SCHEDULED MAINTENANCE
Does carrier velocity saturation help to enhance fmax in graphene field-effect transistors?†
*a
Francisco
Pasadas,
a
Marlene
Bonmann,
b
Muhammad
Asad,
b
Xinxin
Yang,
b
Andrey
Generalov,
c
Andrei
Vorobiev,
b
Luca
Banszerus,
d
Christoph
Stampfer,
d
Martin
Otto,
e
Daniel
Neumaier,
e
Jan
Stake
b
and
David
Jiménez
a
Abstract
It has been argued that current saturation in graphene field-effect transistors (GFETs) is needed to get optimal maximum oscillation frequency (fmax). This paper investigates whether velocity saturation can help to get better current saturation and if that correlates with enhanced fmax. We have fabricated 500 nm GFETs with high extrinsic fmax (37 GHz), and later simulated with a drift–diffusion model augmented with the relevant factors that influence carrier velocity, namely: short-channel electrostatics, saturation velocity effect, graphene/dielectric interface traps, and self-heating effects. Crucially, the model provides microscopic details of channel parameters such as carrier concentration, drift and saturation velocities, allowing us to correlate the observed macroscopic behavior with the local magnitudes. When biasing the GFET so all carriers in the channel are of the same sign resulting in highly concentrated unipolar channel, we find that the larger the drain bias is, both closer the carrier velocity to its saturation value and the higher the fmax are. However, the highest fmax can be achieved at biases where there exists a depletion of carriers near source or drain. In such a situation, the highest fmax is not found in the velocity saturation regime, but where carrier velocity is far below its saturated value and the contribution of the diffusion mechanism to the current is comparable to the drift mechanism. The position and magnitude of the highest fmax depend on the carrier concentration and total velocity, which are interdependent and are also affected by the self-heating. Importantly, this effect was found to severely limit radio-frequency performance, reducing the highest fmax from ∼60 to ∼40 GHz.
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