Prevention of dopant out-diffusion during silicidation and junction formation

High integrity cobalt silicide contacts are formed with shallow source/drain junctions. Embodiments include depositing a layer of cobalt on a substrate above intended source/drain regions, followed by silicidation and diffusing impurities from a doped film during or after silicidation in an environment which discourages out-diffusion of the impurities to the environment. The resulting source/drain junctions are self-aligned to the cobalt silicide/silicon substrate interface, thereby preventing junction leakage while advantageously enabling forming the cobalt silicide contacts at optimum thickness to avoid parasitic series resistances. The formation of self-aligned source/drain junctions to the cobalt silicide/silicon substrate interface facilitates reliable device scaling, while the avoidance of unwanted diffusion of impurities to the environment assures adequate doping of the source/drain regions.

FIELD OF THE INVENTION

The present invention relates to a method of manufacturing a semiconductor device comprising refractory metal silicide contacts to source/drain and silicon gate regions. The present invention has particular applicability in manufacturing reliable high density semiconductor devices with submicron design features, shallow junction depths and cobalt silicide contacts to source/drain regions.

BACKGROUND ART

Current demands for high density and performance associated with ultra large scale integration require design rules of about 0.18 microns and under, increased transistor and circuit speeds and improved reliability. As device scaling plunges into the deep sub-micron ranges, it becomes increasingly difficult to maintain performance and reliability.

In the manufacture of conventional complementary metal oxide semiconductor (CMOS) devices, referring to FIG. 1A , isolation regions 110 , called field oxide regions, are formed in a semiconductor substrate 100 of silicon dioxide by local oxidation of silicon (LOCOS) or by shallow trench isolation (STI). A conductive gate 130 , such as polysilicon, is also formed on substrate 100 , with a gate oxide layer 120 in between. Dielectric spacers 140 are formed on sidewalls of the gate 130 , and source/drain regions 150 are formed on either side of gate 130 by implantation of impurities.

As gate lengths are reduced to below 0.5 , refractory metal silicide layers, such as titanium silicide, are typically formed over source/drain regions 150 and gate 130 to reduce the sheet resistivity of these components, thereby improving device performance. Referring to FIG. 1B , a titanium layer 160 is deposited, as by sputtering, over the entire substrate 100 as well as field oxide 110 , gate 130 and spacers 140 . A low temperature rapid thermal anneal (RTA) reaction creates a first-phase titanium silicide (C 49 ) on the exposed silicon of gate 130 and source/drain regions 150 . The unreacted titanium over field oxide 110 and spacers 140 is then removed, and a high temperature RTA reaction changes the first-phase titanium silicide into a low-resistivity second-phase titanium silicide 170 (C 54 ), as shown in FIG. 1 C. Since the titanium silicide does not form on field oxide 110 or spacers 140 , it is self-aligned to the gate 130 and source/drain regions 150 . Hence, the titanium silicide formed in this process is known as titanium salicide (self-aligned silicide).

Titanium salicide is effective in decreasing sheet resistivity if the gate length is greater than about 0.25 . At a gate length of about 0.25 the titanium silicide sheet resistance rises dramatically due to narrow-line effects; that is, the low-resistivity silicide C 54 does not completely form because first-phase C 49 grains are very large (about 0.5 ), and hence it is not possible to fit enough grains on the gate to nucleate and grow a sufficient amount of C 54 .

To maintain low sheet resistance as gate lengths are decreased in scale below about 0.25 , cobalt is typically used instead of titanium in silicide formation. Cobalt silicide does not display the undesirable narrow-line effects of titanium silicide because the conversion from its first-phase cobalt silicide to its low-resistivity second-phase cobalt silicide is a diffusion reaction, rather than the nucleation and growth reaction of titanium silicide, and therefore the relationship of grain size to gate size is not a limiting factor.

However, the cobalt salicide process has a drawback in that cobalt silicide is more likely than titanium silicide to cause source and drain junction leakage, which can result in unacceptably high power dissipation as well as functional failure. This problem becomes especially critical as gate lengths are scaled below 0.25 , and source and drain junctions are typically made shallower to prevent transistor short-channel effects. Since shallow junctions are more susceptible to junction leakage than deep junctions, cobalt silicide related junction leakage effectively limits CMOS device scaling.

A cause of this junction leakage, referring to FIG. 2 , is the unevenness of the interface between the cobalt silicide 210 and the silicon source/drain regions 220 , which results in an insufficient distance between portions of the bottom of the cobalt silicide 210 and source/drain junctions 220 a . When a junction 220 a is biased, a depletion region (i.e., an area depleted of free carriers) is formed which extends on either side of the junction 220 a . Since the distance the depletion region spreads from the junction 220 a is inversely proportional to the doping of the region, and source/drain region 220 is more heavily doped than substrate 200 , the depletion region spreads mainly into substrate 200 . Nevertheless, if cobalt silicide 210 extends into the depletion spread, leakage can occur as carriers are swept across this highly charged region.

Junction leakage also occurs due to consumption of silicon of substrate 200 during silicide formation. For example, when cobalt silicide is formed to a given thickness, a thickness of substrate silicon slightly greater than the thickness of the silicide is consumed. As junctions become shallower with device scaling, consumption of substrate silicon during silicidation results in an insufficient distance between portions of the bottom of the cobalt silicide 210 and source/drain junctions 220 a and, hence, junction leakage. Junction integrity can be maintained by providing a large enough distance between junction 220 a and the interface of silicide 210 and source/drain region 220 ; i.e., by reducing the thickness of cobalt silicide 210 . However, reducing its thickness increases the sheet resistivity of cobalt silicide 210 , thus reducing its effectiveness.

Copending U.S. patent application Ser. No. 09/187,427 and U.S. Pat. No. 6,096,399 disclose methodologies for forming junctions self-aligned to the bottom of the cobalt silicide, thus avoiding junction leakage by addressing the problem of insufficient distance between portions of the bottom of the silicide and the source/drain junctions. According to these methodologies, a doped film is deposited on top of the cobalt or cobalt silicide, from which impurities are diffused through the cobalt silicide to form source/drain regions having a junction depth which is substantially evenly spaced from the metal silicide/silicon interface.

Copending U.S. patent application Ser. No. 09/318,824 addresses the problem of substrate silicon consumption during silicidation, facilitating the formation of shallower source/drain junctions demanded as devices are further scaled. According to this methodology, a doped amorphous silicon film is deposited on top of the cobalt. The amorphous silicon film is consumed during silicidation, thereby decreasing the amount of substrate silicon consumed, and the dopant is diffused through the cobalt silicide to form source/drain regions having ultra-shallow junctions substantially evenly spaced from the metal silicide/silicon interface.

Disadvantageously, when implementing the methodologies of U.S. Pat. No. 6,096,599 and copending applications Ser. Nos. 09/187,427 and 09/318,824, the impurities may diffuse, upon heating, out of the doped film and into the environment rather than into the substrate. This may occur whether the diffusion step is carried out at the low temperature RTA step, the high temperature RTA step, or at a separate heating step. As a result of unwanted out-diffusion, the amount of impurities available to dope the substrate may be insufficient to properly form the source/drain regions.

There exists a need for a method of manufacturing a semiconductor device by diffusing impurities from a doped layer into the substrate during or after silicidation to form source/drain regions, without a loss of dopant due to out-diffusion of impurities to the environment.

SUMMARY OF THE INVENTION

An advantage of the present invention is a method of manufacturing a semiconductor device having source/drain regions formed by diffusion of impurities from a doped layer during or after silicidation which avoids out-diffusion of impurities from the doped layer to the environment.

According to the present invention, the foregoing and other advantages are achieved in part by a method of manufacturing a semiconductor device, which method comprises forming a metal layer on a main surface of a semiconductor substrate containing silicon;

heating to form a layer of metal silicide; forming a doped layer having impurities on the metal layer or the metal silicide layer; and heating to diffuse the impurities into the substrate to form source/drain regions having a junction depth below the metal silicide layer, in an environment that substantially prevents out-diffusion of the impurities from the doped layer to the environment.

DESCRIPTION OF THE INVENTION

When employing the methodologies of U.S. Pat. No. 6,096,599 and copending U.S. patent applications Ser. No. 09/187,427 and Ser. No. 09/318,824 to form source/drain regions by diffusing impurities from a doped layer into the substrate during or after silicidation, the impurities may diffuse out of the doped film away from the substrate and into the ambient, resulting in insufficient doping of the substrate. The present invention addresses and solves problems stemming from unwanted out-diffusion of impurities into the environment, thereby ensuring the formation of adequately doped source/drain regions.

According to the methodology of the present invention, a layer of metal, e.g., cobalt, is deposited on a substrate before forming the source/drain implants, i.e., above intended source/drain regions, field oxide regions, gates and spacers. As used throughout the present disclosure and claims, the term substrate denotes a semiconductor substrate or an epitaxial layer formed on the semiconductor substrate. A two-step silicidation process is then carried out, as by RTA, as described in U.S. Pat. No. 6,096,599 and copending applications Ser. No. 09/187,427 and Ser. No. 09/318,824, wherein a doped film is deposited on either the cobalt layer, the high resistivity first-phase cobalt silicide, or the low-resistivity second-phase cobalt silicide so that the dopants diffuse through the silicide into the substrate when heated to form source/drain regions having a junction depth which is substantially evenly spaced from the metal silicide/silicon interface. However, the heating step in which impurities from the doped film are to diffuse out of the doped film and towards the substrate; i.e., the high- or low-temperature RTA or a separate heating step, is performed in an environment that substantially prevents out-diffusion of the impurities to the environment.

In one embodiment of the present invention, the environment is saturated with a species of the impurities, thus creating a high concentration of impurities at the top surface of the doped film. Since dopants tend to diffuse from areas of high concentration to areas of low concentration, the presence of a high concentration of impurities in the environment will cause the impurities in the doped film to tend to diffuse towards the substrate, thereby minimizing unwanted out-diffusion of impurities into the environment, and ensuring the formation of adequately doped source/drain regions.

In another embodiment of the present invention, the diffusion step is carried out in an inert gas atmosphere, such as nitrogen or argon, maintained at a pressure of about 770 Torr. The pressure substantially prevents the impurities from diffusing upward and out of the doped film into the environment, thereby minimizing losses of impurities to the environment.

In all embodiments of the present invention, the impurities, which gain mobility when the doped film is heated, readily diffuse out of the doped film and diffuse through the cobalt silicide into the substrate, as cobalt silicide does not have as great an affinity for dopants as the substrate silicon. Due to the high diffusivity of the impurities in the cobalt silicide, the impurities form a shallow source/drain junction self-aligned to the cobalt silicide/silicon interface, thus avoiding junction leakage independently of the interface shape and the cobalt silicide thickness.

An embodiment of the present invention is illustrated in FIGS. 3A-3G . As shown in FIG. 3A , field oxide regions 310 are formed on substrate 300 , as by LOCOS or STI, followed by a thermally grown gate oxide layer 320 and a polysilicon gate 330 , typically by low pressure chemical vapor deposition (LPCVD), masking and etching. Dielectric spacers 340 are thereafter formed on sidewalls of gate 330 , such as silicon dioxide LPCVD and anisotropically etched.

Referring to FIG. 3B , a layer of cobalt 350 is deposited across substrate 300 , including field oxide regions 310 , spacers 340 and gate 330 , as by sputtering. Next, referring to FIG. 3C , a low temperature RTA is performed at about 400 C. to about 600 C.; e.g., about 470 C., to cause portions of cobalt layer 350 above the silicon of gate 330 and substrate 300 to react and form a high resistivity first phase cobalt silicide 360 a . Portions of cobalt layer 350 above field oxide regions 310 and dielectric spacers 340 do not react to form a silicide, so cobalt siuicide 360 a is self-aligned to gate 330 and the intended source/drain regions of substrate 300 . Thereafter, the unreacted portions of cobalt layer 350 above field oxide regions 310 and spacers 340 are stripped away, as by wet etching.

A high-temperature RTA is next performed at about 700 C. to about 900 C.; e.g., about 825 C., to convert high resistivity phase cobalt silicide 360 a into a low-resistivity second phase cobalt silicide 360 b (see FIG. 3 D). A first doped film 370 is then deposited on cobalt silicide 360 b , as by LPCVD (see FIG. 3 E). First doped film 370 is doped with a first conductivity type of impurities, either n-type impurities such as phosphorus or arsenic, or P-type impurities such as boron or indium, which will subsequently dope substrate 300 to form source/drain regions having ultra-shallow junctions. First doped film 370 is formed of a material which allows the impurities to diffuse out, and should be a dielectric if it is not to be stripped off after diffusion of the impurities. Suitable materials include silicon dioxide, silicon oxynitride or silicon nitride.

A photoresist mask 380 is formed on first doped film 370 , and has openings 381 to expose portions 370 a of first doped film 370 corresponding to selected portions 361 a of region 360 b which are not to receive dopant from first doped film 370 . First doped film 370 is then etched, as depicted in FIG. 3F , to form through-holes 370 b in first doped film 370 , thus exposing selected portions 361 b of region 360 b , and a second doped film 371 is deposited over selected portions 361 b and over first doped film 370 , as depicted in FIG. 3 G. Second doped film 371 is doped with a second conductivity type of impurities different than the first impurity type of first doped film 370 , and like first doped film 370 can be silicon dioxide, silicon oxynitride or silicon nitride, deposited as by LPCVD, contain impurities such as boron, arsenic, antimony, phosphorus, or indium depending on its impurity type, and must be a dielectric if it is to remain on the device after diffusion of the impurities.

Thereafter, as depicted in FIG. 3H , a heating step is carried out in an environment saturated with a species S of the second conductivity type of impurities of doped film 371 . For example, if the second conductivity type of impurities is phosphorus, species S is phosphene; if the second conductivity type of impurities is arsenic, species S is arsene. Likewise, species S may also be boron fluoride, antimony or indium depending on the second conductivity type of impurities.

The heating step is performed at a temperature such that the stability of cobalt silicide 360 b is maintained. At temperatures about 950 C., unwanted agglomeration occurs in cobalt silicide. Therefore, the heating step is carried out at about 850 C. to about 950 C. for about 10 seconds to about 60 seconds; e.g., about 925 C. for about 10-60 seconds.

The heating step diffuses impurities out of first and second doped films 370 , 371 , through cobalt silicide 360 b and into gate 330 and substrate 300 to form source/drain regions 390 below cobalt silicide 360 b and to form shallow junctions J at a depth of about 2000 or less; e.g., about 500 . Because the impurities readily diffuse through the cobalt silicide 360 b , junctions J are self-aligned to the cobalt silicide/silicon interface and substantially equidistant therefrom; i.e., the shape of junctions J substantially correspond to the shape of the bottom of cobalt silicide 360 b , thus assuring a sufficient distance between the bottom of cobalt silicide 360 b and junction J to avoid junction leakage, regardless of the interface shape and the thickness of cobalt silicide 360 b . Moreover, because species S saturates the environment in which the diffusion step is carried out with a species of the second conductivity type of impurities, impurities do not out-diffuse from second doped film 371 into the environment, but rather diffuse towards substrate 300 , thereby ensuring the formation of adequately doped source/drain regions 390 .

In another embodiment of the present invention, instead of the environment being saturated by species S, the heating step leading to formation of source/drain regions 390 and junctions J may be carried out in an inert gas atmosphere maintained at a pressure of about 770 Torr; e.g., an atmosphere of nitrogen or argon at about 770 Torr. The elevated pressure prevents impurities from diffusing upward and out of second doped film 371 into the environment, thereby minimizing losses of impurities to the environment.

Each of the first doped film 370 and the second doped film 371 have an impurity concentration great enough to form junctions J; i.e., an impurity concentration of about 1 10 21 cm 3 to about 2 10 21 cm 3 .

Second doped film 371 partially overlays first doped film 370 , as depicted in FIGS. 3G and 3H ; however, the second conductivity type of impurities, initially carried by second doped film 371 , should not be allowed to diffuse through the first doped film 370 (during the low temperature RTA) and counter-dope source/drain regions 390 . Several methods for preventing such unwanted diffusion are disclosed in, for example, copending application Ser. No. 09/187,427, which is hereby incorporated by reference.

In another embodiment of the present invention, as shown in FIGS. 4A-4B , doped films 400 , 401 are formed, as described above, on cobalt layer 350 , then the low-temperature RTA step is performed in an environment saturated with species S to form high resistivity cobalt silicide layer 360 a and to diffuse impurities from doped films 400 , 401 into or through cobalt silicide layer 360 a (see FIG. 4 A). Alternatively, the low-temperature RTA can be performed in an inert gas atmosphere under pressure, as described above. The high-temperature RTA is then performed to form low resistivity cobalt silicide layer 360 b and source/drain regions 390 and junctions J self-aligned to the bottom of cobalt silicide layer 360 b (see FIG. 4 B). This embodiment enables formation of self-aligned junctions J without adding an additional heating step to the silicidation process.

In another embodiment of the present invention, depicted in FIGS. 5A-5B , doped films 500 , 501 are formed on high resistivity cobalt silicide layer 360 a (see FIG. 5 A), then the high-temperature RTA step is performed in an environment saturated with species S to form low resistivity cobalt silicide layer 360 b and to diffuse impurities from doped films 500 , 501 through cobalt silicide layer 360 b to form source/drain regions 390 and junctions J self-aligned to the bottom of cobalt silicide layer 360 b (see FIG. 5 B). Alternatively, the low-temperature RTA can be performed in an inert gas atmosphere under pressure, as described above. This embodiment enables formation of self-aligned junctions J without adding an additional heating step to the silicidation process.

In still another embodiment of the present invention, depicted in FIGS. 6A-6B , doped amorphous silicon films 600 , 601 are deposited on cobalt layer 350 , then the low-temperature RTA step is performed in an environment saturated with species S to consume amorphous silicon films 600 , 601 , form high resistivity cobalt silicide layer 380 a and diffuse impurities from amorphous silicon films 600 , 601 through cobalt silicide layer 380 a to form source/drain regions 390 (see FIG. 6 A). Alternatively, the low-temperature RTA can be performed in an inert gas atmosphere under pressure, as described above. The high-temperature RTA is then performed to form low resistivity cobalt silicide layer 380 b and junctions J self-aligned to the bottom of cobalt silicide layer 380 b (see FIG. 6 B). The consumption of amorphous silicon films 600 , 601 during silicidation results in less consumption of silicon of substrate 300 , enabling the formation of ultra-shallow source/drain junctions J.

The methodology of the present invention enables utilization of the methodologies of U.S. Pat. No. 6,096,599 and copending U.S. patent applications Ser. No. 09/187,427 and Ser. No. 09/318,824 to form shallow source/drain regions having ultra-shallow junctions of high integrity, with cobalt silicide contacts of optimized thickness thereon, by diffusing impurities from a doped layer into the substrate during or after silicidation without diffusion of the impurities out of the doped film away from the substrate and into the ambient. The present invention enables formation of cobalt silicide which is sufficiently spaced apart from the source/drain junctions to avoid junction leakage, regardless of the shape of the cobalt silicide/silicon interface or the thickness of the cobalt silicide layer, while ensuring the formation of adequately doped source/drain regions by avoiding unwanted out-diffusion of impurities into the environment. Thus, the present methodology facilitates device scaling by enabling the formation of low-resistivity, properly doped, silicided source/drain regions having ultra-shallow junctions without silicide-related junction leakage. The present invention is applicable to the manufacture of various types of semiconductor devices having silicided source/drain regions, particularly high density semiconductor devices having a design rule of about 0.18 and under.