Method for bottom electrode of capacitor

Semiconductor device manufacturing: process – Making field effect device having pair of active regions... – Having insulated gate

Reexamination Certificate

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C438S398000

Reexamination Certificate

active

06204121

ABSTRACT:

BACKGROUND OF THE INVENTION
1. Field of Invention
The present invention relates to fabrication of a semiconductor device. More particularly, the present invention relates to a method of fabricating a bottom electrode of a capacitor.
2. Description of Related Art
A conventional DRAM cell is constructed from a MOS transistor and a capacitor. The capacitor functions as a signal storage device, and therefore plays an important role in the operation of a DRAM cell. If the number of charges stored in a capacitor is high, noise interference when data are read from the capacitor are less and refresh frequency is lower.
In the design of very large scale integrated (VLSI) circuits, one method of increasing a capacitor's capacitance is to increase storage node surface area. This is because capacitance value is proportional to the surface area of the storage node or electrode, which are made from a conductive material. At present, fin types or hemispherical grained structures are used to increase the surface area of storage nodes. However, manufacturing methods for fin-type or hemispherical grained structures are quite complicated, and hence mass production is rather difficult. Therefore, the simpler, stacking method of increasing surface area is still employed. Nevertheless, one common method of increasing surface area and hence charge storage capacity of a capacitor is to form a layer of hemispherical grained (HSG) polysilicon over the lower electrode.
In the conventional method of manufacturing DRAM capacitors, hemispherical grained silicon (HSG) is directly grown over the surface of a polysilicon bottom electrode. The HSG is a layer having a large number of hemispherical grains which increase the surface area of an electrode plate.
In general, the HSG layer is fabricated on a substrate by heating the substrate to a temperature of about 530° C. so that an amorphous silicon layer forms on the substrate surface. This amorphous silicon layer is also know as a—silicon. By heating to the phase transfer temperature of about 560° C. to 590° C., a hemispherical grained silicon layer is grown over the a—silicon. Therefore, the surface area of an electrode plate is increased.
FIG.
1
A through
FIG. 1E
are schematic, cross-sectional views showing a conventional method of fabricating a bottom electrode of a capacitor.
As shown in
FIG. 1A
, a semiconductor substrate
100
is provided. A transistor is formed on the substrate
100
, wherein the transistor contains a metal-oxide semiconductor (MOS)
101
and a source/drain region
102
. An insulating layer
103
having a contact hole
104
is formed over the substrate
100
. and a portion of the source/drain region
102
is exposed by the contact hole
104
.
As shown in
FIG. 1B
, a doped amorphous silicon layer
106
is formed over the substrate
100
and the contact hole
104
is filled with the doped amorphous layer
106
. The doped amorphous silicon is commonly used to increase conductivity. The dopants of the doped amorphous silicon layer
106
are phosphorous ions or arsenic ions. The doped amorphous silicon layer
106
is formed by low-pressure chemical vapor deposition (LPCVD).
As shown in
FIG. 1C
, the doped amorphous silicon layer
106
on the dielectric layer
103
is defined to leave the amorphous silicon layer
106
a
directly above the contact hole
104
. The amorphous silicon layer
106
a
directly above the contact hole
104
is the main structure of a bottom electrode of a capacitor.
As shown in
FIG. 1D
, a seeding process and an annealing process are performed on the substrate
100
. Hemispherical grained silicon (HSG) layer
108
grows on the surface of the amorphous silicon layer
106
a
so that the surface area of the amorphous silicon layer
106
a
is increased. A bottom electrode is composed of the amorphous silicon layer
106
a
and the HSG layer
108
.
Generally, the operating conditions for forming an amorphous silicon layer by LPCVD are similar to those for forming a polysilicon layer by LPCVD. The greatest difference is their operating temperatures. The operating temperature of the polysilicon layer is higher than the one of the amorphous silicon layer. The operating temperature of the polysilicon layer is from about 600° C. to about 650° C. The operating temperature of the amorphous silicon layer is from about 500° C. to about 550° C. Because of the higher depositing temperature, molecules have higher kinetic energy and are easily mobile on the wafer so that molecules aggregate to easily form crystals. Therefore, formation of amorphous silicon has to be performed at lower temperature. However, when amorphous silicon is formed at a lower temperature, the depositing rate is greatly reduced. For example, depositing rate is about 100 Å/min at 600° C.; depositing rate is reduced to about 25 Å/min at 550° C.; and depositing rate is only about 8 Å/min at 520° C.
About 16 hours are required to deposit the amorphous silicon layer
106
on the substrate
100
by LPCVD at 800K and implanting ions with concentration of about 3×10
20
/cm
3
. The process is time-consuming; therefore, the process is not suitable for mass production.
Implanting a high concentration of ions in the conventional method cannot lower contact resistance between the contact and the source/drain region
102
. More energy is added during implanting high concentration ions. Molecules obtain more energy to easily move on the wafer. Therefore, crystals are easily formed in the amorphous silicon layer
106
so that hemispherical grains form only with difficulty on the surface of the amorphous silicon layer
106
.
Additionally, in the conventional method, the amorphous silicon layer
106
is used to adjust the thickness of the bottom electrode. In order to increase the surface area of the bottom electrode, a thicker amorphous silicon layer is deposited. However, depositing a too thick amorphous silicon layer
106
is time consuming and leads to crystal formation at the bottom of the amorphous silicon layer
106
. Thus, hemispherical grains are not easily formed. The aforementioned condition is called bald defect.
In the other hand, during the step of etching the amorphous silicon layer to form the main structure of the bottom electrode, the amorphous silicon layer is difficult to etch. Therefore, taper occurs after etching the amorphous silicon layer
106
a,
as shown in FIG.
1
E. If etching conditions are not controlled well, bridging occurs between the two neighboring amorphous silicon layers
106
b,
leading to malfunction of devices.
SUMMARY OF THE INVENTION
Accordingly, the present invention provides a method of fabricating a bottom electrode of a capacitor. The invention uses hemispherical grained silicon layer to increase surface area of the bottom electrode.
The invention provides a method of fabricating a bottom electrode of a capacitor. The method well controls formation of the bottom electrode so that bridging, leading to malfunction of devices, can be avoided.
To achieve these and other advantages and in accordance with the purpose of the invention, as embodied and broadly described herein, the invention provides a method of fabricating a bottom electrode of a capacitor. A semiconductor substrate is provided wherein a transistor is formed thereon and the transistor contains a source/drain region. A dielectric layer having a contact hole is formed over the substrate wherein a portion of the source/drain region is exposed by the contact hole. A doped polysilicon layer is formed over the substrate. An insulating layer is formed on the doped polysilicon layer. An amorphous silicon layer is formed on the insulating layer. The amorphous silicon layer, the insulating layer and the doped polysilicon layer are defined to form a main structure of the bottom electrode. Amorphous silicon spacers are formed on sidewalls of the main structure. A hemispherical grained silicon layer is formed on the amorphous silicon layer and the amorphous silicon spacers.
It is to be understood that both the foregoing general description and the follow

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