1. Field of the Invention
The present invention relates to a semiconductor device capable of operating at low voltage and a manufacturing method therefor.
2. Description of the Related Art
In recent years, demand is growing for electronic equipment, such as mobile phones, PDAs, DVCs and DSCs, to be not only more functionally sophisticated (e.g., multifunctional) but also smaller in size and more power-saving. To lower the power consumption of electronic equipment, it is essential that the power consumption of large scale integration circuits (LSIs) incorporated in such electronic equipment be held low. To reduce the power consumption of LSIs, it is necessary that the semiconductor devices that constitute each LSI be made less power-consuming. And to make a semiconductor device less power-consuming, the operating voltage of the semiconductor device must be lowered, and this requires a technology for lowering the threshold voltage of the semiconductor device.
Thus, as the operating voltage of the semiconductor device has been made lower, the thickness of gate insulator (EOT: Equivalent Oxide Thickness) has approached about 1 nm. A problem with this trend, however, is that for a conventional polysilicon gate electrode, a depleted layer is formed on a gate electrode side and thus the gate insulator is effectively thickened. To solve this problem, there has been technology development to use metal for the gate electrode.
Related Art List
(1) Japanese Patent Application Laid-Open No. 2000-068507.
The metal gate without depletion, which is the problem with the polysilicon gate, makes it possible to avoid the effective increase in gate insulator thickness due to depletion. However, the metal gate has it own problem in that it does not allow easy control of the threshold voltage.
The present invention has been made to solve such problems, and a general purpose thereof is to provide a technology for making the operating voltage of a semiconductor device lower and at the same time making the control of a threshold voltage easier.
One embodiment of the present invention relates to a semiconductor device. This semiconductor device comprises: a semiconductor substrate; a source region and a drain region formed on the semiconductor substrate; a gate electrode formed between the source region and the drain by way of a gate insulator; and a plurality of insulating particles, embedded in the gate electrode in a scattered manner at interface between the gate insulator and said gate electrode and in contact with the gate insulator. Here, the form of silicon nitride particles is not subject to any particular limitation. And it may be spherical or polygonal or in an island-like thin film or a partially holed sheet not really forming a layer.
According to this embodiment, carriers mainly go in and out of a carrier trap formed at the interface between the gate insulator and the silicon nitride particles, from a gate electrode side. As a result, an electric charge is maintained at the interface between the gate insulator and the silicon nitride particles, without a tunnel current delivered, so that the threshold voltage and the effective capacity of the gate can be changed at low voltage. Utilizing this, conceivable is an application to a MOSFET where the threshold voltage is set higher by 0.1 to 0.2 V in the case of a low-voltage operation memory or in the neighborhood of the threshold voltage so as to suppress the off-leak current and, with a supply voltage applied to the gate, the device changes to a low-threshold-voltage FET so as to increase a saturation current.
In the above-described embodiment, a metal may be interposed partially between the insulating particles and the gate insulator. According to this embodiment, the amount of electric charge retained at the interface between the gate insulator and the silicon nitride particles can be increased, so that the threshold voltage of the semiconductor device and the effective capacitance change of the gate can be maintained for a long time.
In the above-described embodiment, an average particle diameter of the insulating particle may be approximately 1 to 5 nm. Also, the insulating particle may be a combination of one or more materials selected from a group of high-k materials including silicon nitride, Hf oxide, Al oxide, Zr oxide and lanthanum oxide.
Another embodiment of the present invention relates to a method of manufacturing a semiconductor device. This method for manufacturing a semiconductor device comprises: forming a gate insulator on a semiconductor substrate provided between a source region and a drain region; scattering a plurality of insulating particles on the gate insulating film; and forming a gate electrode above the gate insulator.
Still another embodiment of the present invention relates also to a method of manufacturing a semiconductor device. This method for manufacturing a semiconductor device comprises: forming a gate insulator on a semiconductor substrate provided between a source region and a drain region; scattering a plurality of metal particles on the gate insulating film; scattering a plurality of insulating particles and interposing the metal particles between one or more insulating particles and the gate insulator; forming a gate electrode above the gate insulator.
In either one of the above-described methods, an average particle diameter of the plurality of insulating particles may be approximately 1 to 5 nm. The insulating particle may be a combination of one or more materials selected from a group of high-k materials including silicon nitride, Hf oxide, Al oxide, Zr oxide and lanthanum oxide.
The above-described semiconductor device may be used as a memory device that differentiates a state by making use of a difference in an electric charge retained in an interface between the gate insulator and the insulating particles. In such a case, a drain region of the memory device mutually insulated from a memory device adjacent thereto by an element isolation region may be connected to a drain of the adjacent memory device thereto via a diode structure.
It is to be noted that any arbitrary combinations or rearrangement, as appropriate, of the aforementioned constituting elements and so forth are all effective as and encompassed by the embodiments of the present invention.
Moreover, this summary of the invention does not necessarily describe all necessary features so that the invention may also be sub-combination of these described features.
Embodiments will now be described by way of examples only, with reference to the accompanying drawings which are meant to be exemplary, not limiting and wherein like elements are numbered alike in several Figures in which:
The invention will now be described by reference to the preferred embodiments. This does not intend to limit the scope of the present invention, but to exemplify the invention.
A plurality of silicon nitride particles 80 are scatteringly embedded in the gate electrode, in contact with the gate insulator 60, at the interface between the gate insulator 60 and the gate electrode 70. The average particle diameter of the plurality of silicon nitride particles 80 is preferably 1 to 5 nm.
In this arrangement, carriers from the gate electrode 70 side go in and out of the carrier trap formed at the interface between the gate insulator 60 and silicon nitride particles 80. As a result, an electric charge is maintained at the interface between the gate insulator 60 and the silicon nitride particles 80, so that the threshold voltage and the effective capacity of the gate can be changed at low voltage.
In the present embodiment, silicon nitride particles are used as insulating particles present on the interface between the gate insulator 60 and the gate electrode 70. However, the insulating particles are not limited thereto and a high-k material where a level or trapping occurs on the interface may be used. For example, the insulating particles may be Hf oxides such as HfO2, HfAlO and HfON, Al oxides such as Al2O, Zr oxides such as ZrO2, or lanthanum oxides such as La2O3. Also, the insulating particle may be a combination of one or more above-described compounds.
CV Characteristic Evaluation
The CV characteristic of the gate insulator accompanied by the silicon nitride particles of a semiconductor device according to the present embodiment was measured using a mercury probe (Hg-CV/IV measuring unit made by SSM Japan K.K.). A film structure with silicon nitride particles deposited on a silicon oxide film of 3.2 nm in thickness was used as the sample.
Manufacturing Method
A manufacturing method of a semiconductor device 10 according to the first embodiment will be described by referring to the process sectional views of
Next, as illustrated in
Next, as illustrated in
Next, as illustrated in
Next, as illustrated in
Through the process as described above, a semiconductor device 10 capable of operating at low voltage can be manufactured easily. Note that while the above process is equal to the manufacturing method for an n-type MOSFET, a p-type MOSFET may also be manufactured by a similar process. Moreover, a CMOS structure may be manufactured using the above-described process as the basic process.
In the above-described method for manufacturing a semiconductor device, silicon nitride particles are used as insulating particles present on the interface between the gate insulator 60 and the gate electrode 70. However, the insulating particles are not limited thereto and a high-k material where a level or trapping occurs on the interface may be used. For example, the insulating particles may be Hf oxides such as HfO2, HfAlO and HfON, Al oxides such as Al2O, Zr oxides such as ZrO2, or lanthanum oxides such as La2O3. Also, the insulating particle may be a combination of one or more above-described compounds. Note that SiO2 particles may be formed on a high-k film such as SiN and HfOx.
The manufacturing method for a semiconductor device 11 according to the second embodiment is the same as that for a semiconductor device 10 according to the first embodiment except the process as illustrated in
Similar to the first embodiment, the above-described various high-k materials may be used in place of he silicon nitride particles 80.
The diode structure 200 according to the present embodiment is a Schottky barrier comprised of a Ti layer 210 formed on an element isolation region 30, a TiSi2 layer 220 formed on the drain region 50, in contact with a Ti layer 210, and a TiN layer 230 formed on the Ti layer 210 and the TiSi2 layer 220. Thereby, the direction of the current flowing from the source region of the unselected cell to the drain region of the selected cell can be set to one direction. Note that the diode structure is not limited thereto and, for example, a TiN/TiO2 interface may be used.
The following Table 1 shows combinations of a source voltage, a gate voltage and a drain voltage when a write or read is performed on a selected cell.
If the operation state of a selected cell (as well as an unselected cell) is to be deleted, the source voltage, the gate voltage and the drain voltage will be set to 0 V, −5 V and 0 V, respectively. As a result, the electric charge is trapped in the interface between the silicon oxide film and the silicon nitride, and a state of reduced gate capacitance or increased gate threshold voltage is created.
If a write is to be performed on the selected cell, the source voltage, the gate voltage and the drain voltage of the selected cell will be set to 0 V, 5 V and 0 V, respectively, and those voltages of the unselected cell will be set to 5 V, 5 V and 0 V, respectively. This releases the electric charge trapped in the interface between the silicon oxide film and the silicon nitride, which in turn results in a gate capacitance 1.6 times the reference value. This is equivalent to the state in which the gate capacitance is relatively low.
Next, if a readout is performed, the source voltage, the gate voltage and the drain voltage of the selected cell will be set to 0 V, 3 V and 3 V, respectively, and those voltages of the unselected cell will be set to “floating”, 3 V and 3 V, respectively. At this time, if a write has already been performed in the selected cell, the current will flow. However, if the selected cell has been deleted, the current will not flow or the current will be much less. As a result, the state of a cell can be distinguished between “1” and “0”. On the other hand, if the source voltage is set to “floating”, the current will not flow regardless of the cell state and therefore the state is retained intact.
While the preferred embodiments of the present invention have been described using specific terms, such description is for illustrative purposes only, and it is to be understood that changes and variations may be made without departing from the spirit or scope of the appended claims.
Number | Date | Country | Kind |
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2006-097066 | Mar 2006 | JP | national |
2007-037169 | Feb 2007 | JP | national |