1. Field of the Invention
The present invention relates to a method of manufacturing a semiconductor device, especially a semiconductor device with an offset sidewall structure.
2. Description of the Background Art
In conventional semiconductor devices, impurity ion implantation is performed with gate electrodes as implant masks thereby to form extension layers in a self-aligned manner. The extension layers here are impurity layers which are formed to produce shallower junctions than main source/drain layers later to be formed. The extension layers are of the same conductivity type as the main source/drain layers and function as source/drain layers; thus, they should be referred to as source/drain extension layers but for convenience's sake, they are referred to herein as the extension layers.
In this method, however, the extension layers extend more than necessary under the gate electrodes due to scattering of impurity ions during implantation and diffusion of impurity ions in a subsequent process. This is shown in
In a MOS transistor M1 shown in
In recent semiconductor devices with minimum gate lengths of less than 0.1 μm, a short channel effect becomes more prominent and a slight reduction of the gate length from the design value will interfere with transistor operation. That is, the short channel effect has become the leading cause of low manufacturing yield. The gate overlap, which brings about a short channel effect, is thus an undesirable phenomenon.
To eliminate these problems, offset sidewall structures have recently been adopted.
Referring to
In this method, however, the following inconvenience occurs in semiconductor devices with both N-channel MOS transistors (NMOS transistors) and P-channel MOS transistors (PMOS transistors).
Referring to
The PMOS transistor M12 comprises a gate insulating film GX2 selectively formed on the semiconductor substrate SB, a gate electrode GT2 formed on the gate insulating film GX2, an offset sidewall OF2 formed adjacent to the side surfaces of the gate electrode GT2 and the gate insulating film GX2, and a pair of extension layers EX2 formed in the surface of the semiconductor substrate SB on both sides of the gate electrode GT2. In this case, the gate overlap lengths of the extension layers EX2 are represented by L5 and an effective channel length is represented by L6.
A comparison between the NMOS transistor M11 and the PMOS transistor M12 indicates that the gate overlap length L3 of the NMOS transistor M11 is shorter than the gate overlap length L5 of the PMOS transistor M12 and thus, the effective channel length L4 is longer than L6.
This is because boron (B) which is generally used as source and drain impurities for PMOS transistors has a much higher diffusion rate within silicon than arsenic (As) which is generally used as source and drain impurities for NMOS transistors.
That is, even if ion implantations of As and B produce implanted layers of the same shape, B will diffuse more widely in a subsequent heat treatment process and thereby the extension layers EX2 of the PMOS transistor M12 have a greater gate overlap length than the extension layers EX1 of the NMOS transistor M11.
This results in a more prominent short channel effect of the PMOS transistor M12, an increase in gate-drain parasitic capacitance, and an increase in gate-drain current leakage.
By expanding the width of the offset sidewall, the PMOS transistor M22 can have a shorter gate overlap length and a longer effective channel length. In the NMOS transistor M21, however, because of the expanded width of the offset sidewall OF11, doped impurities cannot extend under the gate electrode GT1 even by heat treatment during process, no gate overlaps occur, and thus isolation is established between the source and drain of the NMOS transistor M21, thereby causing a reduction in operating current.
Now, as one example of a conventional method of manufacturing a semiconductor device with both NMOS and PMOS transistors, a method of manufacturing a semiconductor device with CMOS transistors 90A and 90B will be described with reference to
Referring first to
In the surface of the silicon substrate 1, P-well regions PW containing P-type impurities are formed corresponding to the low-voltage NMOS region LNR and the high-voltage NMOS region HNR, and N-well regions NW containing N-type impurities are formed corresponding to the low-voltage PMOS region LPR and the high-voltage PMOS region HPR. In the following description, the P-well regions PW and the N-well regions NW may be simply referred to as the silicon substrate without distinction.
Then, a first insulation film such as silicon oxide film is formed to a first thickness to cover the whole surface of the silicon substrate 1. After that, a resist mask is formed to expose the low-voltage circuit portion and the first insulation film is removed from the low-voltage circuit portion by, for example, hydrofluoric acid treatment.
The resist mask is then removed and a second insulation film such as silicon oxide film is formed to a second thickness to cover the whole surface of the silicon substrate 1. Thereby the low-voltage circuit portion has an insulation film of the second thickness formed thereon and the high-voltage circuit portion has a third insulation film formed thereon which is greater in thickness than the first insulation film.
After a polysilicon layer is formed on the whole surface of the silicon substrate 1, the polysilicon layer and the second and third insulation films thereunder are patterned to selectively form gate electrodes and gate insulating films in both the low voltage and high-voltage circuit portions.
In the step of
The pair of extension layers 63 are opposed to each other with the silicon substrate 1 under the gate electrode 53 sandwiched in between. In this case, an area of the silicon substrate 1 under the gate electrode 53 forms a channel region.
In the step of
The pair of extension layers 64 are opposed to each other with the silicon substrate 1 under the gate electrode 54 sandwiched in between. In this case, an area of the silicon substrate 1 under the gate electrode 54 forms a channel region.
In the step of
In the step of
The pair of extension layers 61 are opposed to each other with the silicon substrate 1 under the gate electrode 51 sandwiched in between. In this case, an area of the silicon substrate 1 under the gate electrode 51 forms a channel region.
In the step of
The pair of extension layers 62 are opposed to each other with the silicon substrate 1 under the gate electrode 52 sandwiched in between. In this case, an area of the silicon substrate 1 under the gate electrode 52 forms a channel region.
In the step of
Thereafter, in the low-voltage NMOS region LNR, using the gate electrode 51, the offset sidewall 9 and the sidewall insulating film 11 as implant masks, an N-type impurity is ion implanted to a relatively high concentration to form a pair of source/drain layers 81. In the low-voltage PMOS region LPR, using the gate electrode 52, the offset sidewall 9 and the sidewall insulating film 11 as implant masks, a P-type impurity is ion implanted to a relatively high concentration to form a pair of source/drain layers 82.
In the high-voltage NMOS region HNR, using the gate electrode 53, the offset sidewall 9 and the sidewall insulating film 11 as implant masks, an N-type impurity is ion implanted to a relatively high concentration to form a pair of source/drain layers 83. In the high-voltage PMOS region HPR, using the gate electrode 54, the offset sidewall 9 and the sidewall insulating film 11 as implant masks, a P-type impurity is ion implanted to a relatively high concentration to form a pair of source/drain layers 84.
Through the aforementioned steps, the semiconductor device with the CMOS transistors 90A and 90B can be obtained.
In conventional techniques, as above described, although the extension layers in the low-voltage circuit portion and those in the high-voltage circuit portion have been formed in different steps, impurity ion implantations into the PMOS transistor and the NMOS transistor for formation of the extension layers have been performed under the same implant conditions.
Thus, the degrees of gate overlaps of the extension layers vary between the NMOS transistor and the PMOS transistor depending on a difference in diffusion rate in the silicon substrate between the N-type impurity (As) and the P-type impurity (B).
It is an object of the present invention to provide a method of manufacturing a semiconductor device with NMOS and PMOS transistors, which is capable of lessening a short channel effect, reducing gate-drain current leakage and reducing parasitic capacitance due to gate overlaps, thereby preventing a reduction in the operating speed of circuits.
According to the present invention, the method of manufacturing a semiconductor device includes the following steps (a) to (c). The step (a) is to section a major surface of a semiconductor substrate into at least a first NMOS region for forming a first NMOS transistor and a first PMOS region for forming a first PMOS transistor. The step (b) is to selectively form a first gate insulating film in both the first NMOS region and the first PMOS region to form a first gate electrode and a second gate electrode on the first gate insulating film in the first NMOS region and the first PMOS region, respectively. The step is to ion implant an N-type impurity using at least the first gate electrode as part of an implant mask to form a pair of first extension layers in the surface of the semiconductor substrate outside a side surface of the first gate electrode, and to ion implant a P-type impurity using at least the second gate electrode as part of an implant mask to form a pair of second extension layers in the surface of the semiconductor substrate outside a side surface of the second gate electrode. The step (c) includes the step of (c-1) forming first ion-implanted layers by ion implantation of the N-type impurity and second ion-implanted layers by ion implantation of the P-type impurity so that a spacing between the second ion-implanted layers is wider than a spacing between the first ion-implanted layers.
In the method of manufacturing a semiconductor device according to the present invention, since the spacing between the second ion-implanted layers formed by ion implantation of a P-type impurity is wider than that between the first ion-implanted layers formed by ion implantation of an N-type impurity, the second ion-implanted layers are spaced from the second gate electrode. Thus, even if the P-type impurity which diffuses more easily is diffused by a subsequent heat treatment process, the gate overlap length of the second extension layers can be prevented from being longer than that of the first extension layers. Such a configuration can prevent the PMOS transistor from having a more prominent short channel effect and can prevent a reduction in the operating speed of circuits due to an increase in gate-drain parasitic capacitance. It can also prevent an increase in gate-drain current leakage, thereby inhibiting an increase in standby power consumption.
These and other objects, features, aspects and advantages of the present invention will become more apparent from the following detailed description of the present invention when taken in conjunction with the accompanying drawings.
As one example of a method of manufacturing a semiconductor device according to a first preferred embodiment of the present invention, a method of manufacturing a semiconductor device with CMOS transistors 100A and 100B will be described with reference to
Referring first to
In the surface of the silicon substrate 1, P-well regions PW containing P-type impurities are formed corresponding to the low-voltage NMOS region LNR and the high-voltage NMOS region HNR, and N-well regions NW containing N-type impurities are formed corresponding to the low-voltage PMOS region LPR and the high-voltage PMOS region HPR. In the following description, the P-well regions PW and the N-well regions NW may be referred to simply as the silicon substrate without distinction.
Then, a first silicon oxide film with a thickness of 2 to 8 nm is formed to cover the whole surface of the silicon substrate 1. After that, a resist mask is formed to expose the low-voltage circuit portion and the first silicon oxide is removed from the low-voltage circuit portion by, for example, hydrofluoric acid treatment.
The resist film is then removed and a second silicon oxide film with a thickness of 0.5 to 3 nm is formed to cover the whole surface of the silicon substrate 1. Thereby the low-voltage circuit portion has the second oxide film formed thereon, and the high-voltage circuit portion has a third insulation film formed thereon which has a thickness of 2 to 9 nm greater than that of the first insulation film.
After a polysilicon layer is formed on the whole surface of the silicon substrate 1, the polysilicon layer and the second and third insulation films thereunder are patterned to selectively form gate electrodes and gate insulating films in both the low-voltage and high-voltage circuit portions. At this time, the minimum gate length is in the range of 0.015 to 0.10 μm.
The film thickness of the polysilicon layer is in the range of, for example, 50 to 200 nm. The polysilicon layer may be replaced by a polysilicon germanium layer or a multilayer structure of a polysilicon layer and a polysilicon germanium layer. Further, the polysilicon layer may previously be implanted with impurities; or after formation of an undoped polysilicon layer, the undoped polysilicon layer in NMOS regions may be implanted with an N-type impurity such as phosphorous (P) and the undoped polysilicon layer in PMOS regions may be implanted with a P-type impurity such as boron (B). Of course, the undoped polysilicon may be used without any implantation. The concentration of impurities in the polysilicon layer should be in the range of 1×1019 to 1×1021 cm−3.
In the step of
The ion implant conditions for arsenic are an implant energy of 10 to 50 keV and a dose of 5×1012 to 1×1014 cm−2. The ion implant conditions for phosphorous (P) are an implant energy of 10 to 30 keV and a dose of 5×1012 to 1×1014 cm−2. Alternatively, implantation may be performed with a mixture of those ions.
Then, a P-type impurity such as boron (B) is ion implanted into the silicon substrate 1 to form a pair of P-type impurity layers 731 (pocket implantation). The implant conditions at this time are an implant energy of 3 to 15 keV and a dose of 1×1012 to 1×1013 cm−2.
The pair of N-type impurity layers 631 and the pair of P-type impurity layers 731 grow into a pair of extension layers 63 and a pair of pocket layers 73 respectively through heat treatment. The pair of extension layers 63 are opposed to each other with the silicon substrate 1 under the gate electrode 53 sandwiched in between. In this case, an area of the silicon substrate 1 under the gate electrode 53 forms a channel region. The pair of extension layers 63 and the pair of pocket layers 73 are shown in
In the pocket implantation, the silicon substrate 1 is inclined at a predetermined angle relative to an axis of implantation and when implantation from a predetermined direction is completed, then the silicon substrate 1 is rotated a predetermined angle for next implantation. That is, with intermittent rotation of the silicon substrate 1, an N-type impurity may be implanted at an angle into the silicon substrate 1 outside the side surface of the gate electrode 53.
If we assume that the angle of inclination of the silicon substrate 1 is 0° when the silicon substrate 1 is perpendicular to the axis of implantation, it should be in the range of 0° to 50°. By inclining the silicon substrate 1, the pocket layers 73 are formed extending at an angle with respect to the major surface of the silicon substrate 1 and have their respective tip portions extending under the gate electrode 53. It is desirable that the pocket layers 73 extend as far as possible under the gate electrode 53; however, even if the inclination angle is 0°, i.e., when the axis of implantation is perpendicular to the silicon substrate 1, implanted ions will spread out horizontality due to scattering and a subsequent thermal diffusion process and thereby the pocket layers 73 will extend under the gate electrode 53.
Further, ion scattering becomes more prominent as the implantation becomes deeper and the pocket implantation is performed in a deeper region than the extension implantation. From this, the pocket implantation causes a more lateral spread of ions, whereby the extension layers 63 are covered with the pocket layers 73.
The pocket layers 73 contain an impurity of the opposite conductivity type to the source/drain layers and are provided for the purpose of restricting the lateral spread of a depletion layer from the drain layer to prevent punch-through. The pocket layers 73, however, increase the impurity concentration only locally under the gate electrode 53 and thus never increase the threshold voltage. It should be noted that the pocket implantation is not an absolute necessity.
In the step of
The ion implant conditions for boron are an implant energy of 3 to 20 keV and a dose of 5×1012 to 1×1014 cm−2. The ion implant conditions for boron difluoride (BF2) are an implant energy of 15 to 100 keV and a dose of 5×1012 to 1×1014 cm−2.
Then, an N-type impurity such as arsenic is ion implanted into the silicon substrate 1 to form a pair of N-type impurity layers 741. The ion implant conditions for arsenic are an implant energy of 40 to 140 keV and a dose of 1×1012 to 1×1013 cm−2. The ion implant conditions for phosphorous are an implant energy of 20 to 70 keV and a dose of 1×1012 to 1×1013 cm−2. Alternatively, implantation may be performed with a mixture of those ions. In the pocket implantation, it is desirable, as above described, that the silicon substrate 1 be inclined at a predetermined angle relative to the axis of implantation and rotated intermittently.
The pair of P-type impurity layers 641 and the pair of N-type impurity layers 741 grow into a pair of extension layers 64 and a pair of pocket layers 74 respectively through heat treatment. The pair of extension layers 64 are opposed to each other with the silicon substrate 1 under the gate electrode 54 sandwiched in between. In this case, an area of the silicon substrate 1 under the gate electrode 54 forms a channel region. The pair of extension layers 64 and the pair of pocket layers 74 are shown in
In the step of
In the formation of the offset sidewalls 9, the etch back of the silicon oxide film OX1 is performed, in which case the silicon substrate 1 can be etched slightly (a few nanometers). Thus, selective epitaxial growth may be performed after the formation of the offset sidewalls 9 to restore the silicon substrate 1 removed by etching.
Selective epitaxial growth uses silane gas as a source gas in a CVD (chemical vapor deposition) apparatus at a growth temperature of 500 to 800° C., thereby allowing crystal growth of silicon only on silicon layers such as the source/drain layers. In this case, in order to prevent the growth of silicon on oxide films, a crystal-growth rate should preferably be maintained at 10 Å/sec or less. It goes without saying that when the etching of the silicon substrate 1 does not present much of a problem, this process is unnecessary.
In the step of
The ion implant conditions for arsenic are an implant energy of 0.1 to 10 keV and a dose of 2×1014 to 5×1015 cm−2.
Then, a P-type impurity such as boron is ion implanted into the silicon substrate 1 to form a pair of P-type impurity layers 711. The ion implant conditions at this time are an implant energy of 3 to 15 keV and a dose of 1×1013 to 5×1013 cm−2. In the pocket implantation, it is desirable, as above described, that the silicon substrate 1 be inclined at a predetermined angle relative to the axis of implantation and rotated intermittently.
The pair of N-type impurity layers 611 and the pair of P-type impurity layers 711 grow into a pair of extension layers 61 and a pair of pocket layers 71 respectively through heat treatment. The pair of extension layers 61 are opposed to each other with the silicon substrate 1 under the gate electrode 51 sandwiched in between. In this case, an area of the silicon substrate 1 under the gate electrode 51 forms a channel region. The pair of extension layers 61 and the pair of pocket layers 71 are shown in
In the step of
In the step of
The ion implant conditions for boron are an implant energy of 0.1 to 5 keV and a dose of 1×1014 to 5×1015 cm−2. When the extension implantation is performed without removing the silicon oxide film OX2 on the surface of the silicon substrate 1, some of implanted boron ions will stay within the silicon oxide film OX2. Such boron ions in the silicon oxide film OX2, however, will be diffused into the silicon substrate 1 by a subsequent heat treatment process and will join the extension layers.
Then, an N-type impurity such as arsenic is ion implanted into the silicon substrate 1 to form a pair of N-type impurity layers 721. The ion implant conditions at this time are an implant energy of 30 to 120 keV and a dose of 1×1013 to 5×1013 cm−2. In the pocket implantation, it is desirable, as above described, that the silicon substrate 1 be inclined at a predetermined angle relative to the axis of implantation and rotated intermittently.
The pair of P-type impurity layers 621 and the pair of N-type impurity layers 721 grow into a pair of extension layers 62 and a pair of pocket layers 72 respectively through heat treatment. The extension layers 62 are opposed to each other with the silicon substrate 1 under the gate electrode 52 sandwiched in between. In this case, an area of the silicon substrate 1 under the gate electrode 52 forms a channel region. The pair of extension layers 62 and the pair of pocket layers 72 are shown in
In the step of
In the step of
The offset sidewalls 10 are obtained by, after the etch back of the silicon nitride film SN1, removing the silicon oxide film OX2 formed on the gate electrodes 51 to 54 and on the silicon substrate 1.
In the step of
The ion implant conditions for arsenic are an implant energy of 10 to 100 keV and a dose of 1×1015 to 5×1016 cm−2.
After the source/drain implantation, implanted impurity ions are activated by heat treatment. The heat treat conditions employed herein are a heat treatment temperature of 800 to 1100° C. and a heat treatment time (which is defined as the time during which the maximum temperature can be maintained) of 0 to 30 seconds. Even if the heat treatment time is 0 seconds, the heat treatment can proceed during times until the maximum temperature is reached and until the maximum temperature drops to room temperatures.
In the step of
The ion implant conditions for boron are an implant energy of 1 to 10 keV and a dose of 1×1015 to 5×1016 cm−2. The ion implant conditions for boron difluoride are an implant energy of 5 to 50 keV and a dose of 1×1015 to 5×1016 cm−2.
After the source/drain implantation, implanted impurity ions are activated by heat treatment. The heat treat conditions employed herein are a heat treatment temperature of 800 to 1100° C. and a heat treatment time (which is defined as the time during which the maximum temperature can be maintained) of 0 to 30 seconds.
In the step of
As above described, in the manufacturing method according to the first preferred embodiment, the extension layers 61 of the NMOS transistor in the low-voltage compliant CMOS transistor 100A are formed using the gate electrode 51 and the offset sidewall 9 as implant masks and the extension layers 62 of the PMOS transistor are formed using the gate electrode 52 and the offset sidewalls 9 and 10 as implant masks. Thus, the ion-implanted layers 621 formed for the formation of the extension layers 62 are more spaced from each other and more away from their gate electrode than the ion-implanted layers 611 formed for the formation of the extension layers 61 are. From this, even if implanted impurity ions are diffused by a subsequent heat treatment process, the gate overlap length of the extension layers 62 can be prevented from being longer than that of the extension layers 61.
Such a configuration can prevent the PMOS transistor from having a more prominent short channel effect and can also prevent a reduction in the operating speed of circuits due to an increase in gate-drain parasitic capacitance. It can also prevent an increase in gate-drain current leakage, thereby inhibiting an increase in standby power consumption.
Since the extension layers 61 are formed using the gate electrode 51 and the offset sidewall 9 as implant masks, the ion-implanted layers 611 formed for the formation of the extension layers 61 are formed close to the gate electrode 51. This eliminates the occurrence of a problem that no overlaps exist because of the extension layers 61 not extending under the gate and thus isolation is established between the channel and the source/drain of the NMOS transistor, thereby causing a reduction in operating current.
According to this preferred embodiment, although the low-voltage CMOS transistor 100A is formed such that the spacing between the ion-implanted layers 621 formed for the formation of the extension layers 62 becomes greater than that between the ion-implanted layers 611 formed for the formation of the extension layers 61, the high-voltage compliant CMOS transistor 100B is formed by a conventional technique. This is because it is important for CMOS transistors in the high-voltage circuit portion to maintain hot carrier resistance than reducing a short channel effect. That is, a trade-off exists between the reduction of the short channel effect and the maintenance of the hot carrier resistance; therefore, the high-voltage circuit portion sacrifices the reduction of the short channel effect for maintaining the hot carrier resistance.
As one example of a method of manufacturing a semiconductor device according to a second preferred embodiment of the present invention, a method of manufacturing a semiconductor device with CMOS transistors 200A and 200B will be described with reference to
First, as shown in
In the step of
In the step of
The ion implant conditions for arsenic are an implant energy of 10 to 50 keV and a dose of 5×1012 to 1×1014 cm−2. The ion implant conditions for phosphorous are an implant energy of 10 to 30 keV and a dose of 5×1012 to 1×1014 cm−2. Alternatively, implantation may be performed with a mixture of those ions.
Then, a P-type impurity such as boron is ion implanted into the silicon substrate 1 to form the pair of P-type impurity layers 731 (pocket implantation). The ion implant conditions at this time are an implant energy of 3 to 15 keV and a dose of 1×1012 to 1×1013 cm−2. In the pocket implantation, it is desirable, as described in the first preferred embodiment, that the silicon substrate 1 be inclined at a predetermined angle relative to the axis of implantation and rotated intermittently. Further, the pocket implantation is not an absolute necessity.
The pair of N-type impurity layers 631 and the pair of P-type impurity layers 731 grow into the pair of extension layers 63 and the pair of pocket layers 73 respectively through heat treatment. The pair of extension layers 63 are opposed to each other with the silicon substrate 1 under the gate electrode 53 sandwiched in between. In this case, an area of the silicon substrate 1 under the gate electrode 53 forms a channel region. The pair of extension layers 63 and the pair of pocket layers 73 are shown in
In the step of
The ion implant conditions for boron are an implant energy of 3 to 20 keV and a dose of 5×1012 to 1×1014 cm−2. The ion implant conditions for boron difluoride are an implant energy of 15 to 100 keV and a dose of 5×1012 to 1×1014 cm−2.
Then, an N-type impurity such as arsenic is ion implanted into the silicon substrate 1 to form the pair of N-type impurity layers 741. The ion implant conditions for arsenic are an implant energy of 40 to 140 keV and a dose of 1×1012 to 1×1013 cm−2. The ion implant conditions for phosphorous are an implant energy of 20 to 70 keV and a dose of 1×1012 to 1×1013 cm−2. Alternatively, implantation may be performed with a mixture of those ions. In the pocket implantation, it is desirable, as described in the first preferred embodiment, that the silicon substrate 1 be inclined at a predetermined angle relative to the axis of implantation and rotated intermittently.
The pair of P-type impurity layers 641 and the pair of N-type impurity layers 741 grow into a pair of extension layers 64 and the pair of pocket layers 74 respectively through heat treatment. The pair of extension layers 64 are opposed to each other with the silicon substrate 1 under the gate electrode 54 sandwiched in between. In this case, an area of the silicon substrate 1 under the gate electrode 54 forms a channel region. The pair of extension layers 64 and the pair of pocket layers 74 are shown in
In the step of
Then, in the step of
In the step of
The ion implant conditions for arsenic are an implant energy of 0.1 to 10 keV and a dose of 2×1014 to 5×1015 cm−2.
Then, a P-type impurity such as boron is ion implanted into the silicon substrate 1 to form the pair of P-type impurity layers 711. The ion implant conditions at this time are an implant energy of 3 to 15 keV and a dose of 1×1013 to 5×1013 cm−2. In the pocket implantation, it is desirable, as previously described, that the silicon substrate 1 be inclined at a predetermined angle relative to the axis of implantation and rotated intermittently.
The pair of N-type impurity layers 611 and the pair of P-type impurity layers 711 grow into the pair of extension layers 61 and the pair of pocket layers 71 respectively through heat treatment. The pair of extension layers 61 are opposed to each other with the silicon substrate 1 under the gate electrode 51 sandwiched in between. In this case, an area of the silicon substrate 1 under the gate electrode 51 forms a channel region. The pair of extension layers 61 and the pair of pocket layers 71 are shown in
In the step of
In the step of
The ion implant conditions for boron are an implant energy of 0.1 to 5 keV and a dose of 1×1014 to 5×1015 cm−2. When the extension implantation is performed without removing the silicon oxide film OX13 formed on the surface of the silicon substrate 1, some of implanted boron ions will stay within the silicon oxide film OX13. Such boron ions in the silicon oxide film OX13, however, will be diffused into the silicon substrate 1 by a subsequent heat treatment process and then will join the extension layers 62.
Then, an N-type impurity such as arsenic is ion implanted into the silicon substrate 1 to form the pair of N-type impurity layers 721. The ion implant conditions at this time are an implant energy of 30 to 120 keV and a dose of 1×1013 to 5×1013 cm−2. In the pocket implantation, it is desirable, as previously described, that the silicon substrate 1 be inclined at a predetermined angle relative to the axis of implantation and rotated intermittently.
The pair of P-type impurity layers 621 and the pair of N-type impurity layers 721 grow into the pair of extension layers 62 and a pair of pocket layers 72 respectively through heat treatment. The pair of extension layers 62 are opposed to each other with the silicon substrate 1 under the gate electrode 52 sandwiched in between. In this case, an area of the silicon substrate 1 under the gate electrode 52 forms a channel region. The pair of extension layers 62 and the pair of pocket layers 72 are shown in
In the step of
In the step of
The offset sidewalls 10 are obtained by, after the etch back of the silicon nitride film SN1, removing the silicon oxide film OX13 formed on the gate electrodes 51 to 54 and on the silicon substrate 1.
In the step of
The ion implant conditions for arsenic are an implant energy of 10 to 100 keV and a dose of 1×1015 to 5×1016 cm−2.
After the source/drain implantation, implanted impurity ions are activated by heat treatment. The heat treat conditions employed herein are a heat treatment temperature of 800 to 1100° C. and a heat treatment time (which is defined as the time during which the maximum temperature can be maintained) of 0 to 30 seconds.
In the step of
The ion implant conditions for boron are an implant energy of 1 to 10 keV and a dose of 1×1015 to 5×1016 cm−2. The ion implant conditions for boron difluoride are an implant energy of 5 to 50 keV and a dose of 1×1015 to 5×1016 cm−2.
After the source/drain implantation, implanted impurity ions are activated by heat treatment. The heat treat conditions employed herein are a heat treatment temperature of 800 to 1100° C. and a heat treatment time (which is defined as the time during which the maximum temperature can be maintained) of 0 to 30 seconds.
In the step of
As above described, in the manufacturing method according to the second preferred embodiment, the extension layers 61 of the NMOS transistor in the low-voltage compliant CMOS transistor 200A are formed using the gate electrode 51 and the offset sidewall 90 as implant masks and the extension layers 62 of the PMOS transistor are formed using the gate electrode 52 and the offset sidewalls 90 and 10 as implant masks. Thus, the ion-implanted layers 621 formed for the formation of the extension layers 62 are more spaced from each other and more away from their gate electrode than the ion-implanted layers 611 formed for the formation of the extension layers 61 are. From this, even if implanted impurity ions are diffused by a subsequent heat treatment process, the gate over length of the extension layers 62 can be prevented from being longer than that of the extension layers 61.
Such a configuration can prevent the PMOS transistor from having a more prominent short channel effect and can also prevent a reduction in the operating speed of circuits due to an increase in gate-drain parasitic capacitance. It can also prevent an increase in gate-drain current leakage, thereby inhibiting an increase in standby power consumption.
Since the extension layers 61 are formed using the gate electrode 51 and the offset sidewall 90 as implant masks, the ion-implanted layers 611 formed for the formation of the extension layers 61 are formed close to the gate electrode 51. This eliminates the occurrence of a problem that no overlaps exist because of the extension layers 61 not extending under the gate and thus isolation is established between the channel and the source/drain of the NMOS transistor, thereby causing a reduction in operating current.
In the low-voltage compliant CMOS transistor 200B, since the extension layers 64 of the PMOS transistor are formed using the gate electrode 54 and the offset sidewall 90 as implant masks, the ion-implanted layers 641 formed for the formation of the extension layers 64 are more spaced from each other and more away from the gate electrode. Thus, even if implanted impurity ions are diffused by a subsequent heat treatment process, the gate overlap length of the extension layers 64 can be prevented from being longer than required. Accordingly, even a short channel effect of the high-voltage compliant CMOS transistor 200B can be reduced, which improves the balance between the maintenance of the hot carrier resistance and the reduction of the short channel effect.
As one example of a method of manufacturing a semiconductor device according to a third preferred embodiment of the present invention, a method of manufacturing a semiconductor device with CMOS transistors 300A and 300B will be described with reference to
In the third preferred embodiment, as shown in
In the step of
In the step of
In the step of
The ion implant conditions for boron are an implant energy of 1 to 10 keV and a dose of 1×1015 to 5×1016 cm−2. The ion implant conditions for boron difluoride are an implant energy of 5 to 50 keV and a dose of 1×1015 to 5×1016 cm−2.
After the source/drain implantation, implanted impurity ions are activated by heat treatment. The heat treat conditions employed herein are a heat treatment temperature of 800 to 1100° C. and a heat treatment time (which is defined as the time during which the maximum temperature can be maintained) of 0 to 30 seconds.
Then, in the step of
As above described, in the manufacturing method according to the third preferred embodiment, the ion-implanted layers 621 formed for the formation of the extension layers 62 in the low-voltage compliant CMOS transistor 300A are more spaced from each other and more away from their gate electrode than the ion-implanted layers 611 formed for the formation of the extension layers 61 are. Thus, even if implanted impurity ions are diffused by a subsequent heat treatment process, the gate overlap length of the extension layers 62 can be prevented from being longer than that of the extension layers 61. Further in the low-voltage compliant CMOS transistor 300A and the high-voltage compliant CMOS transistor 300B, the ion-implanted layers formed for the formation of the source/drain layers 82 and 84 of the PMOS transistors are more spaced from each other and more away from their respective gate electrodes than the ion-implanted layers formed for the formation of the source/drain layers 81 and 83 of the NMOS transistors. Thus, even if implanted impurity ions are diffused by a subsequent heat treatment process, the diffusion of impurity ions from the source/drain layers into the channel regions can be prevented.
Such a configuration can prevent the PMOS transistor from having a more prominent short channel effect and can also prevent a reduction in the operating speed of circuits due to an increase in gate-drain parasitic capacitance. It can also prevent an increase in gate-drain current leakage with reliability, thereby inhibiting an increase in standby power consumption.
Since the extension layers 61 are formed using the gate electrode 51 and the offset sidewall 9 as implant masks, the ion-implanted layers 611 formed for the formation of the extension layers 61 are formed close to the gate electrode 51. This eliminates the occurrence of a problem that no overlaps exist because of the extension layers 61 not extending under the gate and thus isolation is established between the channel and the source/drain of the NMOS transistor, thereby causing a reduction in operating current.
While the invention has been shown and described in detail, the foregoing description is in all aspects illustrative and not restrictive. It is therefore understood that numerous modifications and variations can be devised without departing from the scope of the invention.
Number | Date | Country | Kind |
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2001-288918 | Sep 2001 | JP | national |
This application is a continuation of and claims the benefit of priority under 35 U.S.C. §120 from U.S. Ser. No. 13/964,849 filed Aug. 12, 2013, which is a continuation of U.S. Ser. No. 13/833,891 filed Mar. 15, 2013 (now U.S. Pat. No. 8,541,272 issued Sep. 24, 2013), which is a continuation of U.S. Ser. No. 13/185,624 filed Jul. 19, 2011 (now U.S. Pat. No. 8,415,213 issued Apr. 9, 2013), which is a continuation of U.S. Ser. No. 12/484,618 filed Jun. 15, 2009 (now U.S. Pat. No. 7,998,809 issued Aug. 16, 2011), which is a continuation of U.S. Ser. No. 11/743,021 filed May 1, 2007 (now U.S. Pat. No. 7,563,663 issued Jul. 21, 2009), which is a continuation of U.S. Ser. No. 10/212,252 filed Aug. 6, 2002 (now U.S. Pat. No. 7,220,637 issued May 22, 2007), and claims the benefit of priority under 35 U.S.C. §119 from Japanese Patent Application No. 2001-288918 filed Sep. 21, 2001, the entire contents of each of which are incorporated herein by reference.
Number | Date | Country | |
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Parent | 13964849 | Aug 2013 | US |
Child | 14140168 | US | |
Parent | 13833891 | Mar 2013 | US |
Child | 13964849 | US | |
Parent | 13185624 | Jul 2011 | US |
Child | 13833891 | US | |
Parent | 12484618 | Jun 2009 | US |
Child | 13185624 | US | |
Parent | 11743021 | May 2007 | US |
Child | 12484618 | US | |
Parent | 10212252 | Aug 2002 | US |
Child | 11743021 | US |