DAN Lin1,2,4, YAN Hui1,2,3, WANG Jin1,2, ZHAN Ming-Sheng1,2
1State Key Laboratory of Magnetic and Atomic and Molecular Physics, and Wuhan National Laboratory for Optoelectronics, Wuhan Institute of Physics and Mathematics, Chinese Academy of Sciences, Wuhan 430071 2Center for Cold Atom Physics, Chinese Academy of Sciences, Wuhan 430071 3Laboratory of Quantum Information Technology, ICMP and SPTE, South China Normal University, Guangzhou 510006 4Graduate School of Chinese Academy of Sciences, Beijing 100049
Chip-Based Square Wave Dynamic Micro Atom Trap
DAN Lin1,2,4, YAN Hui1,2,3, WANG Jin1,2, ZHAN Ming-Sheng1,2
1State Key Laboratory of Magnetic and Atomic and Molecular Physics, and Wuhan National Laboratory for Optoelectronics, Wuhan Institute of Physics and Mathematics, Chinese Academy of Sciences, Wuhan 430071 2Center for Cold Atom Physics, Chinese Academy of Sciences, Wuhan 430071 3Laboratory of Quantum Information Technology, ICMP and SPTE, South China Normal University, Guangzhou 510006 4Graduate School of Chinese Academy of Sciences, Beijing 100049
摘要We propose a scheme for a chip-based dynamic micro atom trap where the trap potentials are created by square wave radiation and an inhomogeneous static magnetic field. The parameters of this kind of trap array can be modulated dynamically. Both one-dimensional (1-D) and two-dimensional (2-D) trap array potentials for 6Li atoms are discussed. The 1-D trap is combined by a square wave radiation (6 kHz) and a gradient magnetic field (300 G/cm), the array constant of 1-D trap is 0.85 μm. Since the trap array does not require any laser field, it can be easily integrated on a chip and it is useful in applications of scalable quantum information processing.
Abstract：We propose a scheme for a chip-based dynamic micro atom trap where the trap potentials are created by square wave radiation and an inhomogeneous static magnetic field. The parameters of this kind of trap array can be modulated dynamically. Both one-dimensional (1-D) and two-dimensional (2-D) trap array potentials for 6Li atoms are discussed. The 1-D trap is combined by a square wave radiation (6 kHz) and a gradient magnetic field (300 G/cm), the array constant of 1-D trap is 0.85 μm. Since the trap array does not require any laser field, it can be easily integrated on a chip and it is useful in applications of scalable quantum information processing.
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2010, Vol. 27 
