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Experimental realization of spatial entanglement for bright optical beams

机译:明亮光束空间缠结的实验实现

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We present the latest results on the experimental generation of the position and momentum (x-p) entanglement for bright optical beams as proposed by Hsu et al. [1]. Spatial entanglement is a direct test of the proposal by Einstein, Podolsky and Rosen (EPR), using beam momentum and position, which to the best of our knowledge has never been demonstrated with light. The scheme for generating spatial entanglement is based on the concept of position squeezed beams, first introduced in ref. [2], where the mode corresponding to the first derivative of the mean field has to be squeezed. In the case of a TEM{sub}00 carrier, which defines the position of the beam, this corresponds to the squeezed TEM{sub}10 mode. In particular the real and imaginary parts of the TEM{sub}10 mode represent changes in transverse position, δd, and tilt, δθ, of a TEM{sub}00 carrier beam. Only the TEM{sub}10 mode is occupied by a vacuum squeezed mode whereas all the other modes are occupied by vacuum fluctuations. The position squeezed beams are generated by a lossless combination of a vacuum amplitude squeezed TEM{sub}10 beam with a coherent TEM{sub}00 carrier beam in a Mach-Zehnder interferometer (MZI). We demonstrate measurements of the quantum correlations in the TEM{sub}10 mode with two optical parametric amplifiers. We produce stable locked squeezing at -2.5 dB below the quantum noise limit (QNL) at the detection frequency 5 MHz, as shown in Fig. 1. The measurements of the squeezing spectra show that mixing the TEM{sub}10 squeezed beam with the TEM{sub}00 carrier beam in the MZI has no influence on the amount of squeezing. The only difference is equal increase in noise power of all the traces due to the noise of the carrier beam. This proves that the x-p entanglement using the position squeezed beams is possible.
机译:我们介绍了Hsu等人提出的明亮光束的位置和动量(X-P)缠结的实验生成的最新结果。 [1]。空间纠缠是Einstein,Podolsky和Rosen(EPR)的提案的直接测试,使用光束势头和位置,这是我们最好的知识,从未用过光照证明。用于产生空间纠缠的方案基于位置挤压光束的概念,首先在参考中引入。 [2],其中必须挤压对应于平均场的第一导数的模式。在定义光束位置的TEM {SUB} 00载波的情况下,这对应于挤压的TEM {SUB} 10模式。特别地,TEM {sub} 10模式的实部和虚部表示TEM {SUB} 00载波的横向位置,ΔD和倾斜,Δθ的变化。只有TEM {sub} 10模式被真空挤压模式占用,而所有其他模式都被真空波动占据。通过在Mach-Zehnder干涉仪(MZI)中的相干TEM {sub} 00载波(MZI)中的真空幅度挤压TEM {SUB} 10波束的无损组合产生位置挤压梁。我们展示了具有两个光学参数放大器的TEM {sub} 10模式中量子相关的测量。在检测频率5 MHz的量子噪声极限(QNL)下,我们在低于量子噪声限制(QNL)下方的稳定锁定挤压,如图1所示。挤压光谱的测量结果显示将TEM {Sub} 10挤压梁MZI中的TEM {Sub} 00载波光束对挤压量没有影响。由于载体光束的噪声,唯一的差异是所有迹线的噪声功率的相同增加。这证明了使用使用位置挤压梁的X-P缠结是可能的。

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