聚焦离子束在SiO2和玻璃基板上制造金和铜纳米棒互连的电气特性、稳定性、电迁移、焦耳加热和可靠性方面

A. Singh, J. Kumar
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引用次数: 1

摘要

由于矩形纳米棒互连在电子器件中的重要性和可靠性问题,对其电学特性和稳定性进行了研究。用30 keV的Ga+离子探针(尺寸10-20 nm)在约1 nA的电流下,分别铣削制备了金纳米棒和铜纳米棒(截面150-180 × 80-150 nm2,长度3.0-5.0 μm),研究了它们的电流承载能力和焦耳加热引起的温度分布。所达到的温度取决于杆的长度,在杆的中心有一个最大值。物质的电迁移(金的漂移速度为~ 0.92 nm/s)在电流密度为~ 1011 a m−2时形成空洞并导致棒材断裂。这种现象受棒材长度、盛行温度梯度、晶体缺陷和晶界的控制。热迁移过程促进或阻碍电迁移效应取决于热梯度和电场的方向。金条的电流-电压特性的差距∼44 nm∼10−真空下的标称遵循古典Child-Langmuir V3/2法律10-45 V的电压范围,但铜电极和一个巨大的差距∼250海里(由离子铣)演示V0.05-dependence多达32 V, V 39-58 V1/2-law, Fowler-Nordheim发射(与一个有效面积1600 nm2和场增强因子为8.1)高于66 V。
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Electrical characteristics, stability, electromigration, Joule heating, and reliability aspect of focused ion beam fabricated gold and copper nanobar interconnects on SiO2 and glass substrates
The electrical characteristics and stability of rectangular nanobar interconnects are investigated owing to their importance and reliability concern in electronic devices. One dimensional gold and copper nanobars (cross section 150–180 × 80–150 nm2 and length 3.0–5.0 μm), fabricated by milling of respective thin films with a 30 keV Ga+ ion probe (size 10–20 nm) at a current of ∼1 nA, are studied for their current bearing capacity and temperature profile caused by Joule heating. The temperature attained is shown to depend on the length with a maximum lying at the bar center. The electromigration of species (drift velocity for gold being ∼0.92 nm/s) forms void and induces breakage in the bar at a current density of ∼1011 A m−2. The phenomenon is governed by the bar length, prevailing temperature gradient, crystal defects, and grain boundaries. The thermo-migration process facilitates or impedes the electromigration effects depending upon the direction of the thermal gradient and electric field. The I–V characteristics of a gold bar with a gap of ∼44 nm under a vacuum of ∼10−6 mbar follow a classical Child–Langmuir V3/2 law in the voltage range of 10–45 V, but the copper electrodes with a large gap of ∼250 nm (created by ion milling) demonstrate V0.05-dependence up to 32 V, V1/2-law at 39–58 V, and Fowler–Nordheim emission [with an effective area of 1600 nm2 and a field enhancement factor of 8.1] above 66 V.
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