The patent badge is an abbreviated version of the USPTO patent document. The patent badge does contain a link to the full patent document.

The patent badge is an abbreviated version of the USPTO patent document. The patent badge covers the following: Patent number, Date patent was issued, Date patent was filed, Title of the patent, Applicant, Inventor, Assignee, Attorney firm, Primary examiner, Assistant examiner, CPCs, and Abstract. The patent badge does contain a link to the full patent document (in Adobe Acrobat format, aka pdf). To download or print any patent click here.

Date of Patent:
Aug. 14, 2012

Filed:

Jun. 22, 2010
Applicants:

Francesca Iacopi, Leuven, BE;

Anne S. Verhulst, Houtvenne, BE;

Arturo Sibaja-hernandez, Leuven, BE;

Inventors:

Francesca Iacopi, Leuven, BE;

Anne S. Verhulst, Houtvenne, BE;

Arturo Sibaja-Hernandez, Leuven, BE;

Assignee:

IMEC, Leuven, BE;

Attorney:
Primary Examiner:
Int. Cl.
CPC ...
H01L 21/336 (2006.01);
U.S. Cl.
CPC ...
Abstract

Embodiments of the present disclosure provide a method to fabricate a hetero-junction in a Tunnel Field Effect Transistor (TFET) device configuration (e.g. in a segmented nanowire TFET). Since in prior art devices the highly doped source is in direct contact with the lowly doped or undoped channel, some amount of dopants will diffuse from the source to the channel which cannot be avoided due to the source deposition thermal budget. This out-diffusion reduces the steepness of the doping profile and hence deteriorates the device operation. Particular embodiments comprise the insertion of a thin transition layer in between the source region and channel region such that the out-diffusion is within a very limited region of a few nm, guaranteeing extremely good doping abruptness thanks to the lower diffusion of the dopants in the transition layer. The transition layer avoids the direct contact between the highly doped (e.g. Ge or SiGe) source region and the lowly doped or undoped (e.g. Si) channel and allows to contain the whole doping (e.g. B atoms) entirely within the source region and transition layer. The thickness of the transition layer can be engineered such that the transition layer coincides with the steep transition step from the highly doped source region to the intrinsic region (channel), and hence maximizing the tunneling current.


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