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Localized surface plasmon resonance of cylindrical magneto optical particles provides an important mechanism for the formation of chiral edge states in two-dimensional magneto-optical photonic crystals. These states are an electromagnetic analogy of the so-called chiral edge state's (CESs) in a quantum Hall system where the power transmission is unidirectional due to particular topological properties of the bands. Just like their electronic counterpart, the number of optical CESs in the band gap opened by an applied magnetic field is determined by the sum of the Chern numbers of the lower bands. For a two-dimensional photonic crystal composed of ferrite rods magnetized along their axis, the coupling of the localized surface plasmon resonance states of each rod results in a narrow flat band-gap, which contains one-way edge modes arising from the circulation of the energy flow around each rod excited by the resonance with broken time-reversal symmetry. So far the interpretation of the resonance-related chiral edge states are based on the long-wavelength approximation of the localized surface plasmon resonance of an individual magneto-optical particle. Though the results agree with the experimental results qualitatively, an obvious quantitative deviation is still obvious. In this work we apply the scattering theory to analyze the resonance condition and the features of both the far-field and the near-field at resonance for cylindrical magneto-optical particles. Our calculation shows that the splitting of scattering peaks of different orders will occur due to the magneto-optical effect. Such a split is observed between an (+n)-peak and an (-n) peak, as a sign of the broken time-reversal symmetry, and also between peaks of lower-order and higher-order. Another important feature is the simultaneous occurring of the far-field resonance and the near-field resonance, where the latter is characterized by a peak of energy-flow circulation around the particle. Based on this model the effects of particle size on the resonance peaks are discussed. It is shown that the resonance peaks are moved and broadened with the particle size increasing. The results explain the obvious deviation of the position of the resonance band-gap from the predicted frequency according to the previous long-wavelength approximation. Furthermore, the calculation of a particle of moderately-large size (nearly one-tenth of the incident wavelength) demonstrates the appearance of higher-order modes up to n=4 circling around the particle surface. This implies that these higher-order modes may also make non-trivial contribution to the formation of the flat band-gap observed in a photonic crystal of ferrite-rods and affect the behaviours of the chiral-edge state existing in such a gap. Particularly, it may be helpful in realizing the multimodes of chiral edge states in magneto-optical photonic crystals.
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Keywords:
- magneto-optic effects /
- surface plasmon /
- photonic crystals
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[7] Fang K, Yu Z, Fan S 2011 Phys. Rev. B 84 075477
[8] Skirlo S A, Lu L, Soljacic M 2014 Phys. Rev. Lett. 113 113904
[9] Liu S Y, Lu W L, Lin Z F, Chui S T 2011 Phys. Rev. B 84 045425
[10] Lian J, Fu J X, Gan L, Li Z Y 2012 Phys. Rev. B 85 125108
[11] Poo Y, Wu R, Liu S, Yang Y, Lin Z, Chui S T 2012 Appl. Phys. Lett. 101 081912
[12] Chui S T, Liu S, Lin Z 2013 Phys. Rev. B 88 031201
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[14] Fan X, Zheng W, Singh D J 2014 Light: Sci. Appl. 3 e179
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[16] Zou W B, Zhou J, Jin L, Zhang H P 2012 Acta Phys. Sin. 61 097805 (in Chinese) [邹伟博, 周骏, 金理, 张昊鹏 2012 61 097805]
[17] Zhu H, Yan Z D, Zhan P, Wang Z L 2013 Acta Phys. Sin. 62 178104 (in Chinese) [朱华, 颜振东, 詹鹏, 王振林 2013 62 178104]
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[1] Inoue M, Fujii T 1997 J. Appl. Phys. 81 5659
[2] Temnov V V, Armelles G, Woggon U, Guzatov D, Cebollada A, Garcia-Martin A, Garcia-Martin J M, Thomay T, Leitenstorfer A, Bratschitsch R 2010 Nat. Photo. 4 107
[3] Liang H, Liu H, Zhang Q, Fu S F, Zhou S, Wang X Z 2015 Chin. Phys. B 24 067807
[4] Haldane F D M, Raghu S 2008 Phys. Rev. Lett. 100 013904
[5] Wang Z, Chong Y D, Joannopoulos J D, Soljacic M 2009 Nature 461 772
[6] Poo Y, Wu R, Lin Z, Yang Y, Chan C T 2009 Phys. Rev. Lett. 106 093903
[7] Fang K, Yu Z, Fan S 2011 Phys. Rev. B 84 075477
[8] Skirlo S A, Lu L, Soljacic M 2014 Phys. Rev. Lett. 113 113904
[9] Liu S Y, Lu W L, Lin Z F, Chui S T 2011 Phys. Rev. B 84 045425
[10] Lian J, Fu J X, Gan L, Li Z Y 2012 Phys. Rev. B 85 125108
[11] Poo Y, Wu R, Liu S, Yang Y, Lin Z, Chui S T 2012 Appl. Phys. Lett. 101 081912
[12] Chui S T, Liu S, Lin Z 2013 Phys. Rev. B 88 031201
[13] Chui S T, Lin Z 2014 Chin. Phys. B 23 117802
[14] Fan X, Zheng W, Singh D J 2014 Light: Sci. Appl. 3 e179
[15] Cong C, Wu D J, Liu X J 2012 Acta Phys. Sin. 61 047802 (in Chinese) [丛超, 吴大建, 刘晓峻 2012 61 047802]
[16] Zou W B, Zhou J, Jin L, Zhang H P 2012 Acta Phys. Sin. 61 097805 (in Chinese) [邹伟博, 周骏, 金理, 张昊鹏 2012 61 097805]
[17] Zhu H, Yan Z D, Zhan P, Wang Z L 2013 Acta Phys. Sin. 62 178104 (in Chinese) [朱华, 颜振东, 詹鹏, 王振林 2013 62 178104]
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