Supplemental material Partially inverse spinel ZnFe2O4 with high saturation magnetization synthesized via a molten salt route Jiangtao Wu1, Nan Li1, Jun Xu1, Yaqi Jiang1, Zuo-Guang Ye1,2*, Zhaoxiong Xie1*, and Lansun Zheng1 1 State Key Laboratory for Physical Chemistry of Solid Surface & Department of Chemistry, College of Chemistry and Chemical Engineering, Xiamen University, Xiamen 361005, China 2 Department of Chemistry and 4D LABS, Simon Fraser University, 8888 University Drive, Burnaby, British Colombia, V5A1S6 Canada Figure S1. Non-magnetic part of the molten salt synthesis: () ZnO, () -Fe2O3. Figure S1 shows the XRD patterns of non-magnetic part of molten salt synthesis, consisting of ZnO and -Fe2O3. These by-products were separated from PI-ZFO with a magnet. 1 Figure S2. XRD patterns of inversed spinel LiFe5O8. Figure S2 shows the inversed spinel LiFe5O8 prepared by mixing 1 mmol Fe2(SO4)3 5H2O and 0.1 mol LiCl H2O and heating at 850 °C for 1 hour. The product has been washed by distilled water to remove excess LiCl. Diffraction patterns can be well indexed by inversed spinel LiFe5O8. (JCPDS No. 13-0273) 2 Figure S3. XRD patterns of the final product of LiFe 5 O8 powder reacting with ZnSO47H2O at 850 °C without LiCl for 1 hour. (): ZnFe2O4, () ZnO, () -Fe2O3. 1 mmol LiFe5O8 powder and 2.5 mmol ZnSO47H2O were grinded without LiCl H2O. The mixture was heated at 850 °C for 1 hour. XRD pattern (Figure S3) reveals the products are the mixture of ZnFe2O4, ZnO and -Fe2O3. However, this ZnFe2O4 product is antiferromagnetic. 3 Table SІ. Reported values of saturation magnetization and coercive field for ZnFe2O4 prepared by various methods. MS (emu.g-1) Coercive Temperature Size field (Oe) (K) (nm) Synthesis method Ref. 80 117 65.4 38 7 19 102.4 114 300 2 10 6 5000 5000 9.8 4 Molten salt Molten salt Thermal decomposition Hydrothermal method This work This work 1 2 25 400 5 12 Sonochemical emulsification 3 76.8 42.5 200 400 5 5 6.6 14.8 Polyol hydrolysis Polyol hydrolysis 4 4 70 310 3 3.7 Micelles 5 30 650 3 2.8 Micelles 5 61.87 54.64 11.9 110 50 544.8 80 300 2 300 300 32 Hydrothermal Hydrothermal Self-propagating combustion 6 6 7 37 73 10 88.4 56.6 Not given 15 Not given Not given Not given 4.2 10 300 4.2 300 47 Ball milling 10 Aerogel procedure+ball milling 11 Ball milling 10 Ball milling Thin film Pulsed laser deposition 20.7 40.3 58 35 Not given Not given Not given Not given 4.2 4.2 5 4.2 36 50 9 5.5 8 9 10 11 12 Ball milling 13 Ball milling +calcinations at 773 K 13 Ball milling 14 Coprecipitation 15 Table SІ presents the values of saturation magnetization and coercive field for ZnFe2O4 so far reported in literatures, in comparison with values obtained in this work. It can be found from these data that the saturation magnetization of our PI-ZFO is the highest to date (117 emu/g at 2 K, 80 emu/g at 300 K). Furthermore, the coercive field of our PI-ZFO is almost one-tenth of those reported both at 300 K and 2 K. 4 References 1 C. G. Yao, Q. S. Zeng, G. F. Goya, T. Torres, J. F. Liu, H. P. Wu, M. Y. Ge, Y. W. Zeng, Y. W. Wang, and J. Z. Jiang, J. Phys. Chem. C 111, 12274 (2007). 2 C. Upadhyay, H. C. Verma, V. Sathe, and A. V. Pimpale, J. Magn. Magn. Mater. 312, 271 (2007). 3 M. Sivakumar, T. Takami, H. Ikuta, A. Towata, K. Yasui, T. Tuziuti, T. Kozuka, D. Bhattacharya, and Y. Iida, J. phys. Chem. B 110, 15234 (2006). 4 S. Ammar, N. Jouini, F. Fiévet, Z. Beji, L. Smiri, P. Moliné, M. Danot, and J-M. Grenéche, J. Phys.: Condens. Matter 18, 9055 (2006). 5J. F. Hochepied, P. Bonville, and M. P. Pileni, J. Phys. Chem. B 104, 905 (2000). 6S. H. Yu, T. Fujino, and M. Yoshimura, J. Magn. Magn.Mater. 256, 420 (2003). 7H. Xue, Z. H. Li, X. X. Wang, and X. Z. Fu, Mater. Lett. 61, 347 (2007). 8G. F. Goya and H. R. Rechenberg, J. Magn. Magn.Mater. 203, 141 (1999). 9H. H. Hamdeh, J. C. Ho, S. A. Oliver, R. J. Willey, G. Oliveri, and G. Busca, J. Appl. Phys. 81, 1851 (1997). 10C. N. Chinnasamy, A. Narayanasamy, N. Ponpandian, K. Chattopadhyay, H. Guérault, and J. M. Creneche, J. Phys.: Condens. Matter. 12, 7795 (2000). 11G. F. Goya and H. R. Rechenberg, J. Magn. Magn. Mater. 197, 191 (1999). 12N. Wakiya, K. Muraoka, T. Kadowaki, T. Kiguchi, N. Mizutani, H. Suzuki, and K. Shinozaki, J. Magn. Magn. Mater. 310, 2546 (2007). 13G. F. Goya, H. R. Rechenberg, M. Chen, and W. B. Yelon, J. Appl. Phys. 87, 8005 (2000). 14F. J. Burghart, W. G. Potzel, M. Kalvius, E. Schreier, G. Grosse, D. R. Noakes, W. Schäfer, W. Kockelmann, S. J. Campbell, W. A. Kaczmarek, A. Martin, and M. K. Krause, Physica B 289, 286 (2000). 15T. Sato, K. Haneda, M. Seki, and T. Iijima, Appl. Phys. A 50, 13 (1990). 5