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At the end of 2010, St.
Petersburg State University purchased our product NanoMaker to be hooked
on Carl
Zeiss SMT ORION® Helium-ion Microscope. During installation several
tests (together with the University staff, Prof. O. Vyvenko and Dr. Yu.
Petrov) were carried out to assess possibilities of the instrument-driven
milling and exposure of a positive PMMA 950K resist using a focused helium
ions beam. All tests were performed at accelerating voltage of about
17 kV. Ion beam current range was limited to an upper limit of about 1 pA
at 50 um aperture to achieve high resolution. |
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Milling
Several attempts to mill a silicon substrate at different currents and
exposure times (dwell time) in the range of 0.5-10 C/cm2
were undertaken. Unfortunately, we could not observe any milling of the
silicon surface. Instead, at long exposures contamination deposition was
observed. A similar negative result was also observed when attempting
to mill a thick gold film (thickness about 100 nm). Milling of thin gold
films on carbon (gold resolution standard sample) was achieved at good
beam focusing, i.e. at creating a sufficiently high current density. An
example of patterning on a gold film by milling is shown in Fig. 1.
The etching was performed with the current of 1 pA in little less than
3 minutes. Distortion of the last letter and of the emphasizing line observed
on the right side is due to curvature of the gold particle surface. Evaluation
of the sensitivity to milling for this case gives ~ 106 C/cm3.
PMMA resist exposure
Silicon substrates coated with positive PMMA 950 K resist of 150 nm thickness
were used for exposure. at accelerating voltage of about 17 kV and ion
beam current of 0.5 pA. Exposure steps (point-to-point distance) have been set to 4 nm.
Two structures of dose wedge with different exposure times (dwell time)
per point - 1 us and 2 us in order to assess the sensitivity of resists
to ion beam irradiation had been drawn.
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Fig. 1. An example of patterning
on a gold film,
resolution better than 10 nm was easily achieved |
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Fig. 2 shows an optical microscope
image of the dose wedge exposed at 1 us per point after 5 seconds of development.
Waviness of the wedge surface is related to oscillations of the probe current
(due to helium in bottle was nearing to the end and the system was trying
to regulate gas flow with a period of approximately 15 seconds).
The experiment showed significantly higher efficiency of the resist exposure in comparison with electron beam
lithography (more than 50 times).
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Fig. 2. An optical microscope
image of the dose wedge |
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To estimate resolution of the ion lithography method for given parameters
of the microscope and the exposed substrate (150 nm PMMA resist on
Si) a structure containing a set of long, repetitive lines of 700 nm,
400 , 200 nm and 100 nm width was exposed. Dose of all elements
in the structure was equal to 100 %.
The structure was exposed twice with different exposure times (dwell time) per point
- 1.5 us and 1.7 us. The sample was developed for 15 seconds.
At inspection in an optical microscope with 1000x zoom the lines of 700 nm,
400 nm and 200 nm width were distinctly observed in both structures.
Fig. 3 shows an optical microscope photo of the structure with 1.7 us exposure time per point.
For inspection in the ion microscope a gold-palladium film of 5 nm
thickness was deposited above the resist.
It was found that all lines of 100 nm, 200 nm, 400 nm and 700 nm width are not developed to the bottom
in the structure with 1.5 us exposure time, but lateral dimensions are sustained.
Pictures on Fig. 4 and Fig. 5 demonstrate fragments of the structure. Fig. 4 presents central part of
the structure and Fig. 5 shows 100 nm lines.
For another structure where the dwell time per point was 1.7 us the lines of 700 nm and 400 nm
width are developed to the bottom. Whereas lines of 200 nm and of 100 nm
width look underdeveloped. In addition, there is a degradation of the lateral
size by 16-18 nm demonstrated in photos of Fig. 6 - central part
of the structure, of Fig. 7 - 100 nm lines, of Fig. 8 - 200 nm
lines, of Fig. 9 - 400 nm lines.
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Fig. 3. An optical microscope
image of a resolution test structure.
Dwell time 1.7 us |
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All photos obtained with the 30 deg tilt of the sample. Note that the waviness
clearly visible for exposed structure (Fig. 2) is hardly noticeable in diagnostic
(observation) mode. |
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Fig. 4. SIM image of structure central
part.
Dwell time 1.5 us
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Fig. 5. SIM image of 100 nm
lines.
Dwell time 1.5 us
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Fig. 6. SIM image of structure central
part.
Dwell time 1.7 us
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Fig. 7. SIM image of 100 nm
lines.
Dwell time 1.7 us
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Fig. 9. SIM image of 400 nm lines.
Dwell time 1.7 us
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We made a simulation of the helium
ions beam scattering in the PMMA resist using TRIM program by James F. Ziegler,
(http://www.srim.org/). At the accelerating voltage of 17 kV infinitely
thin beam of helium ions in 150 nm PMMA resist |
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Fig. 8. SIM image of 200 nm
lines.
Dwell time 1.7 us
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at the interface with silicon dissipates
to a diameter of 100 nm. This, in principle, agrees with our experimental
data and limits of the method resolution for given parameters of the microscope-sample
system.
As follows from the results of the dose wedge exposure, the ion structuring
method used has a very high sensitivity to variations in dose. We have
tried to use this to create 3D structure in 150 nm resist. As initial
drawing the emblem of the University was chosen. Using functions implemented
in NanoMaker a bitmap picture was imported into NanoMaker Editor as "DoseMap"
structure. The dose range was adjusted by using the Transform by Formula
option so that an exposure dose at a point is proportional to grayscale
level of the picture. Structure size was chosen about 66 um x 66 um,
so that the smallest details of the image was about 100 nm. A few
structures were exposed with a small variation of dwell time. Fig 10
and Fig. 11 shows photos of one of the resulting structures, observed
in the optical and helium ion microscopes, respectively. SIM image is
acquired with the tilt of the sample by 45 deg.
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One can see clearly the influence of the probe
current oscillations mentioned. |
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Fig. 10. An optical microscope
image of 3D structure in PMMA resist of 150 nm thickness |
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Conclusions
High resolution in milling mode on thin gold film has been demonstrated. Evaluation of the sensitivity
to milling gives ~ 106 C/cm3. Exposure of positive resist by ion beam has been investigated,
sensitivity of the resist has been determined. It was found significantly higher efficiency
of the resist exposure, however, for 17 kV acceleration voltage the resolution was lower than
in electron-beam lithography, which is due to high lateral scattering of ions at resist thickness of 150 nm.
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Fig. 11. SIM image of the
same structure |
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Date Added: Feb 17, 2011 |
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