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arXiv:1508.00033 · Nature Communications

Implementation of quantum and classical discrete fractional Fourier transforms

Steffen Weimann, Armando Pérez-Leija, Maxime Lebugle, Robert Keil, Malte C. Tichy, Markus Gräfe, René Heilmann, Stefan Nolte, H. M. Moya-Cessa, Gregor Weihs, Demetrios N. Christodoulides, Alexander Szameit

Published Mar 23, 2016• 120 citations
arXivHTMLPDF

Abstract

Fourier transforms, integer and fractional, are ubiquitous mathematical tools in basic and applied science. Certainly, since the ordinary Fourier transform is merely a particular case of a continuous set of fractional Fourier domains, every property and application of the ordinary Fourier transform becomes a special case of the fractional Fourier transform. Despite the great practical importance of the discrete Fourier transform, implementation of fractional orders of the corresponding discrete operation has been elusive. Here we report classical and quantum optical realizations of the discrete fractional Fourier transform. In the context of classical optics, we implement discrete fractional Fourier transforms of exemplary wave functions and experimentally demonstrate the shift theorem. Moreover, we apply this approach in the quantum realm to Fourier transform separable and path-entangled biphoton wave functions. The proposed approach is versatile and could find applications in various fields where Fourier transforms are essential tools.

DOI
10.1038/ncomms11027

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We present a new number theoretic definition of discrete fractional Fourier transform (DFrFT) . In this approach the DFrFT is defined as the N×NN \times NN×N dimensional unitary representation of the generator of the arithmetic rotational group SO2[ZN]SO_{2}[\mathbb{Z}_N]SO2​[ZN​], which is the finite set of  mod N\bmod NmodN integer, 2×22\times 22×2 matrices acting on the points of the discrete toroidal phase space lattice ZN×ZN\mathbb{Z}_N \times \mathbb{Z}_NZN​×ZN​, preserving the euclidean distance  mod N\bmod NmodN. We construct explicitly, using techniques of the Finite Quantum Mechanics (FQM), the pnp^npn dimensional unitary matrix representation of the group SO2[Zpn]SO_{2}[\mathbb{Z}_{p^n}]SO2​[Zpn​] and especially we work out in detail the one which corresponds to the generator. This is our definition of the arithmetic fractional Fourier transform (AFrFT). Following this definition, we proceed to the construction of efficient quantum circuits for the AFrFT, on sets of nnn ppp-dimensional qudits with ppp a prime integer, by introducing novel quantum subcircuits for diagonal operators with quadratic phases as well as new quantum subcircuits for multipliers by a constant. The quantum subcircuits that we introduce provide a set capable to construct quantum circuits for any element of a more general group, the group of Linear Canonical Transformations (LCT), SL2[ZN]SL_{2}[\mathbb{Z}_N]SL2​[ZN​] of the toroidal phase space lattice. As a byproduct, extensions of the diagonal and multiplier quantum circuits for both the qudit and qubit case are given, which are useful alone in various applications. Also, we analyze the depth, width and gate complexity of the efficient AFrFT quantum circuit and we estimate its gate complexity which is of the order O(n2)O(n^2)O(n2), its depth which is of the order O(n)O(n)O(n) with depth nnn, while at the same time it has a structure permitting local interactions between the qudits.
This paper presents a generalized circuit framework for constructing Shih-type fractionalizations of unitary operators of dyadic order, i.e., operators UUU satisfying U2n=IU^{2^n}=IU2n=I. Building upon the architecture of the quantum fractional Fourier transform (QFrFT), we show that fractionalization can be implemented coherently as a weighted superposition of integer powers, ∑kck(α)Uk\sum_k c_k(α)U^k∑k​ck​(α)Uk, where the coefficients are generated through an ancilla-domain quantum Fourier transform and a diagonal phase modulation. Under the assumption that controlled implementations of the required powers of UUU are available, the resulting circuit yields a parameterized family of operators that interpolates the integer powers of UUU and satisfies the additive property of fractional transforms. As concrete applications, we derive explicit quantum circuit realizations of the quantum fractional Hartley transform (QFrHT) and of the fractional cosine-transform families associated with Types~I and~IV. These constructions demonstrate the versatility of the proposed dyadic-order fractionalization framework for structured operators arising in quantum signal processing.