Enhanced High-Frequency Performance of Top-Gated Graphene FETs Due to Substrate- Induced Improvements in Charge Carrier Saturation Velocity

The high-frequency performance of top-gated graphene field-effect transistors (GFETs) depends to a large extent on the saturation velocity of the charge carriers, a velocity limited by inelastic scattering by surface optical phonons from the dielectrics surrounding the channel. In this work, we show...

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Bibliographic Details
Published inIEEE transactions on electron devices Vol. 68; no. 2; pp. 899 - 902
Main Authors Asad, Muhammad, Jeppson, Kjell O., Vorobiev, Andrei, Bonmann, Marlene, Stake, Jan
Format Journal Article
LanguageEnglish
Published New York IEEE 01.02.2021
The Institute of Electrical and Electronics Engineers, Inc. (IEEE)
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Summary:The high-frequency performance of top-gated graphene field-effect transistors (GFETs) depends to a large extent on the saturation velocity of the charge carriers, a velocity limited by inelastic scattering by surface optical phonons from the dielectrics surrounding the channel. In this work, we show that, by simply changing the graphene channel surrounding dielectric with a material having higher optical phonon energy, one could improve the transit frequency and maximum frequency of oscillation of GFETs. We fabricated GFETs on conventional SiO 2 /Si substrates by adding a thin Al 2 O 3 interfacial buffer layer on top of SiO 2 /Si substrates, a material with about 30% higher optical phonon energy than that of SiO 2 , and compared performance with that of GFETs fabricated without adding the interfacial layer. From S-parameter measurements, a transit frequency and a maximum frequency of oscillation of 43 and 46 GHz, respectively, were obtained for GFETs on Al 2 O 3 with 0.5-<inline-formula> <tex-math notation="LaTeX">\mu \text{m} </tex-math></inline-formula> gate length. These values are approximately 30% higher than those for state-of-the-art GFETs of the same gate length on SiO 2 . For relating the improvement of GFET high-frequency performance to improvements in the charge carrier saturation velocity, we used standard methods to extract the charge carrier velocity from the channel transit time. A comparison between two sets of GFETs with and without the interfacial Al 2 O 3 layer showed that the charge carrier saturation velocity had increased from <inline-formula> <tex-math notation="LaTeX">1.5\cdot 10^{{7}} </tex-math></inline-formula> to <inline-formula> <tex-math notation="LaTeX">2\cdot 10^{{7}} </tex-math></inline-formula> cm/s.
ISSN:0018-9383
1557-9646
1557-9646
DOI:10.1109/TED.2020.3046172