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Optical Properties of Pure and Alloyed Silver-Copper Nanoparticles Embedded and Coupled in Dielectric Matrixes

机译:嵌入和耦合在介电基质中的纯和合金银铜纳米粒子的光学性质

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In this study by using the boundary element method, influence of various parameters on the response to electromagnetic radiation for pure and alloyed silver-copper was investigated. The results demonstrate decreasing interparticle gap from 20 nm to 1 nm for silver coupled nanoparticles leads to shifting the wavelength of optical extinction peak from 362 nm to 393 nm. Decreasing interparticle gap from 20 nm to 1 nm for Cu coupled nanoparticles leads to shifting the wavelength of optical extinction peak from 323 nm to 336 nm. By an increase in the medium refractive index of 1 to 2 the peak of optical extinction for a coupled Cu nanoparticles with 1 nm gap distance the wavelength of plasmon resonance peak shifted from 336 nm to 366 nm and longitudinal plasmon resonance peak shifted from 498 nm to 559 nm. By changing the composition of an alloy of copper and silver nanoparticles with diameter of 10 nm in dielectric matrix with refractive index 1.3 the wavelength of plasmon resonance peak shifted from 378 nm for pure silver nanoparticles to 530 nm for pure copper nanoparticles. In addition for Cu-Ag alloy coupled nanoparticles with 1 nm interparticle gap, the wavelength of resonance peak shifted from 420 nm for pure silver nanoparticles to 544 nm for pure copper nanoparticles. In the case of embedded nanoparticles for coupled silver nanoparticles with 6 nm gap distance, the wavelength of resonance peak shifted from 396 nm to 409 nm, and for coupled silver nanoparticles with 2 nm gap distance, the wavelength of resonance peak shifted from 414 nm to 430 nm. Furthermore for coupled Cu nanoparticles with 2 nm gap distance, the wavelength of resonance peak shifted from 575 nm to 582 nm. The results could be employed for plasmatic sensor design and fabrication.
机译:在本研究通过使用边界元方法,研究了各种参数对纯和合金化银铜的电磁辐射响应的影响。结果表明,对于银偶极纳米颗粒20nm至1nm的颗粒间隙降低,导致从362nm至393nm的光学消光峰的波长移位。从20nm偶联纳米颗粒从20nm至1nm减小颗粒间隙导致从323nm至336nm的光学消光峰的波长移位。通过增加1至2的介质折射率,对于具有1nm间隙距离的偶联Cu纳米颗粒的光学消光峰值从336nm到366nm偏移的等离子体共振峰的波长从498nm移位到366nm至366nm且纵向等离子体共振峰559 nm。通过在介电基质中改变直径为10nm的铜和银纳米颗粒的组合物,折射率1.3从378nm偏移378nm的纯银纳米颗粒的波长为530nm,用于纯铜纳米粒子。另外,对于具有1nm颗粒间隙的Cu-Ag合金偶联纳米颗粒,共振峰的波长从420nm移位,纯银纳米颗粒均为纯铜纳米颗粒的544nm。在嵌入式纳米颗粒的嵌入式纳米颗粒具有6nm间隙距离的情况下,共振峰的波长从396nm至409nm移位,并且对于具有2nm间隙距离的耦合银纳米颗粒,共振峰的波长从414nm移位430 nm。此外,对于具有2nm间隙距离的偶联Cu纳米颗粒,共振峰的波长从575nm偏移到582nm。结果可以用于粒子传感器设计和制造。

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