,p), hence ∑s(−1)sCN,sM(N−s,p)=0 for every p. Substituting t=N−s and using CN,N−t=CN,t (so that (−1)N−t is the global factor (−1)N) gives ∑t(−1)tCN,tM(t,p)=0 for every p; by the symmetry of step 2.2 this is ∑p(−1)pCN,pM(t,p)=0 for every t. Hence step 2.2 gives ⟨ζt,z⟩=0 for every t.

4.1step 2.2step 3.1step 2.3algebra∎

A shuffle product [x1]∗⋯∗[xm] of one-letter words is homogeneous of color degree deg⁡x1+⋯+deg⁡xm, and ⟨V⟩ is generated by the one-letter words, so every x∈⟨V⟩ is a finite sum of such products. Unless the letters are exactly N copies of vi and one copy of vj, their color degree differs from that of z, so the diagonal pairing vanishes. In the remaining case the letter weights agree with the two-letter computation of step 2.2, and step 3.1 gives ⟨[x1]∗⋯∗[xm],z⟩=0. By linearity ⟨x,z⟩=0 for every x∈⟨V⟩, that is, z∈⟨V⟩⊥. Consequently every Serre generator lies in the two-sided ideal ⟨V⟩⊥ of step 2.3, and hence so does the ideal J− they generate: ⟨⟨V⟩,J−⟩=0. This is the stated annihilation and the asserted descent of the wordwise pairing.

Remarks

The literal analogue of (ii) with all of Sh(V) in place of ⟨V⟩ is false, so the restriction of the domain is necessary: the tensor word [vi∣⋯∣vi∣vj] with N copies of vi pairs with the p=0 term of the Serre generator and with no other term, giving ℏ−(N+1)di−Ndj−1≠0. The source's literal full-Sh(V) radical clause therefore fails for the diagonal pairing. The restricted generated-half annihilation used here is proved independently above and supplies the final half-to-half duality. Printed formula (28) also has a single ℏ−1 prefactor; the multiplicative adjunction with generator weights ℏ−1di−1 requires the length-k weight ℏ−k∏tdit−1 used in this item and verified in step 1.2.

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