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arXiv:2610.41608

Quantum Bernstein--Kolmogorov--Arnold approximation

Sviatoslav V. Dzhenzher

quant-phmath.FASubmitted Oct 30, 2026• Announced Nov 2, 2026
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Abstract

This paper addresses the expressivity and representation gap in Quantum Neural Networks by establishing a quantum analogue of the classical Kolmogorov--Arnold representation theorem. We propose a constructive approximation framework over fixed input coherent states, where the dependence of the function argument is embedded entirely in coordinate qubits, while the target function dictates a single outer unitary evolution. By applying a Sprecher-type representation to the rotation angle of the state, we demonstrate that the multidimensional operator factorises into \(2d+1\) commuting universal inner observables. We prove that the resulting measurement probability precisely reproduces the multidimensional Bernstein polynomial of the target function. For any continuous multivariate function, the joint quantum state converges uniformly to the target output register, linking classical superposition theory with probabilistic and coherent quantum circuits.

AI Summary

The paper asks whether function approximation from copies of coordinate-encoded qubits admits a Kolmogorov–Arnold representation with target-independent inner observables. Its input is $n$ copies of each of $d$ coordinate states, with all dependence on $x\in[0,1]^d$ confined to those states; the subsequent unitary depends on the target $f:[0,1]^d\to[0,1]$ and $n$, but not on $x$. For $d>1$, it constructs $2d+1$ commuting Hermitian observables $H_q^{(n)}$ and a single target-dependent scalar function $g$, independent of $n$, such that $U_n=\prod_{q=0}^{2d}\exp[-i g(H_q^{(n)})\otimes Y]$ produces an ancilla measurement probability exactly equal to the multivariate Bernstein polynomial $B_nf(x)$. When $f$ is continuous, $g$ can be chosen continuous, and the full output converges uniformly in norm to the original input tensored with $\sqrt{1-f(x)}|0\rangle+\sqrt{f(x)}|1\rangle$. An exact squared-norm error formula is given in terms of Bernstein approximations to $\sqrt f$ and $\sqrt{1-f}$. The construction applies a classical Sprecher-type superposition theorem to $\arcsin\sqrt f$, substitutes commuting normalized zero-count operators for the coordinates, and uses their binomial statistics to establish the probability and coherent-convergence statements. The theorem also gives exact Bernstein probabilities for discontinuous targets, but does not guarantee approximation in that case. No elementary-gate complexity bound is asserted. The discussion describes compression to $d\lceil\log_2(n+1)\rceil$ qubits using the symmetric-subspace structure and notes that Lipschitz regularity permits quantitative convergence estimates.

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This paper addresses the expressivity and representation gap in Quantum Neural Networks by establishing a quantum analogue of the classical Kolmogorov--Arnold representation theorem.
We propose a constructive approximation framework over fixed input coherent states, where the dependence of the function argument is embedded entirely in coordinate qubits, while the target function dictates a single outer unitary evolution.
By applying a Sprecher-type representation to the rotation angle of the state, we demonstrate that the multidimensional operator factorises into (2d+1) commuting universal inner observables.
We prove that the resulting measurement probability precisely reproduces the multidimensional Bernstein polynomial of the target function.
For any continuous multivariate function, the joint quantum state converges uniformly to the target output register, linking classical superposition theory with probabilistic and coherent quantum circuits.
The paper asks whether function approximation from copies of coordinate-encoded qubits admits a Kolmogorov–Arnold representation with target-independent inner observables. Its input is nnn copies of each of ddd coordinate states, with all dependence on x∈[0,1]dx\in[0,1]^dx∈[0,1]d confined to those states; the subsequent unitary depends on the target f:[0,1]d→[0,1]f:[0,1]^d\to[0,1]f:[0,1]d→[0,1] and nnn, but not on xxx.
For d>1d>1d>1, it constructs 2d+12d+12d+1 commuting Hermitian observables Hq(n)H_q^{(n)}Hq(n)​ and a single target-dependent scalar function ggg, independent of nnn, such that Un=∏q=02dexp⁡[−ig(Hq(n))⊗Y]U_n=\prod_{q=0}^{2d}\exp[-i g(H_q^{(n)})\otimes Y]Un​=∏q=02d​exp[−ig(Hq(n)​)⊗Y] produces an ancilla measurement probability exactly equal to the multivariate Bernstein polynomial Bnf(x)B_nf(x)Bn​f(x). When fff is continuous, ggg can be chosen continuous, and the full output converges uniformly in norm to the original input tensored with 1−f(x)∣0⟩+f(x)∣1⟩\sqrt{1-f(x)}|0\rangle+\sqrt{f(x)}|1\rangle1−f(x)​∣0⟩+f(x)​∣1⟩. An exact squared-norm error formula is given in terms of Bernstein approximations to f\sqrt ff​ and 1−f\sqrt{1-f}1−f​.
The construction applies a classical Sprecher-type superposition theorem to arcsin⁡f\arcsin\sqrt farcsinf​, substitutes commuting normalized zero-count operators for the coordinates, and uses their binomial statistics to establish the probability and coherent-convergence statements. The theorem also gives exact Bernstein probabilities for discontinuous targets, but does not guarantee approximation in that case. No elementary-gate complexity bound is asserted. The discussion describes compression to d⌈log⁡2(n+1)⌉d\lceil\log_2(n+1)\rceild⌈log2​(n+1)⌉ qubits using the symmetric-subspace structure and notes that Lipschitz regularity permits quantitative convergence estimates.
The classical Kolmogorov--Arnold representation theorem states that any continuous multivariate function can be exactly decomposed into a finite composition of univariate continuous functions and addition operations. This foundational result has recently inspired the development of Kolmogorov--Arnold Networks (KANs) in classical machine learning, as well as their extensions into the quantum domain (QKANs). In this paper, we establish two quantum analogues of the Kolmogorov--Arnold representation theorem for continuous unitary-valued maps of several variables within an open 111-neighbourhood of the identity matrix O1(I)⊂U(n)O_1(\mathbf{I}) \subset \mathcal{U}(n)O1​(I)⊂U(n). First, we prove a representation theorem that yields an exact additive decomposition inside the matrix exponent of anti-Hermitian-valued maps. Second, due to the non-commutative nature of quantum operators, we derive a factorised version expressing the target unitary map as a finite sequential product of univariate matrix exponentials. Finally, we provide a concrete topological counterexample based on the lifting property of SU(2)\mathcal{SU}(2)SU(2) to demonstrate that these local representation theorems cannot be globally extended to the entire unitary group U(n)\mathcal{U}(n)U(n) without encountering fundamental structural obstructions.
We establish an operational framework connecting the classical Kolmogorov--Arnold (KA) representation theorem to quantum information theory. By introducing and proving an algebraic, bounded-degree polynomial version of the theorem, we demonstrate that any target physical property of an unentangled multi-qubit product state can be exactly decomposed using a finite, fixed set of local ``inner'' observables and a shallow architecture of univariate polynomials. We further analyse the stability of this Quantum Kolmogorov--Arnold (QKA) representation under adversarial perturbations. In stark contrast to the pathological instabilities and severe reparameterisation sensitivities inherent to the classical Kolmogorov--Arnold representation theorem, our algebraic quantum framework exhibits remarkable resilience. We prove that the representation remains stable against bounded physical perturbations acting on the inner measurement operators, and show via the Heisenberg picture that it is inherently immune to adversarial quantum channel attacks acting on the input states.
In this work, we address the question whether a sufficiently deep quantum neural network can approximate a target function as accurate as possible. We start with simple but typical physical situations that the target functions are physical observables, and then we extend our discussion to situations that the learning targets are not directly physical observables, but can be expressed as physical observables in an enlarged Hilbert space with multiple replicas, such as the Loshimidt echo and the Renyi entropy. The main finding is that an accurate approximation is possible only when the input wave functions in the dataset do not exhaust the entire Hilbert space that the quantum circuit acts on, and more precisely, the Hilbert space dimension of the former has to be less than half of the Hilbert space dimension of the latter. In some cases, this requirement can be satisfied automatically because of the intrinsic properties of the dataset, for instance, when the input wave function has to be symmetric between different replicas. And if this requirement cannot be satisfied by the dataset, we show that the expressivity capabilities can be restored by adding one ancillary qubit where the wave function is always fixed at input. Our studies point toward establishing a quantum neural network analogy of the universal approximation theorem that lays the foundation for expressivity of classical neural networks.
Quantum Signal Processing is a powerful quantum framework for generating and approximating univariate polynomials. However, QSP is often limited by circuit-depth bottlenecks and parity constraints on the class of realizable polynomials. In this work, we introduce Weighted Quantum Signal Processing, an extension of QSP in which a weight function is assigned to the central rotation operator. This formulation provides a deeper understanding of QSP, which emerges as the special case of WQSP with unit weights. The choice of weights determines the structure and expressive capabilities of WQSP circuits. When the weights are natural numbers greater than one, WQSP reduces to a pruned version of QSP, revealing parameter redundancies in the standard framework. Through appropriate selection of integer weights, WQSP achieves linear-to-exponential reductions in the number of parameters required to realize arbitrary bounded univariate polynomials while preserving approximation quality. For generic weights, we establish corresponding approximation error bounds and show that, in many cases, the approximation is exact. We analyze WQSP from both a deterministic perspective, where polynomial generation is formulated as the solution of a linear system, and a quantum machine learning perspective, where WQSP serves as a structured and expressive quantum learning model. We further employ this learning framework to parameterize learnable activation functions in Kolmogorov--Arnold Networks for multivariate function approximation. Our results show that WQSP provides a compact, flexible, and theoretically grounded framework for realizing arbitrary univariate polynomials while requiring significantly fewer trainable parameters than conventional QSP. This yields expressive and parameter-efficient neural architectures, highlighting the potential of WQSP as a scalable primitive for quantum-enhanced machine learning.
The conventional paradigm of quantum computing is discrete: It utilizes discrete sets of gates to realize bitstring-to-bitstring mappings, some of them arguably intractable for classical computers. In parametrized quantum approaches, the input becomes continuous and the output represents real-valued functions. While the universality of discrete quantum computers is well understood, basic questions remained open in the continuous case. We focus on universality of multivariate functions. Current approaches require either a number of qubits scaling linearly with the dimension of the input for fixed encodings or a tunable encoding procedure in single-qubit circuits. The question of whether universality can be reached with a fixed encoding and sublinearly many qubits remained open for the last five years. In this paper, we answer this question in the affirmative for arbitrary multivariate functions. We provide two methods: (1) a single-qubit circuit where each coordinate of the arguments to the function to represent is input independently and (2) a multiqubit approach where all coordinates are input in one step, with number of qubits scaling logarithmically with the dimension of the argument of the function of interest. We view the first result of inherent and fundamental interest, whereas the second result opens the path toward representing functions whose arguments are densely encoded in a unitary operation, possibly encoding, for instance, quantum processes.
We introduce quantum Kolmogorov-Arnold networks (QKAN), a quantum algorithmic framework inspired by the recently proposed Kolmogorov-Arnold Networks (KAN). QKAN inherits the compositional structure of KAN and is based on block-encodings, constructed recursively from a single layer using quantum singular value transformation. We demonstrate the algorithmic utility of QKAN in two applications. First, we introduce and analyze QKAN as a quantum learning model, treating the eigenvalues of block-encoded matrices as neurons and applying parametrized activation functions on the edges of the network. We show that QKAN is a wide-and-shallow neural architecture, where shallow depth is compensated by exponentially wide layers whenever efficient block-encodings of inputs are available. We further discuss how to parametrize and train QKAN using parametrized quantum circuits and quantum linear algebra subroutines. Second, we demonstrate that QKAN can serve as a multivariate quantum state-preparation protocol for functions with shallow compositional structure. We demonstrate this by efficiently preparing a multivariate Gaussian quantum state using a two-layer QKAN. Looking forward, we anticipate that QKAN's compositional and modular design will enable new applications in quantum machine learning and quantum state preparation.