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METHOD FOR STRENGTHENING THE MAGNETO-OPTICAL EFFECT OF KERR BY USING PHOTON-CRYSTAL STRUCTURES

机译:利用光子晶体结构增强KERR的磁光效应的方法

摘要

1. A method of enhancing the magneto-optical Kerr effect by forming a magnetic photonic crystal with a periodically structured surface of a magnet. 2. The method according to claim 1, characterized in that the magnet has an inverted colloidal crystal structure with a period of structure from 250 to 1900 nm. The method according to claim 2, characterized in that the surface morphology of the magnetic photonic crystal is determined by the cutoff level of the densest face-centered cubic packing of microspheres in the 111 plane within the colloidal crystal layer. The method according to claim 3, characterized in that the formation of the magnetic photonic crystal is carried out by the template method by electrodeposition of metal in the pores of synthetic opal, followed by removal of the matrix. The method according to claim 4, characterized in that the magnetic photonic crystal is a film with a thickness of from 0.1 to 60 microns. The method according to claim 4, characterized in that the inverted photonic crystal consists of Ni, Co, Fe or alloys containing these metals. The method according to claim 4, characterized in that the degree of filling the voids of the colloidal crystal with a metal is more than 95%. The method according to claim 4, characterized in that the cut-off level of the structure of the inverted photonic crystal is controlled by reflection spectroscopy during metal deposition. The method according to claim 4, characterized in that the heterogeneity of the cutoff level of the outer layer of the magnetic photonic crystal within the layer does not exceed 10% of the structure period over an area of 1 cm. The method according to claim 9, characterized in that the position of the reflection maxima in the spectra of the magnetic photonic crystal in the range of 300-2000 nm is determined by the surface morphology of the outer layer of the
机译:1.一种通过形成具有磁体的周期性结构化表面的磁性光子晶体来增强磁光克尔效应的方法。 2.根据权利要求1所述的方法,其特征在于,所述磁体具有倒置的胶体晶体结构,其结构周期为250至1900nm。 3.根据权利要求2所述的方法,其特征在于,所述磁性光子晶体的表面形态由所述胶体晶体层内的<111>面中的最密集的以面心为中心的微球立方堆积的截止水平来确定。 4.根据权利要求3所述的方法,其特征在于,所述磁性光子晶体的形成是通过模板方法通过将金属电沉积在合成蛋白石的孔中,然后去除所述基质来进行的。 5.根据权利要求4所述的方法,其特征在于,所述磁性光子晶体是厚度为0.1至60微米的膜。 5.根据权利要求4所述的方法,其特征在于,所述反向光子晶体由Ni,Co,Fe或包含这些金属的合金组成。 5.根据权利要求4所述的方法,其特征在于,用金属填充所述胶体晶体的空隙的程度大于95%。 5.根据权利要求4所述的方法,其特征在于,在金属沉积期间,通过反射光谱法控制所述倒置光子晶体的结构的截止水平。 5.根据权利要求4所述的方法,其特征在于,在该层内的磁性光子晶体的外层的截止能级的异质性在1cm的面积内不超过结构周期的10%。 10.根据权利要求9所述的方法,其特征在于,在所述磁光子晶体的光谱中,在300-2000nm范围内的反射最大值的位置由所述外层的外层的表面形态确定。

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