Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Quantum Information Processing

Quantum representation of 1-D signals on the unit circle

Artyom M. Grigoryan, Sos S. Agaian

Published Dec 28, 2021• 7 citations
Publisher
DOI
10.1007/s11128-021-03237-3

Related papers

PT-invariance and representations of the Temperley-Lieb algebra on the unit circle

Christian Korff

We present in detail a recent conjecture on self-adjoint representations of the Temperley-Lieb algebra for particular values on the unit circle. The formulation in terms of graphical calculus is emphasized and discussed for several examples. The role of PT (parity and time reversal) invariance is highlighted as it might prove important for generalising the construction to other cases.

arXiv:0712.2205•ENLIGHTEN (Jurnal Bimbingan dan Konseling Islam)•Dec 13, 2007•0 citations

Quantum Representation and Basic Operations of Digital Signals

Panchi Li, Bing Wang, Hong Yu Xiao +1 more

International Journal of Theoretical Physics•Aug 4, 2018•23 citations

Complementary Polynomials in Quantum Signal Processing

Bjorn K. Berntson, Christoph Sünderhauf

Abstract Quantum signal processing is a framework for implementing polynomial functions on quantum computers. To implement a given polynomial P, one must first construct a corresponding complementary polynomial Q. Existing approaches to this problem employ numerical methods that are not amenable to explicit error analysis. We present a new approach to complementary polynomials using complex analysis. Our main mathematical result is a contour integral representation for a canonical complementary polynomial. On the unit circle, this representation has a particularly simple and efficacious Fourier analytic interpretation, which we use to develop a Fast Fourier Transform-based algorithm for the efficient calculation of Q in the monomial basis with explicit error guarantees. Numerical evidence that our algorithm outperforms the state-of-the-art optimization-based method for computing complementary polynomials is provided.

arXiv:2406.04246•Communications in Mathematical Physics•Jun 4, 2025•8 citations

Multiplicative group of quantum representations of signals

Artyom M. Grigoryan, Sos S. Agaian

Quantum Information Processing•Jan 19, 2023•5 citations

The Mathematical Aspects of Quantum Maps

Mirko Degli Esposti, S. Graffi

Springer eBooks•Jan 1, 2003•56 citations

Floquet operator dynamics and orthogonal polynomials on the unit circle

Hsiu-Chung Yeh, Aditi Mitra

Operator spreading under stroboscopic time evolution due to a unitary is studied. An operator Krylov space is constructed and related to orthogonal polynomials on a unit circle (OPUC), as well as to the Krylov space of the edge operator of the Floquet transverse field Ising model with inhomogeneous couplings (ITFIM). The Verblunsky coefficients in the OPUC representation are related to the Krylov angles parameterizing the ITFIM. The relations between the OPUC and spectral functions are summarized and several applications are presented. These include derivation of analytic expressions for the OPUC for persistent $m$-periodic dynamics, and the numerical construction of the OPUC for autocorrelations of the homogeneous Floquet-Ising model as well as the $Z_3$ clock model. The numerically obtained Krylov angles of the $Z_3$ clock model with long-lived period tripled autocorrelations show a spatial periodicity of six, and this observation is used to develop an analytically solvable model for the ITFIM that mimics this behavior.

arXiv:2506.20611•Physical review. B./Physical review. B•Dec 15, 2025•0 citations
Abstract Quantum signal processing is a framework for implementing polynomial functions on quantum computers. To implement a given polynomial P, one must first construct a corresponding complementary polynomial Q. Existing approaches to this problem employ numerical methods that are not amenable to explicit error analysis. We present a new approach to complementary polynomials using complex analysis. Our main mathematical result is a contour integral representation for a canonical complementary polynomial. On the unit circle, this representation has a particularly simple and efficacious Fourier analytic interpretation, which we use to develop a Fast Fourier Transform-based algorithm for the efficient calculation of Q in the monomial basis with explicit error guarantees. Numerical evidence that our algorithm outperforms the state-of-the-art optimization-based method for computing complementary polynomials is provided.
Operator spreading under stroboscopic time evolution due to a unitary is studied. An operator Krylov space is constructed and related to orthogonal polynomials on a unit circle (OPUC), as well as to the Krylov space of the edge operator of the Floquet transverse field Ising model with inhomogeneous couplings (ITFIM). The Verblunsky coefficients in the OPUC representation are related to the Krylov angles parameterizing the ITFIM. The relations between the OPUC and spectral functions are summarized and several applications are presented. These include derivation of analytic expressions for the OPUC for persistent mmm-periodic dynamics, and the numerical construction of the OPUC for autocorrelations of the homogeneous Floquet-Ising model as well as the Z3Z_3Z3​ clock model. The numerically obtained Krylov angles of the Z3Z_3Z3​ clock model with long-lived period tripled autocorrelations show a spatial periodicity of six, and this observation is used to develop an analytically solvable model for the ITFIM that mimics this behavior.