5.2 Patterning ITO
Patterning ITO is necessary not only for appraising the quality of the film (using TLM method for example) but also for fabricating useful micro-contacts to devices. As for metals and semiconductors, there are two potential methods of patterning ITO:
Due to the high velocity particles involved in a reactive r.f. sputtering system, the liftoff
technique was not satisfactory. Both thin (< 1 mm) and thick (> 3 mm) photoresists (PR) were
used in the experiments for ITO deposition by liftoff technique; whereas the thin PR was not
removable in acetone, by flood exposure under UV lamp or in heated KOH solution, the
thicker PR was less difficult to remove. However, the walls of the thick PR were rigidly stuck
to the substrate. Microscopic examination of the thin PR showed numerous cracks on its
surface most probably caused by PR hardening and baking as a result of penetration of
incident particles through its entire depth. In case of the thick PR, the side walls are most
probably damaged by bombardment of high velocity plasma particles reflected from the
deposited ITO as shown in Figure 5.9:
Figure 5.9: Photoresist wall hardening by reflected plasma particles
In another experiment, the substrate was patterned with PR as usual and placed on the
Nordiko substrate table at a 45 degree angle to reduce damage to the PR. However, the PR
was still difficult to remove while the ITO deposition rate dropped below satisfactory levels (<
1 Å/sec).
Therefore, ITO patterning was carried out by etching methods only. These include wet
chemical etching and ion milling or dry etching as presented in the following sub-sections.
It was found that ITO readily etches in HF solution (HF:H2O2:10H2O) and HCl solutions of
various strengths. However, ITO cannot be etched in ammonia solutions
(8NH3:3H2O2:400H2O). The etch rates in HF were very high (between 100Å/sec to
150Å/sec) and often uncontrollable. Subsequently HCl solution was used for wet etching ITO
in majority of the cases.
Figure 5.10: Wet Chemical Etch Rate of ITO as a function of HCl concentration at room
temperature and controlled humidity
The undiluted etch solution contained 36% HCl corresponding to a molar solution.
Figure 5.10 shows the etch rate of ITO deposited on S.I. GaAs
substrates as a function of HCl
concentration in the etchant. These reactions were carried out in the cleanroom under
controlled conditions where the temperature was kept below 20°C and the humidity below
60%. Although not documented here, excess temperature and humidity resulted in increased
etch rates. Therefore, to avoid undesirable results, the above ambient conditions were
maintained for subsequent ITO etching.
As mentioned earlier, the wet chemical etch process is highly dependent on a number of
ambient conditions. In addition, we noticed that a certain amount of ITO - varying from
0.5mm to 1.5mm was often etched away from underneath the photoresist. In severe cases, thin
traces of the photoresist remained on the substrate.
Figure 5.11 is a photo-micrograph of a TLM pattern chemically etched
using HCl to produce ITO mesas on S.I. GaAs substrate. The mesas are
110mm wide; the amount of ITO removed completely due to
under etching was 1.5mm. This is an extreme example of lack
of control of wet chemical etching technique.
Figure 5.11: Photo Micrograph of an ITO mesa, etched using HCl solution. The figure shows
characteristic coarse edges due to solvents creeping under the resist; blemishes and traces of
thin photoresist can also be seen
For relatively large dimensions (> 100 mm), wet chemical
etching using the above solution was
both adequate, repeatable and relatively easy to accomplish. During the course of this
investigation, the most frequently used chemical for wet etching ITO, where deemed suitable,
was a 1HCl : 1H2O solution corresponding to 18% HCl by content. The corresponding etch
rate was 8Å/sec.
The addition of zinc dust to the ITO surface is said to enhance wet chemical etching in HCl
solutions. A GaAs sample with ITO was first left in a mixture of water and Zn powder. It
was then dried by leaving it on a "blotting" surface (i.e. cleanroom wipe) which left fine
granules of Zn powder on the sample surface. The sample was then immersed in the HCl
solution.
The ITO removal did not seem to be affected by the immersion in the Zn:H2O suspension;
also the etch on the surface was non-uniform. The residue Zn was removed from the sample
by placing it in a 3H2O:1HNO3 bath. But this latter solution seemed to etch the GaAs
substrate. Therefore, this method of ITO patterning was deemed to be unsuitable for
controlled and uniform micro patterning of ITO as required in this project.
The commonly used solution of HCl for ITO definition by wet chemical etching results in
removals of approximately 0.5 mm of ITO underneath the photoresist mask. Thus where near
micron structures need to be reproduced, wet chemical etching techniques are often
unsuitable. Although CH4/H2 mixtures can be used for reactive ion etching of ITO [148], this
is a potentially explosive gas mixture which is unsuitable for use in environments without
relatively expensive exhaust set-ups operating round the clock to remove any build-ups. Dry
etching of ITO using a gas mixture of acetone, argon and oxygen - essentially a hydrocarbon
etch with acetone being the source of reactive organic radicals in the plasma discharge - has
also been reported [149]. However, this technique needs
cumbersome optimisation of the various constituent gas partial pressures to ensure that no
carbon debris is left on the surface.
Therefore we investigated the suitability of a number of gases for dry etching ITO: freon,
oxygen and argon. Dry etching using Ar was found to be the most suitable in terms of speed
and selectivity. Figure 5.12 and Figure 5.13
show the results of this investigation.
Figure 5.12: ITO Etched Thickness in argon ambient versus time under various r.f. powers
A 4300Å ITO layer was deposited on a Si substrate by reactive r.f. sputtering, the sample was
then patterned using standard photolithography process to enable thickness measurements to
be carried out following dry etching. Thick photoresist (> 3 mm) was used as the mask for
these experiments which were performed at three suitable r.f. powers of 100W, 150W, and
200W. The dry etching chamber was pumped to pressures better than 1e-4 torr; Ar was
then flowed in at a constant rate to maintain a chamber pressure of 11 mtorr prior to exciting
the plasma.
The last point on the 150W power line in Figure 5.12 (corresponding to
40 minutes and 6300Å) was not used for the least square fit as the Si substrate was found to have
been etched also. Etch rates of 35Å/min, 111Å/min and 131Å/min were obtained for 100W,
150W and 200W respectively.
Figure 5.13: ITO Etch Rate in Argon ambient vs. r.f. power of RIE
Figure 5.13 shows that the etch rate is non-linearly dependent on the
r.f. power. Also pin-holes were visible on substrates etched at higher powers. Both these
effect suggest that the process produces substrate heating and that the process of ITO removal
in an Argon plasma is that of a physical knocking of the ITO species rather than by a chemical
reaction [150]. Based on these findings, the r.f. power of 100W
was decided to be the most controllable and suitable for further dry etching work.
As even the thick photoresist was damaged during the RIE process and was therefore difficult
to remove, an alternative material for the mask was necessary. A metal which has a
sufficiently lower etch rate than ITO in the Ar plasma but nevertheless can be subsequently
removed chemically in preference to ITO would be the ideal substitute. Aluminium was the
preferred candidate on both counts.
A resistively evaporated layer of Al was therefore used as a mask. ITO is selectively dry
etched over Al in argon plasma. Figure 5.14 shows that while the ITO
etch rate at 100W r.f. power and 11 mtorr pressure, is 35Å/min, the corresponding figure for
Al is only 8Å/min making Al a more than adequate candidate to be used as a mask for dry
etching ITO.
Figure 5.14: Selective RIE of ITO over Al in argon plasma at a r.f. power of 100W
Following dry etching, the Al is selectively removed by placing the sample in a super saturated
luke warm solution (» 30°C) of KOH for app. 2 minutes. A 1000Å
layer of Al was found to be adequate. Thicker layers of Al were difficult to remove chemically;
although further heating the KOH solution accelerated Al removal, this also caused partial etching
of the ITO. Hence, all subsequent dry etching of delicate ITO patterns were masked using 1000Å of
thermally evaporated Al.
In comparison to the ITO dry etching techniques of Adesida et al
[148] using CH4/H2
mixtures, these etch rates are an order lower. This difference most likely arises from a
variation in the etch mechanisms involved in the two cases: whereas the carbon in the
methane/hydrogen mixture is said to react with the oxygen in ITO, there are no similar
reactive species in the Ar plasma. Therefore, it is postulated that the etching of ITO in Ar
plasma is essentially an ion milling process.
The etch rates obtained in this investigation for the RIE of ITO is, however, comparable to
those reported by Saia et al [149]: 22Å/min in C3H6O/Ar/O2 or 60Å/min in hydrogen chloride
gas.
Figure 5.15 shows a photo micrograph of a TLM mesa pattern etched
on a test ITO sample using the dry etching technique discussed thus far. In comparison with
the results obtained for a similar test sample etched using HCl solution, these results show near
perfect edges replicated from the mask. There is no apparent lateral etching or residue of debris
on the substrate.
Figure 5.15: Photo micrograph of an ITO mesa pattern, etched using RIE. The figure shows
near perfect edges while the substrate appears remarkably clean
As discussed in Chapter 6, using this dry etching technique with Al as the mask, a 2mm FET
gate structure was successfully produced in the fabrication of the first transparent gate HEMT.
Therefore, this technique was used in all subsequent fabrication ITO structures below 50mm
and proved to be a reliable and very convenient method for patterning delicate ITO structures.
5.2.1 ITO Patterning by Lift-off Lithography
5.2.2 Wet Chemical Etching

5.2.3 Effect of Adding Zn Dust to HCl Solution
5.2.4 Selective RIE of ITO in Argon Plasma



© 1998: Shabbir A. Bashar (in accordance with paragraph 8.2d, University of London
Regulations for the Degrees of M.Phil. and Ph.D., October 1997). The Copyright of
this thesis rests with the author, and no quotation from it or information derived
from it may be published without the prior written consent of the author.
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