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Towards coherent manipulation of the ground states of single cesium atom confined in a microscopic far-off-resonance optical dipole trap

机译:朝着单铯原子的接地状态局限于微观偏离共振光学偶极子阱的相干操纵

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This work deals with the cooling and trapping of single cesium (Cs) atoms in a large-magnetic-gradient magneto-optical trap (MOT) and the confinement of single Cs atoms in a far-off-resonance optical dipole trap (FORT). The experiment setup is based on two large-numerical-aperture lens assemblies which allow us to strongly focus a 1064-nm TEM_(00)-mode Gaussian laser beam to a 1/e~2 radius of ~ 2.3 μm to form a microscopic FORT for isolating single atom with environment and to efficiently collect the laser-induced-fluorescence photons emitted by single atoms for detecting and recognizing single atom's internal state. We have tried both of "bottom-up" and "top-down" loading schemes to confine single atoms in the microscopic FORT. In the "bottom-up" scheme, we have successfully prepared single Cs atoms in the MOT and transferred it into FORT with a probability of almost 100%. In the "top-down" scheme, we have achieved ~ 74% of single atom loading probability in the FORT using light-assisted collisions induced by blue detuning laser and with prepared many Cs atoms in the MOT. The relaxation time in hyperfine level of ground state of trapped single Cs atom is measured to be ~5.4 s. To coherently manipulate atomic quantum bits (qubit) encoded in the clock states (mF = 0 states in F_g = 3 and 4 hyperfine levels) of single Cs atom via the two-photon simulated Raman adiabatic passage (STIRAP), we have prepared two phase-locked laser beams with a frequency difference of ~ 9.192 GHz by optically injecting an 852-nm master laser to lock the +1-order sideband of a 9-GHz current-modulated slave diode laser. The two phase-locked laser beams are used to drive STIRAP process in the Λ-type three-level system consists of Cs |6S_(1/2) F_g = 4, m_F = 0> and |6S_(1/2) F_g = 3, m_F = 0< long-lived clock states and Cs |6S_(1/2) F_e = 4, m_F = +1 > excited state with the single-photon detuning of ~ -20 GHz. Rabi flopping experiments are in progress.
机译:该工作涉及在大磁梯度磁光阱(MOT)中的单个铯(CS)原子的冷却和诱捕,以及在远谐振光学偶极阱(FORT)中的单CS原子的限制。实验设置基于两个大数字 - 孔径透镜组件,其允许我们强烈地将1064-nm tem_(00)-mode高斯激光束焦点为1 / e〜2半径为〜2.3μm以形成微观堡用于将单个原子与环境隔离,并有效地收集由单个原子发射的激光诱导的荧光光子,以检测和识别单个原子的内部状态。我们尝试了两个“自下而上”和“自上而下”的装载方案来限制微观堡中的单个原子。在“自下而上”方案中,我们在MOT中成功准备了单个CS原子,并将其转移到堡垒,概率近100%。在“自上而下”方案中,我们在堡垒中实现了约74%的单个原子加载概率,使用蓝色损伤激光器引起的光辅助碰撞,并在MOT中制备许多CS原子。测量捕获的单CS原子的地面状态的高血清水平的放松时间为〜5.4 s。通过双光子模拟拉曼绝热通道(STICAP)将单个CS原子的时钟状态(MF = 3和4个Hyperfine水平中的MF = 3和4个高血清水平中的MF = 3和4个Hyperfine级别中的Qubit)合持原子量子位(Qubit)。我们制备了两相通过光学注入852-nm主激光器来锁定〜9.192GHz的频率差​​,以锁定9-GHz电流调制的从二极管激光器的+ 1阶边界的频率差。两个锁相激光束用于驱动λ型三级系统中的卷曲过程,包括CS | 6S_(1/2)F_G = 4,M_F = 0>和| 6S_(1/2)F_G = 3,M_F = 0 <长寿时钟状态和CS | 6S_(1/2)F_E = 4,M_F = +1>激励状态,具有〜-20 GHz的单光子损伤。 Rabi撤销实验正在进行中。

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