Revealing the Broadband Terahertz Faraday Rotation Mechanism in Rare-Earth Doped Yttrium Iron Garnets

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As a magneto-optical effect, the Faraday effect depends on the Verdet constant of the magnetic materials and enables integrated optical modulators and nonreciprocal photonic devices. Ferrimagnetic garnet, e.g. yttrium iron garnet (YIG) is the most studied material for terahertz (THz) Faraday effects. However, current works neglect the correlation between the Verdet constant and the electromagnetic (EM) parameters, which is vital for the design of high-performance THz non-reciprocal devices. Here, we investigate the mechanisms of the broadband THz rotations in undoped YIG and rare-earth doped YIG (La-doped) by polarization-sensitive THz time-domain spectroscopy. We observe a frequency-independent THz rotation angle (11/30 degree/mm) and related Verdet constant (70/170 degree/mm/T) for the YIG/ La-YIG, and further retrieve the EM parameters of YIG within the test range (0.3-2.5 THz). Based on these results, we establish a systematic methodology to describe the connections between the THz Faraday effects and corresponding materials. Our works provide critical foundation for the design and applications of the low-loss nonreciprocal THz devices in the future.

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Solid State Phenomena (Volume 369)

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59-65

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March 2025

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© 2025 Trans Tech Publications Ltd. All Rights Reserved

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[1] Rayleigh. Nature Vol. 64(1901), p.577–578.

Google Scholar

[2] P. Zhou, G. Liu, Y. Yang, Y. Hu, S. Ma, H. Xue, Q. Wang, L. Deng, and B. Zhang. Phys. Rev. Lett. vol.125(2020), p.263603.

Google Scholar

[3] G. Liu, Y. Yang, X. Ren, H. Xue, X. Lin, Y. Hu, H. Sun, B. Peng, P. Zhou, Y. Chong, and B. Zhang. Phys. Rev. Lett. vol. 125(2020), p.133603.

Google Scholar

[4] Y. Li, D. Zhang, M. Luo, Q. Yang, F. Fan, S. Chang, and Q. Wen. Opt. Express vol. 29(2021), pp.23540-23548.

Google Scholar

[5] Y. Li, T. Li, Q. Wen, F. Fan, Q. Yang, and S. Chang. Opt. Express vol. 28(2020), pp.21062-71.

Google Scholar

[6] Q. Xue, Y. Zhang, D. Zhao, Q. Yang, H. Zhang, F. Fan, and Q. Wen. Appl. Phys. Lett. vol. 123(2023), p.141903(1-8).

Google Scholar

[7] K. R. Wangsness. Phys. Rev. vol. 95(1954), pp.339-346.

Google Scholar

[8] G. S. Krinchik and M. V. Chetkin. Soviet Physics Uspekhi vol. 39(1969), pp.307-319.

DOI: 10.1070/pu1969v012n03abeh003902

Google Scholar

[9] V. Dmitriev. Photonics and Nanostructures – Fundamentals and Applications vol. 11(2013), p.203–209.

Google Scholar

[10] A. J. Sievers, and M. Tinkham. Phys. Rev. vol. 24(1961), pp.321-325.

Google Scholar

[11] G. A. Allen and G. F. Dionne. J. of Appl. Phys. vol. 93(2003), pp.6951-6853.

Google Scholar

[12] G. S. Krinchik and M. V. Chetkin. J. Exptl. Theoret. Phys. vol. 41(1961), pp.673-680.

Google Scholar

[13] L. D Landau, and E. M. Lifshitz. Sov. Phys. vol. 8(1935), pp.153-169.

Google Scholar

[14] J. Kaplan, C. Kittel. J. Chem. Phys. vol. 21(1953), p.760–761.

Google Scholar

[15] A. K. Zvedin and V. A. Kotov. Modern Magnetooptics and Magnetooptical Materials (Institute of Physics Publishing, Moscow, 1983).

Google Scholar

[16] G. S. Krinchik and M. V. Chetkin. J. Exptl. Theoret. Phys. vol. 4(1961), pp.729-733.

Google Scholar

[17] M. V. Exter, Ch. Fattinger, and D. Grischkowsky. Opt. Lett. vol. 14(1989), pp.1128-1130

Google Scholar

[18] T. Horák, G. Ducournau, M. Mičica, K. Postava, J. B. Youssef, J. Lampin, and M. Vanwolleghem. IEEE Transactions on THz Sci. and Techn. vol. 7(2017), pp.563-570.

Google Scholar

[19] M. Shalaby, M. Peccianti, Y. Ozturk1, and R. Morandotti. Nat. Commun., vol. 4(2012), pp.1558-1562.

Google Scholar