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Optoelectronics Letters

Preparation and transfer of entanglement in atomic ensembles interacting with cavity fields

杨雄, 邹红梅

Published Jan 1, 2010• 0 citations
OpenAlex

Abstract

在与洞地交往的原子整体的纠纷的准备和转移被调查。结果显示出那二伪 -- 在二个原子整体之间的贝尔国家(纠缠的协调国家) 能明确地通过伪被产生 -- 洞领域上的贝尔大小。在二块洞地之间的量纠纷能完美地被变成二个原子整体,这也被显示。这个工作被湖南省教育局(号码 08C851 ) 的科学搜索基础支持了。

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•Jan 1, 2010•0 citations
在与洞地交往的原子整体的纠纷的准备和转移被调查。结果显示出那二伪 -- 在二个原子整体之间的贝尔国家(纠缠的协调国家) 能明确地通过伪被产生 -- 洞领域上的贝尔大小。在二块洞地之间的量纠纷能完美地被变成二个原子整体,这也被显示。这个工作被湖南省教育局(号码 08C851 ) 的科学搜索基础支持了。
For the Raman interaction between an atom and a two-mode cavity field prepared in the state |01> or |10>, the atom and the field can be disentangled periodically. Such a property of Raman atom-field interaction allows the full entanglement transfer among many atoms and bimodal cavities. In the calculations, each atom is assumed to interact with its own cavity at a different time and so non-identical atoms can be treated conveniently. Entanglement sudden death is discussed too. Though atom-field interaction greatly changes the values of the concurrence for two atoms, configuration of the concurrence is almost not affected. When there is entanglement sudden death, atoms and cavities can still be entangled with one another. However, full entanglement transfer cannot be achieved for such systems with Raman atom-field interaction.
我们建议为为在三个远洞套住的多重原子的纠缠的状态的产生的一个计划由二相同单个模式的纤维连接了。与以前的计划相比,建议计划的明显的优点是:首先,在建议协议的所有洞能自由地与对方一起交往,它在量通讯和分布式的量计算是重要的。第二,在计划,原子,洞,和纤维,模式在回声。因此,要求的相互作用时间是短的,鉴于 decoherence,它是重要的。原则上,建议计划能被扩大产生 n 原子纠缠的状态。[从作者抽象]
We investigate the process of entanglement transfer from a three-mode quantized field to a system of three spatially separated qubits, each one made of a two-level atom resonantly coupled to a cavity mode. The optimal conditions for entanglement transfer, evaluated by atomic tripartite negativity, are derived for radiation prepared in qubitlike and Gaussian entangled states in terms of field parameters, atom-cavity interaction time, cavity mirror losses, and atomic preparation. For qubitlike states we find that for negligible cavity losses some states may completely transfer their entanglement to the atoms and/or be exactly mapped to the atomic state, whereas for Gaussian states we find a range of field parameters needed to obtain a large entanglement transfer. The purity of the three-qubit states and the entanglement of two-qubit subsystems are also discussed in some detail.