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1.
J Microsc ; 291(2): 156-162, 2023 Aug.
Article in English | MEDLINE | ID: mdl-37151081

ABSTRACT

The precise extraction of a thin slice (lamellae) from nano electronic devices using a focused ion beam (FIB) is crucial for transmission electron microscopy analysis, but it remains a challenge for 100 nm and beyond scale device components. In this study, we introduce a new method that utilises the device's own features as markers during FIB thinning process by continuously monitoring the intermediate structures with secondary electron scanning electron microscopy (SE-SEM) imaging. This allows for the targeted extraction of the desired device component with high precision. We successfully demonstrate the effectiveness of this approach by extracting lamellae from 100 nm length channel in arrayed carbon nanotube film field-effect transistors using FIB lift-out.

2.
ACS Appl Mater Interfaces ; 15(8): 10830-10837, 2023 Mar 01.
Article in English | MEDLINE | ID: mdl-36795423

ABSTRACT

An aligned semiconducting carbon nanotube (A-CNT) array has been considered an excellent channel material to construct high-performance field-effect transistors (FETs) and integrated circuits (ICs). The purification and assembly processes to prepare a semiconducting A-CNT array require conjugated polymers, introducing stubborn residual polymers and stress at the interface between A-CNTs and substrate, which inevitably affects the fabrication and performance of the FETs. In this work, we develop a process to refresh the Si/SiO2 substrate surface underneath the A-CNT film by wet etching to clean the residual polymers and release the stress. Top-gated A-CNT FETs fabricated with this process show significant performance improvement especially in terms of saturation on-current, peak transconductance, hysteresis, and subthreshold swing. These improvements are attributed to the increase in carrier mobility from 1025 to 1374 cm2/Vs by 34% after the substrate surface refreshing process. Representative 200 nm gate-length A-CNT FETs exhibit an on-current of 1.42 mA/µm and a peak transconductance of 1.06 mS/µm at a drain-to-source bias of 1 V, subthreshold swing (SS) of 105 mV/dec, and negligible hysteresis and drain-induced barrier lowering (DIBL) of 5 mV/V.

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