PROCESS FOR FORMING ULTRATHIN OXYNITRIDE LAYERS AND THIN LAYER DEVICES CONTAINING ULTRATHIN OXYNITRIDE LAYERS
TECHNICAL FIELD
The present invention relates to processes for forming ultrathin oxynitride layers
such as submicron dielectric layers and devices containing these layers; more specifically,
the present invention relates to oxynitride dielectric layers which reduce leakage currents in
MOS devices and which provide improved resistance to boron penetration from overlying
boron doped electrodes.
BACKGROUND OF THE INVENTION
There is increasing interest in semiconductor devices having gate dimensions less
than 0.25 micron such as the gates in MOS dual-gate integrated circuits. As will be
appreciated by those skilled in the art, devices with such small structures encounter obstacles
that are not serious problems in devices where the gate dimensions are greater than 1.0
micron. Most notably, these very small devices require submicron gate oxide layers,
typically from 30 angstroms to 70 angstroms in thickness. It has been found that the
performance of conventional gate dielectric layers formed of thermally grown silicon
dioxide is often less than ideal when fabricated in these submicron ranges. For example,
ultrathin SiO2 layers typically have a high density of pinholes. Importantly, ultrathin SiO2
layers have high boron permeability. As will be known by those skilled in the art, this
susceptibility to boron penetration can result in channel contamination. More specifically,
boron from a p+ doped polysilicon gate electrode may penetrate the thin SiO2 layer during
high temperature processing, thereby contaminating the underlying channel.
The ability to control the thickness of the ultrathin SiO2 layers is a function of
growth rate. Conventional SiO2 layers are usually grown at temperatures between 900 and
1000 degrees C or more. It is known that oxidation at these high temperatures is so rapid
that uniform film thickness is difficult to achieve. Moreover, if the process temperature is
reduced to gain greater control over the oxidation rate (for example, less than 900 degrees
C, the SiO2 layers exhibit a significant increase in compressive stress that produces an
accumulation of electric charge at the semiconductor interface, leading to increased current
leakage.
In order to address the limitations of SiO2 ultrathin films, oxynitride (SixOyNz)films
have been proposed for use as gate dielectrics. For example, it is known in the art that
silicon oxynitride films are less permeable to diffusing boron atoms than silicon dioxide
films.
One such prior art technique uses NH3 for thermal nitridation of Si or SiO . 2
Although the resultant films have some desirable properties when compared to SiO2 films,
the hydrogen atoms produce a significant number of electron traps (which may be reduced
somewhat through reoxidation) and the films exhibit a fixed-charge build-up.
There has also been some discussion in the prior art on the use of N2O to produce
thin dielectrics by rapid thermal processing as well as in conventional furnaces. In the case
of N2O nitridation of silicon (lightly doped with boron), it has been demonstrated that peak
nitrogen concentration is found in the SiO2 at the SiO2/Si interfacial region.
In addition, pure NO has been used for nitridation of SiO2 in order to lower the
thermal budget required with nitridation using N2O. In this process, higher concentrations
of nitrogen in the oxynitride layer were obtained than with the use of N2O, presumably due
to complete disassociation of NO. Also, NO direct nitridation of silicon has been proposed
for the fabrication of gate dielectric layers comprising a layer of silicon oxynitride underlain
by a layer of silicon dioxide. These composite films may be made by thermally growing a
thin layer of silicon dioxide, and then forming a layer of silicon oxynitride or silicon nitride
by chemical vapor deposition (CVD).
In U.S. Patent No. 5,464,792, entitled, PROCESS TO INCORPORATE
NITROGEN AT AN INTERFACE OF A DIELECTRIC LAYER IN A
SEMICONDUCTOR DEVICE, there is disclosed a semiconductor device which includes
a substrate on which a first dielectric layer is formed on the substrate with a buffer layer
disposed on the first dielectric layer. The buffer layer is exposed to a nitrogen source and
nitrogen is diffused through the buffer layer and into the first dielectric layer to create a
region of high nitrogen concentration near an interface between the buffer layer and the first
dielectric layer. It is disclosed that either N2O or NO can be used as the nitrogen source.
Finally, the use of a mixture of NO and O2 has been used to produce an oxynitride
layer in a semiconductor device. In United States Patent No. 5,512,519 entitled, METHOD
OF FORMING A SILICON INSULATING LAYER IN A SEMICONDUCTOR DEVICE,
there is provided a method of forming an insulating layer of a semiconductor device in
which an oxide layer having a preselected nitrogen concentration and also a preselected
thickness is prepared by independently regulating the flow rate of NO and O2 gas into a
reaction chamber. This method is such that the NO and O2 gas is supplied to the chamber
by regulating the gas flow while maintaining the inside of the chamber at a temperature of
about 750 to 1050 degrees C for a predetermined time, wherein nitrogen is included at the
Si/SiO2 interface.
SUMMARY OF THE INVENTION
In one aspect the present invention provides a method of forming an insulating layer
in a semiconductor device. A substrate is provided having a silicon surface in the [100] or
[111] crystalline orientation. The silicon surface is prepared in the customary manner for
thermal growth of an oxide layer. The substrate is placed in a chamber which is purged prior
to oxide growth. A source of nitrous oxide and a source of nitric oxide are provided in
communication with the chamber. The substrate is heated to an appropriate temperature for
oxide formation. The two gases are metered into the chamber where they contact the
prepared silicon surface of the substrate. A reaction occurs at the silicon surface in which
a layer of oxynitride (SixOyNz) is formed on the silicon surface. The reaction is allowed to
proceed until the desired thickness of the oxynitride layer is achieved.
In another aspect the present invention provides an improved semiconductor device
in which a gate oxynitride dielectric layer is provided having an unequal distribution of
nitrogen with the peak nitrogen concentration being present at the region of said layer
adjacent the gate electrode.
These and other aspects and advantages of the present invention will be more fully
appreciated in the following detailed description of the preferred embodiments of the
invention with reference to the drawings.
BRIEF DESCRIPTION OF THE DRAWINGS
Figure 1 is a flow diagram illustrating the steps of the present invention in one
embodiment.
Figure 2 is a diagrammatic view of an oxynitride layer made in accordance with the
present invention.
Figure 3 is a diagrammatic view of an MOS device which incorporates the oxynitride
layer of the present invention.
Figure 4 is a graph illustrating boron penetration and effectiveness of the barrier
properties of the present invention.
Figure 5 is a graph illustrating interface state densities at various temperatures which
are a function of suppressed boron penetration.
Figure 6 is a graph illustrating charge-to-breakdown characteristics under -V stress.
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS OF THE INVENTION
Referring now to Figure 1 of the drawings, the process of the present invention
begins in step 1 with the preparation of a substrate on which an oxynitride layer is formed.
In the most preferred embodiment the substrate is part of a semiconductor device, most
preferably a metal-oxide-semiconductor (MOS) device. The substrate includes a region of
silicon and will generally comprise a silicon wafer of orientation [100] or [111], i.e. single
crystal silicon. The preparation of the surface will follow customary procedures for
removing a native oxide in a reaction chamber.
Although the present invention is preferably used with a conventional semiconductor
fabrication furnace which includes a vacuum chamber having the usual gas ports, it is also
contemplated that the techniques disclosed herein can be used with Rapid Thermal
Processing (RPT) techniques.
Following preparation of the silicon substrate, the chamber is purged in step 2 prior
to introduction of the nitrogen-containing gases used to form the oxynitride layer. The purge
gas may comprise an inert gas such as nitrogen or the chamber may be purged using the
novel nitrogen-containing gas mixture of the present invention.
In step 3, the prepared silicon substrate is heated to a temperature of at least about
700 degrees C, and more preferably from about 750 to about 1100 degrees C. As stated,
in the most preferred embodiment, the reaction chamber will comprise a conventional
semiconductor fabrication furnace. In step 4, the prepared surface is contacted with a
mixture of nitrous oxide (N2O) and nitric oxide (NO) gases in the chamber. In order to
better control the growth characteristics of the oxynitride layer, the substrate is preferably
heated to reaction temperature, i.e. 750 to 1100 degrees C, prior to introduction of N2O and
NO in the chamber.
In the present invention, N2O constitutes from about 50 to about 95 percent by
volume of the gas mixture in the chamber and more preferably from about 70 to about 95
percent by volume at reaction temperature and pressure. NO constitutes from about 5 to
about 50 percent by volume of the gas mixture in the chamber and more preferably from
about 5 to about 30 percent by volume at reaction temperature and pressure. In the most
preferred embodiment, the mixture in the chamber contains from about 90 to about 95
percent by volume N2O and from about 5 to about 10 percent by volume NO. That is, a
volumetric ratio of N2O to NO of about 20 to 9 to about 9 to 5.
The N2O and NO gas mixture is created in one of two ways. Most preferably the
N2O and NO are metered into the chamber as separate gas streams through discrete gas
ports. Alternatively, the two gases may be premixed and then introduced into the chamber
as a single gas stream. The flow rate of gas into the chamber may very, but preferably will
be from about 1000 to about 10,000 standard cubic centimeters per minute (SCCM) and
more preferably from about 1000 to about 5000 SCCM. The gas pressure within the
chamber during formation of the oxynitride layer is preferably from about 500 to about 760
torr. and more preferably form about 600 to about 760 torr. The gases used are high-purity,
i.e. 99.99% and above.
Under these conditions, an oxynitride layer begins to form having an overall
composition of silicon, oxygen and nitrogen, where the concentration of N is from about 0.5
to about 10% (atomic %) and more preferably from about 1 to about 5% (atomic %). The
reaction is not fully understood, but it has been determined that the process of the present
invention results in an oxynitride layer having multiple identifiable layers or regions with
different nitrogen concentrations as will be more fully described herein.
As stated above, the present invention is particularly useful in the preparation of the
gate dielectric layer of a MOS device. In the fabrication of a MOS device, the gate integrity
of the dielectric material is a key factor in determining the long term reliability
characteristics of the device. In a MOS transistor, the gate dielectric material must support
a substantial voltage difference between the gate electrode and the semiconductor substrate.
The gate dielectric material must also maintain its ability to support the voltage difference
between the gate and the substrate, while being subjected to the electron and hole injection
from both the gate electrode and the substrate. In the case of very-large-scale-integration
(VLSI) devices, the effective gate lengths are on the order of less than 1 micron and often
less than .25 micron. At such small effective gate lengths, electrons can be injected into the
dielectric layer during periods when the transistor is switched on and off. The injection of
electrons into the dielectric material can, over time, cause a shift in the threshold voltage of
the transistor. Over an extended period of time, a continual shift in the threshold voltage
eventually results in an inability to switch the transistor on and off. Therefore, it is
important in the fabrication of a MOS transistor that a high quality dielectric material be
provided in order to insure long term reliability of the transistor.
Accordingly, in the present invention the reaction conditions are maintained until an
oxynitride layer of from about 30 to about 100 angstroms and more preferably from about
30 to about 50 angstroms is formed. In the preferred reaction temperature, the reaction will
be carried out for from about 1/2 to about 2 minutes and more preferably from about 1 to
about 1 1/2 minutes.
Referring to Figure 2 of the drawings, oxynitride layer 20 is shown as formed in
accordance with the present invention having three generally defined layers or regions, peak
nitrogen layer or gate interface region 22, bulk region 24 and channel interfacial region 26.
It is to be understood that these areas or regions have no precise lines of demarcation but
consist of gradual transitions based on nitrogen content. As stated, region 22 contains the
peak concentration of nitrogen (preferably from about 5 to about 10 atomic % and more
preferably from about 5 to about 7 atomic %) which provides a barrier against boron
migration from the overlying gate electrode. Bulk region 24 preferably has from about 2 to
about 1 atomic % nitrogen. Region 26 preferably has from about 0.5 to about 0.1 atomic %
nitrogen. In an alternative embodiment of the present invention these regions are created
by ion implantation using nitrogen.
Referring now to Figure 3 of the drawings, the present invention is illustrated as
semiconductor device 30 which is shown as an n-channel MOS transistor. Therein, source
32 and drain 34 are shown formed as n+ doped regions in p type silicon wafer or body 36.
Channel 38 is defined underlying gate 40. Oxynitride layer 42 made in accordance with the
present invention is shown overlying channel 38 and electrically separating gate electrode
44 therefrom. Gate electrode 44, as stated, is preferably boron doped (p+) polysilicon.
Preferably, the microelectronic device made in accordance with the present invention is a
dual gate CMOS device. Most preferably the device is a surface channel p+ -poly gate
PMOSFET. For a general description of these types of devices (without the oxynitride layer
of the present invention) reference is made to "Design Tradeoffs Between Surface and
Buried-Channel FET's," IEEE Trans. Electron Devices. Vol. ED-32, p. 584, 1985, the entire
disclosure of which is incorporated herein by reference.
EXAMPLES
The following examples are provided to more fully illustrate the present invention
and are in no way intended to limit the full scope of the invention.
P+-poly PMOS devices were fabricated on n-type Si (100) substrates. Gate oxides
(53 A) were grown at 900°C in pure 02 ambient. Some oxides received a short 15-second
NO anneal at 900°C. After undoped polysilicon deposition (-3000A), samples with and
without NO anneal received nitrogen implantation at 40KeV to a dose of 5xl015cm"2,
followed by a N2 anneal for 30 minutes at 900°C to drive in nitrogen to the poly/SiO 2
interface. BF2 implantation was performed at 50KeV to a dose of 5xl015cm 2, followed by
dopant activation in N2 for 30 minutes at 850 °C, 900°C, or 950°C. For reference, POCl3-
doped n+-polysilicon gate MOS devices were fabricated on p-type (100) substrates
following the same process conditions. Three different nitrogen profiles in gate dielectrics
(confirmed by SIMS) were generated: nitrogen peak at the Si02/Si interface (NO annealed
Si02) [6], nitrogen peak at the poly/Si02 interface (N implant), and nitrogen peaks at the both
poly/Si02 and Si02/Si interfaces (combination of NO anneal and N implant). We have
compared the diffusion barrier properties, interfacial characteristics, and gate oxide
reliability on these devices.
Boron penetration and effectiveness of the barrier properties in the PMOS devices
are shown in Fig. 1. As can be seen, flatband voltage (VFB) shift is suppressed in all the
oxynitride devices regardless of the N peak positions. The slight NO anneal (900°C, 15s)
produces a very effective diffusion barrier at the Si02/Si interface without suffering from
channel mobility degradation caused by nitrogen-induced fixed charges [6]. Devices with
a nitrogen peak at the poly/Si02 interface also exhibit enhanced immunity to boron
penetration, similar to observed in [7]. However, the best diffusion barrier is obtained by
the "double N peaks", i.e., the combination of NO anneal and N implantation, for high
thermal budgets (e.g. 950°C).
Initial interface state density (Dit) is also much reduced in the oxynitride devices
compared to control devices due to suppressed boron penetration [8]. As shown in Fig. 2,
good interface properties after 900°C drive-in are obtained by any of the diffusion barriers.
At high drive-in temperature (950°C), however, boron penetration also occurs in oxynitride
devices except devices with "double N peaks", which exhibit superior immunity against the
creation of interface states (Fig.l). It is interesting to note the correlation between the
amount of B penetration and interface states density (Figs. 1 and 2). The formation of B-F
complexes increases Dit as well as weakens the Si02/Si interface structure, and is precursor
for the generation of interface states during subsequent electrical stress. Devices with B
penetration to the Si02/Si interface show significant distortion of the quasi-state C-V curves
after stressing (now shown), except the devices with double N peaks, in which B penetration
is completely suppressed.
The charge-to-breakdown characteristics under-Vg stress are shown in Fig. 3. As can
be seen, the gate dielectric reliability is significantly influenced by the nitrogen peak
position. Compared to control devices, QBD of oxynitride devices is improved by having
the diffusion barrier at the poly/Si02 interface and is degraded by having the diffusion barrier
at the Si02/Si interface. The additional diffusion barrier at the Si02/Si interface in double N-
peak devices does not further improve the oxide reliability; instead it slightly degrades QBD
(compared to the device containing only a N peak at the poly/Si02 interface). In contrast,
QBD of NMOS devices with these dielectrics under-Vg stressing are comparable regardless
of the N peak position (not shown). As indicated by charge trapping study during constant
current stress (not shown), devices with more degraded QBD show higher charge trapping
[4], caused by the formation of B-F complexes in Si02 [9] pr creation of strained and broken
Si-0 bonds due to boron penetration [5].
Thus, it is apparent that there has been provided in accordance with the invention a
method and apparatus that fully satisfies the objects, aims and advantages set forth above.
While the invention has been described in connection with specific embodiments thereof it
is evident that many alternatives, modifications, and variations will be apparent to those
skilled in the art in light of the foregoing description. Accordingly, it is intended to embrace
all such alternatives, modifications and variations that fall within the spirit and broad scope
of the appended claims.