Wang Ying-Ju, Anderson Dana Z, Bright Victor M, Cornell Eric A, Diot Quentin, Kishimoto Tetsuo, Prentiss Mara, Saravanan R A, Segal Stephen R, Wu Saijun
Department of Physics, University of Colorado, and JILA, National Institute of Standards and Technology and University of Colorado, Boulder, Colorado 80309-0440, USA.
Phys Rev Lett. 2005 Mar 11;94(9):090405. doi: 10.1103/PhysRevLett.94.090405.
An atom Michelson interferometer is implemented on an "atom chip." The chip uses lithographically patterned conductors and external magnetic fields to produce and guide a Bose-Einstein condensate. Splitting, reflecting, and recombining of condensate atoms are achieved by a standing-wave light field having a wave vector aligned along the atom waveguide. A differential phase shift between the two arms of the interferometer is introduced by either a magnetic-field gradient or with an initial condensate velocity. Interference contrast is still observable at 20% with an atom propagation time of 10 ms.
一个原子迈克尔逊干涉仪在“原子芯片”上得以实现。该芯片利用光刻图案化导体和外部磁场来产生并引导玻色 - 爱因斯坦凝聚体。凝聚体原子的分裂、反射和重组是通过一个波矢沿原子波导排列的驻波光场来实现的。干涉仪两臂之间的差分相移可通过磁场梯度或初始凝聚体速度来引入。在原子传播时间为10毫秒时,干涉对比度仍能在20%时被观测到。