TAILORING NANOCRYSTALLINE DIAMOND FILM PROPERTIES

Abstract

A method for controlling the crystallite size and growth rate of plasma-deposited diamond films. A plasma is established at a pressure in excess of about 55 Torr with controlled concentrations of hydrogen up to about 98% by volume, of unsubstituted hydrocarbons up to about 3% by volume and an inert gas of one or more of the noble gases and nitrogen up to about 98% by volume. The volume ratio of inert gas to hydrogen is preferably maintained at greater than about 4, to deposit a diamond film on a suitable substrate. The diamond film is deposited with a predetermined crystallite size and at a predetermined growth rate.

Description

BACKGROUND OF THE INVENTION

[0002] Polycrystalline diamond films whose microstructure typically consist of crystallites with sizes on the order of microns have been synthesized by a variety of chemical vapor deposition (CVD) techniques from methane-hydrogen mixtures. Atomic hydrogen has been recognized to play a crucial role in the growth of phase-pure microcrystalline diamond films by the CVD techniques, typically using hydrocarbons as the carbon source. Atomic hydrogen is thought to play a number of roles including abstraction reactions, termination of carbon dangling bonds, and regasification of nondiamond materials at the growth surface. Reducing the concentration of hydrogen while continually increasing the hydrocarbon content of the plasma normally causes the growth of nondiamond phases and eventually the complete absence of the diamond phase. The grain size, surface morphology, and surface roughness of the polycrystalline diamond films prepared from hydrogen-rich plasmas depend strongly on the film thickness. Generally, the thicker the film, the larger the grain size and the rougher the surface of the film. This behavior is generally ascribed to growth competition between differently oriented grains, with grain growth in turn being strongly correlated with surface roughness as discussed in more detail below. Many applications of CVD diamond films, however, require smooth surfaces, which are not readily prepared from hydrogen-rich plasmas. The ability to control the microstructure and the surface morphology of diamond films, therefore, could be important for tailoring this unique material to a variety of applications.

[0003] It has been found that a number of properties, including surface morphology and crystal orientation of microcrystalline diamond films, depend on a variety of factors such as the nucleation process and film deposition conditions. Microcrystalline diamond films grown from randomly oriented nuclei exhibit columnar growth, which is caused by an “evolutionary selection” of crystallites. Because crystals with a direction of fastest growth more or less perpendicular to the substrate grow at the expense of less favorably oriented ones, only a few crystallites survive, and a highly textured film consisting of larger, columnar crystallites is formed after a longer period of growth. The grain size therefore increases with the thickness of the films, and usually the larger the grains the rougher the surface of the films. Therefore, if it were possible to reduce the grain size in a controlled way, smoother surfaces should result.

[0004] In order to understand and control surface morphology and crystal orientation, both the nucleation and deposition processes have been investigated extensively. It has been found that diamond films can be grown with a preferred orientation, such as (111) or (110), by precisely controlling the prenucleation treatments and the deposition process parameters. Moreover, it has been recognized that nitrogen and oxygen additions in the plasmas have a strong effect on the growth morphology of diamond films. It is known that to increase the electron density of the plasma and to modify diamond film morphology, argon has been added to plasmas. Argon has also been used in place of hydrogen in a carbon-oxygen-argon system, but oxygen was found to be a critical parameter for the phase purity of the deposited diamond films. Furthermore, in a microwave methane-hydrogen plasma, noble gases were found to have a profound effect on plasma chemistry, including additional ionization and dissociation. Upon adding a noble gas such as Ar, the emission intensity of various species changes and the growth rate of diamond is enhanced. However, the effect of Ar addition to the microwave discharges, and thus the microstructures of the deposited films at concentrations higher than about 30 vol. % heretofore were unknown.

[0005] Recently, it has been reported that nanocrystalline diamond films can be grown from an Ar—C60 microwave plasma without adding molecular hydrogen to the reactant gas. Fullerenes such as C60 and C70 have been used as the carbon source for nanocrystalline diamond growth. Fragmentation of the fullerenes in the plasma results in strong Swan band emission due to C2 radicals. The C2 dimer appears to be the growth species for nanocrystalline diamond. Furthermore, nanocrystalline diamond films have also been synthesized from Ar/CH4 microwave discharges, without the addition of molecular hydrogen. Atomic force microscopy (AFM) shows that the surface roughness is in the range of 20-50 nm, independent of the film thickness, thus suggesting that grain size remains in the nanometer range. Some of the unique properties of such nanocrystalline films have been characterized, including their tribiological and electron field emission properties.

[0006] The present invention relates to a method that allows control of the microstructure of diamond films grown from Ar/H2/CH4 plasmas. Some of the factors leading to a transition from microcrystalline to nanocrystalline diamond have been determined. The as-grown films produced from Ar/H2/CH4 plasmas with different ratios of Ar to H2 have been characterized by scanning electron microscopy (SEM), micro-Raman spectroscopy, transmission electron microscopy (TEM), x-ray diffraction (XRD), and AFM.

SUMMARY OF THE INVENTION

[0007] An object of the present invention is to provide a method for controlling the crystallite size of plasma-deposited diamond films with a plasma consisting of hydrogen, inert gas and a hydrocarbon.

[0008] Yet another object of the invention is to provide a method of controlling the crystallite size of a plasma-deposited diamond film wherein a three-part plasma of hydrogen, hydrocarbon and inert gas contains at least 40% by volume inert gas.

[0009] Yet another object of the present invention is to provide a method of depositing a nanocrystalline diamond film from a three part plasma wherein the ratio of inert gas to hydrogen is not less than 4 and preferably not less than about 9.

[0010] Another object of the invention is to provide a method of controlling the growth rate of plasma-deposited diamond films from a three part plasma wherein the pressure of the plasma is maintained between about 55 and about 150 Torr during deposition.

[0011] The invention consists of certain novel features and a combination of parts hereinafter fully described, illustrated in the accompanying drawings, and particularly pointed out in the appended claims, it being understood that various changes in the details may be made without departing from the spirit, or sacrificing any of the advantages of the present invention.

BRIEF DESCRIPTION OF THE DRAWINGS

[0012] FIG. 1 is a plan view of the SEM images of the as-grown films prepared from microwave plasmas with various mixtures of Ar, H2 and CH4 listed in Table 1 hereafter corresponding (a) film 1, (b) film II, (c) film III, (d) film IV; (e) film V; (f) film VI; (g) film VII; and (h) film VIII reported in Table 1;

[0013] FIG. 2 is a cross-section SEM image of the as-grown films with FIG. 2(a) being film I; FIG. 2b is film V; FIG. 2c is film VI; and FIG. 2d is film VII;

[0014] FIG. 3 shows the Raman spectra of the as-grown films deposited from Ar/H2/CH4 microwave plasmas with different reactant gases which show that the Raman scattering is strongly influenced by grain size; whereas (a) is film I; (b) is film II; (c) is film II; (d) is film IV; (e) is film V; (f) is film VI and (g) is film VII;

[0015] FIG. 4 shows the x-ray diffraction patterns of the as-grown films deposited from microwave plasmas with different mixtures of Ar, H2 and CH4 as the reactant gases showing that the films consist of crystalline diamond. The diffraction peaks broaden with increasing concentration of Ar due to decreasing grain size; (a) is film I; (b) is film II; (c) is film IV; (d) is film V and (e) is film VII;

[0016] FIG. 5 is a plan-view TEM image of nanocrystalline diamond films produced from Ar/H2/CH4 microwave discharges showing the effect of the concentration of Ar or H2 on the grain size: (a) is film VI with grain sizes ranging from 30 to 50 nm; (b) is film VII with grain sizes in the range of 10-30 nm;

[0017] FIG. 6 shows (a) A plan-view TEM image of diamond film (VIII) produced from 1% CH4+99% Ar composition, demonstrating that the film consists of very small grains ranging from 30 to 25 nm: (b) a high-resolution lattice fringe TEM image of the film, (c) electron energy loss spectrum of the film from an area over 10 μm in diameter showing the σ* edge. The insert images show the selected area electron diffraction patterns of the film;

[0018] FIG. 7 shows a three-dimensional AFM images of the as-grown diamond films deposited from Ar/H2/CH4 microwave plasmas with different reactant gases showing the effects of increasing the ration of Ar to H2 in the reactant gas on the surface morphology and surface roughness of the as-grown films: (a) film I; (b) film IV; (c) film VI; and (d) film VII;

[0019] FIG. 8 is a plot of the surface roughness of the as-grown diamond films versus the concentration of Ar in the Ar/H2/CH4 microwave plasmas;

[0020] FIG. 9 shows the optical emission spectra of the Ar/H2/CH4 microwave plasmas with different mixtures of Ar, H2 and CH4 in the reactant gases: (a) 2% Ar+97% H2+1% CH4; (b) 20% Ar+69% H2+1% CH4; (c) 60% Ar+39% H2+1% CH4; (d) 80% AR+19% H2+1% CH4; (c) 90% Ar+99% H2+1% CH4; (f) 97% Ar+2% H2+1% CH4;

[0021] FIG. 10 shows the plots of the emission intensity of C2 and the ratio of the emission intensities of C2 to Ha vs the concentrations of Ar in the reactant gases;

[0022] FIG. 11 shows the growth rates of the diamond films from the Ar/H2/CH4 microwave discharge vs the concentrations of Ar in the reactant gases; and

[0023] FIG. 12 shows the plots of growth rates of nanocrystalline diamond films grown from Ar/CH4 microwave plasmas and the emission intensities of C2 vs reactant gas pressures for the discharges.

DESCRIPTION OF THE PREFERRED EMBODIMENT

[0024] As used herein, plasma means any plasma wherein energy is imparted to a gas mixture by any of the usual forms of forming a plasma. A DC arc, an RF discharge, a plasma jet or a microwave may be used as energy sources to create the plasma hereinafter described. For purposes of simplicity only, a microwave has been used to describe the plasma source in the following specification but it is for brevity and not to limit the scope of the invention.

[0025] Similarly, the use of any hydrocarbon which consists fundamentally of carbon and hydrogen without added oxygen, chlorine or other elements may be used. For purposes of simplicity, methane has been illustrated but it is clear that various C70 buckyballs may be also used as may C60 fullerene, as is well known in the art. The reference to hydrocarbon hereafter refers to any hydrocarbon which may be suitable for the deposition of diamond films.

[0026] Similarly, the third component of the plasma in the subject invention is an inert gas. For purposes of simplicity, argon has been used as the inert gas but it is understood by those of ordinary skill in the art that any of the noble gases as well as nitrogen or any mixtures of the noble gases and nitrogen may be used in lieu of argon as an inert gas. Where argon is used in the specification hereafter, it is for purposes of illustration only and not for purposes of limitation.

[0027] It is true that the method of the present invention permits controlling the crystal size of plasma-deposited diamond films from about 3 nm to about 10 microns. For many uses, crystallite sizes in nanometer ranges are preferred; however, to the extent that crystallite sizes in the micron size are desired, the inventive method is capable of being used to produce crystallites of micron size.

[0028] The invention also includes process steps for controlling the growth rate of the diamond film deposited by means of plasma. It is understood from the specification as hereinafter set forth that pressures lower than about 55 Torr do not result in significant crystallite growth although crystallite growth has been observed as low as about 40 Torr. Pressures as great as 150 Torr may be used to deposit films in a rapid manner, all as set forth in FIG. 12 and discussed hereinafter.

[0029] A microwave plasma enhanced CVD system (ASTeX PDS-17) has been employed for the diamond film preparations. Mixtures of CH4, Ar, and H2 have been used as the reactant gases for the microwave discharges. The flow rate of CH4 was kept constant at 1 sccm and supplemented by H2 so as to maintain a 100 sccm total flow rate. n-type single crystal silicon wafers with an <100> orientation were used as the substrates, and mechanical polishing with fine diamond powder (0.1 μm) was employed to provide nucleation sites for the diamond film growth. It is understood, however, that any suitable substrate may be used on which to deposit diamond films, as is well known in the art. During the deposition process, the substrate temperature, which was controlled by a separate heater, was maintained at 800° C., while total ambient pressure and input power were kept at 100 Torr and 1200 W, respectively. The reactant gases used for each film deposition are listed in Table I. To investigate the effect of the concentration of the C2 dimer on the growth rate at a given Ar/H2 ratio, the total pressure of the reactant gas (CH4Ar) was varied from 40 to 150 Torr.

TABLE I
Summary of the reactant gases used for diamond film depositions from
microwave discharges.
	Reactant gas (vol %)
	Sample No.	Argon	Hydrogen	Methane
	I	2	97	1
	II	20	79	1
	III	40	59	1
	IV	60	39	1
	V	80	19	1
	VI	90	9	1
	VII	97	2	1
	VIII	99	0	1

[0030] In order to obtain some information on plasma species during the deposition process, optical emission was measured using a spectrometer equipped with a 1200 grooves/mm grating and a water-cooled photomultiplier tube (Interactive Technology). The concentration of C2 dimers could be determined from the emission spectra because it was found in earlier work that emission is linearly correlated with quantitative absorption measurements. Emission from the plasma was collected with a quartz optical fiber viewing a region 1-2 cm above the substrate. The monochromater was stepped in 2.0 Å increments with a dwell time of 100 ms from 3000 to 7000 Å. The emission intensity of C2 was measured from the C2 Swan system at 5165 Å. The growth rates of diamond thin films deposited from the Ar/H2/CH4 plasmas were determined by monitoring modulations of the surface reflectivity versus deposition time with a He—Ne laser (6328 Å) reflectance interferometer during the deposition process. One peak-to-peak modulation represents 130 nm, and depositions were carried out until film thicknesses of about 5 μm were obtained.

[0031] The as-grown films were then investigated using a JEOL 840A SEM with a tungsten filament operating at 10 KV accelerating voltage and a probe current of 3×10−11 A. Both plan-view and cross-section SEM images were obtained to examine the surface and growth morphologies as a function of added Ar. A high-resolution JEOL 4000EX TEM operated at 400 kV accelerating voltage and a Philips CM 30 analytical TEM equipped with a Gatan electron energy loss spectroscopy (EELS) spectrometer were employed for detailed microstructural characterization of selected films. The planview TEM samples were prepared by the conventional methods, i.e., mechanical cutting, shaping, dimpling, and ion milling. In order to confirm the crystalline structure of the films, x-ray diffraction was conducted by using a Philips x-ray spectrometer with a copper Ka target. The starting and ending angles (2θ) for the x-ray diffraction are 20° and 120°, respectively. A Renishaw Raman Microscope (System 2000), which can capture both Raman spectra and images, was used for further characterization of the as-grown films. The light source for illuminating the sample was provided by a He-Ne laser (6328 Å). Raman spectra and images were obtained via a grating or filter system. The Raman scattering produced by a sample was measured by a charge-coupled device (CCD) camera. To obtain the planography and the surface roughness of the as-grown films, a Burleigh ARIS-3300 personal AFM with image resolution of x-y axes <30 Å and z axis <3 Å was used. The true image software managed the secondary signals sent to the electronic controller and displayed the resulting images in close to real time.

[0032] The as-grown films were first examined by SEM in order to obtain the surface and growth morphologies as a function of added Ar. The plan-view SEM images shown in FIG. 1 demonstrate a dramatic change in the surface morphology of the films when adding Ar gas to the H2/CH4 microwave plasma. FIG. 1(a) shows the surface morphology of film I, displaying a well-facetted microcrystalline diamond surface with grain sizes ranging from 0.5 to 2.0 μm. The surface is very rough and consists of a combination of {111} and {110} facets. This SEM image suggests that the crystallite morphology of film I is independent of crystal orientation and that secondary nucleation rates must be very low. A plan-view SEM image of film II {FIG. 1(b)] shows that {111} planes are still the preferred growth planes, but small diamond particles start to form on the surface of bigger diamond grains during the deposition process, suggesting that secondary nucleation or renucleation occurs when 20% of Ar gas has been added to the microwave plasma. The number density of the small crystals increases significantly at the level of 40 to 60 volume % Ar [FIGS. 1(c) and 1(d) for films III and IV]. Note that these SEM images also show that most of the small diamond crystals nucleate and grow at the edges (twin boundaries) of larger diamond crystals. At 80 volume % Ar, the edges or the twins of the large-size diamond crystals begin to disappear, and well-facetted {111} as well as {110} diamond crystallites of micron size no longer exist, while small diamond crystals mixed with large diamond flakes are found in the plan-view SEM image {FIG. 1(e) for film V}. When 90 volume % Ar is added to the Ar/H2/CH4 plasma, the crystal sizes are greatly reduced to the nanometer scale, and the surface structure of the diamond film {FIG. 1(f) for film VI} changes from microcrystalline to nanocrystalline. At this point, facetted micron-size diamond has disappeared, and nanocrystalline diamond begins to predominate. FIGS. 1(g) and 1(h) show the plan-view images of films VII and VIII, respectively, revealing that the crystal sizes of the nanocrystalline diamond can be further reduced when the plasma consists of 97% Ar (FIG. 1(g)) or 99% Ar {FIG. 1(h)). In the latter case, the film was grown in the absence of added hydrogen.

[0033] This series of SEM micrographs demonstrates the transition of the microstructure of the films from microcrystalline to nanocrystalline diamond. In order to obtain information on the development of the growth morphology, films I, V, VI, and VII were selected for further investigation by cross-section SEM. FIG. 2(a) shows the cross-section SEM image of film I with a columnar growth structure, which is typical of the growth morphology from H2/CH4 plasmas and reflects the van der Drift growth mechanism. This columnar growth phenomenon suggests that atomic hydrogen plays an important role in suppressing secondary nucleation by regasifying small or nondiamond phase nuclei. Thus, only a few larger diamond crystals of micron size survive after a longer period of growth. The greater the Ar content of the microwave plasma, the greater the fraction of small diamond crystals. FIG. 2(b) shows the cross-section SEM image of the as-grown diamond film V, displaying that the film still has columnar growth, but the columns are much narrower than those in film I. As the Ar volume fraction increases to 90 or 97 volume %, the columnar structure totally disappears from the cross-section SEM images of films VII and VIII [see FIGS. 2(c) and 2(d)]. Instead, the cross-sectional views show smooth fracture surfaces, which suggests that the nanocrystalline diamond does not grow from the initial nuclei at the substrate film interface, but is the result of very high renucleation rates. The cross-section SEM images clearly show columnar growth, which gives way to highly dense continuous films with no distinctive growth morphology. The lack of morphological features is probably due to the fact that the crystallites are too small to be resolved in the SEM.

[0034] X-ray powder diffraction has been used to characterize the crystalline structures of the films. FIG. 3 shows the x-ray diffraction of films I, II, IV, V and VI. The diffraction peaks can be indexed according to the cubic diamond structure, which means that all the films produced from either hydrogen-rich or argon-domain microwave plasmas consist of diamond crystals. The diffraction spectra show that with increasing volume percent of Ar, the widths at half height of the diffraction peaks increase significantly, which may be correlated with decreasing grain sizes. There is no evidence for the presence of graphitic or amorphous carbon in the x-ray diffraction patterns of both microdiamond and nano-diamond films. The ratio of the (111) to the (110) diffraction peak [see FIGS. 3(a)-3(e)] increases greatly with increasing ratio of Ar to H2, indicating that the diamond grains tend to orient with the crystallographic planes parallel to the substrate surface when their sizes change to the nanometer scale. The silicon diffraction peak from Si planes derives from the substrate used for the film depositions.

[0035] X-ray electron diffractions are sensitive to the presence of crystalline carbons such as diamond or graphite but less sensitive to amorphous carbon. In contrast, Raman scattering is about 50 times more sensitive to π-bonded amorphous carbon and graphite than to the phonon band of diamond, and hence it is frequently used to characterize CVD diamond films. FIG. 4 shows the plots of Raman spectra of the as-grown films produced from Ar/H2/CH4 microwave plasmas with different ratios of Ar/H2 in the reactant gases, revealing the transition from microcrystalline to nanocrystalline diamond films. For film I grown from the Ar/H2/CH4 microwave plasma with 2 volume % Ar addition, the spectrum shows a sharp Raman band at 1332 cm−1, characteristic of diamond. Little Raman scattering in the range 1450-1490 cm−1, (graphite band) caused by carbon sp2 bonded carbon is observed. When adding argon to the reactant gas up to 40 volume %, the Raman spectra of films II and III still demonstrate the presence primarily of microcrystalline diamond, although the spectra are slightly broadened. Further increasing the concentration of Ar in the plasmas results in the shrinking of the diamond band and increasing its width at full width half maximum (FWHM) (see spectra for the films IV and V). When more than 90 volume % of Ar is added to the plasma, Raman spectra of the films VI and VII typically show nanocrystalline features. The diamond band at 1332 cm−1 is significantly broadened, and Raman scattering intensity in the 1400-1600 cm−1 region is pronounced. It has been shown that broadening of the diamond band is caused by decreasing the grain size to the nanometer scale, and the development of the “so called graphite” band is due to increasing π-bonded carbon at the grain boundaries in the nanocrystalline films. The grain boundaries consist of carbon atoms with a sp2 electron configuration. In addition to the diamond and graphite bands, the spectra also have an extra Raman shift around 1150 cm−1, which may be caused by nanocrystalline diamond. Therefore, in addition to SEM images and x-ray diffraction, Raman spectra of the as-grown films further confirm the transition of microdiamond to nanodiamond prepared from microwave plasmas as argon is added to CH4H2 mixtures. Nanocrystalline defines a size range such that when the volume ratio of Ar to H2 is about 4, the crystal structure is classified nanocrystalline but is the largest of the nanocrystalline material. When the volume ratio of Ar to H2 is about 9, the nanocrystalline structure contains smaller material.

[0036] A powerful way to study the effect of added Ar on grain size with TEM. Examples of the application of this technique to the present study are given below. FIG. 5(a) shows a plan-view TEM image of film VI (90 volume % Ar) with grain sizes ranging from 30 to 50 nm. However, film VII (97 volume % Ar) has grain sizes in the range of 10-30 nm (FIG. 5(b)). Thus, the grain size of the nanocrystalline diamond decreases strongly in the range 90-97 volume % Ar. Further characterization of the nanocrystalline film Vil (99 volume % Ar) has been conducted by high resolution TEM and EELS observations. FIG. 6(a) shows a plan-view TEM image of film VIII with grain sizes ranging from 3 to 20 nm. The inset image is a selected area (over 10 μm in diameter) electron diffraction pattern, which can be fully indexed on the diamond structure. A high-resolution TEM image shown in FIG. 6(b) demonstrates that individual grains are single crystals with sizes in the 10-20 nm range. The image of lattice fringes has a spacing of 0.205 nm, which is the interplanar distance between diamond planes {111}. The lattice image of diamond can only be observed on planes and only when they are properly oriented, since the TEM resolution is about 1.8 Å EELS has been employed as a diagnostic for amorphous or disordered carbon with sp2 bonding. It is known that the different carbon phases have very distinct K-shell absorption edge structures. Diamond has a single EELS feature with an onset at 289 eV, due to its σ* electronic state, while graphitic or amorphous carbon has an additional EELS edge starting at 284 eV, owing to its lower lying antibonding π* state. (The use of an asterisk denotes an excited state) FIG. 6(c) shows an EELS spectrum of the nanocrystalline diamond film produced from an Ar/CH4 plasma acquired over an area ˜10 μm in diameter, displaying only an EELS edge at 289 eV, characteristic of diamond. No energy loss feature at 284 eV has been observed, demonstrating the absence of an amorphous or graphitic phase in the film. These TEM analyses (plan-view and high resolution TEM images as well as the EELS spectrum) confirm that film VIII prepared from an Ar/CH4 microwave discharge without any H2 addition is composed of nanocrystalline diamond.

[0037] To obtain information on planigraphy and surface roughness, AFM has been employed. Note that all of the films for the AFM analyses have similar thicknesses of about 5 μm. FIG. 7(a) shows a three-dimensional AFM image of film I (2 volume % Ar) with an rms (root mean square) surface roughness of about 425.43 nm. Addition of Ar up to 60 volume % decreases the rms roughness of film III to 262.876 nm, because this film consists of a significant amount of small diamond particles (FIG. 7b). When Ar in the plasma is further increased, the surface roughness of film VI (90 volume % Ar) is greatly reduced to 54.19 nm (FIG. 7c). With a reactant gas mixture of 97 volume % Ar, 2 volume % H2, and 1 volume % CH4, the AFM image shown in FIG. 7(d) reveals that the surface roughness of film VII is just 18.84 nm, a typical value for our nanocrystalline diamond films. Note that the rms roughness of film VII is about 25 times smaller than that of microcrystalline diamond film I. The detailed surface analytical data acquired by AFM characterization for films I, III, VI, and VII are listed in Table II, where Z-rms is the root mean square of the surface, Z-var is the average height of the surface, and Z-peak is the height difference between the highest and lowest points on the surface. A plot of the surface roughness of the films versus the concentration of Ar in the reactant gas is shown in FIG. 8. A plot of the data suggests an almost linear relationship between surface roughness of the films and volume % Ar. Since the ratio of Ar to H2 in the reactant gas strongly affects the surface morphology and microstructure of the diamond films, this parameter can clearly be very useful in tailoring important properties of this material.

TABLE II
Summary of the surface morphologies of selected diamond films,
measured by AFM. Z-rms is the root means square of the surface; Z-var is
the average height of the surface; Z-peak is the height difference between
the highest and lowest points on the surface.
Sample No.	Z-avg (nm)	Z-rms (nm)	Z-var (nm)	Z-peak (nm)
I	1215.94	425.43	390.03	2249.02
IV	722.01	262.76	206.29	2011.31
VI	176.07	54.19	42.47	477.81
VII	58.38	18.84	14.84	187.51

[0038] These profound changes in microstructure apparently reflect equally profound changes in the plasma chemistry. Optical emission spectroscopy has been employed to investigate the Ar/H2/CH4 plasmas in order to monitor C2 dimer and atomic hydrogen concentrations in the microwave discharges. It has earlier been proposed that C2 dimer is the growth species for nanocrystalline diamond. The emission intensities of C2 dimer from the discharges which correlate linearly with the absolute C2 concentration in Ar/H2/CH4 microwave plasmas, are directly measured using the C2 Swan system (5165 Å bands). FIG. 9 shows the optical emission spectra of plasmas with different ratio of Ar to H2. At 2% Ar the major optical emission peak is due to atomic hydrogen (H∝). Under these conditions, CH3. is generally believed to be the important growth species, and its concentration has been measured by others in absorption. Increasing the Ar concentration to 20 volume percent, Hα emission is still the major feature (FIG. 9b). At 60 volume % Ar, we begin to observe emission from C2 dimers in addition to Hα (FIG. 9c). Increasing the concentration of Ar increases the emission intensity of C2 dimers (FIGS. 9(d)-9(f)) still further. The emission intensities of C2 and ratios of the emission intensities of C2 to Hα versus volume % Ar are plotted in FIG. 10. both are seen to increase by an order of magnitude in the range 80-97 volume % Ar. This has already been shown to be the region of most profound and rapid change in the microstructure of the diamond films.

[0039] Besides surface morphology, microstructure, and growth mechanism, the growth rate of diamond film has also been found to depend significantly on the ratio of Ar to H2 in the reactant gas presumably because of effects on the microwave discharge chemistry. FIG. 11 shows the growth rates of diamond films grown from 1% CH4 in Ar—H2 mixtures as a function of volume % Ar. The growth rates of the films were determined by monitoring modulations of the surface reflectivity versus deposition time with a He—Ne laser (6328 Å) reflectance interferometer. According to FIG. 11, the growth rate approximately doubles with Ar addition up to 60 volume % Ar and then decreases quite rapidly in the range of 80-97 volume % Ar. Although increasing Ar in the reactant gas from 80 to 99 volume % significantly increases the concentration of C2 dimer in the discharge (FIG. 10), the growth rate in this region nonetheless decreases. Theoretical calculations have shown that there is a pathway for the growth of diamond with C2 as the growth species that involves hydrogen addition. This pathway has a lower energy of activation than the alternative pathway that does not involve the intervention of hydrogen, thus rationalizing the effect of hydrogen on the growth rate of nanocrystalline diamond in the range 80-99 volume % Ar.

[0040] We investigated the effect of the C2 concentration on the growth rate under the condition of constant hydrogen concentration. The reactant gas for this investigation was Ar/CH4 without the addition of molecular hydrogen. The total pressure of the reactant gas was varied, but the ratio of Ar to CH4 was fixed. FIG. 12 shows plots of the growth rates of nanocrystalline diamond films and emission intensities of C2 from the Ar/CH4 plasmas versus reactant gas pressures ranging from 55 to 150 Torr. We determined that pressure strongly affects both the C2 concentration and film growth rate. When the reactant gas pressure was below 40 Torr, no C2 emission was detected, and no diamond film deposition was observed. Similarly, diamond film growth was not observed from Ar/CH4 plasmas up to 15 Torr. At 55 Torr, there was a very low emission intensity of C2, accompanied by a correspondingly low growth rate of about 0.06 μm/h. As the reactant gas pressure increased, both the emission intensity of the C2 dimers and the growth rate of the nanocrystalline films are increased significantly (FIG. 12). The close relationship between the growth rate and the C2 concentration shown in FIG. 12 suggests that the concentration of C2 in the Ar/CH4 plasma is the factor determining the film growth rate under conditions of low and constant H2 concentration. Our observations demonstrate that the reactant gas pressure plays an important role in enhancing the intensity and therefore the concentration of C2 in Ar/CH4 plasma. That C2 is the growth species for nanocrystalline diamond is confirmed by the functional relationship between the C2 concentration and the growth rate.

[0041] The growth of diamond films from Ar/H2/CH4 microwave discharges has been studied systematically. We have found a new way to control the surface morphology, grain size, and growth mechanism of diamond films by changing the ratio of Ar to H2 in the reactant gases in a systematic way. Based on SEM plan-view images of the films, it has been demonstrated that a transition from microcrystalline to nanocrystalline diamond occurs in the range from 2 to 97 volume % Ar. Cross-section SEM shows that the microcrystalline diamond films grown from the microwave discharges have columnar growth, while the fracture surfaces of the nanocrystalline diamond films are very smooth, thus suggesting a different growth mechanism. This transition from microdiamond to nanodiamond with an increase of the Ar concentration in the reactant gas has been further confirmed by XRD and Raman spectroscopy. TEM and EELS characterization demonstrates the nanocrystalline nature of the films grown from Ar/H2/CH4 microwave plasmas with an Ar concentration in the 80-97 volume %. The grain sizes of the nanodiamond range from 3 to 50 nm, depending on the ratio of Ar to H2 in the reactant gas. The surface roughness of the films is strongly affected by the microstructure and the growth mechanism. AFM analysis shows that the surface roughness of the films with the same thicknesses changes from 425 nm for microdiamond to 18 nm for nanodiamond.

[0042] An optical emission study of the Ar/H2/CH4 microwave discharges shows that the ratio of Ar to H2 in the reactant gas strongly affects the discharge chemistry. Increasing the concentration of Ar in the reactant gas significantly promotes the concentration of C2 dimer in the discharge, which is important for nanocrystalline growth. By varying the reactant gas (CH4/Ar) pressure from 40 to 150 Torr, a close relationship between the growth rate of the nanocrystalline diamond film and the concentration of C2 dimer in the plasma has been observed, confirming that C2 dimer is the growth species of the nanocrystalline diamond.

[0043] While there has been disclosed what is considered to be the preferred embodiment of the present invention, it is understood that various changes in the details may be made without departing from the spirit, or sacrificing any of the advantages of the present invention.

Claims

1. A method of controlling the crystallite size of plasma-deposited diamond films, comprising establishing a plasma containing controlled concentrations of hydrogen, an inert gas and a hydrocarbon, and depositing a diamond film on a suitable substrate, wherein the ratio of inert gas, hydrogen and hydrocarbon is varied to produce diamond crystals in the range of from about 3 nanometers to about 10 microns.

2. The method of claim 1, wherein the plasma is microwave generated and the concentrations of inert gas and hydrogen are varied in the plasma while the concentration of hydrocarbon is maintained substantially constant.

3. The method of claim 2, wherein the concentration of inert gas in the plasma is varied in the range of from about 2% by volume to about 98% by volume of the plasma.

4. The method of claim 2, wherein the concentration of inert gas in the plasma is varied in the range of from about 40% by volume to about 80% by volume.

5. The method of claim 4, wherein the concentration of inert gas is about 60% by volume.

6. The method of claim 2, wherein the concentration of hydrogen gas in the plasma is varied in the range of from about 1% by volume to about 97% by volume.

7. The method of claim 2, wherein the concentration of hydrocarbon is varied in the range of from about 1% by volume to about 3% by volume.

8. The method of claim 1, wherein the inert gas is selected from the noble gases, nitrogen and mixtures thereof.

9. The method of claim 1, wherein the inert gas is Ar.

10. The method of claim 1, wherein the hydrocarbon is selected from C1 to C70 hydrocarbons.

11. The method of claim 1, wherein the hydrocarbon includes methane.

12. The method of claim 1, wherein the inert gas is argon and the hydrocarbon is methane, and the ratio of Ar/H2 is at least 4.

13. The method of claim 12, wherein gas pressure during deposition of the diamond film is maintained above 40 Torr.

14. The method of claim 13, wherein the gas pressure is in range from about 40 Torr to about 150 Torr.

15. The method of claim 13, wherein the gas pressure during deposition of the diamond film is maintained above about 120 Torr.

16. A method of controlling the crystallite size of plasma-deposited diamond films, comprising establishing a plasma containing controlled concentrations of hydrogen, argon and a non-substituted hydrocarbon, controlling the ratio of inert gas to hydrogen while maintaining the concentration of hydrocarbon substantially constant, depositing a diamond film on a suitable substrate with the diamond film having a predetermined morphology.

17. The method of claim 16, wherein the plasma is generated from a DC arc, a plasma jet, an RF discharge or a microwave.

18. The method of claim 16, wherein ratio of Ar/H2 is at least 4.

19. The method of claim 16, wherein ratio of Ar/H2 is not less than about 9.

20. The method of claim 18, wherein the hydrocarbon is selected from the C1 to C70 hydrocarbons.

21. The method of claim 20, wherein the hydrocarbon is essentially CH4.

22. The method of claim 20, wherein the hydrocarbon is CH4.

23. The method of claim 16, wherein the hydrocarbon concentration is maintained in the range of from about 1% by volume to about 3% by volume.

24. The method of claim 16, wherein the argon concentration is maintained in the range of from about 40% by volume to about 80% by volume.

25. The method of claim 23, wherein the gas pressure during deposition of the diamond film is maintained above about 120 Torr.

26. A method for controlling the crystallite size and growth rate of plasma-deposited diamond films, comprising establishing a plasma at a pressure in excess of about 55 Torr and with controlled concentrations of hydrogen up to about 98% by volume, of unsubstituted hydrocarbons up to about 3% by volume and an inert gas of one or more of the noble gases and nitrogen up to about 98% by volume, maintaining the volume ratio of inert gas to hydrogen greater than about 4, and depositing a diamond film on a suitable substrate, whereby a diamond film is deposited having a predetermined crystallite size and at a predetermined growth rate.

27. The method of claim 26, wherein the plasma is generated by microwave energy.

28. The method of claim 27, wherein the noble gas is Ar.

29. The method of claim 28, wherein the pressure is maintained above about 120 Torr during diamond deposition.

30. The method of claim 29, wherein the volume ratio of inert gas to hydrogen is maintained at not less than about 9.