Generalized Locally Toeplitz (GLT) *-Algebras

• GLT *-algebras are defined as maximal *-algebras of matrix-sequences with unique measurable symbols that govern asymptotic spectral and singular value distributions.
• They unify classical Toeplitz matrices with variable-coefficient, block, and quasi-Hermitian extensions, providing a comprehensive algebraic toolkit for matrix analysis.
• The framework supports practical applications in numerical discretizations, preconditioning, and quantum many-body modeling through robust symbol calculus and closure properties.

Generalized Locally Toeplitz (GLT) $*$-algebras comprise the maximal $*$-algebraic structure of matrix-sequences that simultaneously encode the collective asymptotic spectral and singular-value distributions of highly structured matrices. Every GLT matrix-sequence admits a unique measurable GLT symbol, determining its asymptotic behavior under a variety of algebraic, analytic, and topological operations. The GLT framework unifies classical Toeplitz, block Toeplitz, variable-coefficient, and locally stationary discretization schemes, and it encompasses both commutative and noncommutative, multilevel, block, and quasi-Hermitian extensions. The theory provides a robust toolkit for modern matrix analysis, especially for the paper of discretizations of differential and integral operators, preconditioning, and quantum many-body models.

1. Foundation and Definition of the GLT $*$-algebra

The core object of paper is a class of matrix-sequences $\{A_n\}_n$, $A_n \in \mathbb{C}^{d_n\times d_n}$, equipped with a distributional limit called the GLT symbol. In the unilevel scalar setting, the GLT algebra is the smallest $*$-algebra of matrix-sequences, closed in the approximating-classes-of-sequences (a.c.s.) topology, containing three generating classes:

• Zero-distributed sequences $\{Z_n\}$, for which $\{Z_n\}\sim_\sigma 0$,
• Toeplitz sequences $\{T_n(f)\}$ generated by $f\in L^1([-\pi,\pi])$,
• Diagonal sampling sequences $\{D_n(a)\}$ for Riemann-integrable $a:[0,1]\to\mathbb{C}$ (Ven et al., 9 Apr 2025, Khan, 9 Nov 2025, Barbarino, 2017).

A GLT symbol is a measurable function $\kappa:D\to\mathbb{C}^{r\times r}$ ($D=[0,1]^d\times[-\pi,\pi]^d$), unique almost everywhere, governing the limiting singular/eigenvalue distribution of the sequence. The quotient algebra of matrix-sequences modulo zero-distributed elements is a $C^*$-algebra isometrically $*$-isomorphic to the algebra of measurable functions $(L^1(D),+,\cdot,*)$ (Barbarino, 2017).

2. Axiomatic Structure and Symbol Calculus

The GLT $*$-algebra satisfies a precise set of axioms, which in the scalar, unilevel case are:

1. Distribution: $$\{A_n\}\sim_{\mathrm{GLT}}\kappa \implies \{A_n\}\sim_\sigma \kappa$$ on $[0,1]\times [-\pi,\pi]$; if $A_n$ are Hermitian, also $\sim_\lambda\kappa$.
2. Generators: Toeplitz, diagonal sampling, and zero-distributed sequences correspond to $f(\theta)$, $a(x)$, and $0$, respectively.
3. Algebraic operations: $*$ (adjoint), addition, multiplication, and inversion (where the symbol is nonzero a.e.) pass to the symbol:

$$\{A_n^*\}\sim_{\mathrm{GLT}}\kappa^*,\quad \{\alpha A_n+\beta B_n\}\sim_{\mathrm{GLT}}\alpha\kappa+\beta\varsigma,\quad \{A_nB_n\}\sim_{\mathrm{GLT}}\kappa\,\varsigma,\quad \{A_n^{-1}\}\sim_{\mathrm{GLT}}\kappa^{-1}$$

1. Closure under a.c.s.: GLT sequences are limits (in a.c.s.) of finite algebraic combinations of generators, with symbols converging in measure.
2. Quasi-Hermitian spectral theorem: If $\{A_n\}\sim_{\mathrm{GLT}}\kappa$, $A_n = X_n + Y_n$ with $X_n$ Hermitian, $\|X_n\|, \|Y_n\|\le C$, and $\|Y_n\|_1/n\to0$, then $\{A_n\}\sim_\lambda\kappa$.
3. Functional calculus: If $\{A_n\}\sim_{\mathrm{GLT}}\kappa$, all $A_n$ Hermitian, then for any continuous $f$, $\{f(A_n)\}\sim_{\mathrm{GLT}}f(\kappa)$ (Ven et al., 9 Apr 2025, Barakitis et al., 30 Jun 2024, Khan, 9 Nov 2025).

In the multilevel, block case, these axioms generalize immediately for $d$-level, $r$-block GLT sequences, with the measurable matrix-valued symbol $$\kappa:[0,1]^d\times[-\pi,\pi]^d\rightarrow\mathbb{C}^{r\times r}$$ (Serra-Capizzano, 23 Sep 2025).

3. Asymptotic Distribution of Spectra and Singular Values

A sequence $\{A_n\}_n$ has:

• Asymptotic singular-value distribution $\psi$: For every $F\in C_c(\mathbb{R})$,

$$\lim_{n\to\infty}\frac{1}{d_n}\sum_{i=1}^{d_n}F(\sigma_i(A_n)) = \frac{1}{|D|}\int_D F(|\psi(\bm{x})|)\,d\bm{x}$$

• Asymptotic eigenvalue distribution $\psi$ (Hermitian/quasi-Hermitian case): For $F\in C_c(\mathbb{C})$,

$$\lim_{n\to\infty}\frac{1}{d_n}\sum_{i=1}^{d_n}F(\lambda_i(A_n)) = \frac{1}{|D|}\int_D F(\psi(\bm{x}))\,d\bm{x}$$

If $\{A_n\}\sim_{\mathrm{GLT}}\kappa$, these relations hold with $\psi = \kappa$ (Ven et al., 9 Apr 2025, Serra-Capizzano, 23 Sep 2025). For block symbols, eigenvalues of the symbol replace scalar values in the integration. The symbol calculus ensures that under $*$-operations, the limiting distributions are governed by the corresponding operation on the symbol (Serra-Capizzano, 23 Sep 2025).

For quasi-Hermitian sequences, a bounded perturbation in trace norm does not alter the eigenvalue distribution (Ven et al., 9 Apr 2025, Khan, 9 Nov 2025).

4. Symbol Map, Uniqueness, and Algebraic Isomorphism

The GLT symbol map

$$S: \mathcal{G}_{d,r} \to L^1([0,1]^d \times [-\pi,\pi]^d; \mathbb{C}^{r \times r}), \qquad S(\{A_n\}) = \kappa,\; \text{where}\;\{A_n\}\sim_{\mathrm{GLT}}\kappa$$

is a $*$-algebra homomorphism, and is one-to-one up to almost everywhere equivalence of $\kappa$. The kernel consists of all zero-distributed sequences.

Upon quotienting by zero-distributed elements, the GLT $*$-algebra is isomorphic to the algebra of measurable functions, with the isometry

$$d_{\mathrm{acs}}(\{A_n\},\{B_n\}) = d_m(\kappa,h) \quad\text{whenever}\; \{A_n\}\sim_{\mathrm{GLT}}\kappa, \;\{B_n\}\sim_{\mathrm{GLT}}h$$

where $d_{\mathrm{acs}}$ is the a.c.s.-induced pseudometric, and $d_m$ is the $L^1$ (measure) metric (Barbarino, 2017, Serra-Capizzano, 23 Sep 2025).

5. Construction and Classification of GLT Sequences

A concrete matrix sequence is GLT if it can be written (up to a zero-distributed remainder) as a finite sum/product of Toeplitz matrices $T_n(e^{ik\theta})$, diagonal samplings $D_n(\alpha)$, and zero-distributed terms (Barakitis et al., 30 Jun 2024, Khan, 9 Nov 2025). The symbol is constructed algebraically from the generating symbols, mirroring the explicit algebraic form of the sequence:

• $T_n(f)$ yields $f(\theta)$,
• $D_n(a)$ yields $a(x)$,
• finite algebraic combinations yield the corresponding function combinations.

The a.c.s. topology enables sophisticated limiting constructions, critical for sequences arising from variable-coefficient, nonuniform-grid, and even momentary symbol (higher-order) expansions (Barakitis et al., 30 Jun 2024).

GLT theory is maximally closed under $*$-algebra operations; no larger $*$-algebra preserving the distributional calculus exists (Khan, 9 Nov 2025).

6. Applications: Numerical Analysis, Physics, and Beyond

GLT $*$-algebras provide the structural backbone for the spectral analysis of:

• Discretizations of variable-coefficient elliptic, integral, and fractional operators,
• Multilevel and block Toeplitz matrix-sequences,
• Variable-step BDF (backward differentiation formula) matrix-sequences (Barakitis et al., 30 Jun 2024),
• Discretizations on nonuniform meshes and manifolds via reduced GLT algebras,
• Mean-field quantum spin Hamiltonians, e.g., Curie–Weiss models. For instance, the restricted Curie–Weiss Hamiltonian leads to the explicit symbol

$$h_0(x,\theta) = -\frac\Gamma2(2x - 1)^2 - 2B\sqrt{x(1-x)}\,\cos\theta$$

and the eigenvalue distribution of its normalizations converges accordingly (Ven et al., 9 Apr 2025, Khan, 9 Nov 2025).

GLT methods are intrinsic to advanced preconditioning theory, outlier-clustering analysis, and quantification of symmetry-breaking in differential and quantum spin models.

7. Generalizations, Open Problems, and Research Directions

Recent research focuses on:

• Momentary and higher-order GLT symbols to capture refined spectral features not covered by leading-order (e.g., zero-distributed) analysis (Ven et al., 9 Apr 2025, Barakitis et al., 30 Jun 2024),
• Multilevel and block-reduced GLT algebras for exploiting symmetry and geometric features, including discretizations on spheres and manifolds,
• Generalization to random matrices and stochastic-discretization schemes,
• Tensor-valued or noncommutative generating symbols (e.g., quaternionic GLT),
• Algorithmic and machine-learning approaches for automatic symbol computation and data-driven spectral clustering,
• Maximality conjecture: determining whether all maximal $*$-algebras of matrix-sequences of a given block size are GLT (up to similarity),
• Bridging discrete and continuous spectral theory, making links explicit with Weyl/Szegő laws in the functional-analytic setting of (pseudo)differential operators (Serra-Capizzano, 23 Sep 2025, Ven et al., 9 Apr 2025).

Key open problems include analytic derivations for the rates of spectral extremal clustering, full characterization of degenerate symbol phenomena, and the development of symbolic-computation frameworks for high-level matrix discretizations. The theory's thorough integration of algebraic, topological, and analytic aspects continues to drive advances in numerical linear algebra, operator theory, and mathematical physics.