An approach to compute the polarizability tensor of magnetic nanoparticles having general ellipsoidal shape is presented. We find a surprisingly excellent quantitative agreement between calculated and experimental magneto-optical spectra measured in the polar Kerr configuration from nickel nanodisks of large size (exceeding 100 nm) with circular and elliptical shape. In spite of its approximations and simplicity, the formalism presented here captures the essential physics of the interplay between magneto-optical activity and the plasmonic resonance of the individual particle. The results highlight the key role of the dynamic depolarization effects to account for the magneto-optical properties of plasmonic nanostructures.
©2013 Optical Society of AmericaOCIS codes: (290.5850) Scattering, particles; (160.1190) Anisotropic optical materials; (160.3820) Magneto-optical materials.
References and links1. M. Sandtke and L. Kuipers, "Slow guided surface plasmons at telecom frequencies," Nat. Photonics 1(10), 573-576 (2007). 2. V. E. Ferry, L. A. Sweatlock, D. Pacifici, and H. A. Atwater, "Plasmonic nanostructure design for efficient light coupling into solar cells," Nano Lett. 8(12), 4391-4397 (2008). 3. S. Lal, S. Link, and N. J. Halas, "Nano-optics from sensing to waveguiding," Nat. Photonics 1(11), 641-648 (2007 5333-5338 (2011). 12. J. Chen, P. Albella, Z. Pirzadeh, P. Alonso-González, F. Huth, S. Bonetti, V. Bonanni, J. Åkerman, J. Nogués, P.Vavassori, A. Dmitriev, J. Aizpurua, and R. Hillenbrand, "Plasmonic nickel nanoantennas," Small 7 ( Ration. Mech. Anal. 188(1), 93-116 (2008). 47. W. L. Bragg and A. B. Pippard, "The form birefringence of macromolecules," Acta Crystallogr. 6(11), 865-867 (1953). 48. One should consider also the phase difference due to the incoming light hitting a finite size body. There are several ways to account for this phase difference reported in literature [30,32, 49]. Although, we verified that inclusion of these corrections have negligible effects, and therefore for sake of clarity we neglect them. We point out, in addition, that for the particular geometry used in our experiments, namely perpendicular incidence over flat disks, this phase difference effects are rigorously zero. 385-420 (1904). 60. A. Lakhtakia, "General theory of Maxwell-Garnett model for particulate composites with bi-isotropic host materials," Int. J. Electron. 73(6), 1355-1362 (1992). 61. M. Abe, "Derivation of non-diagonal effective dielectric-permeability tensors for magnetized granular composites," Phys. Rev. B 53(11), 7065-7075 (1996). 62. M. Abe and T. Suwa, "Surface plasma resonance and magneto-optical enhancement in composites containing multicore-shell structured nanoparticles," Phys. 50(15), 950-952 (1987). 64. T. K. Xia, P. M. Hui, and D. Stroud, "Theory of Faraday rotation in granular magnetic materials," J.