Research on the comprehensive performance of PrFeB magnets for synchrotron radiation and free electron laser

Research on the comprehensive performance of PrFeB magnets for synchrotron radiation and free electron laser 1 corresp first-author Corresponding author, heyongzhou@sinap.ac.cn Corresponding author, heyongzhou@sinap.ac.cn heyongzhou@sinap.ac.cn 2 1 1 The Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai 201800, China The Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai 201800, China The University of Science and Technology Beijing (USTB), Beijing 100083, China The University of Science and Technology Beijing (USTB), Beijing 100083, China PrFeB magnets, which possess excellent magnetic properties at low temperatures, have important application value as cryogenic permanent magnet undulators for synchrotron radiation sources and free electron lasers. In this research study, several high-performance PrFeB magnets (P42H, P48SH, and P48UH) were prepared, and their performance was comprehensively examined, including evaluations of their magnetic properties, microstructures, uniformity, and stability. Next, their application prospects were analyzed and discussed. In China, the first cryogenic permanent magnet undulators (CPMU) with P48SH magnets with 18 mm cycle lengths have been developed. When the temperature is 80 K and the gap is 6.0 mm, the magnetic field measurement results of the CPMU showed that the effective magnetic field peak was approximately 0.92 T, yielding an increase of 11.76 % relative to operation at 300 K, with an RMS phase error of about 4.99°. PrFeB magnets Cryogenic permanent magnet undulators Grain boundary diffusion method Free electron laser 1. Introduction 1 Permanent magnet undulators are typical Halbach magnetic structures [ 1 1 ] . They have become one of the key pieces of equipment used in high energy physics and are commonly used in synchrotron radiation facilities and free electron laser devices [ 2 2 , 3 3 ] . NdFeB magnets [ 4 4 ] , which were discovered in 1983, have been widely applied, and are currently one of the key permanent magnets used for undulators [ 5 5 ] . PrFeB and NdFeB have similar crystal structures, and their theoretical remanence Br and intrinsic coercivity Hcj are very similar at about 25 ℃ . The aforementioned PrFeB magnets are characterized by a lack of spin reorientation effects (SRT) [ 6 6 ] , which results in excellent magnetic properties at low temperatures; they have therefore been found to be more suitable as magnetic sources for cryogenic permanent magnet undulators (CPMU) [ 7 7 - 9 9 7-9 ] . However, if PrFeB magnets are to be used in synchrotron radiation and free electron laser applications, the following problems must be resolved: 1) With higher comprehensive magnetic properties, the higher Br at low temperature can potentially result in the CPMU having a higher magnetic field peak value. Furthermore, the higher Hcj at room temperature can potentially cause certain anti-demagnetization effects, which can affect the properties of the CPMU. Owing to the temperature coefficient and other factors, differences in the magnetic properties at room temperature and at low temperatures have often been observed. 2) With their excellent magnetic field homogeneity, the magnetic deflection angle of a PrFeB magnet with a small length and diameter ratio for a typical CPMU is approximately less than 1 degree. In addition, the consistency of the total magnetic moment, Mr, has been observed to be less than 2 %. Moreover, the magnetic field uniformity is known to be closely related to the preparation methods and composition design. 3) With their favorable magnetic field stability, CPMUs with hundreds of magnets with Halbach magnetic circuit loads are characterized by large demagnetization fields when installed at room temperature. However, the Hcj values of PrFeB magnets will exhibit a significant decline when they undergo higher temperature baking. Therefore, the PrFeB magnets are required to exhibit no obvious irreversible demagnetization in higher temperature environments. In this paper, three types of PrFeB magnets were designed and prepared. Their performance was analyzed comprehensively by studying and analyzing several features, such as their magnetic properties, microstructures, magnetic field uniformity, and magnetic field stability. On this basis, the first cryogenic permanent magnet undulator (CPMU18) with P48SH magnets was developed in China. 2. Preparation of the PrFeB 1 As part of the preparation of the P42H and P48SH CPMUs, appropriate adjustments were made for the NdFeB magnets. The P48SH magnets were used as substrates for the P48UH magnets, which had been developed using a grain boundary diffusion method (GBD) [ 10 10 - 12 12 10-12 ] . The main purpose of preparing the P42H magnets was to understand the performance characteristics of the pure PrFeB magnets. Therefore, the following processes were completed: ① By using pure Pr, the mechanism by which the magnetic properties of the nearly pure PrFeB magnet changed at low temperatures was examined. ② With no heavy rare earth elements, Dy and Tb were used to improve the absolute value of the temperature coefficient. ③ For the purpose of increasing the Hcj, trace elements M (such as Cu, Al, and Nb) were added. The main purpose of preparing the P48SH magnets was to further improve the comprehensive performance. Therefore, this study completed the following processes: ① The Fe content was raised to improve the Br, and the Pr content was reduced to the theoretical value of 31.0 %. ② Trace elements M (such as Ca, Zr, and Cr) were added to further enhance the Hcj. In addition, in order to reate a "residual magnetization Mr platform" at 50 K, 10 % Nd was added to replace part of the Pr. The main purpose of preparing the P48UH magnets was to improve the Hcj of the P48SH through a GBD method, which could potentially greatly improve the stability of the magnetic field. Therefore, the following were determined in this study: ① As a diffusion powder, TbF 3 can partially react with the main phase of Pr 2 Fe 14 B to form (Pr,Tb) 2 Fe 14 B within the higher anisotropic field H A . ② The effects of the GBD process are closely related to the orientation thicknesses of the magnets. Therefore, block P48SH magnets with a thinner orientation thickness were used as the substrate. The components along with some of the parameters of the three types of magnets used in this study are listed in Table 1 Table 1 . 1 1 Grade 5 1 Component (%) 4 1 Partial process parameters 1 1 1 1 Pr 1 1 Nd 1 1 B 1 1 Fe 1 1 M 1 1 Powder size (μm) 1 1 Magnetic field intensity (T) 1 1 Heat treatment temperature (℃) 1 1 Density (g/cm 3 ) 1 1 P42H 1 1 31.80 1 1 0.00 1 1 1.03 1 1 66.00 1 1 1.15 1 1 2-15 1 1 1.80 1 1 1050-890-465 1 1 7.44 1 1 P48SH 1 1 28.08 1 1 3.12 1 1 1.00 1 1 66.60 1 1 1.50 1 1 2-10 1 1 2.02 1 1 1060-890-430 1 1 7.51 1 1 P48UH 5 1 The base material is P48SH, and the GBD powder is TbF 3 1 1 1 1 1 1 890+465 1 1 7.56 3. The performance of PrFeB magnets 1 3.1 Magnetic properties 2 Fig. 1(a) Fig. 1(a) shows the demagnetization curves of the three PrFeB magnets at room temperature [ 13 13 ] . As can be seen in the figure, for the P42H, P48SH, and P48UH magnets, the Br values were 1.30 T, 1.38 T, and 1.37 T, respectively. The Hcj values were 1580 kA/m, 2080 kA/m, and 1400 kA/m, respectively. The (BH) max + Hcj values were 58.8, 65.9, and 74.7 [ 11 11 ] respectively. The (BH) max + Hk values (which are more meaningful in the design of magnetic circuits) were 57.4, 65.3, and 66.1, respectively, and the Hk/Hcj ratios were 0.92, 0.97, and 0.77, respectively. Following the optimization of the composition and preparation method, it was found that the Br, Hcj, and Hk/Hcj values of the P48SH magnet were improved when compared with the P42H magnet. Furthermore, when compared with P48SH, the Br of the P48UH displayed no significant changes. The Hcj had increased by approximately 560 kA/m, and the square degree (Hk/Hcj) had deteriorated. These results were determined to have been caused by the non-uniform diffusion of the TbF 3 in the magnet, which was the result of the demagnetization inconsistency. Fig. 1 (b) Fig. 1 (b) details the typical cryogenic magnetic properties of rare earth magnets. It can be seen in the figure that, at low temperatures, the Br and Hcj of an SmCo magnet (such as the XG30/20(CHC)) were not very high. In addition, the Br and Hcj of NdFeB magnets (such as the N33VH and N50M) increased. However, the SRT only showed a relatively limited increase in the Br. The Br and Hcj of the PrFeB magnets with no SRT were observed to be greatly improved. When compared with the values at 293 K, at 77 K, the Br values of the P42H, P48SH and P48UH were determined to have increased by 15.4 %, 13.9 %, and 13.5 %, respectively, and the Hcj had increased by almost more than three times. It was found that, between 293 and 77 K, the average absolute temperature coefficient values of the Hcj and Br of the three types of magnets had gradually decreased. Between 293 and 77 K the Br of the SmCo (XG30/20) and the NdFeB (N33VH) magnets were determined to have increased by 6.0 % and 8.0 %, respectively. These findings were closely related to the composition design of the permanent magnet. 3.2. Microstructure 2 Figure 2 Figure 2 details the XRD patterns of the P42H, P48SH, and P48UH magnets. As can be seen in the figure, the ratios of the (006) peak to the (105) peak for P42H, P48SH, and P48U were 1.02, 1.16 and 1.31, respectively. Furthermore, when compared with P42H, the orientation degree of P48SH was observed to have been improved (for example, the 006/105 ratio [ 4 4 ] increased) [ 13 13 ] . These findings were determined to be closely related to the increased orientation of the magnetic field and the optimization of the powder particle size distribution. When compared to P48SH, the orientation degree of P48UH displayed further improvements (for example, the 006/105 ratio increased again). This indicated that there was a major difference in the diffusion concentration of TbF 3 along the different crystal faces of the main phase of the Pr 2 Fe 14 B. Furthermore, along the parallel orientation plane (006), the diffusion effects were observed to be stronger than along plane (105), which forms a 15.44° angle with the (006) plane. Figure 3 Figure 3 displays back-scattering images of the P42H, P48SH, and P48UH magnets. The dark gray region represents the base magnetic phase (Pr,Tb) 2 Fe 14 B and the bright white or grayish white region denotes the Pr/Tb rich phase. It can be seen in the figure that the intergranular Pr/Tb rich phase of the P42H magnet was relatively concentrated, and the number of grain boundary cracks was greater. For the P48SH magnets, there was a relatively uniform and very thin Pr/Tb rich phase distributed between the grain boundaries. When compared with the P48SH magnets, the grain boundaries of the P48UH magnet showed a more uniform distribution of the Pr/Tb rich phase, which formed an approximate grid with the Pr/Tb rich phase between the grain boundaries. The grayish white area was increased after the GBD process, which indicated that in the main magnetic phases (Pr,Tb) 2 Fe 14 B [ 12 12 ] , the Pr near the boundaries was replaced by Tb. Fig. 4 Fig. 4 details the relative concentrations of Pr and Tb along the orientation direction (from the surface to the interior) of the P48UH magnet as determined by electron probe micro-analysis (EPMA). As can be seen in Fig. 4(a) Fig. 4(a) , on the surface of the magnet in the 0 to 17 μm range, the relative Pr concentration changed rapidly. For example, the Pr content decreased sharply closer to the surface of the magnet, which was caused by the Pr of the magnet’s surface having undergone major losses during the GBD process. Within the 17 to 105 μm range, the relative concentration of Pr was observed to decrease following the grain boundary diffusion, and the closer to the surface of the magnet, the greater the decrease. These findings indicated that the closer to the surface, the more Pr was replaced by Tb. In Fig. 4(b) Fig. 4(b) , it can also be seen that the relative concentration of Tb increased significantly following the grain boundary diffusion process, and the closer to the surface of the magnet, the more the Tb increased. These findings also indicated that the GBD effect was closely related to the orientation thicknesses of the magnets. For example, smaller thicknesses produced more obvious effects. The GBD process can potentially greatly improve the Hcj of a magnet. However, the technical characteristic constraints tend to result in different positions, and the increased amplitudes of the Hcj have been found to not be uniform. Fig. 1(a) Fig. 1(a) shows that the demagnetization curve of the P48UH had an average value, and it could not display the Hcj value at each point. 3.3. Magnetic uniformity 2 Figure 5 Figure 5 details the total moment Mr consistency, along with the magnetization angle of the PrFeB (sample size: 50 mm × 30 mm × 6.6 mm; orientation: 6.6 mm) [ 14 14 ] . As can be seen in Fig. 5(a) Fig. 5(a) , the differences in the Mr between the three types of magnets were not particularly large, and the Mr value fluctuated within a range of approximately 0.8 %. However, the micro fluctuation displayed obvious differences during the testing of the fifteen samples. For example, in regard to the P42H magnets in exon 5, the other magnets’ fluctuation ranges were only approximately 0.5 %. For the P48SH magnets in exon 5, 11, 14, and 15, the Mr consistencies of the other magnets were less than 0.4 %. There were obvious microscopic fluctuations observed for the P48UH magnets. As detailed in Fig. 5(b) Fig. 5(b) , the magnetic angles of the three types of magnets displayed major differences. The ratio of the P42H, P48SH, and P48UH magnets with less than 1° were approximately 26.7%, 80%, and 46.7%, respectively. Therefore, after optimizing the composition designs and processes, the P48SH magnets exhibited a substantial improvement in orientation degree which gave them a small magnetization angle relative to the P42H magnets. In regard to the P48UH magnets with GBD, although the local orientation near the surface of the magnet was improved, the uneven diffusion caused by the squareness resulted in substantial deterioration (for example, the ratio of Hk/Hcj decreased to a greater degree). 3.4. Magnetic field stability 2 Fig. 6(a) Fig. 6(a) shows the results of irreversible demagnetization experiments at higher temperatures for the CPMU18 made of PrFeB magnets (two 50 mm × 30 mm × 3.3 mm sized magnets spliced with one 50 mm × 30 mm × 6.6 mm sized magnet; orientation: 6.6 mm). As can be seen in the figure, the magnetic fields of the PrFeB magnets were stable at 25 ℃, and following the 75 ℃ or 100 ℃ treatments, the P42H and P48SH magnets displayed obvious irreversible demagnetization. The stability of the P48UH magnet was observed to be improved by 75 ℃ or 100 ℃ treatments. Fig. 6(b) Fig. 6(b) shows the magnetic field stability of the remaining P48SH magnets of the CPMU18 at a no-load state after 13 months (magnet size: 65 mm × 25 mm × 5.9 mm; orientation: 5.9 mm). As detailed in the figure, after a long period in their natural state, the P48SH magnets displayed different degrees of demagnetization. For example, the demagnetization rates of the 10 randomly selected magnets ranged between 1.25 % and 2.15 %. These results were determined to be closely related to such factors as the P48SH being characterized by large temperature coefficients, uneven microstructures, exposure to higher temperature environments during the summer months, and so on. 4. The CPMU18 with PrFeB 1 The design index of the effective magnetic field peak value B eff at 77 K for the first CPMU18 made of PrFeB magnets for SSRF was approximately 0.94 T at a gap of 6.0 mm. Table 2 Table 2 shows the design parameters of the CPMU18 utilizing PrFeB magnets. It can be seen in the table that, if the P42H magnets were used as the magnetic field source, the effective magnetic field peak value could not reach the index, and the smaller Hcj resulted in a poor resistance to demagnetization at room temperature. However, if the P48UH magnets were used as the magnetic field source, the CPMU18 could reach the designed 0.94 T at 77 K. In addition, the CPMU18 using P48UH magnets exhibited better demagnetization resistance. The magnetization angle of the magnets was observed to be poor, and at the same time, it had a relatively higher manufacturing cost. Therefore, further research and improvements are required to obtain an acceptable application level. The P48SH magnets displayed excellent comprehensive performance. The effective magnetic field peak value of the CPMU18 with P48SH magnets reached 0.96 T at 77 K, and the higher Hcj resulted in a stronger anti-demagnetization resistance. Furthermore, the smaller magnetization angle caused the CPMU18 to have a good magnetic field quality. 1 1 Magnet/size 6 1 PrFeB/65.0 mm × 25.0 mm × 5.9 mm 1 1 Pole/size 6 1 DT4C / 43.0 mm × 20.0 mm × 3.0 mm 1 1 Gap/L 6 1 6.0 mm/18.0 mm 1 1 Grade 2 1 P42H 2 1 P48SH 2 1 P48UH 1 1 T(K) 1 1 300 1 1 77 1 1 300 1 1 77 1 1 300 1 1 77 1 1 Br(T) 1 1 1.30 1 1 1.50 1 1 1.38 1 1 1.56 1 1 1.37 1 1 1.53 1 1 Hcj(kA/m) 1 1 1400 1 1 6000 1 1 1580 1 1 6000 1 1 2152 1 1 6000 1 1 B eff (T) 1 1 0.82 1 1 0.93 1 1 0.85 1 1 0.96 1 1 0.85 1 1 0.94 1 1 Hd(kA/m) 1 1 1120 1 1 1265 1 1 1160 1 1 1320 1 1 1160 1 1 1300 Fig. 7(a) Fig. 7(a) shows the effective magnetic field peak values at the different gaps of the CPMU18 with P48SH magnets. It can be seen that the B eff values were 0.82 T and 0.92 T at 300 K and 77 K, respectively, when the gap was 6 mm. However, there was still a difference observed from the designed effective magnetic field. The main reasons for this problem were as follows: ① The finite element calculation accuracy of the magnetic field for the CPMU was approximately 1 %, and a certain amount of error occurred between the measured and calculated values. ② The effective peak magnetic field is closely related to the magnetic gap of the CPMU18, and there may be some error in the calculation of the gap of the CPMU18. ③ The decreases in cycle length experienced by the CPMU18 at low temperatures caused some loss of the magnetic field. ④ The unstable characteristics of the PrFeB magnets themselves caused large, irreversible magnetic field losses. The comprehensive analyses of similar CPMU research results from international research groups along with the experimentally obtained demagnetization data of the P48SH magnets are shown in Fig. 6(b) Fig. 6(b) . It was determined that the irreversible demagnetization caused by the environmental temperatures experienced by the P48SH magnets for the CPMU18 was the main reason for the failure of the CPMU18 magnetic field to reach the design index. The contribution ratios of the magnetic field calculation, gap measurement error, and decreases in CPMU period length to the magnetic field losses remain areas for further study and analysis in the future. Fig. 7(b) Fig. 7(b) shows the magnetic field phase error of CPMU18 with P48SH magnets when gap was 6.0 mm and the temperature was 80 K. It can be seen that the RMS phase error of CPMU18 was about 4.99 °. 5. Conclusion 1 The (BH) max +Hk values of the three kinds of PrFeB magnets (P42H, P48SH, and P48UH) were 57.4, 65.3, and 66.1, respectively. Compared with Sm 2 Co 17 and NdFeB, PrFeB magnets can achieve greatly increased Br and Hcj values at low temperature. Through the optimization of the preparation method and composition design, the orientation degree of the P42H, P48UH, and P48SH magnets gradually improved, while the P48UH magnet exhibited a decreased Hk/Hcj ratio due to the uneven distribution of Tb. The magnetic field uniformity of the P48SH magnets was found to be good, but the magnetization angles of the P42H and P48UH magnets remain to be further improved. With the increase in Hcj, the magnetic field stability of the P42H, P48SH, and P48UH magnets gradually improved; in particular, P48UH was found to withstand high temperature baking of the CPMU. The three kinds of PrFeB magnets prepared in this work have application value in the field of synchrotron radiation, free electron lasers, and space instruments. For P42H magnets, the Hcj is lower and the magnetization angle is too large, so the magnetic circuit design should fully consider demagnetization, uniformity of magnetic field, and other factors. If P48UH can solve the problem of its magnetization angle, it is expected to be more important for practical applications. The comprehensive performance of P48SH magnets was found to be excellent. Using the PrFeB permanent magnet as magnetic field source, the first cryogenic permanent magnet undulator CPMU18 of China has been developed; when the temperature was 80 K and the gap was 6.0 mm, the magnetic field measurement results showed that the effective the peak field was 11.76 % higher than at 300 K, reaching 0.92 T, with an RMS phase error of about 4.99 °. References H. Onuki . Wigglers, Undulators and Their Applications . ( London : Taylor & Francis , 2003 ),pp 176 - 255 . Wigglers, Undulators and Their Applications Z.H. Mai ., Synchrotron light source and its applications . 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Inhomogeneity of external magnetic field for permanent magnet 10.1007/s41365-019-0640-0 This work was supported by project of the State Key Lab of Advanced Metals and Materials (No. 2016-Z03). 2018-11-03 2019-03-05 2019-04-03 2019-07-11 2019-08-01 2021-04-11 © China Science Publishing & Media Ltd. (Science Press), Shanghai Institute of Applied Physics, the Chinese Academy of Sciences, ChineseNuclear Society and Springer Nature Singapore Pte Ltd. 2019 This is a post-peer-review, pre-copyedit version of an article published in Nuclear Science and Techniques. The final authenticated version is available online at: http://dx.doi.org/10.1007/s41365-019-0640-0 http://dx.doi.org/10.1007/s41365-019-0640-0 . 2019 Nuclear Science and Techniques 08 30