Research Article | Open Access
Hong Zhang, Sheng Zou, Xi-Yuan Chen, Wei Quan, "Parameter Modeling Analysis and Experimental Verification on Magnetic Shielding Cylinder of All-Optical Atomic Spin Magnetometer", Journal of Sensors, vol. 2015, Article ID 491746, 7 pages, 2015. https://doi.org/10.1155/2015/491746
Parameter Modeling Analysis and Experimental Verification on Magnetic Shielding Cylinder of All-Optical Atomic Spin Magnetometer
The ultrahigh sensitivity atomic spin magnetometer as the magnetic measurement sensor has received much concern. The performance of the magnetic shielding cylinder is one of the key factors constraining the atomic spin magnetometer’s sensitivity. In order to effectively improve the performances of the magnetic shielding, the parameter optimization models of the magnetic shielding cylinder were established in this paper. Under the condition of changing only one parameter while the others keeping constant, the effects of various parameters influencing the axial shielding coefficient were comprehensively analyzed, and the results showed that the smaller the innermost length, the innermost radius, and the radial spacing were, and the greater the axial spacing was, the better the shielding performance could be obtained. According to these results and the actual needs, the magnetic shielding cylinder was optimally designed, and then the shielding effects were simulated via the software Ansoft. The simulation results showed that the optimized magnetic shielding cylinder had the advantages of small size, high shielding performance, and lager uniformity than that of the nonoptimized one. The actual measurement results showed that the residual magnetism in the optimized magnetic shielding cylinder was below 0.1 nT, which was 2~4 times lower than the nonoptimized one.
The ultrasensitive magnetometers are widely used in many disciplines, such as basic physics [1–4], biology [5, 6], medical imaging [7, 8], and material science and geography [9, 10]. Recently, with the intensive study of the atomic spin theory and the rapid developments of quantum control technology and photoelectric detection technology, the ultrahigh sensitivity spin-exchange relaxation free (SERF) [11–13] atomic magnetometer emerges as the times require. Essentially, the SERF atomic spin magnetometer is a magnetic field measurement device, which is based on the hyperfine levels atomic transition and works at the environment with a weak magnetic field . It is extremely important for the SERF atomic spin magnetometer to isolate the interferences from the external magnetic field, when it is implementing the ultrahigh sensitive magnetic measurement [15, 16]. Therefore, it puts forward strict demands to the performances of the magnetic shielding. Generally, the magnetic shielding is made from ferromagnetic material with high permeability [17, 18], such as μ-metal, and the shapes are mainly spherical, cylindrical, rectangular, and so forth. A closed cylindrical shell of finite length magnetic shielding is used in the SERF atomic spin magnetometer to insulate the magnetic field interference. The existing literatures about the magnetic shielding design mainly analyze the apertures [19, 20], the relative permeability, the shape, and the thickness of the shielding impacting on the shielding performance [21, 22]. However, few researches have been done on the parameters optimization of the magnetic shielding parameter, such as length, radius, radial, and axial clearance. Currently, the designs of the magnetic shielding basically depend on experience, and there is lack of a complete optimization model.
Aiming at the problem of the atomic spin magnetometer’s sensitivity being restricted by the magnetic shielding cylinder, the parameter optimization method and models for the magnetic shielding cylinder were proposed and established, respectively, under the condition of comprehensively considering the various factors affecting the shielding performance. Through the finite element analysis software, the shielding effects of the optimized and the nonoptimized magnetic shielding cylinder were simulated, respectively, and the optimization model and the simulation results were verified by experiments.
2. Parameter Optimization Models of Multilayered Magnetic Shielding Cylinder
2.1. Composition and Principle of SERF Atomic Spin Magnetometer
The SERF atomic spin magnetometer is mainly composed by the pump and probe system, the magnetic shielding and magnetic compensation system, the alkali-metal cell, and the heating system. The SERF atomic spin magnetometer device is shown in Figure 1.
The magnetic shielding is used to isolate the external magnetic field. The cell, which is heated to 180°C by the heating system, contains a droplet of alkali-metal atoms, several atm of 4He and several torr . A circularly polarized pump beam, which is turned to the center of the D1 line of the alkali-metal atoms, is perpendicular to the linearly polarized probe beam. The output signal is modulated and demodulated by the photoelastic modulation (PEM) and the lock-in amplifier, respectively.
Generally, the relaxation time includes the longitudinal relaxation time and the transverse relaxation time :Here is the total relaxation time, is the slowing factor, is the wall-collision relaxation rate, is the spin-exchange broadening factor, is the spin-exchange relaxation rate, and is the broadening.
When the electrons stay in the SERF regime, one of the most important characteristics is that the spin exchange is suppressed; at this moment, is approximately equal to . Under the different magnetic field environments, the temperatures realizing the SERF regime are shown in Figure 2.
Figure 2 shows that with increasing magnetic field, it needs a higher temperature to achieve the SERF regime. For example, at a 0.1 nT and a 1 nT magnetic field, the temperatures of realizing the SERF regime are approximately 120°C and 180°C, respectively, while, in the case of a 10 nT magnetic field existing, the temperature realizing the SERF regime is about 230°C. For a 50000 nT geomagnetic field, if there is no magnetic shielding, the SERF atomic spin magnetometer cannot work due to the extremely high temperature required. Thus, using the magnetic shielding to decrease the geomagnetic field is very important.
Optimizing the parameters of the magnetic shielding to obtain a high-performance and little volume magnetic shielding is vitally necessary.
2.2. Parameter Optimization Models
The shielding performance of the magnetic shielding cylinder is usually evaluated by shielding coefficient. The axial shielding coefficient becomes the key to restrict the shielding performance due to the axial shielding coefficient far less than the transverse shielding coefficient. Based on establishing the parameter optimization models, the influences of various parameters on the axial shielding coefficient were emphatically analyzed.
The transverse and the axial shielding coefficient formulas of -layer magnetic shielding cylinder were described as follows:where is the total transverse shielding coefficient, / and are the transverse shielding coefficient and the average diameter at the th layer, respectively. is the total axial shielding coefficient, and is the average length at the th layer. The axial profile map of the -layer closed magnetic shielding cylinder is shown in Figure 3.
From Figure 3 we know that the thickness , the innermost length , the innermost radius , the radial interval , and the axial clearance are contained between the neighboring shielding cylinder layers. Under the condition of considering these factors, (2) are improved and perfected, and the optimization models can be obtained:Here is the relative permeability. According to (4), with other conditions steadfast, but changing only one parameter, the simulations of the influences from the various parameters on the axial shielding coefficient are shown in Figure 4.
Figure 4(a) shows that with the increasing of the relative magnetic permeability and the thickness of the cylinder, the shielding performances become better and better; Figure 4(b) describes that the axial shielding coefficient varies in inverse proportion to . When changes below 20 cm, the axial shielding coefficient varies greatly. However, if exceeds this range, the axial shielding coefficient varies slowly. Figure 4(c) delineates that with the increasing of the length and the radius of the innermost cylinder, the shielding coefficients become smaller and smaller.
The shielding coefficient of the magnetic shielding cylinder may also be characterized by the demagnetization factor, which is directly determined by the space ratio of the magnetic shielding cylinder:where is the demagnetization factor, and is the space ratio of the magnetic shielding cylinder. The relationship between the demagnetization factor and the shielding coefficient and the relationship between the space ratio and the demagnetization factor are shown in Figures 5(a) and 5(b), respectively.
Figure 5(a) shows that with the shielding coefficient increasing, the demagnetizing factor increases. Figure 5(b) indicates that with the space ratio increasing, the demagnetizing factor reduces, and at , the biggest demagnetizing factor can be realized; meanwhile, the best shielding effect will also be obtained. This conclusion makes the parameter optimization model become more complete.
3. Shielding Performance Simulation and Experimental Verification
3.1. Materials Selection
The permeability performance of the magnetic material is expressed by the relative permeability. The higher the relative permeability is, the better the shield performance will be. Thus, the magnetic material with high relative permeability is used to fabricate the magnetic shielding. The commonly used magnetic materials and their relative permeability are listed in Table 1.
The Permalloy has been chosen to fabricate the magnetic shielding due to its highest relative permeability.
3.2. Simulation Modeling
The software Ansoft, which is based on the finite element method, is used to establish the simulation modeling. A pair of Helmholtz coils was applied to produce a uniform magnetic field about 23000 nT along the axial direction. A five-layer closed magnetic shielding cylinder with trepanning was located in the center of the Helmholtz coils, as shown in Figure 6.
According to the foregoing analysis results and the actual requirements, the main design parameters of the magnetic shielding cylinder are listed in Table 2. The thickness of the magnetic shielding cylinder is 1 mm, and the relative permeability is 10000.
3.3. Analysis and Discussion
The CTM-6W single-axis fluxgate, which is developed by National Institute of Metrology of China, was used to measure the residual magnetism. The resolution and the measurement range of the fluxgate are 0.2 nT and 0 nT~99999.9 nT, respectively. The test points were set along the axial direction with 1 cm intervals. The residual magnetism was measured by the probe positive and reverse placed, respectively. The two measurement results were subtracted in order to eliminate the offset value of the fluxgate, and the average value was the final result. The material objects of the nonoptimization magnetic shielding, which is used in the first generation SERF atomic spin magnetometer, and the optimization one, which will be used in the second generation magnetometer, are shown in Figures 7(a) and 7(b), respectively. The simulation results and the test results of the optimization design and the nonoptimization design are shown in Figure 8.
(a) The nonoptimization magnetic shielding
(b) The optimization magnetic shielding
The simulation results show that the residual magnetic field in the optimized magnetic shielding cylinder is about 0.01 nT; however, the residual magnetic field in the nonoptimization magnetic shielding cylinder is about 0.23 nT. The experimental results showed that the residual magnetic field in the optimized magnetic shielding cylinder was less than 0.1 nT and the uniformity of the magnetic field was very good; however, the residual magnetic field in the nonoptimization magnetic shielding cylinder was between 0.2~0.4 nT. The enlarged drawing showed that there were some deviations between the experimental results and the simulation results. These deviations were mainly caused by three reasons. Firstly, the performance of the magnetic shielding was related to the annealing process, and the nonuniform distribution of the temperature on the magnetic shielding could impact the performance. The volume of the nonoptimization magnetic shielding cylinder was larger, and its shielding performance was easily influenced by the nonuniform distribution of the heat treatment temperature. Secondly, Permalloy was sensitive to the mechanical stress. In the processes of the machining, the transportation, and the assembling, it could not avoid the stress effects on the properties of the magnetic shielding. Thirdly, there were some reading errors during the operation. But the simulation results agreed with the experimental results without considering the influences of errors.
The various factors affecting the shielding performance were analyzed in this paper. Firstly, the parameter optimization formulas of the magnetic shielding cylinder were deduced, and the simulation results indicated that , , , , had a larger effect on the axial total shielding coefficient, while, compared with the other parameters, effected smaller. The magnetic shielding cylinder with small size had the advantages of larger shielding coefficient and better shielding effect. Secondly, at , the biggest demagnetizing factor could be realized. The correctness of the optimization model could be validated by simulations and experiments, and the optimized magnetic shielding cylinder was below 0.1 nT. The magnetic shielding cylinder designed by the optimization modeling approach described in this paper had the advantages of good shielding performance, small volume, light weight, and low cost, and it could provide theoretical guidance to the optimization design of the magnetic shielding structure.
Conflict of Interests
The authors declare that there is no conflict of interests regarding the publication of this paper.
This study was supported by the Major Program of the National Natural Science Foundation of China (Grant no. 61227902), the National Natural Science Foundation of China (Grant no. 51375087), and the Fundamental Research Funds for the Central Universities of Ministry of Education of China (Grant no. CXLX13_083).
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