Bipolar junction transistor with tunneling current through...

Active solid-state devices (e.g. – transistors – solid-state diode – Integrated circuit structure with electrically isolated... – Lateral bipolar transistor structure

Reexamination Certificate

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Details

C257S592000

Reexamination Certificate

active

06246103

ABSTRACT:

TECHNICAL FIELD
The present invention relates generally to integrated circuit devices, and more particularly, to a bipolar junction transistor formed with a scaled down field effect transistor by using the tunneling current through the gate of the field effect transistor having a thin gate dielectric as the base current of the bipolar junction transistor.
BACKGROUND OF THE INVENTION
A long-recognized important objective in the constant advancement of monolithic IC (Integrated Circuit) technology is the scaling-down of IC dimensions. Such scaling-down of IC dimensions reduces area capacitance and is critical to obtaining higher speed performance of integrated circuits. Moreover, reducing the area of an IC die leads to higher yield in IC fabrication. Such advantages are a driving force to constantly scale down IC dimensions.
Referring to
FIG. 1
, a common component of a monolithic IC is a MOSFET (Metal Oxide Semiconductor Field Effect Transistor)
100
which is fabricated within a semiconductor substrate
102
. The conventional MOSFET
100
includes a drain
104
, a source
106
, and a gate structure
108
disposed over a gate dielectric
110
, as known to one of ordinary skill in the art of integrated circuits.
A limitation to further scaling down the dimensions of the MOSFET
100
is scaling down the thickness of the gate dielectric
110
. When the thickness of the gate dielectric
110
is scaled down to below approximately 15 Å (angstroms), charge carriers tunnel through such a thin gate dielectric
110
to form undesired tunneling current through the gate
108
. With such tunneling current, the gate
108
of the MOSFET
100
becomes less capacitive and more resistive, and the MOSFET
100
has lower current drive capability because less charge is induced in the channel region of the MOSFET
100
below the gate dielectric
110
. Such lowered current drive capability degrades the speed performance of the MOSFET
100
.
Referring to
FIG. 2
, another common component of a monolithic IC is a BJT (Bipolar Junction Transistor)
200
. The conventional BJT
200
includes an emitter region
122
and a collector region
124
that are comprised of a semiconductor material having a first type of dopant, as known to one of ordinary skill in the art of integrated circuits. The conventional BJT also includes a base region
126
that is comprised of a semiconductor material having a second type of dopant that is opposite of the first type of dopant, as known to one of ordinary skill in the art of integrated circuits.
For example, for an NPN BJT, the emitter region
122
and the collector region
124
may be comprised of silicon with an N-type dopant while the base region
126
may be comprised of silicon with a P-type dopant. Alternatively, for a PNP BJT, the emitter region
122
and the collector region
124
may be comprised of silicon with a P-type dopant while the base region
126
may be comprised of silicon with an N-type dopant.
The BJT
200
has larger current drive capability than the MOSFET
100
since the transconductance of a BJT is directly proportional to the current through the collector
124
of the BJT whereas the transconductance of a MOSFET is directly proportional to the square root of the current through the drain
104
of the MOSFET, as known to one of ordinary skill in the art of integrated circuits. However, unfortunately, the conventional BJT
200
occupies a relatively large area within an integrated circuit.
Because of the degradation of the current drive capability of a conventional MOSFET as the MOSFET is further scaled down and because of the large area occupied by a conventional BJT, another type of transistor is desired which has the desirable characteristics of both the higher current drive capability of the BJT and the smaller device area of the scaled down MOSFET.
SUMMARY OF THE INVENTION
Accordingly, in a general aspect of the present invention, a MOSBJT (Metal Oxide Semiconductor Bipolar Junction Transistor) is formed to have both the higher current drive capability of the BJT and the smaller device area of the scaled down MOSFET.
In one embodiment of the present invention, the MOSBJT is formed to include a collector region and an emitter region comprised of a semiconductor material with a first type of dopant. A base region is disposed between the collector region and the emitter region, and the base region is comprised of a semiconductor material with a second type of dopant that is opposite of the first type of dopant. In addition, unlike a conventional BJT, a base terminal is comprised of a dielectric structure disposed over the base region and comprised of a gate structure disposed over the dielectric structure. Unlike a conventional MOSFET, the dielectric structure is relatively thin such that a tunneling current through the dielectric structure of the MOSBJT results when a turn-on voltage is applied on the gate structure. The tunneling current is the base current of the MOSBJT. Furthermore, unlike a conventional MOSFET, the dielectric structure and the gate structure are not disposed over the collector region and the emitter region to prevent tunneling current between the gate structure and the collector and emitter regions.
In this manner, the MOSBJT has current characteristics of a bipolar junction transistor device with the tunneling current through the thin gate dielectric being the base current. Thus, the MOSBJT has the larger current drive capability of a bipolar junction transistor. Furthermore, the collector region, the base region, the emitter region, and the gate structure of the MOSBJT are formed within an active device area that typically contains a MOSFET. The MOSBJT is formed by modification of components of a MOSFET with scaled down dimensions such that the MOSBJT occupies the device area of a MOSFET with scaled down dimensions.
In another aspect of the present invention, a buffer region is formed between the collector region and the base region, for preventing base-to-collector junction breakdown and for preventing punch-through effect between the collector region and the emitter region in the MOSBJT.
These and other features and advantages of the present invention will be better understood by considering the following detailed description of the invention which is presented with the attached drawings.

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