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Spin-entangled squeezed state on a Bloch four-hyperboloid

机译:在Bloch四双曲线上旋转缠绕的挤压状态

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摘要

The Bloch hyperboloid H (2) underlies the quantum geometry of the original SO(2, 1) squeezed states. In Hasebe (2020 J. Phys. A: Math. Theor. 53 055303), the author utilized a non-compact 2nd Hopf map and a Bloch four-hyperboloid H (2,2) to explore an SO(2, 3) extension of the squeezed states. In the present paper, we further pursue the idea to derive an SO(4, 1) version of squeezed vacuum based on the other Bloch four-hyperboloid H (4). We show that the obtained SO(4, 1) squeezed vacuum is a particular four-mode squeezed state not quite similar to the previous SO(2, 3) squeezed vacuum. In view of the Schwinger's formulation of angular momentum, the SO(4, 1) squeezed vacuum is interpreted as a superposition of an infinite number of maximally entangled spin-pairs of all integer spins. We clarify basic properties of the SO(4, 1) squeezed vacuum, such as von Neumann entropy of spin entanglement, spin correlations and uncertainty relations with emphasis on their distinctions to the original SO(2, 1) case.
机译:布洛赫双曲面H(2)是原始SO(2,1)压缩态量子几何的基础。在Hasebe(2020 J.Phys.A:Math.Thero.53 055303)中,作者利用非紧二阶Hopf映射和Bloch四双曲面H(2,2)来探索压缩态的SO(2,3)扩展。在本文中,我们进一步在另一个布洛赫四双曲面H(4)的基础上推导出压缩真空的SO(4,1)版本。我们证明了得到的SO(4,1)压缩真空是一种特殊的四模压缩态,与之前的SO(2,3)压缩真空不太相似。根据Schwinger的角动量公式,SO(4,1)压缩真空被解释为所有整数自旋的无限多个最大纠缠自旋对的叠加。我们阐明了SO(4,1)压缩真空的基本性质,如自旋纠缠的冯·诺依曼熵、自旋关联和不确定性关系,重点讨论了它们与原始SO(2,1)情况的区别。

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