Semiconductor device manufacturing: process – Forming bipolar transistor by formation or alteration of...
Reexamination Certificate
2001-03-16
2003-09-09
Nguyen, Tuan H. (Department: 2813)
Semiconductor device manufacturing: process
Forming bipolar transistor by formation or alteration of...
C438S321000, C438S349000, C438S367000, C438S368000
Reexamination Certificate
active
06617220
ABSTRACT:
FIELD OF THE INVENTION
The present invention relates to bipolar transistors, and more particularly to an epitaxial base bipolar transistor having a raised extrinsic base and methods of fabricating the same.
BACKGROUND OF THE INVENTION
High-base resistance in bipolar transistors degrades both the minimum noise and power gain cutoff frequency. A key component of the aforesaid resistance is the extrinsic base resistance. In order to reduce the extrinsic base resistance, it is known to ion implant the base region adjacent to the emitter. Despite being capable of reducing the extrinsic base resistance, ion implantation of the base region causes transient enhanced diffusion of the implanted dopants which widens the intrinsic base, and diffuses the pedestal implant as well as the intrinsic base itself.
Additional diffusion width, which causes subsequent overlap of the implants, leads to high-capacitance devices. Moreover, this increased capacitance results in slower operating devices that have poor performance associated therewith.
FIGS. 1 and 2A
are representative of prior art bipolar transistors in which the extrinsic base region is formed by ion implantation and activation annealing.
Specifically,
FIG. 1
is a cross-sectional view through a prior art silicon germanium (SiGe) bipolar device
10
using implanted extrinsic base regions, while
FIG. 2A
is a top-down view of the raised portion of the device shown in FIG.
1
.
Prior art bipolar device
10
of
FIG. 1
comprises subcollector region (e.g., N+ doped)
14
formed in Si substrate
12
(e.g., N-type). The substrate also includes collector contact region
15
and isolation regions
16
. A base region (e.g., P-type)
18
of silicon (mono-crystalline or epitaxial over the substrate, and polysilicon over the isolation regions) is located on top of the Si substrate. Base region
18
includes both intrinsic (P-doped)
18
i
and extrinsic (N-doped)
18
e
regions. The extrinsic base region surrounds the intrinsic region to a fixed depth below a Ge rich layer
20
. In general, the polysilicon/epitaxial region, i.e., base region
18
, is about 500-3000 Å thick. As stated above, within the base is a Ge rich layer of about 250-1500 Å, located 50-500 Å from the top of the base.
On top of the base region is insulator
22
having an opening exposing the top of the base region. Overlapping this opening is polysilicon emitter (N+ doped)
24
. Some of the doping from the emitter region is diffused into the base region. Surrounding the emitter region are dielectric spacers
26
and a cap layer which is formed on the emitter polysilicon.
Within the silicon substrate is a pedestal region
28
(N+ doped) extending from the subcollector into the base region, but not contacting the isolation regions. The highly doped extrinsic base region of the base extends laterally to contact the pedestal. As shown, prior art implantation and subsequent activation annealing causes overlap between the pedestal and base regions.
In
FIG. 2A
, the result of the extrinsic base region implant on resistance is shown. Note the effect of misalignment on the resistance between the emitter and the extrinsic base. This must be compared to the situation in
FIG. 2B
where no extrinsic base implant exists. The intrinsic portion of the base has a resistance of about 10,000 ohms/square while the extrinsic portion has a resistance of about 200 ohms/square. However, where the extrinsic base contacts or comes in proximity with the pedestal, a capacitance is associated with the PN junction. Equation (1) below shows the relationship between the important parameters:
f
max
&agr;f
t
/(R
B
C
CB
) (I)
where f
max
is the maximum frequency at which there is still power gain, f
t
is the frequency at which the current gain goes to 1 (increases with higher pedestal doping), R
B
is the base resistance and is the sum of both intrinsic and extrinsic resistance, and C
CB
is the collector base capacitance (increases with higher pedestal doping).
In order to achieve higher performance and scale the device, the pedestal dose must be increased while keeping the extrinsic base resistance low. In current devices, this is a difficult problem as the ion dose increases.
In view of the above, there is thus a need to develop a new and improved method that is capable of forming a epitaxial base bipolar transistor in which both the base resistance and the device capacitance is decreased; The new method should avoid the use of ion implanting the base region since the same causes overlap of the diffused regions and increased device capacitance.
SUMMARY OF THE INVENTION
One object of the present invention is to provide an epitaxial base bipolar transistor having a low-base resistance in which the capacitance of the device is not increased.
A further object of the present invention is to provide an epitaxial base bipolar transistor having minimum noise and power gain cutoff frequency.
A still further object of the present invention is to provide an epitaxial base bipolar transistor having high-operating device performance and increased switching speeds as compared to prior art bipolar devices.
An even further object of the present invention is to provide an epitaxial base bipolar transistor wherein the emitter is self-aligned and centered to the base.
These and other objects and advantages are achieved in the present invention by utilizing a raised base structure and by providing a shallow extrinsic base profile utilizing a doped polysilicon layer as the diffusion source for the extrinsic base.
In accordance with one aspect of the present invention, methods of forming an epitaxial base bipolar transistor device having a raised extrinsic base are provided in which the base region is not doped by ion implantation.
In the first method of the present invention, the emitter region is formed prior to forming the base region. Specifically, the first method of the present invention comprises the steps of:
(a) growing at least an epitaxial single crystal layer on a single crystal semiconductor substrate;
(b) forming a raised emitter on a surface of said semiconductor substrate, said raised emitter including insulating material formed on at least sidewalls thereof;
(c) forming a raised extrinsic base on said surface of said semiconductor substrate, wherein the raised emitter and the raised extrinsic base are insulated by said insulating material; and
(d) diffusing dopant from the raised emitter and said raised extrinsic base so as to provide an emitter diffusion and an extrinsic diffusion in the single crystal semiconductor substrate, wherein said emitter diffusion has an emitter diffusion junction depth, and wherein said emitter extends to said substrate surface and said base extends to said substrate surface.
In one preferred aspect of the present invention, the emitter to base surface height difference is less than 20% of the emitter junction depth.
The second method of the present invention forms the raised extrinsic base prior to formation of the emitter region. By forming the raised extrinsic base prior to emitter formation, the emitter will be self-aligned and centered to the base. Specifically, the second method of the present invention comprises the steps of:
(a) growing at least an epitaxial single crystal layer on a single crystal semiconductor substrate;
(b) forming a raised extrinsic base on said surface of said semiconductor substrate;
(c) forming a raised emitter on a surface of said semiconductor substrate, said raised emitter including insulating material formed on at least sidewalls thereof said insulating material electrically isolating said raised extrinsic base from said raised emitter; and
(d) diffusing dopant from the raised emitter and said raised extrinsic base so as to provide an emitter diffusion and an extrinsic diffusion in the single crystal semiconductor substrate, wherein said emitter diffusion has an emitter diffusion junction depth, and wherein said emitter extends to said substrate surface and said base extends to said substrate surfac
Dunn James Stuart
Harame David L.
Johnson Jeffrey Bowman
Johnson Robb Allen
Lanzerotti Louis DeWolf
Canale Anthony
International Business Machines - Corporation
Nguyen Tuan H.
Scully Scott Murphy & Presser
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