Quantum-Classical Algorithm for an Instantaneous Spectral Analysis of Signals: A Complement to Fourier Theory

Mario Mastriani
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引用次数: 2

Abstract

A quantum time-dependent spectrum analysis, or simply, quantum spectral analysis (QSA) is presented in this work, and it’s based on Schrodinger’s equation. In the classical world, it is named frequency in time (FIT), which is used here as a complement of the traditional frequency-dependent spectral analysis based on Fourier theory. Besides, FIT is a metric which assesses the impact of the flanks of a signal on its frequency spectrum, not taken into account by Fourier theory and lets alone in real time. Even more, and unlike all derived tools from Fourier Theory (i.e., continuous, discrete, fast, short-time, fractional and quantum Fourier Transform, as well as, Gabor) FIT has the following advantages, among others: 1) compact support with excellent energy output treatment, 2) low computational cost, O(N) for signals and O(N2) for images, 3) it does not have phase uncertainties (i.e., indeterminate phase for a magnitude = 0) as in the case of Discrete and Fast Fourier Transform (DFT, FFT, respectively). Finally, we can apply QSA to a quantum signal, that is, to a qubit stream in order to analyze it spectrally.
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信号瞬时谱分析的量子经典算法:对傅立叶理论的补充
本文提出了一种基于薛定谔方程的量子时变光谱分析,简称量子光谱分析。在古典世界中,它被命名为时间频率(FIT),它在这里被用作基于傅立叶理论的传统频率相关频谱分析的补充。此外,FIT是一种评估信号侧面对其频谱影响的指标,傅立叶理论没有考虑到这一点,更不用说实时了。更重要的是,与傅立叶理论的所有衍生工具(即连续、离散、快速、短时、分数和量子傅立叶变换,以及Gabor)不同,FIT具有以下优点:1)具有出色能量输出处理的紧凑支持,2)计算成本低,信号为O(N),图像为O(N2),3)它不像离散傅立叶变换和快速傅立叶变换(分别为DFT、FFT)的情况那样具有相位不确定性(即,幅度=0的不确定相位)。最后,我们可以将QSA应用于量子信号,即量子位流,以便对其进行光谱分析。
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