Quantum Fourier Transform in Oscillating Modes

TL;DR

This paper introduces a novel method for implementing quantum Fourier transform using two harmonic resonators, enabling high-dimensional QFT in superconducting circuits without extensive ancilla qubits.

Contribution

The authors propose a new resonator-based protocol for QFT that leverages high-dimensional Hilbert spaces and perfect state transfer, reducing resource requirements.

Findings

A 2^10-dimensional QFT can be realized with current superconducting circuits.

The protocol uses all-resonant and perfect state-transfer methods.

It enables high-precision QFT without extensive ancilla qubits.

Abstract

Quantum Fourier transform (QFT) is a key ingredient of many quantum algorithms where a considerable amount of ancilla qubits and gates are often needed to form a Hilbert space large enough for high-precision results. Qubit recycling reduces the number of ancilla qubits to one but imposes the requirement of repeated measurements and feedforward within the coherence time of the qubits. Moreover, recycling only applies to certain cases where QFT can be carried out in a semi-classical way. Here, we report a novel approach based on two harmonic resonators which form a high-dimensional Hilbert space for the realization of QFT. By employing the all-resonant and perfect state-transfer methods, we develop a protocol that transfers an unknown multi-qubit state to one resonator. QFT is performed by the free evolution of the two resonators with a cross-Kerr interaction. Then, the fully-quantum result can be localized in the second resonator by a projective measurement. Qualitative analysis shows that a 2^10-dimensional QFT can be realized in current superconducting quantum circuits which paves the way for implementing various quantum algorithms in the noisy intermediate-scale quantum (NISQ) era.