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测量两个分离离子的两个束缚电子之间的磁相互作用。

Measurement of the magnetic interaction between two bound electrons of two separate ions.

机构信息

1] Department of Physics of Complex Systems, Weizmann Institute of Science, Rehovot 76100, Israel [2] Physical Measurement Laboratory, National Institute of Standards and Technology, Boulder, Colorado 80305, USA (S.K.); Cavendish Laboratory, University of Cambridge, J. J. Thomson Avenue, Cambridge CB30HE, UK (N.N.).

Department of Physics of Complex Systems, Weizmann Institute of Science, Rehovot 76100, Israel.

出版信息

Nature. 2014 Jun 19;510(7505):376-80. doi: 10.1038/nature13403.

Abstract

Electrons have an intrinsic, indivisible, magnetic dipole aligned with their internal angular momentum (spin). The magnetic interaction between two electronic spins can therefore impose a change in their orientation. Similar dipolar magnetic interactions exist between other spin systems and have been studied experimentally. Examples include the interaction between an electron and its nucleus and the interaction between several multi-electron spin complexes. The challenge in observing such interactions for two electrons is twofold. First, at the atomic scale, where the coupling is relatively large, it is often dominated by the much larger Coulomb exchange counterpart. Second, on scales that are substantially larger than the atomic, the magnetic coupling is very weak and can be well below the ambient magnetic noise. Here we report the measurement of the magnetic interaction between the two ground-state spin-1/2 valence electrons of two (88)Sr(+) ions, co-trapped in an electric Paul trap. We varied the ion separation, d, between 2.18 and 2.76 micrometres and measured the electrons' weak, millihertz-scale, magnetic interaction as a function of distance, in the presence of magnetic noise that was six orders of magnitude larger than the magnetic fields the electrons apply on each other. The cooperative spin dynamics was kept coherent for 15 seconds, during which spin entanglement was generated, as verified by a negative measured value of -0.16 for the swap entanglement witness. The sensitivity necessary for this measurement was provided by restricting the spin evolution to a decoherence-free subspace that is immune to collective magnetic field noise. Our measurements show a d(-3.0(4)) distance dependence for the coupling, consistent with the inverse-cube law.

摘要

电子具有内在的、不可分割的磁偶极子,与它们的内部角动量(自旋)对齐。因此,两个电子自旋之间的磁相互作用可以导致它们的取向发生变化。类似的偶极磁相互作用存在于其他自旋系统中,并已进行了实验研究。例如,电子与其原子核之间的相互作用以及几个多电子自旋复合物之间的相互作用。观察两个电子之间的这种相互作用具有双重挑战。首先,在原子尺度上,耦合相对较大,它通常由大得多的库仑交换对应物主导。其次,在远大于原子尺度的尺度上,磁耦合非常弱,可能远低于环境磁场噪声。在这里,我们报告了在两个(88)Sr(+)离子的两个基态自旋 1/2 价电子之间的磁相互作用的测量结果,这些离子被共捕获在一个电 Paul 阱中。我们改变了离子间距 d,范围从 2.18 到 2.76 微米,并在磁场噪声比电子相互施加的磁场大六个数量级的情况下,测量了电子在弱、毫赫兹范围内的磁相互作用作为距离的函数。在 15 秒内,协同自旋动力学保持相干,这一点通过测量得到的交换纠缠见证值为-0.16 而得到验证。这种测量所需的灵敏度是通过将自旋演化限制在一个不受集体磁场噪声影响的无退相干子空间来提供的。我们的测量结果表明,耦合具有 d(-3.0(4))的距离依赖性,与逆立方定律一致。

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