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物理学前沿:英文版

On the core of the fractional Fourier transform and its role in composing complex fractional Fourier transformations and Fresnel transformations

Hong-Yi, Fan, Junhua, Chen

Published Jan 1, 2015• 0 citations
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Abstract

[F [f]]=F 哪个的+[f],部分 Fourier 转变( FrFT ) F [f]应该满足,我们表明相互转变的操作员是的位置动量为构造 FrFT 的集成内核的核心元素。基于这观察并且二互相结合纠缠状态的代表,我们然后为启用复杂部分 Fourier 转变(CFrFT ) 导出一个核心操作员,它也服从添加剂规则。以一种类似的方式,我们也为夫累X尔操作员的一种类型揭示部分转变性质。

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[F [f]]=F 哪个的+[f],部分 Fourier 转变( FrFT ) F [f]应该满足,我们表明相互转变的操作员是的位置动量为构造 FrFT 的集成内核的核心元素。基于这观察并且二互相结合纠缠状态的代表,我们然后为启用复杂部分 Fourier 转变(CFrFT ) 导出一个核心操作员,它也服从添加剂规则。以一种类似的方式,我们也为夫累X尔操作员的一种类型揭示部分转变性质。
By a quantum mechanical analysis of the additive rule F α[F β[f]]=F α+β[f], which the fractional Fourier transformation (FrFT) F α[f] should satisfy, we reveal that the position-momentum mutual-transformation operator is the core element for constructing the integration kernel of FrFT. Based on this observation and the two mutually conjugate entangled-state representations, we then derive a core operator for enabling a complex fractional Fourier transformation (CFrFT), which also obeys the additive rule. In a similar manner, we also reveal the fractional transformation property for a type of Fresnel operator.
We employ the recently established basis (the two-variable Hermite-Gaussian function) of the generalized Bargmann space (BGBS) [Phys. Lett. A303, 311 (2002)] to study the generalized form of the fractional Fourier transform (FRFT). By using the technique of integration within an ordered product of operators and the bipartite entangled-state representations, we derive the generalized generating function of the BGBS with which the undecomposable kernel of the two-dimensional FRFT [also named complex fractional Fourier transform (CFRFT)] is obtained. This approach naturally shows that the BGBS is just the eigenfunction of the CFRFT.