Department of Physics, FM-15, University of Washington, Seattle, WA 98195.
Proc Natl Acad Sci U S A. 1986 Apr;83(8):2291-4. doi: 10.1073/pnas.83.8.2291.
A nondestructive type of Stern-Gerlach effect for an individual electron is described that has been thoroughly demonstrated in experiments at the University of Washington. This "continuous Stern-Gerlach effect" makes use of an inhomogeneous magnetic field provided by a weak auxiliary magnetic bottle and is nondestructive in contrast to all previous versions of the effect. As in the classic Stern-Gerlach effect, changes in the spin state are detected via changes in classical particle trajectories; however, what is observed now is not a deflection of the orbit but rather a change of its frequency in the storage well. A simplified model of the continuous Stern-Gerlach effect at zero temperature is introduced to develop the relation between minimum measurement time required for determination of spin state, driven oscillation amplitude, and zero-point fluctuations in the storage well. The problem of the reduction of the wavefunction by the interaction of the electron with the apparatus is addressed following W. Pauli.
描述了一种用于单个电子的非破坏性 Stern-Gerlach 效应,该效应已在华盛顿大学的实验中得到了彻底验证。这种“连续 Stern-Gerlach 效应”利用弱辅助磁瓶产生的不均匀磁场,与之前所有版本的效应相比是非破坏性的。与经典的 Stern-Gerlach 效应一样,自旋状态的变化是通过经典粒子轨迹的变化来检测的;然而,现在观察到的不是轨道的偏转,而是存储阱中频率的变化。引入了零温度下连续 Stern-Gerlach 效应的简化模型,以建立确定自旋状态所需的最小测量时间、驱动振荡幅度和存储阱中零点波动之间的关系。根据 W. Pauli 的理论,解决了电子与仪器相互作用导致波函数减少的问题。