Imec

Katholieke Universiteit Leuven, Ku Leuven R&d

Katholieke Universiteit Leuven

K.u. Leuven Research & Development

William G Vandenberghe

Anne S Verhulst

A tunnel field effect transistor (TFET) is disclosed. In one aspect, the transistor comprises a gate that does not align with a drain, and only overlap with the source extending at least up to the interface of the source-channel region and optionally overlaps with part of the channel. Due to the shorter gate, the total gate capacitance is reduced, which is directly reflected in an improved switching speed of the device. In addition to the advantage of an improved switching speed, the transistor also has a processing advantage (no alignment of the gate with the drain is necessary), as well as a performance improvement (the ambipolar behavior of the TFET is reduced).

Tunnel field-effect transistor with gated tunnel barrier

Tunnel field-effect transistors (TFETs) are regarded as successors of metal-oxide semiconductor field-effect transistors (MOSFETs), but silicon-based TFETs typically suffer from low on-currents, a drawback related to the large resistance of the tunnel barrier. To achieve higher on-currents an elongate monocrystalline nanostructure-based TFET with a heterostructure made of a different semiconducting material (e.g. germanium (Ge)) is used. An elongate monocrystalline nanostructure made of a different semiconducting material is introduced which acts as source (or alternatively drain) region of the TFET. The introduction of the heterosection is such that the lattice mismatch between silicon and germanium does not result in a highly defective interface. A dynamic power reduction as well as a static power reduction can result, compared to conventional MOSFET configurations. Multiple layers of logic can therefore be envisioned with these elongate monocrystalline nanostructure Si/Ge TFETs resulting in ultra-high on-chip transistor densities.

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Herverlee, Belgium

William G Vandenberghe