Literature DB >> 22481430

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

Richard A Farrell1, Niall T Kinahan, Stefan Hansel, Karl O Stuen, Nikolay Petkov, Matthew T Shaw, Laetitia E West, Vladimir Djara, Robert J Dunne, Olga G Varona, Peter G Gleeson, Soon-Jung Jung, Hye-Young Kim, Maria M Koleśnik, Tarek Lutz, Christopher P Murray, Justin D Holmes, Paul F Nealey, Georg S Duesberg, Vojislav Krstić, Michael A Morris.   

Abstract

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 L(0) (pitch) of 42 nm, on chemically pre-patterned surfaces. Parallel arrays (5 × 10(6) 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) × 10(5)Ωcm) 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 Ωcm) 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.

Entities:  

Year:  2012        PMID: 22481430     DOI: 10.1039/c2nr00018k

Source DB:  PubMed          Journal:  Nanoscale        ISSN: 2040-3364            Impact factor:   7.790


  2 in total

1.  Fabrication of Dimensional and Structural Controlled Open Pore, Mesoporous Silica Topographies on a Substrate.

Authors:  Tandra Ghoshal; Atul Thorat; Nadezda Prochukhan; Michael A Morris
Journal:  Nanomaterials (Basel)       Date:  2022-06-28       Impact factor: 5.719

2.  Creating Active Device Materials for Nanoelectronics Using Block Copolymer Lithography.

Authors:  Cian Cummins; Alan P Bell; Michael A Morris
Journal:  Nanomaterials (Basel)       Date:  2017-09-30       Impact factor: 5.076

  2 in total

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