Quantum Cheshire cat: a physically realistic interpretation by invokingentangled correlations

物理 光子 极化(电化学) 量子 示意图 干涉测量 理论物理学 量子力学 电子工程 工程类 物理化学 化学
作者
Muhammad Haroon Saeed,Muhammad Imran,Hinna Tariq,Rameez‐ul‐Islam,Manzoor Ikram
出处
期刊:Journal of The Optical Society of America B-optical Physics [Optica Publishing Group]
卷期号:38 (4): 1147-1147 被引量:3
标识
DOI:10.1364/josab.414000
摘要

The phenomenon of the quantum Cheshire cat (QCC) and its interpretation by Aharanov et al. [ New J. Phys. 15 , 113015 ( 2013 ) NJOPFM 1367-2630 10.1088/1367-2630/15/11/113015 ], with the conjecture that any quantum entity can be disembodied from its physical attributes, has resulted in a heated debate leading to interpretational controversy as well as practical consequences. Here, we propose an experimentally testable and physically more realistic and logically plausible interpretation. We utilize a specifically engineered Mach–Zehnder-type interferometeric setup that is quite similar to the original QCC setup but with the slight difference that now a single-photon, bipartite entangled state traverses the interferometer such that each path is designated to a photon with different tags. With this specific setup, we demonstrate that the photon’s polarization is never physically separated from the photon itself. Rather, it becomes dormant and hence inaccessible along the designated interferometric path. We also generalize the schematics and show that any precisely oriented photon’s polarization that stands inaccessible or dormant re-emerges along the same spatially separated and isolated arm as we tune the polarization vector away from the selected angle. Thus our proposal persuasively proves that polarization is never stripped off the photon itself and instead becomes inaccessible along the interferometeric arm for a certain particularly selected orientation. The schematics further reveal that this inaccessibility of the photon’s polarization is not permanent, fixed, and universal, but rather it is entirely constrained to a specific orientation in the Hilbert space, governed by the particular pre- and post-selected state under two-state vector formalism.

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