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Ultrasmooth metal nanolayers for plasmonic applications: surface roughness and specific resistivity

机译:用于等离子体的超光滑金属纳米层:表面粗糙度和比电阻

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摘要

The future of plasmonic devices depends on effective reduction of losses of surface plasmon-polariton waves propagating along metal-dielectric interfaces. Energy dissipation is caused by resistive heating at the skin-deep-thick outer layer of metal and scattering of surface waves on rough metal-dielectric interfaces. Fabrication of noble metal nanolayers with a smooth surface still remains a challenge. In this paper, Ag layers of 10, 30, and 50 nm thickness deposited directly on fused-silica substrates and with a 1 nm wetting layer of Ge, Ti, and Ni are examined using an atomic-force microscope and four-probe resistivity measurements. In the case of all three wetting layers, the specific resistivity of silver film decreases as the thickness increases. The smallest, equal 0.4 nm root mean squared roughness of Ag surface of 10 nm thickness is achieved for Ge interlayer; however, due to Ge segregation the specific resistivity of silver film in Ag/Ge/SiO_2 structures is about twice higher than that in Ag/Ti/SiO_2 and Ag/Ni/SiO_2 sandwiches.
机译:等离子体设备的未来取决于有效减少沿金属-电介质界面传播的表面等离子体激元波的损耗。能量耗散是由表皮较厚的金属外层的电阻加热和粗糙的金属-电介质界面上的表面波散射引起的。具有光滑表面的贵金属纳米层的制造仍然是挑战。在本文中,使用原子力显微镜和四探针电阻率测量方法检测厚度为10、30和50 nm的Ag层直接沉积在熔融石英衬底上,并具有1 nm的Ge,Ti和Ni润湿层。 。在所有三个润湿层的情况下,银膜的电阻率随厚度增加而减小。 Ge夹层的厚度为10 nm的Ag表面最小,均等的0.4 nm均方根粗糙度;然而,由于Ge的偏析,Ag / Ge / SiO_2结构中银膜的电阻率比Ag / Ti / SiO_2和Ag / Ni / SiO_2夹层的电阻率高约两倍。

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