• Acta Physica Sinica
  • Vol. 68, Issue 8, 084203-1 (2019)
Dong Yan1,*, Bin-Bin Wang1, Wen-Jie Bai1, Bing Liu1..., Xiu-Guo Du2 and Chun-Nian Ren3|Show fewer author(s)
Author Affiliations
  • 1Key Laboratory of Materials Design and Quantum Simulation, School of Science, Changchun University, Changchun 130022, China
  • 2Department of Basic Courses, Changchun University of Science and Technology, Changchun 130000, China
  • 3College of Information Science and Technology, Qingdao University of Science and Technology, Qingdao 266046, China
  • show less
    DOI: 10.7498/aps.68.20181938 Cite this Article
    Dong Yan, Bin-Bin Wang, Wen-Jie Bai, Bing Liu, Xiu-Guo Du, Chun-Nian Ren. Phase in Rydberg electromagnetically induced transparency[J]. Acta Physica Sinica, 2019, 68(8): 084203-1 Copy Citation Text show less
    (a) Under the control of a classical field , a quantum probe field propagates in a one-dimensional cold atomic ensemble of non-interacting superatoms. (b) Left, level structure of the three-level interacting cold atoms described by a vdW potential; right, an equivalent energy level structure of a non-interacting superatom.(a)量子探测场在控制场相干作用下的一维冷原子系综中传播, 原子系综可以看作是由独立的超级原子构成的; (b)左侧为具有vdW 相互作用的三能级原子结构图; 右侧为等价的无相互作用超级原子能级结构图
    Fig. 1. (a) Under the control of a classical field , a quantum probe field propagates in a one-dimensional cold atomic ensemble of non-interacting superatoms. (b) Left, level structure of the three-level interacting cold atoms described by a vdW potential; right, an equivalent energy level structure of a non-interacting superatom. (a)量子探测场 在控制场 相干作用下的一维冷原子系综中传播, 原子系综可以看作是由独立的超级原子构成的; (b)左侧为具有vdW 相互作用的三能级原子结构图; 右侧为等价的无相互作用超级原子能级结构图
    (a) The transmitted probe intensity , (b) the second-order correlation function , (c) probe phase as a function of the probe detuning . The black solid, blue dashed and red dotted curves are corresponding to incident probe Rabi frequencies , and , respectively. The single-photon detuning and the Rabi frequency of control field . Other parameters are described in the text.(a)探测场透射率, (b)二阶关联函数, (c)探测场相位作为探测失谐的函数. 黑色实线, 蓝色折线以及红色点线分别对应入射探测场拉比频率, 0.3 MHz和0.6 MHz的情况. 单光子失谐, 控制场拉比频率, 其他参数见正文描述
    Fig. 2. (a) The transmitted probe intensity , (b) the second-order correlation function , (c) probe phase as a function of the probe detuning . The black solid, blue dashed and red dotted curves are corresponding to incident probe Rabi frequencies , and , respectively. The single-photon detuning and the Rabi frequency of control field . Other parameters are described in the text. (a)探测场透射率 , (b)二阶关联函数 , (c)探测场相位 作为探测失谐 的函数. 黑色实线, 蓝色折线以及红色点线分别对应入射探测场拉比频率 , 0.3 MHz和0.6 MHz的情况. 单光子失谐 , 控制场拉比频率 , 其他参数见正文描述
    (a) The transmitted probe intensity , (b) the second-order correlation function , (c) the probe phase as a function of the probe detuning and theRabi frequency of the incident probe field . Other parameters are the same as in Fig. 2.(a)探测场透射率, (b)二阶关联函数, (c)探测场相位作为探测失谐和入射探测场拉比频率的函数. 其他参数同图2
    Fig. 3. (a) The transmitted probe intensity , (b) the second-order correlation function , (c) the probe phase as a function of the probe detuning and theRabi frequency of the incident probe field . Other parameters are the same as in Fig. 2. (a)探测场透射率 , (b)二阶关联函数 , (c)探测场相位 作为探测失谐 和入射探测场拉比频率 的函数. 其他参数同图2
    (a) The transmitted probe intensity , (b) the second-order correlation function , (c) probe phase as a function of the probe detuning and the initial second-order correlation function . The Rabi frequency of the incident probe field and other parameters are the same as in Fig. 2.(a)探测场透射率, (b)二阶关联函数, (c)探测场相位作为探测失谐和初始二阶关联函数的函数. 入射探测场拉比频率, 其他参数同图2
    Fig. 4. (a) The transmitted probe intensity , (b) the second-order correlation function , (c) probe phase as a function of the probe detuning and the initial second-order correlation function . The Rabi frequency of the incident probe field and other parameters are the same as in Fig. 2. (a)探测场透射率 , (b)二阶关联函数 , (c)探测场相位 作为探测失谐 和初始二阶关联函数 的函数. 入射探测场拉比频率 , 其他参数同图2
    Probe phase as a function of the Rabi frequency of the incident probe field and initial second-order correlation function : (a) Probe detuning ; (b) probe detuning . Other parameters are the same as in Fig. 2.探测场相位作为入射探测场拉比频率和初始二阶关联函数的函数 (a)探测失谐; (b)探测失谐. 其他参数同图2
    Fig. 5. Probe phase as a function of the Rabi frequency of the incident probe field and initial second-order correlation function : (a) Probe detuning ; (b) probe detuning . Other parameters are the same as in Fig. 2. 探测场相位 作为入射探测场拉比频率 和初始二阶关联函数 的函数 (a)探测失谐 ; (b)探测失谐 . 其他参数同图2
    Probe phase as a function of (a)the principal quantum number and (b) the atomic density . The incident probe intensity and the initial second-order correlation function . Other parameters are the same as in Fig. 2.探测场相位作为(a)主量子数和(b)原子密度的函数. 入射探测场拉比频率, 初始二阶关联函数. 其他参数同图2
    Fig. 6. Probe phase as a function of (a)the principal quantum number and (b) the atomic density . The incident probe intensity and the initial second-order correlation function . Other parameters are the same as in Fig. 2. 探测场相位 作为(a)主量子数 和(b)原子密度 的函数. 入射探测场拉比频率 , 初始二阶关联函数 . 其他参数同图2
    Dong Yan, Bin-Bin Wang, Wen-Jie Bai, Bing Liu, Xiu-Guo Du, Chun-Nian Ren. Phase in Rydberg electromagnetically induced transparency[J]. Acta Physica Sinica, 2019, 68(8): 084203-1
    Download Citation