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Large-scale parallel arrays of silicon nanowires via block copolymer directed self-assembly

机译:通过块共聚物定向自组装的硅纳米线的大规模平行阵列

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Extending the resolution and spatial proximity of lithographic patterning below critical dimensions of 20 nm remains a key challenge with very-large-scale integration, especially if the persistent scaling of silicon electronic devices is sustained. One approach, which relies upon the directed self-assembly of block copolymers by chemical-epitaxy, is capable of achieving high density 1 : 1 patterning with critical dimensions approaching 5 nm. Herein, we outline an integration-favourable strategy for fabricating high areal density arrays of aligned silicon nanowires by directed self-assembly of a PS-b-PMMA block copolymer nanopatterns with a L0 (pitch) of 42 nm, on chemically pre-patterned surfaces. Parallel arrays (5 x 106 wires per cm) of uni-directional and isolated silicon nanowires on insulator substrates with critical dimension ranging from 15 to 19 nm were fabricated by using precision plasma etch processes; with each stage monitored by electron microscopy. This step-by-step approach provides detailed information on interfacial oxide formation at the device silicon layer, the polystyrene profile during plasma etching, final critical dimension uniformity and line edge roughness variation nanowire during processing. The resulting silicon-nanowire array devices exhibit Schottky-type behaviour and a clear field-effect. The measured values for resistivity and specific contact resistance were ((2.6 ± 1.2) x 10~5 Qcm) and ((240 ± 80) Ωcm~2) respectively. These values are typical for intrinsic (un-doped) silicon when contacted by high work function metal albeit counterintuitive as the resistivity of the starting wafer (~10 Qcm) is 4 orders of magnitude lower. In essence, the nanowires are so small and consist of so few atoms, that statistically, at the original doping level each nanowire contains less than a single dopant atom and consequently exhibits the electrical behaviour of the un-doped host material. Moreover this indicates that the processing successfully avoided unintentional doping. Therefore our approach permits tuning of the device steps to contact the nanowires functionality through careful selection of the initial bulk starting material and/or by means of post processing steps e.g. thermal annealing of metal contacts to produce high performance devices. We envision that such a controllable process, combined with the precision patterning of the aligned block copolymer nanopatterns, could prolong the scaling of nanoelectronics and potentially enable the fabrication of dense, parallel arrays of multi-gate field effect transistors.
机译:将光刻图案的分辨率和空间接近度扩大到20 nm的临界维度以下仍然是一个非常大尺度整合的关键挑战,尤其是如果持续持续硅电子设备的持续缩放。一种方法依赖于通过化学播放的块共聚物的定向自组装,能够实现高密度1:1构图,临界尺寸接近5 nm。本文中,我们概述了一种综合策略,用于通过PS-B-PMMA块共聚物纳米纳米纳米模式的定向自组装,以42 nm为42 nm的PS-B-PMMA块共聚物纳米图案的定向自组装,以化学预先预制的表面,以化学预先组合的自我组装来制造综合的策略。 。通过使用精确的等离子体蚀刻工艺制造了临界尺寸范围为15至19 nm的绝缘体底物上的单向和孤立的硅纳米线的平行阵列(每厘米5 x 106线)。每个阶段都通过电子显微镜监测。这种逐步的方法提供了有关设备硅层的界面氧化物形成,血浆蚀刻过程中的聚苯乙烯曲线,最终临界尺寸均匀性和线边缘粗糙度变化纳米线的详细信息。所得的硅 - 纳米线阵列设备表现出Schottky型行为和明确的场效应。电阻率和特定接触电阻的测量值分别为((2.6±1.2)x 10〜5 qcm)和((240±80)ωCM〜2)。当通过高功函数金属接触时,这些值对于固有(未掺杂)硅是典型的,尽管违反直觉,但由于起始晶片的电阻率(〜10 QCM)低4个数量级。从本质上讲,纳米线是如此之小,由很少的原子组成,从统计上讲,在原始掺杂水平上,每种纳米线含有小于一个掺杂剂原子,因此表现出未掺杂的宿主材料的电气行为。此外,这表明处理成功地避免了无意的掺杂。因此,我们的方法允许对设备步骤进行调整,以通过仔细选择初始散装的启动材料和/或通过后处理步骤来接触纳米线功能。金属接触的热退火以生产高性能设备。我们设想,这种可控的过程,结合对齐的块共聚物纳米模式的精确图案,可以延长纳米电子的缩放,并有可能使多门磁场效应晶体管的密集,平行阵列的制造。

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