与相位检索矢量相关的投影希尔伯特空间的拓扑结构

Fahimeh Arabyani Neyshaburi, Ali Akbar Arefijamaal, Ghadir Sadeghi
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引用次数: 0

摘要

作为本文基础空间的投影希尔伯特空间是通过识别希尔伯特空间 $\mathcal{H}$ 的两个矢量得到的,这两个矢量具有相同的相位,用 $\hat\{mathcal{H}}$ 表示。对于 $\Phi$ 的向量族,我们在 $\hat{mathcal{H}}$ 上引入了拓扑 $\tau_{\Phi}$ 并提供了一种基于拓扑的分析 $\hat{mathcal{H}}$ 的方法。这导致了一种新的相位检索属性分类。我们证明了$(\hat{mathcal{H}}, \tau_{\Phi})$是$\sigma$-compact的,并且当且仅当$\Phi$做相位检索时,它是Hausdorff的。特别地,如果 $\Phi$ 是相检索的,那么我们证明 $(\hat{mathcal{H}}, \tau_{Phi})$ 是可三维的,并且 $\hat{mathcal{H}}$ 通过直接极限拓扑是准紧凑的。同时,我们比较了 $\tau_{Phi}$ 和一些已知拓扑,包括商拓扑、弱拓扑和直接极限拓扑。此外,我们还在 $\hat{mathcal{H}}$ 上建立了一个度量 $d_{/Phi}$,并证明 $d_{/Phi}$ 比 $\hat{mathcal{H}}$ 上的布雷斯-瓦瑟斯坦距离(Bures-Wasserstein distance)更弱。因此,在有限维的情况下,我们证明了$\tau_{\Phi}$与$\hat{mathcal{H}}$上的弱拓扑和$\tau_{d_{Phi}$重合,当且仅当$\Phi$是相检索时。
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Topological structure of projective Hilbert spaces associated with phase retrieval vectors
Projective Hilbert spaces as the underlying spaces of this paper are obtained by identifying two vectors of a Hilbert space $\mathcal{H}$ which have the same phase and denoted by $\hat{\mathcal{H}}$. For a family $\Phi$ of vectors of $\mathcal{H}$ we introduce a topology $\tau_{\Phi}$ on $\hat{\mathcal{H}}$ and provide a topology-based approach for analyzing $\hat{\mathcal{H}}$. This leads to a new classification of phase retrieval property. We prove that $(\hat{\mathcal{H}}, \tau_{\Phi})$ is $\sigma$-compact, as well as it is Hausdorff if and only if $\Phi$ does phase retrieval. In particular, if $\Phi$ is phase retrieval, then we prove that $(\hat{\mathcal{H}}, \tau_{\Phi})$ is metrizable and $\hat{\mathcal{H}}$ is paracompact by a direct limit topology. Also, we make a comparison between $\tau_{\Phi}$ and some known topologies including the quotient topology, the weak topology and the direct-limit topology. Furthermore, we establish a metric $d_{\Phi}$ on $\hat{\mathcal{H}}$ and show that $d_{\Phi}$ is weaker than the Bures-Wasserstein distance on $\hat{\mathcal{H}}$. As a result, in the finite dimensional case, we prove that $\tau_{\Phi}$ coincides with the weak topology and $\tau_{d_{\Phi}}$ on $\hat{\mathcal{H}}$ if and only if $\Phi$ is phase retrieval.
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