• Laser & Optoelectronics Progress
  • Vol. 60, Issue 17, 1736001 (2023)
Yuqing Li1,2, Huiying Du1, Yunfei Wang1, Jizhou Wu1,2..., Wenliang Liu1,2, Peng Li3, Yongming Fu3, Jie Ma1,2,*, Liantuan Xiao1,2 and Suotang Jia1,2|Show fewer author(s)
Author Affiliations
  • 1State Key Laboratory of Quantum Optics and Quantum Optics Devices, Institute of Laser Spectroscopy, College of Physics and Electronics Engineering, Shanxi University, Taiyuan 030006, Shanxi , China
  • 2Collaborative Innovation Center of Extreme Optics, Shanxi University, Taiyuan 030006, Shanxi , China
  • 3College of Physics and Electronic Engineering, Shanxi University, Taiyuan 030006, Shanxi , China
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    DOI: 10.3788/LOP231417 Cite this Article Set citation alerts
    Yuqing Li, Huiying Du, Yunfei Wang, Jizhou Wu, Wenliang Liu, Peng Li, Yongming Fu, Jie Ma, Liantuan Xiao, Suotang Jia. [J]. Laser & Optoelectronics Progress, 2023, 60(17): 1736001 Copy Citation Text show less
    Schematic of the vacuum apparatus (the Cs atomic oven is heated up to 60 ℃ to provide a high flux of atoms. A Zeeman slower is installed between the gate valve connected the oven chamber and the science chamber. Two ion pumps with the speeds of 50 L/s and 150 L/s are connected with the oven chamber and the science chamber, respectively. In addition, each of the oven chamber and the science chamber has a Ti sublimation pump. The designed cold nipple is enlarged in the dashed box. The cold nipple consists of a 60 mm long tube connected with two 1.33″ flanges, the temperature control unit, and the water cooling device. The temperature control unit includes two TECs, a thermistor, the temperature controller and the aluminum mount. The plastic screws are used to prevent the heat conduction)
    Fig. 1. Schematic of the vacuum apparatus (the Cs atomic oven is heated up to 60 ℃ to provide a high flux of atoms. A Zeeman slower is installed between the gate valve connected the oven chamber and the science chamber. Two ion pumps with the speeds of 50 L/s and 150 L/s are connected with the oven chamber and the science chamber, respectively. In addition, each of the oven chamber and the science chamber has a Ti sublimation pump. The designed cold nipple is enlarged in the dashed box. The cold nipple consists of a 60 mm long tube connected with two 1.33″ flanges, the temperature control unit, and the water cooling device. The temperature control unit includes two TECs, a thermistor, the temperature controller and the aluminum mount. The plastic screws are used to prevent the heat conduction)
    Construction of a Zeeman slower for Cs atoms (the Zeeman slower consists of a slower tube with 8 mm inner diameter and five segments of magnetic field coils, which are manufactured by using 2 mm square copper wires. The two layers of bias coils at the bottom create an uniform magnetic field of 45 G at a current of 3.4 A and each layer has 180 turns. The structurally tapered coils are wrapped on the surface of the bias coils and have the optimized currents of 1.0, 1.2, -1.2, and -3 A for the A, B, C, and D segments, respectively)
    Fig. 2. Construction of a Zeeman slower for Cs atoms (the Zeeman slower consists of a slower tube with 8 mm inner diameter and five segments of magnetic field coils, which are manufactured by using 2 mm square copper wires. The two layers of bias coils at the bottom create an uniform magnetic field of 45 G at a current of 3.4 A and each layer has 180 turns. The structurally tapered coils are wrapped on the surface of the bias coils and have the optimized currents of 1.0, 1.2, -1.2, and -3 A for the A, B, C, and D segments, respectively)
    Vacuum pressure in the oven chamber as a function of the controlled temperature for the nipple (the red line is from theoretical calculation)
    Fig. 3. Vacuum pressure in the oven chamber as a function of the controlled temperature for the nipple (the red line is from theoretical calculation)
    A comparison between the simulated (red line) and measured (black dots) variations of the axial magnetic field in the Zeeman slower tube with the position by using the parameters shown in Fig. 2. A theoretical calculation (blue line) is presented with the efficiency of Zeeman slower η = 0.85
    Fig. 4. A comparison between the simulated (red line) and measured (black dots) variations of the axial magnetic field in the Zeeman slower tube with the position by using the parameters shown in Fig. 2. A theoretical calculation (blue line) is presented with the efficiency of Zeeman slower η = 0.85
    Dependence of the number of Cs atoms in MOT on the detuning of slowing laser (each point is an average of five measurements, solid line is the Gaussian fit for the guide to the eye)
    Fig. 5. Dependence of the number of Cs atoms in MOT on the detuning of slowing laser (each point is an average of five measurements, solid line is the Gaussian fit for the guide to the eye)
    Yuqing Li, Huiying Du, Yunfei Wang, Jizhou Wu, Wenliang Liu, Peng Li, Yongming Fu, Jie Ma, Liantuan Xiao, Suotang Jia. [J]. Laser & Optoelectronics Progress, 2023, 60(17): 1736001
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