领结纳米天线的电场增强

Gufran A. Hassana, J. A. Hassan
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引用次数: 1

摘要

纳米天线被设计用来将高频转化为能量。所提出的天线是铝制的。是由一对纳米粒子靠近而形成的。天线被印在硅层上的小缝隙隔开,硅层被设计成一个平边领结,在基板的最下方有一个接地面,领结天线的缝隙中有一个馈电。该天线采用3d电磁求解(CST)程序进行设计,并对金属厚度、间隙尺寸和几何长度进行优化分析。模拟研究了线极化平面波照射下纳米天线的特性。通过改变纳米天线的衬底厚度、馈电尺寸、馈电类型和馈电材料等参数来选择具有较大指向性的最有效的纳米天线,研究发现纳米天线在其间隙区域具有较高的电场增强。该专业可用于SERS或生物传感,以提高检测限和测量单个分子的存在。为此,有必要制造具有足够小间隙的天线,以能够补偿在制造过程中产生的缺陷,并达到接近模拟预测的天线特性。为了提高天线在250 ~ 700太赫兹频率范围内的最佳电磁场,进行了数值模拟研究。该天线在310太赫兹频段具有多谐振频率和良好的回波损耗,输出电场为5.48 v/m ~ 7.8 v/m。改变间隙馈电方式(不馈电、空气馈电、介质硅馈电或馈电),我们发现,在间隙间使用空气时,在(531.3)THz谐振频率下s参数为(-12.9)dB,在666 THz入射频率下指向性为7.41 dB。
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Enhancement of electric field of bowtie nanoantenna
A nanoantenna is designed to transform high frequency into energy. The proposed antenna is made of aluminuim. are shaped with a pair of nanoparticles brought in close nearness. Antennas separated by small gaps printed on a Si layer, which is designed as a flat-edge bowtie, with a ground plane at the under most of the substrate with a feeding putting in the gap of the bowtie antenna. The proposed antenna is designed using 3D-electromagnetic solver (CST) programs and analysed for the optimisation of metal thickness, gap size, and geometrical length. Simulations are conducted to investigate the behaviour of the nanoantenna illuminated by the linearly polarized plane wave. The nanoantenna parameters such as substrate thickness, feeding size, feeding type, and feeding material were changed to select the most efficient nanoantenna with a large directivity in our reaserch find the nanoantenna make a high electric field enhancement in their gap region. This specialty can be employed for SERS or biosensing to improve the detection limit and measure the presence of single molecules. For this, it is necessary to create antennas with enough small gaps, to be capable to recompense for the defects created during the fabrication process and reach antenna characteristics that are close to the ones presage by simulations. The numerical simulations are studied to improve the best E-field of the antenna within the 250–700 THz frequency range. The proposed antenna offers multiple-resonance frequencies and good return loss in the frequency band of 310 THz, as well as an output electric field of 5.48 v/m to 7.8 v/m. Upon changing the type of feeding in the gap (without feeding, air feeding, dielectric silicon, or feeding), and we find that when using the air between the gap, the S-parameter is (-12.9) dB at the resonance frequency of (531.3) THz and the directivity is 7.41 dB at 666 THz incident frequency.
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