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Modular Branching and the Good-Node Crystal — Examples

1 · Prerequisites

2 · Summary

Objective. This companion makes the good-node calculus of modular-branching-and-the-good-node-crystal concrete on the smallest nontrivial instances and stresses the conventions. Both entries are dependency leaves: they consume the parent page's residue, signature and good-node definitions and the branching theorems, and nothing outside this page depends on anything homed here.

A full cogood-addition path from the empty partition to (3,1,1) at p = 3 runs the cogood-addition algorithm from the empty partition to a small p-restricted partition, computing every node, residue, signature word and reduced signature by hand, and checking both directions of the good/cogood inverse property along the chosen path; it verifies the reachability theorem on the instance rather than assuming it.

Normal and good nodes for the partition (6,4,4,3,2) computes Brundan's normal and good rows for (6,4,4,3,2) at quantum characteristics 3 and 4, with a trailing zero included in the lattice tests. At ℓ=3 the normal rows are 1,4,5 and the good rows are 1,5; at ℓ=4 the normal rows are 1,3,5 and the sole good row is 1. In each case, removable nodes of the same residue have the same normality. Good rows are the least normal rows in each residue class. The example records the corresponding source socle labels and the decomposability conclusions that require the branching theorem. Quantum characteristic 4 is not a field characteristic.

The small path uses c−r residues directly. The large example uses Brundan's r−c residues and transpose-labelled ordinary Dipper–James simples; its convention must be translated explicitly when compared with the parent page. Both examples are dependency leaves.

3 · Logical flowchart

4 · Definitions, theorems and proofs

None yet.

5 · Examples, counterexamples and false statements

ExampleConstruction: Literature-sourcedVerification: AI-adaptedprecheck passOpen item page →

A full cogood-addition path from the empty partition to (3,1,1) at p = 3

Example

At p=3 the p-restricted partition (3,1,1) is reached from the empty partition by the five cogood additions ∅→ 0 (1)→ 2 (1,1)→ 1 (1,1,1)→ 1 (2,1,1)→ 2 (3,1,1), that is, (1)=f~0∅, (1,1)=f~2(1), (1,1,1)=f~1(1,1), (2,1,1)=f~1(1,1,1), (3,1,1)=f~2(2,1,1), where the labels record the residues of the added nodes (Good-node deletion and cogood-node addition operators). Reversing the path gives the good deletions (3,1,1)→ 2 (2,1,1)→ 1 (1,1,1)→ 1 (1,1)→ 2 (1)→ 0 ∅. The relevant reduced signatures are: (1) at i=0: (−); (1,1) at i=2: (−); (1,1,1) at i=1: (+,−); (2,1,1) at i=1: (−,−); (3,1,1) at i=2: (−); and (1,1) at i=1: (+,+), (2,1,1) at i=2: (+). The word (−,−) for (2,1,1) has two normal nodes of the same residue, while (+,−) for (1,1,1) shows that a reduced signature may contain both signs.

Facts & Assumptions

Given: The prime p=3, the residues of a node computed as c−r mod 3, and the partitions ∅, (1), (1,1), (1,1,1), (2,1,1), (3,1,1).

[F1]

The reduced i-signature of a partition is obtained by listing the addable and removable i-nodes top to bottom, marking them + and −, and cancelling −+ pairs; the good i-node is the removable node of the first surviving −, the cogood i-node is the addable node of the last surviving +, and e~i,f~i delete the good node and add the cogood node (Good-node deletion and cogood-node addition operators, Residue signatures, normal, good, conormal and cogood nodes).

[F2]

For p-restricted μ,ν one has μ=f~iν if and only if ν=e~iμ, with both sides defined simultaneously (Good-node deletion and cogood-node addition operators).

[F3]

The reachability proposition guarantees that a path of cogood additions from ∅ to every p-restricted partition exists; the present example exhibits one explicitly and checks it node by node (Every p-restricted partition is reached from the empty partition by cogood additions).

Verification

technique · direct
1.1givenF1

The 0-nodes of ∅ and (1). The empty partition has the single addable node (1,1) of residue c−r=0, so its residue-0 word is (+) and the cogood node is (1,1), whence f~0∅=(1); the partition (1) has the single removable node (1,1) of residue 0, so its residue-0 word is (−) with good node (1,1) and e~0(1)=∅.

1.2F1F2

The 1-nodes of (1,1) and (1,1,1). In (1,1) the residue-1 nodes are the addable nodes (1,2) (residue 2−1=1) and (3,1) (residue 1−3=−2≡1), ordered (1,2),(3,1) top to bottom; the word is (+,+), the cogood node is the last surviving +, namely (3,1), and f~1(1,1)=(1,1,1), while adding (1,2) would lead to (2,1). In (1,1,1) the residue-1 nodes are the addable node (1,2) and the removable node (3,1); the word (+,−) is already reduced, so the surviving + is (1,2) and the surviving − is (3,1): the cogood node is (1,2) with f~1(1,1,1)=(2,1,1), and the good node is (3,1) with e~1(1,1,1)=(1,1), in agreement with the inverse property of [F2].

2.1step 1.1F1

The 2-nodes of (1) and (1,1). The residue-2 nodes of (1): the addable node (2,1) has residue 1−2=−1≡2, and there is no other, so the word is (+) with cogood node (2,1) and f~2(1)=(1,1). For (1,1) the residue-2 node is the removable node (2,1) (residue 1−2≡2), the word is (−), the good node is (2,1) and e~2(1,1)=(1).

2.2step 1.2F1F2

The 1-nodes of (2,1,1) and the 2-nodes of (2,1,1) and (3,1,1). In (2,1,1) the residue-1 nodes are the removable nodes (1,2) (residue 2−1=1) and (3,1) (residue 1−3≡1), listed (1,2),(3,1): the word (−,−) is reduced, so the good node is the first surviving −, namely (1,2), and e~1(2,1,1)=(1,1,1). The residue-2 nodes of (2,1,1) are the single addable node (1,3) (residue 3−1=2): the word is (+) with cogood node (1,3) and f~2(2,1,1)=(3,1,1). In (3,1,1) the only residue-2 boundary node is the removable node (1,3); the interior node (2,1) has the same residue but does not enter the signature; the word is (−) with good node (1,3) and e~2(3,1,1)=(2,1,1).

3.1step 1.1step 2.1step 1.2step 2.2F2

The path and its reverse. Step 1.1, step 2.1, step 1.2 and step 2.2 exhibit, successively, ∅→(1)→(1,1)→(1,1,1)→(2,1,1)→(3,1,1) as cogood additions with residues 0,2,1,1,2, and each reverse step as the deletion of the good node of the same residue; by [F2] this is exactly the assertion that each forward step is a cogood addition and each reverse step a good deletion, and the five residue labels match the displayed path.

4.1step 1.1step 2.1step 1.2step 2.2F3∎

All reduced signatures claimed in the example are the ones computed: (−) for (1) at i=0 in step 1.1, (−) for (1,1) at i=2 in step 2.1, (+,+) for (1,1) and (+,−) for (1,1,1) at i=1 in step 1.2, and (−,−) for (2,1,1) at i=1, (+) for (2,1,1) at i=2 and (−) for (3,1,1) at i=2 in step 2.2; in particular (−,−) exhibits two normal nodes of one residue and (+,−) exhibits both signs in a reduced word, and the path still exists as [F3] predicts.

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Normal and good nodes for the partition (6,4,4,3,2)

Example

Let F be a field and q∈F×, and use the Hecke algebra H(r) with (Tj−q)(Tj+1)=0 (The generic type-A Hecke algebra). Here ℓ=e(F,q) is its quantum characteristic (The quantum characteristic of an invertible Hecke parameter), taken in turn to be 3 or 4. The case ℓ=4 means a parameter of order 4 and is not a field of characteristic 4; both cases occur over F=C with q a primitive root of the specified order. Use Brundan's restricted DJ labels: Sλ here denotes the ordinary right Specht module labelled by λ′ and Dλ its simple head, as in his §2.1. Right modules may be carried to left modules through the Hecke anti-involution fixing the generators; this preserves socles and direct sum decompositions. These source labels must not be silently identified with the same-shape Murphy labels of the group-theoretic suppliers.

Work Brundan's Example 2.8 (complete 34-page author manuscript, p. 5) in his conventions: λ=(6,4,4,3,2), padded by λ6=0 with n=6, is ℓ-restricted for ℓ=3 and ℓ=4, residues are r−c mod ℓ in the source's orientation (the negative of the c−r convention of this page, Residue signatures, normal, good, conormal and cogood nodes), R(λ)={1,3,4,5} is the set of removable rows, and for i∈R(λ) one compares Bi,6(λ)∩R(λ) with Ci,6(λ)∩R(λ) in the lattice order ↓, where Bi,j(λ)={k∈[i..j):res⁡ℓ(i,λi)=res⁡ℓ(k+1,λk+1+1)},Ci,j(λ)={k∈(i..j):res⁡ℓ(i,λi)=res⁡ℓ(k,λk)}, and A↓B means that there is an injection θ:A→B with θ(a)≤a for all a.

For ℓ=3 the removable nodes have residues 1,2,1,0 for i=1,3,4,5 and (B∩R,C∩R)=(∅,{4}), ({4,5},∅),(∅,∅), (∅,∅); hence Rnormal(λ)={1,4,5} and, since rows 4 and 1 share residue 1, Rgood(λ)={1,5}. For ℓ=4 the residues are 3,3,1,3 and (B∩R,C∩R)=(∅,{3,5}), (∅,{5}),({5},∅), (∅,∅); hence row 4 is normal-refuted by {5}↓̸∅ and Rnormal(λ)={1,3,5}, and since rows 1,3,5 share residue 3, Rgood(λ)={1}. By the branching theorems the restriction of Dλ to H(r−1) is therefore decomposable for ℓ=3 (socle D(5,4,4,3,2)⊕D(6,4,4,3,1)) and indecomposable for ℓ=4 (socle D(5,4,4,3,2)).

Facts & Assumptions

Given: The partition λ=(6,4,4,3,2) of r=19, the field and invertible Hecke parameters with quantum characteristics ℓ=3 and ℓ=4, and Brundan's index sets and lattice order as displayed.

[F1]

The source's definitions: R(λ)={i:λi≠λi+1} is the set of removable rows, the node (i,λi) has residue i−λi mod ℓ, Rnormal(λ)={i∈R(λ):Bi,n(λ)↓Ci,n(λ)} with n=6, and Rgood(λ)={i∈Rnormal(λ): no j∈Rnormal(λ) with j<i and the same residue}; there is at most one good row per residue (Brundan §2.2-2.4 and Remark 2.7, printed pp. 3-5). These are this page's normal and good nodes on the same partition, with residue names negated; Remark 2.4(II) instead compares Brundan's convention with Kleshchev's older convention on the transpose (Residue signatures, normal, good, conormal and cogood nodes).

[F2]

The actual general-Hecke endpoint General Hecke residue branching endpoints from normalized Schur cells gives the multiplicity-free good-deletion socle for Murphy restricted labels. Brundan's source-labelled simple here is Dsourceλ≅DM(λ)θ, where θ(Tj)=q−1−Tj: this is the actual unit-scaled ordinary module/form dictionary applied at ordinary shape λ′ (Ordinary Specht modules are the signed conjugate Murphy cells). The automorphism respects the tower, so twisting both sides transfers the socle and all direct-sum conclusions without renaming a Murphy simple as an untwisted source simple. Distinct good-deletion source simples are separated by the central operator θ(∑a=1r−1La): on DM(μ)θ its scalar is the actual Murphy scalar ∑A∈[μ][c(A)]q of Central Hecke Jucys–Murphy scalars separate q-Schur residue contents. For two deletions of different residues their scalar difference is the difference of their distinct q-contents, hence nonzero. Polynomial primary projectors in this central operator separate the full restricted module, not merely its socle. This proves the required separation without a sufficient same-content block-classification premise.

[F3]

A nonzero finite-dimensional module has nonzero socle: choose a nonzero submodule of least positive dimension. Thus a module with simple socle is indecomposable, because the socle of a direct sum is the direct sum of the summand socles (The radical, socle, head, and Loewy series of a finite-dimensional module). No self-duality of cell modules is assumed.

Verification

technique · direct
1.1givenF1

Removable rows and residues. λ=(6,4,4,3,2) has consecutive differences 2,0,1,1,2, so R(λ)={1,3,4,5} and λ is ℓ-restricted for ℓ=3 and ℓ=4; the residues i−λi are, modulo 3, 1,2,1,0 for i=1,3,4,5, and modulo 4, 3,3,1,3 for the same rows.

2.1step 1.1F1

Pad by λ6=0. For k=1,…,5, the integers k−λk+1 are (−3,−2,0,2,5) and k−λk are (−5,−2,−1,1,3). To compute Bi,6 use indices i≤k<6 with the first integer congruent to i−λi; for Ci,6 use i<k<6 with the second integer congruent to i−λi, then intersect with R={1,3,4,5}. For i=1,3,4,5, respectively, this gives (B∩R,C∩R)=(∅,{4}),({4,5},∅),(∅,∅),(∅,∅) modulo 3, and (∅,{3,5}),(∅,{5}),({5},∅),(∅,∅) modulo 4. These are exactly the corrected displayed pairs.

3.1step 1.1step 2.1F1

For ℓ=3, rows 1,4,5 pass the lattice test: their demand sets are empty. Row 3 fails because {4,5}↓̸∅. Hence Rnormal={1,4,5}, with residues 1,1,0; taking the least normal row in each residue gives Rgood={1,5}. For ℓ=4, rows 1,3,5 pass, while row 4 fails because {5}↓̸∅. The normal rows all have residue 3, so Rgood={1}.

4.1step 3.1F2

ℓ=3: decomposability. By [F2] the actual source-labelled restriction M=Dλ↓H(r−1) has the two simple socle factors Dλ(1)=D(5,4,4,3,2) and Dλ(5)=D(6,4,4,3,1). Their removed Murphy node contents are 5 and −3, of residues 2 and 0 modulo 3, so [F2]'s central operator has distinct scalars on them. Its minimal polynomial on M has distinct linear factors at those two scalars; the polynomial CRT produces a central primary projector b selecting the first and annihilating the second (other factors are included in 1−b). Thus M=bM⊕(1−b)M is a sum of submodules and both are nonzero because they contain the respective simple socle factors. This proves decomposability by actual full-module projections.

4.2step 3.1F2F3

ℓ=4: indecomposability. By the proved branching input [F2], the socle of Dλ↓H(r−1) is the single simple module Dλ(1)=D(5,4,4,3,2). By [F3] this makes the restriction indecomposable: a decomposition into two nonzero modules would give two nonzero summand socles. No cell-module self-duality is used.

5.1step 1.1step 2.1step 3.1step 4.1step 4.2F2∎

At ℓ=4, rows 1,3,5 have residue 3 and are all normal, whereas row 4 has residue 1 and fails {5}↓∅. At ℓ=3, both removable rows of residue 1 are normal. Thus these tables do not exhibit same-residue removable nodes of different normality; they do show that good rows are the least normal rows of each residue, rather than rows whose residue occurs once. The branching conclusions in steps 4.1–4.2 use the actual general-Hecke supplier and source-label transport [F2], with ℓ=4 socle label D(5,4,4,3,2).

The general-Hecke input is the actual constructed endpoint supplier in [F2], including quantum characteristic four. The source's negative residue orientation affects color names but leaves residue equality and the selected row unchanged; the actual theta-twist dictionary transfers the displayed module labels and decomposability conclusions. The finite tables verify the concrete signature calculation; the independent endpoint proof supplies its module-theoretic meaning.

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