As Moore’s law is approaching its end, reducing the power consumption of transistors has become the new challenge. It is in fact crucial to increase the energy efficiency of electronics at all levels from system architectures and interconnects down to the individual devices, with the ultimate goal to reduce the carbon footprint of electronics.
The power consumption of electronics is increasingly limiting system performance and simultaneously, massive amounts of data are being generated by the billions of devices we are surrounded by. The generated information needs to be computed, transmitted and stored, increasing the energy consumed by datacenters to an extent that is no longer sustainable by our ecosystem. It is therefore essential to reduce the power consumption of electronics on several fronts, ranging from system architectures and interconnects, down to the individual device level, targeting a reduction of the carbon footprint produced by the ICT industry.
Key to reducing the power consumption of individual components is to reduce the bias voltage at which they operate. This is ultimately limited by the steepness of the transition between “on” and “off“ state – referred to as subthreshold swing: The steeper this transient the less energy is required to turn on/off a transistor. CMOS devices – currently constituting the main building block of electronic circuits – are fundamentally limited by a minimum subthreshold swing of 60 mV/decade at 300 K. This means that for those devices it will ultimately be extremely challenging to reduce the bias voltage beyond the 0.7 V that is seen as the lower limit today. Tunnel field-effect transistors (TFETs) instead, exploit quantum mechanical tunneling to overcome this limitation, hence it is possible to operate these devices at much lower bias levels and with reduced leakage, which can lead to substantial gains in energy efficiency.
Unlike conventional transistors, TFETs have stringent requirements in terms of channel materials, device dimensions and energy band-alignment, hence heterostructures made of III-V compounds are essential to demonstrate superior TFET performance. The tunnel FET unlike a MOSFET is a junction device. Precise alignment of the gate to the tunnel junction is required to achieve simultaneously a steep subthreshold swing and adequate drive current. In this work we demonstrate a scaled TFET platform with sub-50-nm gate lengths in an advanced process, suitable for large scale integration. Key to achieving this is the development of a selective-source approach wherein the GaSb source material is grown only towards the end of the process. The use of digital etching and epitaxial regrowth allows for an accurate alignment with the gate.

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