Walborn S P, Souto Ribeiro P H, Davidovich L, Mintert F, Buchleitner A
Instituto de Física, Universidade Federal do Rio de Janeiro, Caixa Postal 68528, Rio de Janeiro, RJ 21941-972, Brazil.
Nature. 2006 Apr 20;440(7087):1022-4. doi: 10.1038/nature04627.
Nearly all protocols requiring shared quantum information--such as quantum teleportation or key distribution--rely on entanglement between distant parties. However, entanglement is difficult to characterize experimentally. All existing techniques for doing so, including entanglement witnesses or Bell inequalities, disclose the entanglement of some quantum states but fail for other states; therefore, they cannot provide satisfactory results in general. Such methods are fundamentally different from entanglement measures that, by definition, quantify the amount of entanglement in any state. However, these measures suffer from the severe disadvantage that they typically are not directly accessible in laboratory experiments. Here we report a linear optics experiment in which we directly observe a pure-state entanglement measure, namely concurrence. Our measurement set-up includes two copies of a quantum state: these 'twin' states are prepared in the polarization and momentum degrees of freedom of two photons, and concurrence is measured with a single, local measurement on just one of the photons.
几乎所有需要共享量子信息的协议——如量子隐形传态或密钥分发——都依赖于远距离各方之间的纠缠。然而,纠缠很难通过实验来表征。所有现有的用于此目的的技术,包括纠缠见证者或贝尔不等式,都能揭示某些量子态的纠缠,但对其他态却失效;因此,它们一般不能提供令人满意的结果。这些方法与纠缠度量从根本上不同,根据定义,纠缠度量量化任何态中的纠缠量。然而,这些度量存在一个严重的缺点,即它们通常在实验室实验中无法直接获得。在此,我们报告一项线性光学实验,在该实验中我们直接观测到一种纯态纠缠度量,即并发度。我们的测量装置包括量子态的两个副本:这些“孪生”态是在两个光子的偏振和动量自由度中制备的,并且仅通过对其中一个光子进行单次局部测量来测量并发度。