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Second Immanantal Polynomial

Updated 6 July 2026
  • The second immanantal polynomial is a hook immanant defined via the partition (2,1^(n-2)), bridging determinant and permanent frameworks.
  • It uses explicit character formulas and fixed-point statistics to provide concrete combinatorial interpretations in graph and Laplacian matrices.
  • Its structural recurrences and complexity distinctions, depending on hook conventions, reveal key insights into reconstruction and computational tractability.

The second immanantal polynomial is an immanantal polynomial attached to a hook partition of nn, most commonly (2,1n2)(2,1^{n-2}) in the graph, Laplacian, and recent hook-immanant literature, where one writes

d2(M)=σSnχ2(σ)i=1nmi,σ(i)d_2(M)=\sum_{\sigma\in S_n}\chi_2(\sigma)\prod_{i=1}^n m_{i,\sigma(i)}

for the corresponding immanant and d2(xIM)d_2(xI-M) for the polynomial. The terminology is not completely uniform. In some representation-theoretic, hook-inequality, and Newton-polytope discussions, the adjacent hook (n1,1)(n-1,1) is treated as the “second” immanant instead. Complexity-theoretic work on partition-indexed immanants often avoids the phrase entirely and works directly with immλ\mathrm{imm}_\lambda for a partition λn\lambda\vdash n. The resulting ambiguity is substantive rather than cosmetic, because the two hooks are conjugate but support different explicit character formulas, graph-theoretic interpretations, and complexity behavior (Nagar et al., 2017, Wu et al., 18 Feb 2025, Nagar, 2023, Curticapean, 2021).

1. Terminology and defining formulas

For a partition λn\lambda\vdash n and an n×nn\times n matrix A=(aij)A=(a_{ij}), the immanant is

(2,1n2)(2,1^{n-2})0

and the corresponding immanantal polynomial is

(2,1n2)(2,1^{n-2})1

For (2,1n2)(2,1^{n-2})2, this reduces to the characteristic polynomial, while for general (2,1n2)(2,1^{n-2})3 it defines a partition-indexed family interpolating between determinant and permanent (Nagar et al., 2017).

In the usage that is explicit in several graph-matrix papers, the second immanant is the hook case (2,1n2)(2,1^{n-2})4, and the second immanantal polynomial of a matrix (2,1n2)(2,1^{n-2})5 is (2,1n2)(2,1^{n-2})6. This convention is stated directly for general matrices, adjacency matrices, and linear-combination graph matrices, and it is the convention adopted in recent reconstruction and hook-immanant polynomial work (Wu et al., 18 Feb 2025, Dong et al., 25 Aug 2025, Dong et al., 6 Apr 2026).

A different convention appears in some literature organized from the permanent side of the hook chain. There the natural “second” object is the hook (2,1n2)(2,1^{n-2})7, so that the relevant polynomial is (2,1n2)(2,1^{n-2})8 in Laplacian settings, or (2,1n2)(2,1^{n-2})9 in character-immanant settings (Nagar, 2023, Skandera, 30 Sep 2025). This terminological split is one of the central points in any precise account of the subject.

2. Character-theoretic placement within the immanant family

Immanants sit between the determinant and permanent. For the sign character one has

d2(M)=σSnχ2(σ)i=1nmi,σ(i)d_2(M)=\sum_{\sigma\in S_n}\chi_2(\sigma)\prod_{i=1}^n m_{i,\sigma(i)}0

and for the trivial character one has

d2(M)=σSnχ2(σ)i=1nmi,σ(i)d_2(M)=\sum_{\sigma\in S_n}\chi_2(\sigma)\prod_{i=1}^n m_{i,\sigma(i)}1

Thus the hook cases immediately adjacent to these extremes are d2(M)=σSnχ2(σ)i=1nmi,σ(i)d_2(M)=\sum_{\sigma\in S_n}\chi_2(\sigma)\prod_{i=1}^n m_{i,\sigma(i)}2 and d2(M)=σSnχ2(σ)i=1nmi,σ(i)d_2(M)=\sum_{\sigma\in S_n}\chi_2(\sigma)\prod_{i=1}^n m_{i,\sigma(i)}3, which are transposes of each other: d2(M)=σSnχ2(σ)i=1nmi,σ(i)d_2(M)=\sum_{\sigma\in S_n}\chi_2(\sigma)\prod_{i=1}^n m_{i,\sigma(i)}4 This transpose relation is frequently the source of the competing “second” conventions (Curticapean, 2021).

For the determinant-side hook d2(M)=σSnχ2(σ)i=1nmi,σ(i)d_2(M)=\sum_{\sigma\in S_n}\chi_2(\sigma)\prod_{i=1}^n m_{i,\sigma(i)}5, a particularly useful explicit formula is

d2(M)=σSnχ2(σ)i=1nmi,σ(i)d_2(M)=\sum_{\sigma\in S_n}\chi_2(\sigma)\prod_{i=1}^n m_{i,\sigma(i)}6

hence

d2(M)=σSnχ2(σ)i=1nmi,σ(i)d_2(M)=\sum_{\sigma\in S_n}\chi_2(\sigma)\prod_{i=1}^n m_{i,\sigma(i)}7

This gives the second immanant, in the d2(M)=σSnχ2(σ)i=1nmi,σ(i)d_2(M)=\sum_{\sigma\in S_n}\chi_2(\sigma)\prod_{i=1}^n m_{i,\sigma(i)}8 convention, as a sign-weighted deformation of the determinant by a fixed-point factor (Curticapean, 2021).

For the permanent-side hook d2(M)=σSnχ2(σ)i=1nmi,σ(i)d_2(M)=\sum_{\sigma\in S_n}\chi_2(\sigma)\prod_{i=1}^n m_{i,\sigma(i)}9, the corresponding character is

d2(xIM)d_2(xI-M)0

In that convention the immanant is

d2(xIM)d_2(xI-M)1

so the sign factor disappears and the weighting is governed directly by fixed points (Zhang, 8 Apr 2026).

3. Laplacian second immanantal polynomials of trees

For a tree d2(xIM)d_2(xI-M)2 on d2(xIM)d_2(xI-M)3 vertices with Laplacian matrix d2(xIM)d_2(xI-M)4, the Laplacian immanantal polynomial is

d2(xIM)d_2(xI-M)5

The d2(xIM)d_2(xI-M)6-Laplacian is

d2(xIM)d_2(xI-M)7

with d2(xIM)d_2(xI-M)8 when d2(xIM)d_2(xI-M)9, and the corresponding (n1,1)(n-1,1)0-Laplacian immanantal polynomial is

(n1,1)(n-1,1)1

In this setting, the phrase “second immanantal polynomial” is used explicitly for the partition

(n1,1)(n-1,1)2

following Merris’s usage (Nagar et al., 2017).

A central theorem states that if (n1,1)(n-1,1)3 covers (n1,1)(n-1,1)4 in the generalized tree shift poset (n1,1)(n-1,1)5, then for every partition (n1,1)(n-1,1)6 and every (n1,1)(n-1,1)7,

(n1,1)(n-1,1)8

At (n1,1)(n-1,1)9, this yields coefficientwise monotonicity for ordinary Laplacian immanantal polynomials. Specializing to immλ\mathrm{imm}_\lambda0 shows that every coefficient of the second Laplacian immanantal polynomial decreases as one moves upward in immλ\mathrm{imm}_\lambda1 (Nagar et al., 2017).

The second case is distinguished by an especially simple coefficient formula. If immλ\mathrm{imm}_\lambda2 denotes the orientation statistic built from immλ\mathrm{imm}_\lambda3-vertex orientations, then

immλ\mathrm{imm}_\lambda4

For immλ\mathrm{imm}_\lambda5, the coefficient acquires a moment interpretation: immλ\mathrm{imm}_\lambda6 At immλ\mathrm{imm}_\lambda7, this recovers Merris’s theorem relating the second Laplacian immanantal polynomial to the sum of vertex moments and, consequently, to centroid-type structure (Nagar et al., 2017).

4. Coefficients for graph linear-combination matrices

A broad recent framework studies immanantal polynomials of

immλ\mathrm{imm}_\lambda8

where immλ\mathrm{imm}_\lambda9 is the degree matrix and λn\lambda\vdash n0 the adjacency matrix of a graph λn\lambda\vdash n1. For hook partitions λn\lambda\vdash n2, the hook immanantal polynomial is

λn\lambda\vdash n3

Within this family, λn\lambda\vdash n4 is explicitly identified as the second immanant polynomial, while λn\lambda\vdash n5 is the characteristic polynomial and λn\lambda\vdash n6 the permanental polynomial (Dong et al., 25 Aug 2025).

For the second immanantal polynomial of the linear-combination matrix λn\lambda\vdash n7,

λn\lambda\vdash n8

the first coefficients are

λn\lambda\vdash n9

λn\lambda\vdash n0

and

λn\lambda\vdash n1

For the Laplacian specialization λn\lambda\vdash n2, these become

λn\lambda\vdash n3

λn\lambda\vdash n4

λn\lambda\vdash n5

and

λn\lambda\vdash n6

These formulas place the second immanantal polynomial in direct contact with degree symmetric sums, matching statistics, and cycle counts (Dong et al., 6 Apr 2026).

The same framework yields structural equalities and recursions. In particular, for bipartite graphs,

λn\lambda\vdash n7

where λn\lambda\vdash n8 is the signless Laplacian. More generally, the λn\lambda\vdash n9 specialization of the hook recursions expresses n×nn\times n0 in terms of deleted vertices, deleted edges, and, for graphs with cycles, deleted cycle-vertex sets; for trees the cycle terms vanish, leaving especially tractable recurrences (Dong et al., 25 Aug 2025).

5. Complexity-theoretic interpretation and the importance of convention

The complexity of “the” second immanantal polynomial depends decisively on which hook partition is meant. For a partition n×nn\times n1, let

n×nn\times n2

the number of boxes to the right of the first column of the Young diagram. For a family n×nn\times n3, define n×nn\times n4, and let n×nn\times n5 denote the problem of evaluating n×nn\times n6 on input n×nn\times n7 and n×nn\times n8 (Curticapean, 2021).

If one interprets the second immanant as the determinant-side hook n×nn\times n9, then A=(aij)A=(a_{ij})0 and

A=(aij)A=(a_{ij})1

For the family A=(aij)A=(a_{ij})2, one has A=(aij)A=(a_{ij})3, so

A=(aij)A=(a_{ij})4

In this interpretation, the second immanant lies on the polynomial-time side of the dichotomy (Curticapean, 2021).

If instead one interprets the second immanant as the permanent-side hook A=(aij)A=(a_{ij})5, then A=(aij)A=(a_{ij})6 and

A=(aij)A=(a_{ij})7

For the family A=(aij)A=(a_{ij})8, A=(aij)A=(a_{ij})9, indeed linearly growing. The dichotomy then yields much stronger hardness: this family is (2,1n2)(2,1^{n-2})00-hard and (2,1n2)(2,1^{n-2})01-complete, and it admits no (2,1n2)(2,1^{n-2})02-time algorithm unless (2,1n2)(2,1^{n-2})03 fails (Curticapean, 2021).

The complexity paper itself does not use the phrase “second immanantal polynomial”; the specialization to either hook is an inference from partition indexing. That inference, however, is exact enough to show that the terminology is computationally nontrivial: one natural “second” hook is easy, the other is hard (Curticapean, 2021).

6. Reconstruction, inequalities, and later generalizations

In reconstruction theory, the second immanantal polynomial in the (2,1n2)(2,1^{n-2})04 convention satisfies deletion identities analogous to those known for characteristic and permanental polynomials. For a simple graph (2,1n2)(2,1^{n-2})05 with

(2,1n2)(2,1^{n-2})06

one has

(2,1n2)(2,1^{n-2})07

Hence, when (2,1n2)(2,1^{n-2})08, (2,1n2)(2,1^{n-2})09 can be reconstructed from the second immanantal polynomials of the graphs in

(2,1n2)(2,1^{n-2})10

For a digraph (2,1n2)(2,1^{n-2})11, the analogous identity is

(2,1n2)(2,1^{n-2})12

which yields reconstruction of

(2,1n2)(2,1^{n-2})13

from the deleted-edge deck whenever (2,1n2)(2,1^{n-2})14 (Wu et al., 18 Feb 2025).

Under the alternate (2,1n2)(2,1^{n-2})15 convention, a different line of work studies normalized hook immanants on totally nonnegative matrices. There the principal theorem gives the hook chain

(2,1n2)(2,1^{n-2})16

for every totally nonnegative matrix (2,1n2)(2,1^{n-2})17. Since (2,1n2)(2,1^{n-2})18, the normalized (2,1n2)(2,1^{n-2})19-immanant lies immediately below the permanent and above the later hook immanants, and the difference

(2,1n2)(2,1^{n-2})20

is itself totally nonnegative (Skandera, 30 Sep 2025).

Several recent generalizations move beyond the classical symmetric-function setting. Quasi-immanants replace cycle type by cycle composition and symmetric functions by quasisymmetric functions. The quasi-immanant attached to the quasisymmetric Schur function (2,1n2)(2,1^{n-2})21 is presented as an analogue of the second immanant rather than as the classical second immanant itself; its coefficients depend on the first part of (2,1n2)(2,1^{n-2})22 and vanish when (2,1n2)(2,1^{n-2})23 (Campbell, 26 Jan 2025). In another direction, Newton-polytope work treats (2,1n2)(2,1^{n-2})24 as the relevant second immanant: for Jacobi–Trudi matrices (2,1n2)(2,1^{n-2})25 is SNP when (2,1n2)(2,1^{n-2})26 is a border strip, and for Giambelli matrices (2,1n2)(2,1^{n-2})27 is SNP for every (2,1n2)(2,1^{n-2})28, hence in particular for (2,1n2)(2,1^{n-2})29 (Zhang, 8 Apr 2026).

The cumulative picture is therefore bifurcated but coherent. In graph-theoretic and Laplacian applications, the second immanantal polynomial is usually (2,1n2)(2,1^{n-2})30; in some hook-chain, representation-theoretic, and Newton-polytope settings, the label shifts to (2,1n2)(2,1^{n-2})31. The two conventions are linked by conjugation of partitions, yet they lead to different explicit formulas, different monotonicity and positivity statements, and, in families, different computational complexity classes.

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