Note: Descriptions are shown in the official language in which they were submitted.
11 Background of the Invention
12 The invention relates to methods for dielectrically
13 isolating regions of monocrystalline silicon from other
14 regions of monocrystalline silicon.
Description of the Prior Art
-16 In the monolithic integrated circuit technology, it
17 is usually necessary to isolate various active and passive
18 elements from one another in the integrated circuit structure.
19 These devices have been isolated by backbiasing, PN junctions,
partial dielectric isolation and complete dielectric isolation.
21 The dielectric materials used have been silicon dioxide, glass,
22 and so forth. The preferred isolation for these active
23 devices and circuits is some form of dielectric isolation.
24 The dielectric isolation has the substantial advantage~over
the PN junction isolation because it allows the butting of
26 the circuit elements against the isolation and thereby
27 result in greater density of packing of the active and
28 passive devices on the integrated circuit chip.
FI9-77-032 ,-1-
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1 One form of dielectric lsolation involves the
2 formation of grooves or depressions in silicon where
3 the isolation regions are to be forrned. During the
4 groove formation, the remainder of the silicon surface
is protected by a protective film which is substantially
6 unaffected by the silicon etch used to form the grooves.
7 The usual protective layer is a silicon nitride, silicon
8 dioxide sandwich layer. Following the formation of the
9 grooves by conventional chemical etching, the silicon
body is subjected to a conventional oxidation step where-
11 by the silicon in the groove area is oxidized and the
12 silicon dioxide fills up the groove as well as oxidizing
13 further into the silicon to form the isolation region.
14 One of the ma~or problems with this process is what is
known as "bird's beak".
16 The "bird's beak" is a non-planar silicon dioxide
17 formation at the top periphery of the groove and is caused
18 by the lateral oxidation underneath the silicon nitride
19 layer. Since the oxidation of a specific thickness of
silicon requires an almost equivalent amount of free space
21 to expand into, and since the Si3N4-limits the unrestricted
22 expansion, the result is an up-pushing of the silicon
23 nitride at the edge of the groove. The final consequence
~-24 of this is a general stress in the perimeter region of
the groove as well as difficulties in subsequently achiev-
26 ing good butted diffusions against the vertical portion of
27 the silicon dioxide. This non-butting capability defeats
FI9-77-032 ~ -2-
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1 a major benefit of the original purpose of the silicon dioxide
region. This process is described more fully by E. Kooi U.S.
Patent 3,970,486, Clevenger U.S. 3,534,234, Peltzer U.S. 3,648,125
and I. Magdo et al, Canadian Patent Application No. 143,3~8, filed
May 30, 1972.
Another technique for forming d-ielectric isolation is described
in the V. Y. Doo U.S. Patent 3,386,865 and "A Composite Insulator-
Junction Isolation" by R.E. Jones and V. Y. Doo, published in
Electrochemical Technology, Vol. 5, No. 5-6, May-June 1967, pp. 308-
310. This technique involves the formation of a silicon dioxide
layer or similar type of layer on the substrate in the region where
dielectric isolation is desired. An epitaxial layer is grown upon
the substrate in all regions except where the silicon dioxide is lo-
cated. The surface of the epitaxial layer and the sides of the
openings are partially thermally oxidized. The openings are then
- filled by vapor deposition of polycrystalline silicon, silicon dioxide
or similar materials. This technique has some disadvantages. Selec-
` - tive epitaxy, as required by this technique, is very sensitive to f
the area relationship between silicon dioxide and silicon regions.
~ 20 For example, two different s-ize silicon regions would tend to fill in
; at a different rate so that at-the end of a process, the regions are
- filled in to a different extent.- Also, in mesa-type depositions,
crystallographic faceting tends to occur. This results in pyramid-
like growth and tends to widen the isolation regions beyond the
original lithography ,capabilities. The slanted e~
FI9-77-032 - - 3 -
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1 silicon/silicon dioxide interfac~ will again cause
2 difficulties in achieving reliable butted diffusion
3 against the silicon dio~ide region.
4 The formation of grooves and the filling of such 4
5 . grooves have been described by other publications such
6 as the G. L. Kuhn, U.S. Patents 3,892,608 and 3,969,168.
7 In these patents~ chemical etching is used to form a V
8 groove, a rounded bottom groove or a rectangular evacuated
9 space. There is little detail as to how the groove is
10 formed but it is clear that the groove would be limited by t
11 the nature of the chemical etching step. The process does J
12 not necessarily yield a planar surface and it requires
13 photolithography after the formation of the grooves. D. K.
~14 Roberson U.S. 3,956,033 describes a similar chemical etch
15 followed by filling with polycrystalline silicon. Here t~
16 again, the groove is limited by the chemical etching
17 technique and it is unclear how the overgrowth of the
18 polysilicon is removed. U.S. Patents K. E. Bean et al
19 3,725,160 and W. R. Morcom et al 3,979,237 also show
filling of grooves. In these patents, the effect of
21 chemical etching is more clearly brought out where it is
22 shown that monocrystalline silicon are preferentially ~.
23 etched chemically to provide grooves having symmetrical
24 sidewalls sloped at precise angles depending upon the '
particular face crystal to which the silicon surface is
26 aligned.
27 The Brand U.S. Patent 3,979,765 also describes the
28 chemical etching to open rectangular grooves and the
'
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1 filling of the grooYeS with insuldtor material. ~lowever, it is dif-
ficult to unclerstand how some of the principal steps such as etching
and filling are actually e-ffected from the description.
The formation of rectangular yrooves have been rnade in the Hoch-
berg U.S. 3,966,577 and T. Kaji et al U.S. 3,997,378 and S.A. Abbas,
IBM* TDB Vol. 20, No. 1, p.l44, June 1977 entitled "Recessed Oxide
Isolation Process", by reactive ion etching techniques. None of these
references describe the problems and detailed solutions for forming
reactive ion etched grooves in s;licon. Neither do they involve
t~emselves with the problem of effectively filling the groove to form
the best possible isolation for the silicon regions. There are des-
criptions of the reactive ion etching processes in the "A Survey of
Plasma-etching Processes", R. L. Bersin, published in Solid State
Technology, May 19, 1976, pp. 31-36 and particularly for silicon in
J. M. Harvilchuck published German patent application number 26,174,834,
published December 9, 1976 for "Reactive Ion Etching of Silicon".
However, the details of the reactive ion etching in these publications
do not show how the reactive ion etching would be utilized in the
formation of dielectric isolation.
Summary of the Pre_ent Invention
In accordance with the present invention, a method for forming
dielectric isolation is described wherein tapered sided isolation
structures are formed in a specific manner. In the present text, we
use openings,
*Registered Trade Mark
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1 channels, holes, grooves and trenches interchanyeably.
2 Tapered sided openings of less than about 4 micrometers
3 in width at the surface are formed in a silicon body in
4 the areas where dielectric isolation is desired. The
formation of the tapered openings is by reactive ion
6 etching. The taper of the tapersided openings can be
7 from near vertical to as much as 20 from the vertical
8 and terminates into the substantially flat bottom of the
9 openings. The surfaces of the openings are then thermally
oxidized to silicon dioxide. The oxidized openings are
11 filled with a suitable dielectric material to fully
12 isolate the regions of silicon. The dielectric material
13 from above the surface of the body is removed to provide
14 uniformly filled isolation pockets at the surface of the
silicon body. The precise taper of the opening is
16 important so as to balance the need for greater density
17 of devices against the completeness of groove filling by
18 the CVD method. Grooves of insufficient taper will
19 exhibit a CVD SiO2 which could contain an opening or
poor quality dielectric region in the center of the
21 filled groove.
22 The method for dielectrically isolating regions of
23 silicon further overcomes the problem of reactive ion
24 etching through the silicon body which is composed of a
layer of highly doped silicon. The highly doped silicon
26 is etched more isotropically under most conditions of
27 the reactive ion etching than regions of lower doping.
28 The conditions of reactive ion etching through such a
: ,
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1 hiyhly doped layer of silicon involves the use of a
2 reactive chlorine specie ambient having a pressure of
3 between about 2 to 50 micrometers with the chlorine
4 specie percentage in the gas of be-tween about 2 to 10
and etch rate of between about 0.03 and 0.08 micrometers.
6 srief-Description of thc ~ra~.~ings
7 FIGURES lA - lE illustrate a method for forming the
8 dielectric isolated structure of the invention;
9 FIGURE 2 is a graph showing the problem of over-
etching highly doped silicon regions at various etching
11 conditions;
12 FIGURES 3 and 4 illustrate the problem of filling
13 the tapered hole of varying tapered angles from the
14 vertical;
FIGURE 5 illustrates the problem of filling tapered
16 holes of one taper from the vertical for different widths
17 of holes;
18 FIGURE 6 is experimental data of the groove taper
19 angle change as a function of chemical vapor deposited
silicon dioxide filling thickness;
21 EIGURE 7 is experimental data of the extent of
22 crevice above or below the surface versus groove width
23 for different tapers; and
24 FIGURES 8, 9 and 10 are graphical illustrations
which indicate the characteristics of filling the open-
26 ings with dielectr:ic material.
FI9-77-032 -7-
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1 Dcscrlptioll of the Prefcrl-ecl ~mbodimcnts
2 Referring now particularly to FIGU~ES 1~ , the
3 manufacturing steps for the dielect:ric isolation of one
4 form of the invention are shown. The struc-ture of
FIGURE lA includes the monocr~stalline silicon substrate
6 10 which is shown as P- conductivity for illus-tration
7 purposes, an N+ layer 12 over the substrate 10 and an
8 N- conductivity layer 14 on the layer 12. For the
9 purposes of the invention, either all or some of the
layers 10, 12 and 14 could be of opposite conductivity
11 from the conductivity types indicated. However, it is
12 preferred to have the layer 12 to be in a high conduc-
13 tivity region where it will ultimately be the collector
14 of a bipolar transistor. This structure can be fabri-
cated by various techniques. However, the preferred
16 technique is to provide a P- monocrystalline silicon
17 substrate and to diffuse an N+ blanket diffusion into
18 the substrate by using conventional diffusion or ion
19 implantation of an N type impurity such as arsenic,
antimony or phosphorus to produce an N+ xegion with a
21 surface concentration of between about 1 x 1019 or
22 1 x 10 1 atoms/cc. The layer 14 is subsequently grown
23 onto the 10, 12 structure by means of epitaxial growth.
24 This may be done by conventional techniques such as the
use of SiCL4/H2 or SiH4/H2 mixtures at growth temperatures
26 of about 1000C to 1200C. The N+ layer may have a
27 typical thickness of between about 1-3 microns whereas
28 the epitaxial layer has a thickness of from 0.5 to 10
FI9-77-032 -8-
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1 microns, the e~act thicknesses depending upon the device
2 to be built.
3 ~lternatively, the s-tructure could be made by
4 various combinations of thermal diffusion, ion implantation
and/or epitaxial growth which would include the formation
6 of a varied subcollector region where subsequent formation
7 of bipolar devices is desired.
8 In certain device structures, buried highly doped
9 regions or layers are not necessary and can therefore be
omitted. This would be true for FET type devices.
11 Alternatively, multiple buried highly doped regions of
12 different dopant types could be formed by multiple epitaxial
13 and diffusion processing. These structures could be needed
14 for buried subcollector, as well as buried conductor lines.
The next series of steps shown in FIGURES lA and ls
16 are directed to the technique for reactive ion etching
17 of tapered sidewall openings or channels in the silicon
18 structure. A silicon dioxide layer 16 is formed by the
19 conventional techniques of either thermal growth at a
temperature of 970C in a wet or dry oxygen ambient or
21 by chemical vapor deposition. Other mask materials can
22 also be used such as silicon nitride and aluminum oxide
23 or combinations thereof and so forth~ Openings 18 are
24 formed in the oxide in the regions where dielectric
isolation is desired. These openings are formed by the
26 conventional photol:ithography and etching techniques.
27 The FIGURE lA structure is now ready for the reactive
28 ion etching process. This process may be more fully
FI9-77-032 -9-
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1 understood by reference to the J. `~. Ilarvilchuck e-t al
2 patent application referred to above. The ~ induced
3 plasma is reactive chlorine, bromine or iodine specie
4 as specified in the Harvilchuck patent application. The
5 thic~ness of the masking layer 1~ is between about 2,000
6 to 20,000 Angstroms, the exact thickness depending on the
7 depth requirement of the silicon groove. The precise
8 description of the RF glow discharge apparatus is given
9 in the beforementioned patent application. The reactive
ion etch or plasma ambient is preferably a combination of
11 an inert gas such as argon and a chlorine specie. Appli-
12 cation of suitable power in the order of about 0.1 to
13 0.75 watts/cm from an RF voltage source will produce
14 sufficient power density to cause the reactive ion etching
operation of silicon to be carried out at a rate of about
16 0.02 to 0.08 micrometers per minute. The desired result
17 of the etching is shown in FIGURE lB wherein the openings
18 or channels at least partially penetrate through the P-
19 conductivity region 10. The channels or openings may go
substantially through the N+ region 12.
21 It is important that the openings or channels be
22 tapered at greater than about 2 from the vertical.
23 This is because the subsequent dielectric filling deposi-
24 tion process results in a slightly thicker deposition near
the top of the groove as opposed to the bottom of the
26 groo~e. Thus, in case of vertical grooves, there is at
27 one stage, an overgrowth of the remaining narrow groove
FI9-77-032 -10-
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1 which results in poor dielectric material quality in
2 the region belo~ the overgrown area. In case of a
3 sufficiclltly tapered groove, -the groove is filled up
4 from the bottom. The preferred amount of taper, adequate
for appropriate chemical vapor deposition filling of a
6 dielectric material such as silicon dioxide will in part
7 depend on the groove width as will become clear from
8 FIGURE 6. The taper of much greater than 20 from the
9 vertical will take up an undue amount of space on the
surface of the semiconductor device. This formation of
11 the tapered structure depends upon two principal items.
12 The primary influence on the sidewall formation is the
13 angle of the sidewall of the masking layer 16 in the
14 opening 18. The second dependence is upon the etch rate
difference between the masking material and the substrate
16 material. The higher substrate/masXing material etch rate
17 ratio favors the more vertical walls in the silicon
18 substrate.
19 Standard lithography techniques tend to result in
slightly tapered resist window openings. Whe~ reactive
21 ion etching is used to open the underlying silicon dioxide
22 film through these tapered resist windows, and when the
23 etch rate ratio between the resist and silicon dioxide
24 is near unity, the taper of the resist window is trans-
ferred to the silicon dioxide window. This taper is
26 then, in turn, transîerred into the silicon unless a
27 high etch rate ratio exists between silicon and silicon
28 dioxide. The taper in silicon dioxide mask is preferably
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1 within the range of 5 to 20 from vertical. If the
2 lithography process permits vertical resist window
3 openings, then the silicon dioxide window opening is
4 vertical and under such conditions the tapered shape
of the silicon opening would tend to be near vertical
6 and generally insensitive to the etch rate ratio between
7 silicon and silicon dioxide.
8 The change in etch rates also influences the under-
9 etching of highly doped N+ or P+ regions such as region
12. At etch rates of about 0.07 micrometers per minute,
11 vertical grooves with no lateral N+ undercut etching are
12 formed. Lowering the etch rates will cause increasingly
13 more taper, as indicated in FIGURE 2. FIGURE 2 is a graph
14 which shows the effect of the silicon etch rate in micro-
meters per minute versus the percent of the chlorine specie
16 in argon for various system pressure conditions. Curve 20
17 is at a pressure of 10 micrometers. At this pressure and
18 at the etch rates indicated, there is virtually no under-
19 cutting in the N+ regions no matter what percent of chlorine
specie is used.
21 The taper of curve 20 goes from virtually vertical
22 sidewalls at 10 percent chlorine specie in argon to a
23 20 taper from the vertical at about 3 percent chlorine
24 specie in argon. The power is 0.16 watts/cm2 in all of the
FIGVRE 2 experiments and the cathode is silicon dio~ide.
26 Curve 22 shows that at an etch rate of 0.06 micrometers
27 per minute and approximately 3 percent chlorine in argon,
28 a vertical sidewall groove is obtained. As one moves up
FI~-77-032 -12-
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1 on the curve to the e~ch ra-te of 0.10 micrometers per
2 minute and 5 percent chlorine specie in argon, ~e see
3 undercutting in the N+ region. Eurther, as we proceed
4 up the curve to 0.14 micrometers per minute and approx-
S imately 7 percent chlorine specie in argon, we see ex-
6 tensive undercutting which is very serious. The curve
7 24 shows the situation at pressures of 40 micrometers;
8 at 2 percent chlorine specie in argon and at about 0.06
9 micrometer/min. etch rate, the N+ undercutting is not a
problem. However, as one moves up the curve to 0.08 micro-
11 meters, the undercutting begins to become more apparent.
12 Further up the curve it is expected that further undercutting
13 will occur. The point 26 is reactive etching at 90 micro-
14 meters total pressure and shows extensive undercutting
15 which produces an unsatisfactory product. It can be seen -~
16 from this graph of FIGURE 2 that the useful operative
17 pressure range is from about 2 to 50 micrometers with a
18 chlorine specie concentration of between about 2 and 10
19 percent in the gaseous ambient and an etch rate between
about 0.04 and 0.08 micrometers per minute. The chlorine
21 specie which will operate in this manner are CL2, CCL4,
22 CHC13 and o~her chlorine containing species.
23 The key difficulty with the undercutting of the N+
24 region is that it limits the ability of how close one
isolation region can be placed next to another. If
26 significant underetching occurs and two isolation regions
27 are located very close to each other, a total underetch of
28 the region 14 will occur. Furthermore, the N+ collector
FI9-77-032 -13-
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1 region will be entirely removed and thus no transistor
2 could be built. A still further proble~l would occur for
3 any undercut region in that such non-linear tapered
4 grooves would not be properly filled in with chcmical
vapor deposited dielectric material such as silicon
6 dioxide. The consequence is a filled groove with a buried
7 hole or channel.
8 Referring now to FIGURE lC, the next step in the
9 process is to thermally oxidize the openings or channels
by subjecting the body to an oxidation ambient ~hich may
11 be for example 970C in wet oxygen. The body is subjected
12 to the ambient for about 10 to 30 minutes to produce the
13 preferred silicon dioxide thickness within the opening or
14 channel of about 500 to 2000 Angstroms. The purpose of
the thermal oxide 30 is to assure good silicon/silicon
16 dioxide interface properties, the qualities of which are
17 usually not as good with chemical vapor deposited dielectric
18 material~ Good quality dielectric Material is necessary to
19 permit the subsequent abutting of diffused junctions
against the dielectric isolation.
; 21 The minimum thickness is nominally 500 Angstroms so
22 that a good thermal silicon dioxide layer is formed. Any
23 thinner layer could present difficulties because of pin
24 holes in the oxide and therefore cause electrical integrity
problems.
26 The maximum thickness is primarily dictated by the
27 time required at elevated temperatures. Long times at
FI9-77-032 -14-
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1 high temperatures will tend to move any diffused junction
2 within the silicon regions. Very thic~ oxide films formed
3 at such temperatures will also cause stress problerns in
4 the silicon material.
The grown oxide 30 will follow almost precisely the
6 taper of the sidewalls in the opening formed by the
7 reactive ion etching step. The next step, involviny the
8 filling of the opening with a suitable dielectric material,
9 is shown completed in FIGURE lD wherein the opening or
channel is filled with vapor deposited silicon dioxide
11 layer 32. In order to completely fill the opening or
12 channel, it is necessary to cover the surface of the layer
13 30 not only in the channel or opening, but completely over
14 the surface of the silicon body. The preferred filling
process is a chemical vapor deposition of silicon dioxide
16 using gas mixtures of Co2/SiH4~N2 or N2O/SiH4/N2 at 800 -
17 1000C.
18 Typical deposition rates are of the order of SG - 100
19 Angstroms per minute and total deposition thicknesses are
nominally 3 micrometers for 2 micrometers wide grooves if
21 a near planar surface is desired. The specific relation-
22 ship of planarity and chemical vapor deposited silicon
23 dio~ide thickness is shown in FIGURE 8.
24 The problems involved in the filling of openings or
channels can be more fully appreciated with reference to
26 FIGURES 3, 4 and 5. These figures show the critical
27 importance of the sidewall taper and the problem of si~e
28 of the opening at the silicon surface. As can be seen in
FI9-77-032 -15-
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1 FIGURE 3, the center area of the chemical vapor deposited
2 silicon dioxide filled opening shows a small crevice region
3 40. This crevice is present only after silicon dioxide
4 etching of a cross-sectional surface. The crevice forma-
tion implies a poor oxide in that region and experiments
6 indicate that this is caused by the oversrowth of the
7 silicon dioxide over opening dimensions which are less
8 than about 0.2 micrometers in width and having a wall
9 angle of less than about 20. It has been determined
that the tapered angle of the opening decreases as the
11 opening filling progresses (FIGURE 6). Tilis can affect
12 the overcoating in different ways. The specific effect
13 being related to the groove width and taper. These effects
14 are shown in FIGURES 3, 4 and 5. They illustrate by a
series of lines, which represent equal amounts of chemical
16 vapor deposited silicon dioxide layers, the progression of
17 filling in of the grooves. As can be seen in FIGURE 3,
18 the etched out crevice region 40 tends to be buried further
19 down into the filled in groove as the groove width widens
and the taper increases. FIGURE 4 shows only the taper
21 effect for the same size grooves. Again, the more tapered
22 groove tends to bury the crevice (or poor silicon dioxide
23 region) deeper. FIGURE 5 shows the groove width effect
24 for a specific taper angle. As the groove widens, the
poor oxide region tends to occur at a higher position.
26 These results are summarized in FIGURE 7 in which the
27 extent of the crevice above or below the silicon wafer
FI9-77-032 , -16-
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1 surface is plotted for differen-t groove wldths and
2 different taper angles. ~s is clear, successfully
3 buried poor silicon dioxide regions can be achieved
4 for groove geometries of narrow groove widths and
5 . nominal taper angles. As the groove width widens,
6 the taper must be increased accordingly in order to
7 keep the poor oxide buried.
8 FIGVRE 6 is experimental data indicating the change
9 of a taper angle of a groove as groove filling proceeds.
It is obvious that for vertical grooves, any deposition
11 will cause negative tapered grooves and consequently
12 result in physical silicon dioxide voids.
13 FIGURE 8 is experimental data on the necessary
14 amount of chemical vapor deposited silicon dioxide re-
quired to fully planarize the surface over a groove.
16 The amount to achieve this is related to the width of
j 17 the groove at the top of the groove.
18 FIGURE 9 shows similar experimental data to FIGVRE
19 8 on groove filling and planarity and points out that
the planarization is strictly dependent on the groove
21 width and not on the taper angle.
22 FIGVRE 10 is still another means of expressing the
23 surface planarity of a filled groove, this time showing
24 the effect of groove width and different overcoating
thicknesses.
26 The final step of the process is the reactive ion
27 etching of the silicon dioxide layer 32 shown in FIGURE
28 lD to produce the structure of FIGURE lE. The excess
FI9-77-032 -17-
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1 silicon dioxiae is conveniently removed by reactive
2 ion etching and with the help of an optical film thick-
3 ness monitoring system or by the knowledge of the e-tch
4 rate of the silicon dioxide. The system used for this
process would be of the low pressure sputter etch type
6 system with the wafer positioned on a silicon cathode
7 cover plate. A fluorinated hydrocarbon such as CP~
8 would be used as an etchant so that an SiO2/Si ratio of
9 approximately 1:1 results. The gas pressure could run
from 10 to 70 micrometers with gas flow rates of 2 to
11 50 cc/min. The RF power level would run from 0.1 watts/cm2
12 to 0.5 watts/cm2.
13 The result of the reactive ion etch thinning of the
14 silicon dioxide layer is the possible exposure of the
inadequately buried poor oxide region in the center of
16 the groove. This is a potential problem because any
17 chemical wet etching of the wafer surface with such ex-
18 posed regions of poor silicon dioxide would cause crevice
19 formation in those regions. Such crevices could become
potential traps for dirt or process residues and could
21 negatively influence the device characteristics.
22 An alternative embodiment to overcome some of the
23 undercutting problems would be to form a highly doped
24 region 12 in a manner that this region would be inter-
rupted and set back from the areas where the openings or
26 channels are to be formed. Therefore, a lower doped
27 region of P-, which is to be reactive ion etched, would
28 surround the region. Thus, there would be no undercutting
FI9-77-032 -18-
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1 problem. This alternative requires special oxidation
2 and photolithographic and etching steps to allow for
3 this interrupted region.
4 The formation of a P+ region underneath the isola-
5 . tion region may be useful when tlle substrate is P-. In
6 such cases, the P- region has a tendency to change its
7 resistivity, even to the extent of inverting to N-type
8 material, when it is thermally oxidized. A P+ implant
9 prevents such inversion possibility. This may be formed
by use of a P+ ion implantation of a dopant such as ~oron
11 before the thermal oxidation step of the groove. The
12 preferred technique is the use of a thin chemical vapor
13 deposited silicon dioxide coating of the groove. Such
14 coating of between about 500 to 800 Angstroms will permit
the implantation of for example, boron, through the bottom
16 of the groove into the silicon, but not through the
17 silicon dioxide on the tapered walls. This is true since
18 the slanted walled silicon dioxide represents a much
19 thic~er silicon dioxide than its actual thickness because
of the directionality of the 90 implanting ions. After
21 the implantation and appropriate annealing, the chemical
22 vapor deposited siliFon dioxide is removed and the normal
23 process sequence (i.e. FIGURE lC) is taken up.
24 Another approach to modify the fabricatior process
is to utilize a heat anneal in a steam atmosphere of the
26 sample after process step FIGURE lE~ This anneal at
27 about 900-950C would be to convert any e~posed poor
,, .
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31~72
1 quality silicon dioxide in the center region of the
2 groove to a good quality silicon dioxide_ The benefit
3 of this process modification is that thectaper angle
4 does not become as important for assuring buried poor
5 . quality silicon dioxide regions and ther~fore permits
6 higher device density fabrication. This process can
7 cure poor silicon dioxide in, for example, the smaller
8 taper angles, such as 2 to 4.
9 While the invention has been particularly shown and
1~ desc~ibed with reference to the preferred embodiments
11 thereof, it will be understood by those skilled in the
12 art that various changes in form and de~ail may be made
13 therein without departing from the spiri-t and scope of
14 the invention. For example, devices oth~r than a bi-
polar transistor could be used advantage~usly in the
16 isolated monocrystalline silicon pockets~formed by the
17 process. Such devices would include pas~ive devices
18 such as resistors and active devices suc~ as ~îOSFET
19 devices.
GOS:jr
~/9/77
.~ , .
FI9-77-032 -20-
