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arXiv 2407.18652gr-qc
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纯态下的霍金辐射

Hawking radiation with pure states

K. Sravan Kumar, João Marto

AI总结:

针对霍金辐射中弯曲时空量子场论的幺正性丢失问题,研究采用基于离散时空变换几何超选择规则的直和型QFTCS量子化方法,以黑洞内外分量直和表征纠缠纯态,实现霍金辐射纯态下的幺正性保持。

摘要:

霍金关于黑洞辐射的开创性工作凸显了我们对弯曲时空量子场论(QFTCS)理解中的一个关键问题,即幺正性丢失问题(纯态演化为混合态)。本文研究了近期提出的直和型QFTCS方案,该方案通过一种新颖的量子化方法保持幺正性,该方法采用基于离散时空变换的几何超选择规则。该方法用在完整希尔伯特空间的几何超选择扇区内演化的分量来描述量子态,遵循史瓦西黑洞的离散对称性。因此,它将最大纠缠纯态表示为黑洞内部和外部区域中两个分量的直和,从而通过使霍金辐射保持纯态形式来保留其幺正性。

英文摘要:

Hawking's seminal work on black hole radiation highlights a critical issue in our understanding of quantum field theory in curved spacetime (QFTCS), specifically the problem of unitarity loss (where pure states evolve into mixed states). In this paper, we examine a recent proposal for a direct-sum QFTCS, which maintains unitarity through a novel quantization method that employs geometric superselection rules based on discrete spacetime transformations. This approach describes a quantum state in terms of components that evolve within geometric superselection sectors of the complete Hilbert space, adhering to the discrete symmetries of a Schwarzschild black hole. Consequently, it represents a maximally entangled pure state as a direct-sum of two components in the interior and exterior regions of the black hole, thereby preserving the unitarity of Hawking radiation by keeping it in the form of pure states.

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