Charge injection transistor using high-k dielectric barrier...

Active solid-state devices (e.g. – transistors – solid-state diode – Thin active physical layer which is – Heterojunction

Reexamination Certificate

Rate now

  [ 0.00 ] – not rated yet Voters 0   Comments 0

Details

C257S026000, C257S027000, C257S029000, C257S214000

Reexamination Certificate

active

06303940

ABSTRACT:

FIELD OF THE INVENTION
The present invention relates to a Real Space Transfer (RST) electronic device.
BACKGROUND OF THE INVENTION
Real Space Transfer (RST) describes the process in which carriers in a narrow semiconductor layer, accelerated by an electric field parallel to the layer acquire high average energy and become hot carriers. These carriers surmount or can tunnel through an energy barrier into adjacent layers. This redistribution of carriers between parallel layers having different mobility leads to negative differential resistance (NDR). NDR is the result of the real space transfer of hot carriers' from a hot channel to a cooler channel, thus reducing the source-drain current for an increasing electric field. In gallium arsenide and silicon germanium based heterojunctions, relatively low heterojunction barriers make it possible for carriers in the channel to be accelerated by the source/drain field of a typical FET structure. These carriers may be accelerated to energies high enough to permit real-space transfer through the barrier (tunneling) or over the barrier. This effect is exploited in a variety of structures to include real-space transfer diodes and three and four terminal devices known as negative resistance field effect transistors (NERFET). In NERFETs, electrons heated in the channel of a heterojunction field effect transistor are collected in the gate or back gate electrode (thus the transport is perpendicular to the channel by virtue of RST).
FIG. 4
shows a typical charge injection transistor (CHINT). The basic device has a source
401
, a drain
402
and a collector
403
. In the illustrative CHINT of
FIG. 4
, the collector layer is Si
x
Ge
1−x
, the barrier is Si and the channel is Si
x
Ge
1−x
, although III-V based heterostructure CHINT's function in a similar manner as described herein. In operation, parallel transport is from the source to the drain of the device. When the applied electric field (bias) is increased sufficiently, carriers in the top layer
404
are heated by the source-drain field causing most not to reach the drain
402
. Instead, they are injected over the barrier layer
405
into the collector layer
406
through RST. Si/Si-Ge heterojunctions have also been explored for use in RST based devices for high speed logic and oscillator applications. While silicon/silicon germanium heterostructures are of practical interest because of possibilities of integration of charge injection devices into standard CMOS logic and other devices, there are clearly drawbacks to RST devices based on silicon germnanium. To this end, while silicon germanium is more readily integrated into current CMOS processing sequences, fabrication complexity issues still remain with silicon germanium. Furthermore, the potential barrier between silicon and silicon germanium is on the order of 0.1 eV; and since almost all the bandgap discontinuity between the strained Si
x
Ge
1−x
channel and the Si barrier falls into the valence band, the devices based on RST in SiGe rely on hot holes as the carriers. This is less desirable than the case where the carriers are electrons as the mobility of holes is lower than that of electrons.
Charge injection transistors, have been fabricated using III-V heterostructures to include GaAs/AlGaAs and InGaAs/InAlAs heterostructures. While there are certain benefits achieved through the III-V based heterojunctions there are drawbacks to such structures. Gallium arsenide structures are generally more expensive and more difficult to fabricate than their silicon counterparts due to the complexity of fabrication steps as well as materials required. Furthermore, while AlGaAs/GaAs and InGaAs/InAlAs heterojunctions can be used to form an RST based devices, the potential barrier between the two layers is on the order of 0.3 eV and 0.5 eV, respectively. Further details of Si/SiGe and III-V based CHINT devices can be found in
Functional Devices Based on Real Space Transfer in Si/SiGe Structure, IEEE Transcations on Electron Devices
, Vol 43, No. 10, October 1996, to Mastrapasqua, et al, p 1671-1677 and High Transconductance and Large Peak-to-Valley Ratio of Negative Differential Conductance in Three Terminal InGaAs/InAlAs Real-Space Transfer Devices, Appled Physics Letters Vol. 57, 1990, to Mensz, et al, respectively. The disclosures of these articles are specifically incorporated herein by reference.
Accordingly, leakage current issues tend to plague the gallium arsenide based devices. Thus, the adaptability of gallium arsenide and silicon germanium based heterojunction RST devices is suspect because of the attendant problems associated with fabrication, as well as mobility issues and leakage current issues. Accordingly, what is needed is a structure which can be readily incorporated into silicon MOS process sequences, while improving the performance of RST based devices.
SUMMARY OF THE INVENTION
The present invention relates to a charge injection transistor having a first barrier layer which has a conduction band energy level that is more than 0.5 eV greater than the conduction band of a second barrier layer. The first barrier layer is generally thin to foster tunneling of hot carriers. The second barrier is relatively thick and reduces leakage current. In an exemplary embodiment, a high-k dielectric material is used as the second barrier layer, with a grown silicon dioxide layer having a thickness of less than 20 Å as the first barrier layer. The barrier height differential between the high-k and silicon dioxide fosters RST and the thin silicon dioxide guarantees a good quality interface resulting in higher mobility in the channel and thereby a greater RST current.


REFERENCES:
patent: 5280182 (1994-01-01), Waho
patent: 5625208 (1997-04-01), Jun
patent: 5675157 (1997-10-01), Battersby
patent: 5841152 (1998-11-01), Ishikawa
patent: 5895931 (1999-04-01), Sakurai
patent: 1 391 640 (1975-04-01), None
“Functional Devices Based On Real Space Transfer In Si/SiGe Structure”, M. Mastrapasqua et al.,IEEE Transactions On Electron Devices,vol. 43, No. 10, Oct. 1996, pp. 1671-1677.
“High Transconductance And Large Peak-To-Valley Ratio Of Negative Differential Conductance In Three-Terminal InGaAs/InAIAs Real-Space Transfer Device”, P.M. Mensz et al.,Applied Physics Letters,vol. 57, No. 24, Dec. 10, 1990, pp. 2558-2560.
“Charge Injection Devices,” S. Luryi et al.,Encyclopedia of Electrical and Electronics Engineering,John Wiley & Sons Inc., pp. 3-7.
“Physics of Real-Space Transfer Transistors,” I.C. Kizilyalli et al.,J. Applied Physics Letters,vol. 65, No. 5, pp. 2005-2013.
“Characterization Of Stacked Gate Oxides by Electron Holography,” W. D. Rau et al., Applied Physics Letters 68(24), Jun. 10, 1996.
Patent No. 5,814,562, Filed on Nov. 19, 1995 and issued on Sep. 29, 1998, to Martin Laurence Green et al.
Patent No. 4,851,370, filed on Dec. 29, 1987 and issued on Jul. 25, 1989, to Raymond H. Doklan et al.
“Stacked High-&egr; Gate Dielectric For Gigascale Integration of Metal-Oxide-Semiconductor Technologies”, P.K. Roy et al.,Applied Physics Letter,vol. 72, No. 22, Jun. 1, 1998, pp. 2835-2837.
“MOS Transistors With Stacked SiO2-Ta2O5-SiO2 Gate Dielectrics for Giga-scale Integration Of CMOS Technologies”, I. C. Kizilyalli et al.,IEEE Electron Device Letters,vol. 19, No. 11, Nov. 1998, pp. 423-425.

LandOfFree

Say what you really think

Search LandOfFree.com for the USA inventors and patents. Rate them and share your experience with other people.

Rating

Charge injection transistor using high-k dielectric barrier... does not yet have a rating. At this time, there are no reviews or comments for this patent.

If you have personal experience with Charge injection transistor using high-k dielectric barrier..., we encourage you to share that experience with our LandOfFree.com community. Your opinion is very important and Charge injection transistor using high-k dielectric barrier... will most certainly appreciate the feedback.

Rate now

     

Profile ID: LFUS-PAI-O-2588254

  Search
All data on this website is collected from public sources. Our data reflects the most accurate information available at the time of publication.