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Complete Evolution Algebras Overview

Updated 16 December 2025
  • Complete evolution algebras are commutative, non-associative algebras defined by natural bases that satisfy eₖeₗ = 0 for k ≠ l, modeling hereditary dynamics.
  • They employ a nonlinear polynomial system and structure matrix analysis to detect one-dimensional subalgebras and resolve key classification conjectures.
  • Their rigorous decomposition into fundamental types provides actionable insights on idempotents, solvability, and applications in mathematical genetics.

A complete evolution algebra is a special class of commutative, generally non-associative, algebras introduced to capture specific structural and hereditary extension properties with respect to natural bases and subalgebras. This concept is central in the algebraic study of systems with discrete, independently evolving components, notably in mathematical genetics and related dynamical frameworks. The modern understanding of complete evolution algebras draws from rigorous algebraic geometry and systemic classification efforts, culminating in their exhaustive characterisation and the resolution of key conjectures about their structure.

1. Foundational Definitions and Characterisation

Let $\K$ be a field and EE a commutative, possibly non-associative, $\K$-algebra. An evolution algebra is defined by the existence of a distinguished basis

B={e1,,en}B = \{ e_1,\ldots,e_n \}

(called a natural basis) such that

eiej=0for all ij.e_i e_j = 0 \quad \text{for all}\ i\ne j.

Each basis vector satisfies

$e_i^2 = \sum_{j=1}^n a_{ij}e_j,\quad a_{ij}\in\K,$

and the matrix MB(E)=(aij)1i,jnM_B(E) = (a_{ij})_{1\le i,j\le n} is termed the structure matrix. A subalgebra FEF\subseteq E is said to admit a natural basis if some subset of BB spans FF, and admits a natural basis that extends to one of EE if this subset extends to a full natural basis of EE. The algebra EE is complete if every subalgebra of EE admits a natural basis which extends to a natural basis of EE (García-Martínez et al., 13 Dec 2025).

2. Obstructions and a Polynomial System

Completeness of a regular evolution algebra (i.e., E=E2E=E^2 and $A=M_B(E)\in\GL_n(\K)$) is governed by the existence of one-dimensional subalgebras which do not extend to a natural basis. For u=x1e1++xnenu = x_1e_1+\cdots+x_ne_n, the requirement that uu spans a subalgebra translates algebraically to u2=λuu^2 = \lambda u for some $\lambda\in\K$. Explicitly,

u2=i=1nxi2ei2=i=1nxi2j=1naijej,u^2 = \sum_{i=1}^n x_i^2 e_i^2 = \sum_{i=1}^n x_i^2\sum_{j=1}^n a_{ij}e_j,

reduces (up to scaling) to the nonlinear polynomial system

(x12 x22  xn2)=A(x1 x2  xn).\begin{pmatrix} x_1^2 \ x_2^2 \ \vdots \ x_n^2 \end{pmatrix} = A \begin{pmatrix} x_1 \ x_2 \ \vdots \ x_n \end{pmatrix}.

The existence of a solution $(x_1,\ldots,x_n)\in\K^n$ with all xi0x_i\ne0 identifies a one-dimensional subalgebra not contained in a natural basis extension, certifying incompleteness (García-Martínez et al., 13 Dec 2025).

3. Structure Theorems and Resolution of CKO Conjectures

The classification of complete evolution algebras was consolidated by García-Martínez and Pérez-Rodríguez through analysis of the polynomial system delineated above. Two conjectures of Camacho, Khudoyberdiyev, and Omirov (2019) are resolved as follows:

  • Conjecture 5.2: Every regular, complex evolution algebra of dimension >1>1 is not complete. This follows because the system above always admits a solution with at least two nonzero coordinates when $A\in\GL_n(\C)$ and n>1n>1. This solution corresponds to a one-dimensional subalgebra that cannot be extended to a natural basis, obstructing completeness.
  • Conjecture 5.3: The only non-nilpotent, complete nn-dimensional evolution algebras over $\C$ are isomorphic to either

$\{e_1^2 = e_1\} \oplus \C^{n-1}$

or

$\{e_1^2 = e_1\} \oplus \widetilde E \oplus \C^{n-s-1},$

where E~\widetilde E is an ss-dimensional evolution algebra of maximal nilpotency index and $\C^k$ denotes the kk-dimensional zero algebra. This characterisation hinges on the algebraic-geometric arguments showing that the existence of a nontrivial solution with two or more nonzero coordinates is generic (García-Martínez et al., 13 Dec 2025).

The general classification, including nilpotent cases, is thus:

$\{e_1^2 = e_1\},\quad \widetilde E \oplus \C^{n-s},\quad \{e_1^2 = e_1\} \oplus \C^{n-1},\quad \{e_1^2 = e_1\} \oplus \widetilde E \oplus \C^{n-s-1}$

where E~\widetilde E has maximal nilpotency index.

4. Subalgebras, Extension, and Decomposition

Subalgebras of a complete evolution algebra inherit completeness if and only if they are direct sums of complete coordinate subalgebras. For a complete evolution algebra EE with unique decomposition

$E \cong \left(\{e_1^2 = e_1\}\right)^{\epsilon_1} \oplus \widetilde E^{\epsilon_2} \oplus \C^{\epsilon_3},\quad \epsilon_i\in\{0,1\},$

any subalgebra FEF\subseteq E is complete if and only if F=F1F2F3F = F_1\oplus F_2\oplus F_3, with each FiF_i equal to either $0$ or the full corresponding summand. Consequently, every subalgebra of a complete evolution algebra decomposes as a direct sum of coordinate subalgebras of the four fundamental types (García-Martínez et al., 13 Dec 2025).

5. Idempotents and Regularity

An element uEu\in E is an idempotent (u2=uu^2 = u) if and only if for u=xieiu = \sum x_i e_i, the equation

At(x12  xn2)=(x1  xn)A^t \begin{pmatrix} x_1^2 \ \vdots \ x_n^2 \end{pmatrix} = \begin{pmatrix} x_1 \ \vdots \ x_n \end{pmatrix}

is satisfied. In the regular case ($A\in\GL_n$), this coincides structurally with the system characterising one-dimensional subalgebras. Hence, every finite-dimensional regular complex evolution algebra admits a nonzero idempotent, establishing that no such algebra of dimension >1>1 can be idempotent-free (García-Martínez et al., 13 Dec 2025).

6. Solvable Evolution Algebras: Conjectural Characterisation

An evolution algebra EE is solvable if its derived series

E(1)=E,E(k+1)=E(k)E(k),N: E(N)=0E^{(1)}=E,\quad E^{(k+1)}=E^{(k)}E^{(k)},\quad \exists N:\ E^{(N)}=0

eventually vanishes. A necessary condition for solvability is the absence of nonzero idempotents, since any idempotent persists through all derived products. The authors propose the converse:

  • For a finite-dimensional complex evolution algebra EE, the following are equivalent:

    1. EE is solvable.
    2. EE admits no nonzero idempotents.
    3. The equation for idempotents

    At(x12  xn2)=(x1  xn)A^t \begin{pmatrix} x_1^2 \ \vdots \ x_n^2 \end{pmatrix} = \begin{pmatrix} x_1 \ \vdots \ x_n \end{pmatrix}

    has only the trivial solution (0,,0)(0,\ldots,0).

Verification holds in dimension $1$ trivially and in dimension $2$ follows from explicit classification. Should this conjecture be validated, it would represent the first purely algebraic or polynomial-equation criterion for solvability in complex evolution algebras (García-Martínez et al., 13 Dec 2025).

7. Classification in Low Dimensions

For real (i.e., $\K = \R$), two-dimensional evolution algebras, full classification up to isomorphism is achieved with seven distinct types. Structure constants, automorphism groups, and derivation algebras are catalogued explicitly (Bekbaev, 2017). The tabulation below summarizes the nontrivial two-dimensional real evolution algebras and key invariants.

Algebra Family Multiplicative Structure Automorphism Group
E1(b,c) (bc1)E_1(b,c)\ (bc\ne1) e12=e1+be2e_1^2 = e_1 + b e_2, e22=ce1+e2e_2^2 = c e_1 + e_2 {I}\{I\}; {I,P}\{I, P\} if b=cb=c
E2(b)E_2(b) e12=e1+be2e_1^2 = e_1 + b e_2, e22=e2e_2^2 = e_2 {I}\{I\} or matrices if b=0b=0
E3E_3 e12=e1e2e_1^2 = e_1 - e_2, e22=e1+e2e_2^2 = e_1 + e_2 {I}\{I\}
E4E_4 e12=e1e_1^2 = e_1, e22=0e_2^2 = 0 diag(1,t)\operatorname{diag}(1, t)
E5E_5 e12=e1e2e_1^2 = e_1 - e_2, e22=e1e_2^2 = -e_1 {I}\{I\}
E6E_6 e12=e2e_1^2 = e_2, e22=0e_2^2 = 0 Parametrized family (see above)
E7E_7 e12=0e_1^2 = 0, e22=e1e_2^2 = e_1 Parametrized family (see above)

No two families are isomorphic, and the exhaustive listing affirms the diversity of possible local structures (Bekbaev, 2017).


The theoretical landscape of complete evolution algebras is now sharply delimited: their existence is severely constrained under regularity (invertibility of the structure matrix), and their structure is rigidly specified by a handful of explicit types. This structural rigidity underpins current understanding and further highlights the role of properly formulated algebraic and geometric criteria in classifying and analysing hereditary algebraic systems.

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