Real Nonnegative Inverse Eigenvalue Problem
Investigating real spectra realizable by general nonnegative matrices ($A \ge 0$, $\sigma \subset \mathbb{R}$), non-orthogonal eigenvector geometries, and the symmetry gap.
1. Definition & Eigenvector Degrees of Freedom
Relaxing the symmetry constraint provides significant geometric flexibility.
The Real Nonnegative Inverse Eigenvalue Problem (RNIEP) asks: given a multiset of $n$ real numbers $\sigma = \{\lambda_1, \lambda_2, \dots, \lambda_n\} \subset \mathbb{R}$, does there exist an entrywise nonnegative matrix $A \ge 0$ (not necessarily symmetric) whose spectrum equals $\sigma$?
Definition: The RNIEP
Formal StatementFind an $n \times n$ matrix $A = (a_{ij}) \in \mathbb{R}^{n \times n}$ such that:
Unlike the Symmetric NIEP (SNIEP), where $A = Q \Lambda Q^T$ is always orthogonally diagonalizable, a general real nonnegative realization need not even be diagonalizable—as shown already at order two by $\bigl(\begin{smallmatrix}1 & 1 \\ 0 & 1\end{smallmatrix}\bigr)$. In general, $A$ admits a Jordan decomposition over $\mathbb{C}$ (or real Jordan form):
Both non-orthogonal eigenbases and nontrivial Jordan blocks enlarge the feasible spectral region: an orthogonal matrix $Q \in O(n)$ possesses only $n(n-1)/2$ angular parameters, whereas a general similarity $X \in \mathrm{GL}(n, \mathbb{R})$ has $n^2$ entries, allowing eigenspaces and generalized eigenspaces to tilt relative to the nonnegative orthant.
2. Necessary Invariants for RNIEP
Trace nonnegativity, Newton inequalities, and moment constraints.
Real Spectrum
All candidate eigenvalues are required to be real.
Perron Root
Perron-Frobenius theorem guarantees the maximal root is positive.
Power Sum Traces
Because $A \ge 0$, all powers $A^k \ge 0$, so their traces must be nonnegative.
JLL Inequalities
Johnson–Loewy–London (1978/1979) Hölder trace bounds on diagonal moments.
For real spectra $\sigma \subset \mathbb{R}$, all even power sums $s_{2k} = \sum \lambda_i^{2k} \ge 0$ hold automatically, while odd trace bounds $s_{2k-1} \ge 0$ and the Johnson–Loewy–London (JLL) inequalities $s_k^m \le n^{m-1} s_{km}$ (such as $s_1^2 \le n s_2$ and $s_1^3 \le n^2 s_3$) impose nontrivial constraints on negative eigenvalues.
3. The Advantage of Non-Symmetry: $\operatorname{RNIEP} \supsetneq \operatorname{SNIEP}$
Why non-symmetric realizations can achieve what symmetric realizations cannot.
A major historic milestone in combinatorial matrix theory was establishing whether symmetry is a restrictive requirement for real spectra. For dimensions $n \le 4$, symmetry is non-restrictive:
In 1996, Charles R. Johnson, Thomas J. Laffey, and Raphael Loewy proved that the symmetric and real problems are genuinely different (first constructed at $n = 6$), and subsequent work by Eleanor Meehan (1998), Laffey & Meehan (1999), and Hartwig & Loewy established strict containment for every order $n \ge 5$:
Explicit Order-5 Separating Spectrum
Hartwig–Loewy · Laffey–Meehan (1999)Consider the classical trace-zero family $\sigma(t) = \{3+t, 3-t, -2, -2, -2\}$. Evaluating at $t = \tfrac{1}{2}$ and scaling by $2$ to clear fractions gives the integer list:
Its power sums are $s_1 = 0$, $s_2 = 122$, $s_3 = 276$, $s_4 = 3794$, and $s_5 = 16860$ (satisfying $4s_4 - s_2^2 = 292 > 0$), and it is realized by the explicit zero-diagonal nonnegative integer matrix:
Indeed, $\det(xI - A) = x^5 - 61x^3 - 92x^2 + 912x + 2240 = (x - 7)(x - 5)(x + 4)^3$. Yet no symmetric $5 \times 5$ nonnegative matrix can have spectrum $\sigma$: every trace-zero symmetric nonnegative $5 \times 5$ matrix with ordered eigenvalues $\lambda_1 \ge \dots \ge \lambda_5$ satisfies $\lambda_2 + \lambda_5 \le 0$ (so $\sigma(t) \in \operatorname{SNIEP}(5) \iff t \ge 1$), whereas here $\lambda_2 + \lambda_5 = 5 + (-4) = 1 > 0$. Moreover, $A$ carries a $3 \times 3$ Jordan block at $-4$ (Cronin & Laffey 2018 showed $\sigma(t)$ for $t < 1$ requires non-diagonalizability), while distinct-integer examples such as $\{12, 9, -6, -7, -8\}$ also violate $\lambda_2 + \lambda_5 \le 0$ and separate diagonalizable $\operatorname{RNIEP}(5)$ from $\operatorname{SNIEP}(5)$.
4. Dimension Solvability & The Laffey-Meehan Frontier
Trace conditions suffice for $n \le 4$, but fail definitively at order 5.
Trace & Dominance Criteria
Solved for real spectra by Loewy & London (1978): a real $n$-tuple ($n \le 4$) is realizable if and only if Perron dominance $\lambda_1 \ge |\lambda_i|$ and $s_1 = \sum \lambda_i \ge 0$ hold (general complex $n=4$ solved by Meehan 1998 and Torre-Mayo et al. 2007).
Trace Insufficiency
Laffey and Meehan studied $\{3+t, 3-t, -2, -2, -2\}$: for $0 \le t < \sqrt{16\sqrt{6}-39} \approx 0.438$ (such as $t = 0$), all power-sum and JLL inequalities hold, yet $4s_4 < s_2^2$ rules out any $5 \times 5$ nonnegative realization.
Higher Dimensions
Requires higher-order semi-algebraic polynomial inequalities. Constructive algorithms remain an active field of research.
5. Real Algebraic Geometry & Trace Polytopes
Semi-algebraic solvability and interactive geometric visualizations.
Semi-Algebraic Solvability (Clark, 2024)
Real Algebraic GeometryIn 2024, Benjamin J. Clark demonstrated that the RNIEP forms a semi-algebraic set. By the Tarski-Seidenberg projection theorem, the set of realizable real spectra $\operatorname{RNIEP}(n) \subset \mathbb{R}^n$ can be defined by a finite Boolean combination of polynomial equalities and inequalities:
This confirms that the RNIEP is solvable by finitely many algebraic conditions, shifting modern research toward identifying minimal defining systems.
Interactive Trace Polytope Gallery
Compare order-5 RNIEP vs. SNIEP trace polytopes in real-time 2D and 3D WebGL, inspecting how non-symmetric realizability extends beyond the symmetric boundary.
6. Primary Literature & Citations
Foundational papers from the NIEP Comprehensive Bibliography7. See Also & Related Articles
Symmetric NIEP (SNIEP)
Orthogonal eigenspaces, Fiedler theorems, Soules bases, and trace polytopes.
Suleimanova Spectra
Spectra with a single positive eigenvalue, trace sufficiency, and constructive companion/Fiedler realizations.
Karpelevič Region
Kolmogorov's problem, stochastic eigenvalue boundaries, Farey vertices, and algebraic arcs.
NIEP Overview
The master theoretical survey covering complex spectra, Perron-Frobenius theory, and semi-algebraic sets.