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
“…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
“…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
“…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
Intrinsic localized modes ͑ILMs͒ in a quasi-1D antiferromagnetic material ͑C 2 H 5 NH 3 ͒ 2 CuCl 4 are counted by using a novel nonlinear energy magnetometer. The ILMs are produced by driving the uniform spin wave mode unstable with an intense microwave pulse. Subsequently a subset of these ILMs become captured by and locked to a cw driver so that their properties can be examined at a later time with a tunable cw low power probe source. Four-wave mixing is used to enhance the emission signal from the few large amplitude ILMs over that associated with the many small amplitude plane wave modes. A discrete step structure observed in the emission signal is identified with individual ILMs becoming unlocked from the driver. At most driver power and frequency settings the resulting emission step structure appears uniformly distributed; however, sometimes, nearby in parameter space, families of emission steps are evident as the driver frequency or power is varied. Two different experimental methods give consistent results for counting individual ILMs. Because of the discreteness in the emission both the size of an ILM and its energy can be estimated from these experiments. For the uniformly distributed case each ILM extends over ϳ42 antiferromagnetic unit cells and has an energy value of 1.3ϫ 10 −12 J while for the case with families the ILM length becomes ϳ54 antiferromagnetic unit cells with an energy of 1.5ϫ 10 −12 J. An unresolved puzzle is that the emission step height does not depend on experimental parameters the way classical numerical simulations suggest.
“…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
The results of the study of the electromagnetic waves resonant reflection from and transmission through planar metamaterials based on periodic structures, which are composed of some elements consisted of nonlinear materials are presented.
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