Semiconductor device manufacturing: process – Making field effect device having pair of active regions... – Having insulated gate
Reexamination Certificate
2001-02-26
2002-05-14
Bowers, Charles (Department: 2813)
Semiconductor device manufacturing: process
Making field effect device having pair of active regions...
Having insulated gate
C438S003000, C257S324000
Reexamination Certificate
active
06387762
ABSTRACT:
BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to a method of manufacturing a ferroelectric memory device capable of nonvolatile data storage utilizing a polarization of a ferroelectric layer.
2. Description of Related Arts
A ferroelectric memory device is a nonvolatile memory device in which a ferroelectric layer is used. When an electric field is applied to a ferroelectric layer, a polarization becomes complete in the ferroelectric layer, and the direction of the polarization is retained even after removing the electric field. By utilizing this, nonvolatile data storage can be performed.
FIG. 2
is a schematically sectional view showing the most basic structure of a ferroelectric memory element. A gate structure is formed, in which a ferroelectric layer
5
(F) and a metal layer
6
(M) as a gate electrode are stacked on the surface of a silicon substrate
1
(S). A pair of N-type diffused layers
2
,
2
serving as a source and a drain are formed with the gate structure interposed therebetween. Thereby a MIS transistor using a ferroelectric layer as an insulating layer is fabricated.
By applying a voltage of, e.g. 5V between the metal layer
6
and the silicon substrate
1
, an electric field oriented in a direction from the metal layer
6
toward the silicon substrate
1
or from the silicon substrate
1
toward the metal layer
6
is applied to the ferroelectric layer
5
. This forms, in the ferroelectric layer
5
, a polarization aligned with the direction of the applied electric field. The polarization is retained after removing the electric field applied between the metal layer
6
and the silicon substrate
1
.
As a result, the surface of the silicon substrate
1
between the N-type diffused layers
2
,
2
takes a state in which electrons are induced and a state in which holes are induced. Thereby, the threshold value of a voltage to be applied to the metal layer
6
for making conductive the pair of the N-type diffused layers
2
,
2
changes between two kinds, namely, “high” and “low” in accordance with the direction of the polarization of the ferroelectric layer
5
. Therefore, binary data of “0” or “1” can be stored in a nonvolatile manner.
In the structure shown in
FIG. 2
, it is difficult to form a satisfactorily crystallized ferroelectric layer
5
on the silicon substrate
1
. Further, this structure has another problem that the ferroelectric material is diffused in the silicon substrate
1
. Accordingly, it has been proposed that another insulating layer
3
(I) is interposed between the silicon substrate
1
and the ferroelectric layer
5
as shown in FIG.
3
.
In the structure shown in
FIG. 3
, it is necessary to obtain a favorable alignment in the surface boundary between the silicon substrate
1
and the insulating layer
3
and at the same time obtain a favorable alignment between the insulating layer
3
and the ferroelectric layer
5
. Therefore, this structure has a problem that the material of the insulating layer
3
and the method for forming the same is strictly limited. Further, the insulating layer
3
does not have a satisfactory barrier effect for preventing the diffusion of the ferroelectric material.
On the other hand, in
FIG. 4
, a structure of a ferroelectric memory element is shown in which a metal layer
4
(M) is interposed between the insulating layer
3
and the ferroelectric layer
5
to form a gate structure. In this structure, since the alignment in the surface boundary between the insulating layer
3
and the ferroelectric layer
5
need not be considered, a satisfactorily crystallized insulating layer
3
can be formed on the silicon substrate
1
and at the same time, the ferroelectric layer
5
can be satisfactorily crystallized. Further, the metal layer
4
can prevent the diffusion of the ferroelectric material.
However, both of the structures shown in
FIGS. 3 and 4
have the following problem in the manufacturing process thereof. The pair of N-type diffused layers
2
,
2
serving as a source and a drain are formed by implanting N-type impurity ions in the silicon substrate
1
and thereafter activating the N-type impurities implanted in the surface of the silicon substrate
1
through activated annealing. The activated annealing comprises heating the silicon substrate
1
at a temperature of 900 to 950° C. in a furnace for 1 to 2 hours. However, when the ferroelectric layer
5
is subjected to such a heat treatment, the polarization characteristics of the ferroelectric layer
5
are deteriorated.
In order to avoid this disadvantage, for example, a process of fabricating a MFMIS structure shown in
FIG. 4
is required to comprise steps of fabricating a MIS transistor section, then activating the pair of N-type impurity diffused layers
2
,
2
, and thereafter forming a capacitor section in which the ferroelectric layer is interposed between the metal layers
4
,
6
.
FIG. 5
is a schematically sectional view for explaining a practical structural example of a ferroelectric memory element having the structure shown in FIG.
4
. In this ferroelectric memory element, an insulating layer
3
and a metal layer
4
a
are stacked on the surface of the silicon substrate
1
to form a MIS gate structure, and a pair of N-type diffused layers
2
,
2
are formed on both sides of the MIS gate structure respectively. Then, after the pair of N-type diffused layers are activated by activated annealing, a capacitor structure comprising a metal layer
4
b
, a ferroelectric layer
5
and a metal layer
6
is formed in a different position from that of the MIS transistor. And a connecting section
7
comprising wiring layers and plugs connects the metal layer
4
a
of the MIS transistor and the metal layer
4
b
on the capacitor side.
A disadvantage of the structure shown in
FIG. 5
is that since the transistor section and the capacitor section are formed in the separate regions, the area occupied by a memory cell on the silicon substrate
1
becomes large and high level integration is hard to attain.
This disadvantage is somewhat decreased by adopting the structure shown in FIG.
6
. In the structure shown in
FIG. 6
, a large-sized insulating layer
3
and a similarly large-sized metal layer
4
are stacked on a silicon substrate
1
to form a MIS structure, and thereafter, N-type impurities are implanted in the silicon substrate
1
and activated by annealing to form a pair of N-type diffused layers
2
,
2
in the surface layer section of the silicon substrate
1
. Then, a ferroelectric layer
5
and a metal layer
6
are formed and stacked in order on the silicon substrate
1
.
When this structure is adopted, the area of the gate structure section in which the insulating layer
3
and the metal layer
4
are stacked is required to be larger than the area of the structure section in which the ferroelectric layer
5
and the metal layer
6
is stacked. This is so because it is necessary to secure a margin between a mask for patterning the gate structure section in which the insulating layer
3
and the metal layer
4
are stacked and a mask for patterning the structure section in which the ferroelectric layer
5
and the metal layer
6
are stacked.
Thus, when the structure shown in
FIG. 6
is adopted, a large-sized area of gate structure section is also required. Therefore, in this case, the attainment of high level integration is limited.
SUMMARY OF THE INVENTION
An object of the present invention is to provide a method of manufacturing a ferroelectric memory device capable of advantageously attaining high level integration.
A method of manufacturing a ferroelectric memory device according to the present invention comprises steps of stacking a ferroelectric layer and a conductor layer on a semiconductor substrate in order, forming a gate structure section including the ferroelectric layer and the conductor layer by patterning the ferroelectric layer and the conductor layer through etching using a common mask layer, introducing impurities into a pair of regions spaced apart from each other with t
Nakamura Takashi
Takasu Hidemi
Kielin Erik
Rader & Fishman & Grauer, PLLC
Rohm Co., LTD
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