2000
DOI: 10.1088/0022-3727/33/22/306
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Calculation of nonlinear magnetic susceptibility tensors for a uniaxial antiferromagnet

Abstract: In this paper, we present a derivation of the nonlinear susceptibility tensors for a two-sublattice uniaxial antiferromagnet up to the third-order effects within the standard definition by which the rf magnetization m is defined as a power series expansion in the rf fields h with the susceptibility tensors as the coefficients. The starting point is the standard set of torque equations of motion for this problem. A complete set of tensor elements is derived for the case of a single-frequency input wave. Within… Show more

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Cited by 17 publications
(20 citation statements)
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“…For such states, it is convenient to introduce new variables S + n = S x n + iS y n which satisfy [396] iṠ The anharmonicity due to spin interactions is intrinsically soft [10,243], so that for D = 0 one needs to have a gap in the linear wave spectrum for localized excitations to exist: Ω b < ω 0 for DBs. This gap is generated by the anisotropy J z = J x , J y , see Eq.…”
Section: The Case Of Xy Isotropic Exchange Interactionmentioning
confidence: 99%
“…For such states, it is convenient to introduce new variables S + n = S x n + iS y n which satisfy [396] iṠ The anharmonicity due to spin interactions is intrinsically soft [10,243], so that for D = 0 one needs to have a gap in the linear wave spectrum for localized excitations to exist: Ω b < ω 0 for DBs. This gap is generated by the anisotropy J z = J x , J y , see Eq.…”
Section: The Case Of Xy Isotropic Exchange Interactionmentioning
confidence: 99%
“…Since the third order nonlinearity ͑3͒ of the antiferromagnet makes possible a four-wave mixing experiment [28][29][30] this method has been used to observe in emission the small number of ILMs that remain locked to the driver. The transverse magnetization components oscillating at the different frequencies in the four-wave mixing process are illustrated in Fig.…”
Section: B Nonlinear Measurement Techniquesmentioning
confidence: 99%
“…Here, we review the four wave mixing for the simpler case of an easy z-axis antiferromagnet. 29,30 Writing the torque equation for the uniform mode in circularly polarized modes in the usual way and then taking the next time derivation one obtains the nonlinear equation of motion where the ͑ϩ͒ sign identifies one circularly polarized mode and the ͑Ϫ͒ sign the other for each of the sublattices A and B.…”
Section: Appendix A: the Third Order Nonlinear Magnetization Of An Eamentioning
confidence: 99%
“…The metamaterial parameters are d = d x = d y = 0.3 mm a 1 = 0.11 mm and a 2 = 0.09 mm, λ, nm Luminescence enhancement 2w = 0.004 mm, and h = 0.05 mm. As a material for the substrate, M nF 2 antiferromagnetic film is considered [13], [14]. The external static magnetic field (ESMF) is applied to the system in the Faraday geometry.…”
Section: A Magnetically Controllable Array On Nonlinear Antiferromagmentioning
confidence: 99%