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Hook Immanant Polynomial: Interpolation Theory

Updated 9 July 2026
  • The hook immanant polynomial is an immanantal polynomial defined via hook partitions, serving as a bridge between the determinant and the permanent.
  • It employs representation theory and trace-polynomial methods to derive explicit formulas, monotonicity properties, and matrix inequalities on positive semidefinite and totally nonnegative matrices.
  • The framework extends to graph theory by generating recurrences for graph matrices and extracting invariants such as edge, cycle, and matching counts.

A hook immanant polynomial is the immanantal polynomial attached to a hook partition (k,1nk)(k,1^{n-k}). For an n×nn\times n matrix MM, the hook immanant is dk(M):=d(k,1nk)(M)d_k(M):=d_{(k,1^{n-k})}(M), and the hook immanant polynomial is

Φk(M,x):=dk(xInM)=d(k,1nk)(xInM).\Phi_k(M,x):=d_k(xI_n-M)=d_{(k,1^{n-k})}(xI_n-M).

It interpolates between the characteristic polynomial and the permanental polynomial: Φ1(M,x)=φ(M,x)\Phi_1(M,x)=\varphi(M,x) and Φn(M,x)=ψ(M,x)\Phi_n(M,x)=\psi(M,x). A second, matrix-valued construction arises by specializing the trace-polynomial machinery for immanants to the hook character χ[k,1nk]\chi_{[k,1^{n-k}]}, producing $\widetilde{\imm}_{\chi_{[k,1^{n-k}]}}$. Both constructions are indexed by the irreducible character of SnS_n corresponding to a hook-shaped partition, but they serve different purposes: the former is a scalar polynomial in n×nn\times n0, while the latter is a matrix-valued trace polynomial used in Löwner-order inequalities (Dong et al., 25 Aug 2025, Huber et al., 2021).

1. Definition, notation, and endpoint cases

For a partition n×nn\times n1 and an n×nn\times n2 matrix n×nn\times n3, the immanant is

n×nn\times n4

When n×nn\times n5, this becomes the hook immanant, denoted n×nn\times n6. The convention used is that n×nn\times n7 if n×nn\times n8 or n×nn\times n9 (Dong et al., 25 Aug 2025).

The extreme hook shapes recover the classical endpoint invariants. At MM0, MM1 is the sign character, so MM2. At MM3, MM4 is the trivial character, so MM5. Accordingly,

MM6

The specialization MM7 recovers the hook immanant itself: MM8 Thus the hook family forms a one-parameter interpolation from determinant to permanent (Dong et al., 25 Aug 2025).

A parallel notation appears in the character-immanant literature. For an irreducible character MM9 of dk(M):=d(k,1nk)(M)d_k(M):=d_{(k,1^{n-k})}(M)0,

dk(M):=d(k,1nk)(M)d_k(M):=d_{(k,1^{n-k})}(M)1

In particular, dk(M):=d(k,1nk)(M)d_k(M):=d_{(k,1^{n-k})}(M)2 and dk(M):=d(k,1nk)(M)d_k(M):=d_{(k,1^{n-k})}(M)3. For hooks, the normalized quantity

dk(M):=d(k,1nk)(M)d_k(M):=d_{(k,1^{n-k})}(M)4

is especially important, with

dk(M):=d(k,1nk)(M)d_k(M):=d_{(k,1^{n-k})}(M)5

This binomial dimension formula is one of the reasons hook immanants admit unusually explicit formulas (Skandera, 30 Sep 2025).

2. Representation-theoretic and trace-polynomial realizations

The representation-theoretic formulation starts from the general immanant

dk(M):=d(k,1nk)(M)d_k(M):=d_{(k,1^{n-k})}(M)6

and specializes to hooks by taking dk(M):=d(k,1nk)(M)d_k(M):=d_{(k,1^{n-k})}(M)7. For positive semidefinite dk(M):=d(k,1nk)(M)d_k(M):=d_{(k,1^{n-k})}(M)8, the matrix can be written as a Gram matrix of vectors dk(M):=d(k,1nk)(M)d_k(M):=d_{(k,1^{n-k})}(M)9, and the generalized matrix function has the tensor-trace form

Φk(M,x):=dk(xInM)=d(k,1nk)(xInM).\Phi_k(M,x):=d_k(xI_n-M)=d_{(k,1^{n-k})}(xI_n-M).0

where Φk(M,x):=dk(xInM)=d(k,1nk)(xInM).\Phi_k(M,x):=d_k(xI_n-M)=d_{(k,1^{n-k})}(xI_n-M).1. With the centrally primitive idempotent

Φk(M,x):=dk(xInM)=d(k,1nk)(xInM).\Phi_k(M,x):=d_k(xI_n-M)=d_{(k,1^{n-k})}(xI_n-M).2

one obtains

Φk(M,x):=dk(xInM)=d(k,1nk)(xInM).\Phi_k(M,x):=d_k(xI_n-M)=d_{(k,1^{n-k})}(xI_n-M).3

For hook immanants, Φk(M,x):=dk(xInM)=d(k,1nk)(xInM).\Phi_k(M,x):=d_k(xI_n-M)=d_{(k,1^{n-k})}(xI_n-M).4 and Φk(M,x):=dk(xInM)=d(k,1nk)(xInM).\Phi_k(M,x):=d_k(xI_n-M)=d_{(k,1^{n-k})}(xI_n-M).5, so the hook immanant is realized as a projected squared norm on the hook isotypic component (Huber et al., 2021).

The same framework defines trace polynomials Φk(M,x):=dk(xInM)=d(k,1nk)(xInM).\Phi_k(M,x):=d_k(xI_n-M)=d_{(k,1^{n-k})}(xI_n-M).6 and matrix-valued trace polynomials Φk(M,x):=dk(xInM)=d(k,1nk)(xInM).\Phi_k(M,x):=d_k(xI_n-M)=d_{(k,1^{n-k})}(xI_n-M).7, and hence

Φk(M,x):=dk(xInM)=d(k,1nk)(xInM).\Phi_k(M,x):=d_k(xI_n-M)=d_{(k,1^{n-k})}(xI_n-M).8

For a hook character this becomes

Φk(M,x):=dk(xInM)=d(k,1nk)(xInM).\Phi_k(M,x):=d_k(xI_n-M)=d_{(k,1^{n-k})}(xI_n-M).9

This is the direct hook specialization of the matrix-valued trace-polynomial construction. In this sense, “hook immanant polynomial” may denote not only Φ1(M,x)=φ(M,x)\Phi_1(M,x)=\varphi(M,x)0 but also a noncommutative trace polynomial determined by the same hook character (Huber et al., 2021).

A structural vanishing theorem constrains these matrix-valued forms. If Φ1(M,x)=φ(M,x)\Phi_1(M,x)=\varphi(M,x)1 corresponds to a Young diagram with more than Φ1(M,x)=φ(M,x)\Phi_1(M,x)=\varphi(M,x)2 rows, then

Φ1(M,x)=φ(M,x)\Phi_1(M,x)=\varphi(M,x)3

for all complex Φ1(M,x)=φ(M,x)\Phi_1(M,x)=\varphi(M,x)4 matrices Φ1(M,x)=φ(M,x)\Phi_1(M,x)=\varphi(M,x)5. For the hook Φ1(M,x)=φ(M,x)\Phi_1(M,x)=\varphi(M,x)6, the number of rows is Φ1(M,x)=φ(M,x)\Phi_1(M,x)=\varphi(M,x)7. Hence if Φ1(M,x)=φ(M,x)\Phi_1(M,x)=\varphi(M,x)8, the hook matrix polynomial vanishes identically (Huber et al., 2021).

3. Positivity, monotonicity, and matrix inequalities

For Hermitian positive semidefinite matrices, the normalized hook immanants form a monotone chain from permanent down to determinant: Φ1(M,x)=φ(M,x)\Phi_1(M,x)=\varphi(M,x)9 This is the hook chain conjectured by Merris and proved by Heyfron. Skandera proved that the same chain holds for every Φn(M,x)=ψ(M,x)\Phi_n(M,x)=\psi(M,x)0 totally nonnegative matrix, so the normalized hook immanants are monotone not only on Hermitian positive semidefinite matrices but also on the distinct class of totally nonnegative matrices (Skandera, 30 Sep 2025).

The hook case also sits inside broader inequalities for immanants on positive semidefinite matrices. The appendix of the matrix-inequality framework records Schur’s inequality

Φn(M,x)=ψ(M,x)\Phi_n(M,x)=\psi(M,x)1

which applies in particular to every hook Φn(M,x)=ψ(M,x)\Phi_n(M,x)=\psi(M,x)2. It also records Watkins’s theorem in the form

Φn(M,x)=ψ(M,x)\Phi_n(M,x)=\psi(M,x)3

and Heyfron’s theorem that the normalized hook immanants

Φn(M,x)=ψ(M,x)\Phi_n(M,x)=\psi(M,x)4

form a chain between determinant and permanent on positive semidefinite matrices (Huber et al., 2021).

The matrix-valued trace-polynomial theory lifts such scalar inequalities to the Löwner order. If Φn(M,x)=ψ(M,x)\Phi_n(M,x)=\psi(M,x)5 for all positive semidefinite Φn(M,x)=ψ(M,x)\Phi_n(M,x)=\psi(M,x)6, then

Φn(M,x)=ψ(M,x)\Phi_n(M,x)=\psi(M,x)7

for all positive semidefinite Φn(M,x)=ψ(M,x)\Phi_n(M,x)=\psi(M,x)8 of equal size. Consequently, scalar hook inequalities yield matrix inequalities for the hook trace polynomial Φn(M,x)=ψ(M,x)\Phi_n(M,x)=\psi(M,x)9. In degree χ[k,1nk]\chi_{[k,1^{n-k}]}0, the hook partition χ[k,1nk]\chi_{[k,1^{n-k}]}1 gives an explicit matrix inequality for trace-one positive semidefinite χ[k,1nk]\chi_{[k,1^{n-k}]}2: χ[k,1nk]\chi_{[k,1^{n-k}]}3 This exhibits a concrete low-dimensional hook trace-polynomial inequality (Huber et al., 2021).

4. Hook immanant polynomials of graph and digraph matrices

A major source of explicit hook immanant polynomials is the linear-combination matrix

χ[k,1nk]\chi_{[k,1^{n-k}]}4

for a graph χ[k,1nk]\chi_{[k,1^{n-k}]}5, and similarly

χ[k,1nk]\chi_{[k,1^{n-k}]}6

for a digraph. Here χ[k,1nk]\chi_{[k,1^{n-k}]}7 is the degree matrix and χ[k,1nk]\chi_{[k,1^{n-k}]}8 the adjacency matrix. Specializations include adjacency χ[k,1nk]\chi_{[k,1^{n-k}]}9, Laplacian $\widetilde{\imm}_{\chi_{[k,1^{n-k}]}}$0, signless Laplacian $\widetilde{\imm}_{\chi_{[k,1^{n-k}]}}$1, and $\widetilde{\imm}_{\chi_{[k,1^{n-k}]}}$2 (Dong et al., 25 Aug 2025).

For graphs, the central vertex-deletion formula is

$\widetilde{\imm}_{\chi_{[k,1^{n-k}]}}$3

There is a parallel edge-deletion identity, and both formulas have digraph analogues in which graph cycles are replaced by consistently directed cycles. In the digraph case there is no $\widetilde{\imm}_{\chi_{[k,1^{n-k}]}}$4-neighbor term, because a 2-cycle in the permutation expansion would require both directed arcs (Dong et al., 25 Aug 2025).

These recursions simplify sharply on trees, where all cycle sums vanish. For a tree $\widetilde{\imm}_{\chi_{[k,1^{n-k}]}}$5,

$\widetilde{\imm}_{\chi_{[k,1^{n-k}]}}$6

For adjacency matrices this becomes

$\widetilde{\imm}_{\chi_{[k,1^{n-k}]}}$7

At the endpoints $\widetilde{\imm}_{\chi_{[k,1^{n-k}]}}$8 and $\widetilde{\imm}_{\chi_{[k,1^{n-k}]}}$9, these identities recover classical characteristic-polynomial and permanental-polynomial recurrences (Dong et al., 25 Aug 2025).

The same framework produces direct formulas for hook immanants by setting SnS_n0. It also yields special identities such as

SnS_n1

for bipartite graphs, where SnS_n2 and SnS_n3. The reason given is that bipartite graphs have no odd cycles, so the cycle terms in the Laplacian and signless Laplacian recursions match (Dong et al., 25 Aug 2025).

5. Coefficients, graph invariants, and regular graphs

For the hook partition SnS_n4, the immanantal polynomial of

SnS_n5

is expanded as

SnS_n6

An explicit theorem gives the first six coefficients SnS_n7 for SnS_n8 (Dong et al., 6 Apr 2026).

The first coefficients are

SnS_n9

n×nn\times n00

and

n×nn\times n01

For n×nn\times n02, the formula adds a triangle term

n×nn\times n03

alongside the degree-symmetric and matching-type terms. The formulas for n×nn\times n04 and n×nn\times n05 involve n×nn\times n06, n×nn\times n07, weighted cycle sums n×nn\times n08, weighted matching sums n×nn\times n09, and the triangle-degree quantity n×nn\times n10 (Dong et al., 6 Apr 2026).

The adjacency specialization is especially transparent. With n×nn\times n11 and n×nn\times n12,

n×nn\times n13

n×nn\times n14

n×nn\times n15

The subsequent coefficients show that, for adjacency matrices, the first hook coefficients detect the number of edges, triangles, 2-matchings and 4-cycles, and 5-cycles and triangle-plus-edge configurations (Dong et al., 6 Apr 2026).

A rigidity theorem holds for regular graphs. If n×nn\times n16 and n×nn\times n17 are nonzero real numbers and n×nn\times n18 are regular graphs, then

n×nn\times n19

if and only if

n×nn\times n20

For regular graphs, the hook immanantal polynomial of n×nn\times n21 therefore carries exactly the same information as that of the adjacency matrix (Dong et al., 6 Apr 2026).

6. Complexity and adjacent hook-indexed constructions

The computational complexity of hook immanants is controlled by the Young-diagram parameter

n×nn\times n22

where n×nn\times n23 is the number of parts of n×nn\times n24. For the hook n×nn\times n25,

n×nn\times n26

and in the notation n×nn\times n27,

n×nn\times n28

Thus the governing parameter is the arm length beyond the first column (Curticapean, 2021).

The resulting dichotomy is sharp. If n×nn\times n29, then n×nn\times n30 and n×nn\times n31. For hooks this means bounded arm length, equivalently constant n×nn\times n32 in n×nn\times n33. Hartmann’s algorithm runs in

n×nn\times n34

so hooks of bounded arm length are polynomial-time computable. If n×nn\times n35, then for computationally reasonable families n×nn\times n36, polynomial-time computability is ruled out unless n×nn\times n37, and the algebraic analogue is ruled out unless n×nn\times n38. If n×nn\times n39 grows polynomially, then the corresponding hook family is n×nn\times n40-hard and n×nn\times n41-complete (Curticapean, 2021).

Several neighboring theories use the same hook partitions without defining the classical hook immanant polynomial itself. In chromatic symmetric function theory, the hook coefficient of n×nn\times n42 is

n×nn\times n43

where n×nn\times n44 counts acyclic orientations with n×nn\times n45 sinks; this gives positivity of all hook Schur coefficients for arbitrary graphs, but not a matrix-immanant formula (Kaliszewski, 2014). In the restriction problem for n×nn\times n46 to n×nn\times n47, hook highest weights n×nn\times n48 lead to positive tableau formulas for restriction coefficients n×nn\times n49, again through hook-indexed character theory rather than direct immanant evaluation (Narayanan, 2024). In a different direction, the twisted immanant is defined only for self-conjugate partitions; among hooks, this leaves exactly n×nn\times n50, and for matrices with anticommuting entries one has

n×nn\times n51

That identity belongs to a distinct, twisted theory rather than the ordinary hook immanant polynomial (Itoh, 2015).

These neighboring constructions underscore a recurring fact: the hook partition n×nn\times n52 is unusually tractable across representation theory, symmetric functions, graph polynomials, and positivity theory. For ordinary immanants, that tractability appears most concretely in the binomial dimension formula, the determinant-to-permanent hook inequalities, the explicit graph recursions for n×nn\times n53, and the complete complexity transition governed by hook arm length (Skandera, 30 Sep 2025, Dong et al., 25 Aug 2025, Curticapean, 2021).

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