fluid-mediated parallel self-assembly of polymeric micro-capsules for liquid encapsulation and...
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Fluid-mediated parallel self-assembly of polymeric micro-capsules for
liquid encapsulation and release
Loïc Jacot-Descombes*a, Cristina Martin-Olmos*
a, Maurizio Rosario Gullo
a, Victor Javier Cadarso
a,
Gregory Mermoudb, Luis Guillermo Villanueva
a, Massimo Mastrangeli
a,b, Alcherio Martinoli
b and
Jürgen Bruggera 5
Received (in XXX, XXX) Xth XXXXXXXXX 20XX, Accepted Xth XXXXXXXXX 20XX
DOI: 10.1039/b000000x
Fluid-mediated self-assembly is one of the most promising routes for assembling and packaging smart
microsystems in a scalable and cost-efficient way. In this work the pairwise fluidic self-assembly of 100
µm-sized SU-8 cylinders is studied with respect to two driving mechanisms: capillary forces at the liquid-10
air interface and hydrophobic effect while fully immersed in liquid. The pairwise self-assembly is
controlled by shape recognition and selective surface functionalization. Surface energy contrast is
introduced through oxygen plasma treatment and local deposition of a hydrophobic self-assembled
monolayer, respectively leading to face-selective hydrophilic and hydrophobic behavior. When in bulk
liquid, after less than a day face-wise self-assembly of more than 650 components is achieved with a yield 15
of up to 97% and with less than 1% of the cylinders assembled incorrectly. This technique is subsequently
adopted for self-assembling half-capsules into closed micro-capsules, thereby entrapping a liquid during
their self-assembly. The release of the liquid can subsequently be triggered in another medium, as
intended for applications involving e.g. chemical reactors, environmental engineering and drug release.
20
1. Introduction
The complexity of smart microsystems such as micro-electro-
mechanical-systems (MEMS) has been ever growing in recent
years, while being accompanied by a continuous decrease in their
size.1 For manufacturing devices of sizes well below the 25
millimeter range, assembly and packaging are key issues.2
Today’s methods based on robotic pick-and-place and flip-chip
approaches are not adequate to deal with millions of devices of
sub-millimetric sizes, as typically obtained by wafer-scale
processing. This is mainly due to sequentiality and adhesion 30
issues between the robotic gripper and the device.3 A more
appropriate manufacturing approach needs to be highly parallel,
cost-efficient and scalable, while remaining flexible and
controllable.4 Such an approach would benefit the assembly of
many types of microsystems,5 including notably liquid-filled 35
microcapsules. Robust and barely visible containers affording
controllable liquid release find a large variety of applications,6
such as distributed sensors, self-healing materials, fragrance
release and drug delivery. With specific reference to the latter,
microcapsules for the storage and further release of 40
pharmaceuticals are being developed.7, 8 Fully-integrated and
self-regulating devices might solve issues like secondary side
effects in non-targeted cell locations and stepped dosage
associated to current delivery methods 9, 10 However, integrating
microcapsules with smart (i.e. self-regulating) microsensors 45
requires fabricating, assembling and packaging them in a way
that is efficient and compatible with MEMS fabrication. An
established approach to fabricate such microcapsules consists in
the development of sophisticated containers,11 based on self-
folding 2D structures fabricated by lithography into various 50
polyhedra.12, 13 This technique is also envisioned for non-invasive
tracking by magnetic resonance of encapsulated cells for
application in cellular level therapy.14, 15 This approach, however,
does not easily allow the assembly of heterogeneous components,
barring its deployment into hybrid multi-functional devices. A 55
promising alternative to build hybrid MEMS devices is the
controlled self-assembly16 of micromachined components by
fluid-mediated self-assembly (FSA).17-19
State-of-the-art FSA is based on attractive interactions, e.g.
electrostatic, magnetic, capillary or hydrophobic, to position and 60
align specific units onto patterned substrates.20, 21 FSA is
particularly suited for objects with sizes below 1 mm, where
surface forces and stiction effects become dominant and accurate
assembly and placement rate is reduced.5 At a scale of few tens of
micrometers FSA permitted the highly-accurate integration onto 65
a target substrate of over 60’000 parts in 45 seconds with a yield
above 98%;22 i.e., a much higher rate than 3D robotic
microassembly.4 By combining forces of different nature and
ingenious strategies, complex and functional systems such as
microscale chains or LED arrays have been assembled.23-26 FSA 70
also works for larger scales, e.g. with centimeter-sized building
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Scheme 1 Synopsis of the FSA investigated in this work. a) More than 105 SU-8 micro microparts fabricated by photolithography. b) Microparts released.
c) Parts in liquid, FSA through orbital shaking and pair-wise self-assembled parts d) Assembled pairs; cylinders and capsules entrapping a colored ink. e)
Release of encapsulated ink.
5
blocks at liquid-liquid interface27 and with millimeter-sized ones
fully immersed in liquid.28 At liquid-air interface, dynamical
arrays of objects can also be controlled by magnetohydrodynamic
interactions.29-31 3D structures with specific shapes, such as 10
toroids or rounded tetrahedra could also be built by shape
recognition and selective surface coatings.32, 33 The control over
assemblies of 1-µm-sized polymeric particles depending on the
shape, roughness, electrostatic and depletion interactions has
been studied.34 Below the micrometer scale, 100 nm particles 15
with a selective hydrophobic versus hydrophilic surface behavior
could also be self-assembled into different structures being either
close to the water-air interface or completely immersed.35
Nevertheless, to our knowledge, liquid entrapment into
microcapsules by the self-assembly of half-capsules was not 20
investigated yet.
In this work, pairwise face-selective FSA of 100 µm-sized
polymeric components is investigated at liquid-air interface and
in bulk polar liquid through two different interaction
mechanisms: by capillary interaction, and by hydrophobic 25
effect,36 respectively. More than 105 components are fabricated
on a single 4’’ wafer using SU-8, a negative-tone photo-
structurable epoxy37 that has shown a lot of potential and
versatility for MEMS due to its good mechanical and insulating
properties 38 and for its ability to be functionalized 39, 40 Scheme 1 30
schematizes the microfabrication (Scheme 1a), release (Scheme
1b) and self-assembly in liquid during orbital shaking (Scheme
1c). Two kinds of components are investigated (Scheme 1d): i)
solid cylinders to study the control parameters of FSA, and ii)
half-capsules for liquid encapsulation through self-assembly. In 35
the first study, cylinders of different shapes, i.e. with both bases
flat or with one base rounded, are used to control the self-
assembly. In the second study, a face-selective hydrophobicity
contrast is created on the cylinders, and the time evolution of the
FSA in bulk liquid is studied. Finally, the proposed method is 40
applied to half-capsules in order to entrap liquid during their self-
assembly in pairs (Scheme 1d) and to release the liquid in another
media (Scheme 1e). For demonstration, water-based inks are used
as functional liquid.
2. Results 45
Transferring fabricated micro-cylinders from air into water
results typically in their segregation into two populations. A part
of them remains trapped at the water-air interface, whereas the
rest of them sink to the bottom of the beaker and are thus fully
submerged. At the water-air interface, long-ranged capillary 50
flotation forces are dominant.41 Conversely, in bulk water
flotation forces are not present, and the interactions among
microparts are mainly driven by the hydrophobic effect. In order
to investigate these two cases, a first set of FSA experiment has
been performed with microparts involving different shapes at the 55
liquid-air interface. The second case has been studied with fully
submerged microparts involving a face-selective treatment at the
bottom of the beaker. The SU-8 microparts with different shapes under investigation
are cylinders of 100 µm in diameter and in height with either both 60
bases flat (flat-flat) or with one base flat and one rounded (flat-
rounded). Their fabrication is described in details in the
experimental part (section 4). The second type of microparts
under investigation are flat-flat cylinders that have the same
dimensions but are treated with an O2 plasma to tune their surface 65
hydrophilicity and hydrophobicity in a face-selective way. The
third type is cylindrical flat-flat half-capsules, (i.e. featuring an
internal cavity on one side), involving a face-selective
hydrophobic surface treatment through local self-assembled
monolayer (SAM) deposition. 70
2. 1. Face-selective surface treatment of cylinders
In order to optically distinguish the orientation of the cylinders, a
two-layer SU-8 photolithography process using colored SU-8 is
applied. The bottom layer in contact with the silicon wafer is
blue-dyed SU-8 and the upper layer is colorless SU-8. The face-75
selective surface treatment of the flat-flat cylinders is achieved
with an O2 plasma treatment performed before their release from
the silicon wafer surface. Thereby, the plasma oxydizes all
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Fig. 1 Sketch of selective surface treatment and characterization of
bicolor SU-8 cylinders. a) Fabricated cylinders with one blue and one
colorless side. b) O2 plasma treatment. c) Release. d) Resulting
hydrophobicity contrast ∆θ1, compared to one on half-capsules, ∆θ2. e) 5
AFM line scans of the SU-8 surfaces (bottom surface is done on the
wafer).
exposed surfaces of SU-8, rendering them hydrophilic, except the
one shielded by the wafer (Fig. 1a to 1c). One hour after the 10
treatment, a water contact angle on the hydrophilic surface (θi) of
24° ± 2° and on the untreated surface (θn) of 74 ± 1° are
measured, as shown in Fig. 1d. The hydrophobicity contrast ∆θ1
= θn - θi is characterized over several days 42. Starting from 50° ±
2° one hour after the treatment, ∆θ1 amounts still to 35° ± 1° after 15
4 days, which is the time frame of the experiment (Fig. 1d). The
hydrophobicity contrast is not only a consequence of the surface
oxidation, but also of the induced roughness.43, 44 As expected
from,42 Atomic Force Microscope (AFM) scans show a 4x
increase of roughness from the original, spin-coated SU-8 to the 20
plasma-treated SU-8 (rms of 2.66 nm and 9.35 nm, respectively).
Fig. 2 Surface treatment of the half-capsules. a) Silicon wafer with the
two SU-8 layers after exposure and post exposure bake. b) SAM
deposited on SU-8. c) PGMEA developing the non-cross-linked SU-8 25
only. d) Resulting half-capsule with selective SAM deposition. e)
Released capsule and contact angle measurements on bare SU-8 surface
and on SAM-treated surface.
In addition, the untreated part of the cylinders (assumed to 30
conformally coat the Si substrate) has a surface roughness rms of
0.77 nm. Single AFM scans of roughness cross-sections are
shown in Fig. 1e. In order to avoid chemical wet etching of
silicon, which would affect the SU-8 surface properties, the
cylinders are mechanically released in an ultrasonic bath. 35
2. 2. Functionalization of half-capsules
The half-capsules are fabricated with the base hosting the cavity
on top. To render only the open base surface selectively more
hydrophobic than none treated SU-8, a Trichloro (1H, 1H, 2H,
2H-perfluorooctyl)silane SAM is applied just before developing 40
the SU-8, Fig. 2a and 2b. The covalent bonds are not affected by
the standard SU-8 developer (Propylene glycol monomethyl ether
acetate (PGMEA)). The non-cross-linked SU-8 is thus developed
through the SAM layer, allowing a lift-off-like functionalization
process (Fig. 2c) so that only the top base of the SU-8 half-45
capsules is covered by the hydrophobic SAM, Fig. 2d. In this
case the hydrophobicity contrast ∆θ2 between the SAM layer θo
and the untreated SU-8 (∆θ2 = θo – θn) is 41° ± 4° (see Fig. 2e),
with the respective contact angles being 115° ± 4° and 74° ± 1°.
Both SU-8 surface treatment options, i.e. O2 plasma and 50
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Fig. 3 a) Schemes of possible assemblies with flat-fat or flat-rounded
components. b) Histogram of chain length for self-assembled cylinders
with flat-fat and flat-rounded extremities. c) Optical images with
schematics after self-assembly of the cylinders. 5
silanization, yield similar ∆θ (∆θ1 ≈ ∆θ2), over the time frame of
the experiments, which is 4 days. On the other hand, ∆θ2 is more
constant in time.
2. 3. Pairwise self-assembly by shape recognition 10
We first investigate how microparts with different shapes self-
assemble into pairs at a liquid-air interface. In this case, the
floating microparts are under the influence of strong and long-
ranged capillary interaction, namely flotation forces. Flotation
forces are lateral capillary forces arising from the deformation of 15
the liquid-air interface caused by the floating objects41. The
shapes of the liquid-air meniscii are determined by the objects’
geometry, weight and wettability. Facing menisci induce
attractive (or repulsive) interactions if they have equal (or
opposite) profiles. Minimization of the interfacial and 20
gravitational energies drive the set of floating objects into
configurations of static equilibria27. The way the components
self-assemble can thus be controlled by geometrical design
besides surface chemical modification.32 To benefit from these
phenomena in our study, we used SU-8 cylindrical components 25
with flat-flat and flat-rounded bases. In order to individually
study the influence of the cylinder shape, their surfaces are not
treated and have a contact angle for water of θn, of 74 ± 1°. Under
orbital shaking, the cylinders form chains whose lengths depend
on the cylinder dimensions, the stability of the assemblies and the 30
orbital shaking rate. Focusing herein into one specific size and
orbital shaking rate, the flat-flat configuration can lead to most
stable assemblies as it is the one where components interact
through a surface. On the other hand, flat-rounded or rounded-
rounded configurations lead to less stable assemblies due to 35
point-based interaction only and thus reduced adhesion forces.
Thus, flat-flat components are expected to assemble into chains
whereas the flat-rounded components are expected to assemble
preferentially into pairs with the flat sides facing each other’s
(Fig. 3a). 40
The distributions of the chain lengths obtained for both flat-flat
and flat-rounded cylinders are shown in Fig. 3b. The results are
obtained after 8 hours of orbital shaking and complete
evaporation of the water. All samples are prepared with identical
water volume and number of cylinders. A pair is counted as an 45
assembly only if at least 75% of the facing diameters are
overlapping. The results show that, in the case of flat-flat
cylinders, the probability to reach a given chain is inversely
proportional to its length. In the case of flat-rounded cylinders,
89% of cylinders remain single, and 11% form pairs, without any 50
longer assemblies as shown in Fig. 3b. Optical images with
schematics of typical results for flat-flat and flat-rounded
assembled cylinders are shown in Fig. 3c.
More than twice as many flat-flat cylinder pairs as for flat-
rounded ones are counted. This is expected, as a flat-flat cylinder 55
has twice as many chances to self-assemble as a flat-rounded
cylinder. This is also the reason why the number of singles is
higher for flat-rounded than for flat-flat cylinders. As a summary,
by exploiting shape recognition of floating SU-8 cylinders, we
are able to self-assemble them selectively into pairs, but with a 60
relatively low yield.
2. 4. Pairwise self-assembly by face-selective hydrophobic effect
To increase the percentage of cylinders that assemble while
constraining self-assembly mostly into pairs, the process is then 65
performed with components fully immersed in polar liquid. The
long-ranged capillary interaction is hereby replaced by the short
range hydrophobic effect. 35 The fabricated components are
bicolor flat-flat cylinders with a face-selective hydrophobicity
contrast. Fig. 4a shows schematics and optical images before and 70
after the FSA in bulk liquid. The SU-8 microcylinders in a water-
filled Petri dish are agitated by orbital shaking. The cylinders
self-assemble into different combinations (Fig. 4b). With more
than 650 cylinders, the percentage of each combination of
cylinders (blue to blue, blue to colorless or colorless to colorless) 75
and its time evolution is studied over 4 days. The combinations
shown in Fig. 4b are: i) Correct assemblies defined as the number
of cylinders in contact only by the flat blue faces, ii) Aligned
assemblies, a sub-group of the correct assemblies, when at least
75% of their diameters are overlapping. iii) Wrong assemblies, 80
counting colorless to colorless and colorless to blue surface
assemblies. iv) Singles counting all cylinders which do not
assemble.
It can be seen in Fig. 4b, that after 20 minutes of shaking, both
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Fig. 4 a) Schematics of the fluid-mediated self-assembly (FSA) process and optical images; b) Statistics on FSA; configuration occurrence (percentage)
with legend on the right (see text for definition).
“Correct assemblies” and “Aligned assemblies” show constantly 5
increasing yield. After 15 hours the “Correct assemblies” reach a
stable yield above 97%, while the “Aligned assemblies” exhibits
a yield of 39%, which continues to increase to 59% after 4 days.
The stable yield of the “Correct assemblies” demonstrates that
once two cylinders meet with both hydrophobic surfaces in 10
contact, they form stable pairs. Furthermore, the constantly
increasing yield of the “Aligned assemblies” shows that there is a
relative motion and sliding between two correctly assembled
cylinders, fine tuning their alignment. Conversely, the “Wrong
assemblies” percentage decreases to below 1%, suggesting that 15
such combinations are not stable and can easily be separated by
the effects of the shaking. This proves that our proposed surface
treatment effectively enables the face-wise self-assembly of sub-
millimetric SU-8 microcomponents into pairs.
2. 5. Liquid encapsulation through self-assembling of 20
microcapsules
The face-wise self-assembly of microcomponents into pairs is
then applied to SU-8 half-capsules for liquid encapsulation. The
experiments are performed in the same way as described for the
cylinders. As a proof of principle, water-diluted colored inks 25
(green, yellow and blue) were used instead of pure water. The
half-capsules featuring the face-selective SAM are transferred
into Petri dishes and FSA is initiated with orbital shaking. Fig. 5a
shows a scheme and an optical image of the 100 µm-sized half-
capsules immersed in green ink before assembling. After 1 day of 30
FSA (Fig. 5b), 21% of the half-capsules have assembled pairwise
and face-wise into close capsules. Fig. 5b shows representative
examples of three self-assembled capsules in their respective
inks. The rest of the capsules are either not assembled or
assembled in the wrong orientation (closed bases assembled). For 35
the microcapsules that are fully immersed in water with diluted
ink, the hydrophobic effect is the main force keeping them
together. After draining the solution, the 200 µm-long capsules
entrapping about 1 nL of ink solution (0.5 nL for each half-
capsule) are transferred either onto a microscope glass slide or 40
into water (Fig. 5c). Once dried, the capillary forces exerted by
the entrapped ink keep the capsules together. A mechanical test
using tweezers also showed that by exerting a mechanical force
the capsules can be disassembled. In view of the application of
remote liquid unloading, we showed that the release of the 45
encapsulated ink can be achieved by transferring the capsules into
a less polar liquid, such as isopropanol (IPA), which reduces the
binding force. Fig. 5d shows few self-disassembled half-capsules
in IPA releasing encapsulated blue ink.
3. Discussions 50
Our results demonstrate the pairwise self-assembly of SU-8
micro-components by shape recognition and by face-selective
hydrophobic effect. The latter case has been applied for liquid
encapsulation and demonstrated as a proof-of-concept with
colored inks. The technique can be adopted for aqueous solutions 55
and polar liquids other than water, as well, and more generally for
other functional polar solutions under the condition that they do
not affect the assembly by interacting with the SU-8 surface. In
addition, no bubble has been observed inside the capsules. The
lift-off-like functionalization presented herein could be applied 60
with a different, compatible surface treatment, possibly allowing
other potential release mechanisms. Other photo-structurable
polymers having a contact angle with water significantly lower
than the one of the SAM-treated surface can be used in place of
SU-8 with similar fabrication process. Biodegradable, 65
biocompatible and functional polymers would represent a very
interesting possibility.
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Fig. 5 Functionalized half-capsules self-assembling into complete capsules entrapping colored ink. a) Unpaired half-capsules before FSA; b) Parallel FSA
experiments in blue, green and yellow inks c) Transferred capsules: With green and yellow inks into a drop of water (left), with blue ink onto a
microscope glass (right); d) Release of the encapsulated blue ink by self-disassembly of the capsules in Isopropanol.
A similar approach can be applied to a wide range of materials, 5
such as metals, silicon or oxides among others.
Herein, the focus has been set onto 100 µm-sized micro-capsules for several reasons: our capsules enable the encapsulation of nanoliter volumes, and can be perceived with bare eyes; furthermore, this size range allows the embedding of 10
functional microchips45 such as RFID chips onto the capsules. We argue that the range of capsule dimensions efficiently affordable by our self-assembly approach is mainly defined by the interplay between assembly and disassembly forces. The short-ranged hydrophobic effect driving the assembly of the 15
capsules competes with drag and inertial forces arising from orbital shaking which scale with the surface and the volume of the components, respectively. With millimetric capsule dimensions, the hydrophobic effect may not be sufficient to overcome disassembling forces. When considering downscaling, 20
the limit is set either by the resolution of the available design and patterning technique (e.g. around 10 µm for reproducible capsule fabrication when using standard photolithography) or by the minimum volume of liquid to be encapsulated. In general, as the dimensions of the components approach the spatial range of the 25
hydrophobic effect (e.g. a few hundreds of nanometers) the self-assembly process is expected to become more efficient.46 The self-assembly of 100 nm Ag cubes by hydrophobic interaction into ordered structures has been demonstrated.35
4. Experimental 30
4. 1. SU-8 bicolor cylinder fabrication
SU-8 bicolor (blue and transparent) cylinders are fabricated by
photolithography. Dimensions are 100 µm in diameter and in
height. A 4’’Si wafer is dehydrated and spin-coated (Sawatec
LMS200) with a 50 µm-thick blue colored SU-8 layer 35
(Gersteltec, CH) followed by a soft-bake (Sawatec LMS200). A
50 µm-thick colorless SU-8 layer (GM 1070 Gersteltec, CH) is
then equally spin-coated and soft-baked. Both layers are exposed
at once through a Chromium shadow mask (dose of 850 mJ cm-2
(Süss MA6/BA6)) to pattern the cylinders. After a post-exposure 40
bake (PEB) on a hot plate (Accu-Plate), the SU-8 is PGMEA and
rinsed with IPA. A hard bake process (Sawatec LMS200) is done
to give them more stability and optimize their aging 47.
Hydrophilic behavior of the SU-8 surfaces is induced by
exposure to an O2 plasma for 2’ (0.6 mbar, 100W; Diener 45
Electronic, Femto). The cylinders are released in ultrasonic bath
at 750 kHz in water for 30’. The release is enhanced by a prior
thermal stress between the SU-8 and the Silicon surface induced
by heating the wafer with the SU-8 cylinders at 200°C and fast
cooling by deeping in room-temperature water. To avoid surface 50
contamination, after release the cylinders are stored in water. The
water used throughout all the experiments is deionized (DI).
4. 2. Fabrication flat and rounded half-capsules
SU-8 half-capsules are fabricated with a 100 µm outer diameter,
50 µm inner diameter and 100 µm in height. For the capsules 55
with rounded bases, a 4’’ Si wafer is structured with spherical
holes obtained by isotropic silicon etching. A positive photoresist
(AZ ECI 3027) is deposited by spin-coating (Rite Track 88
Series), patterned by exposure (Süss MA150) and developed
(Rite Track 88 Series). The isotropic etch is subsequently 60
performed by fluorine plasma (Alcatel 601E). The photoresist
mask is then stripped and the wafer cleaned by O2 plasma at 1000
W (Tepla 300) for 7’. For both rounded and flat capsules, the
fabrication process starts with a thin aluminium layer deposition.
A 40 µm-thick layer of SU-8 (GM 1070, Gersteltec, CH) is 65
subsequently spin-coated (Sawatec LMS200), soft-baked
(Sawatec LMS200) and exposed (361 mJ cm-2, Süss MA6/BA6).
A second, 60 µm-thick SU-8 layer (GM 1070, Gersteltec, CH) is
then spin-coated and soft-backed (Sawatec LMS200). The layer
is exposed through a Chromium shadow mask with ring-shaped 70
holes (Süss MA6/BA6). Both SU-8 exposure doses are adapted
for the capsules with rounded bases. After PEB (Accu-Plate), the
SU-8 is developed in two PGMEA baths for 10’ and rinsed with
isopropanol. Hard bake process also helps to remove possible
cracks 47. The release is done by etching the aluminium layer in 75
water-diluted KOH (40 %) at 80 °C for a few minutes. SU-8 half-
capsules are rinsed with water and filtered subsequently through
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filters with 4-7 µm and 4-12 µm pores (Macherey & Nagel,
Whatman) up to 5 times.
4. 3. Selective surface treatment of half-capsules
For surface-treated half-capsules, a 7 W O2 plasma, at 0.6 mbar
for 30’’ is performed before developing the SU-8. Next, a SAM 5
layer (Trichloro (1H, 1H, 2H, 2H-perfluorooctyl)silane) (Sigma
Aldrich) is deposited in vapour phase at room temperature for 1
hour. The half-capsules are released in an ultrasonic bath.
4. 4. Self-assembly experiments
For capillary FSA, flat and rounded half-capsules are left at the 10
water surface of petri dishes containing 40 ml of water with
diameters of 70 mm, and orbitally shaken till full water
evaporation (about 8 hours). Same water volume and same
number of half-capsules is used in all experiments. Samples are
imaged with an optical microscope to quantify the FSA yields. 15
FSA of bicolor cylinders and half-capsules is performed by
submerging them in water at the bottom of 9 ml Petri dishes with
diameters of 30 mm. The beakers are covered with parafilm to
avoid water evaporation and so keeping the same water volume
during the entire experiments. Petri dishes with bicolor cylinders 20
are put on an orbital shaker for 4 days; only one day for the half-
capsules. Self-assembly yields are quantified by stopping the
shaking at prefixed times and counting the cylinder
configurations under an optical microscope. For the statistics
shown in Fig. 3, each counting involves 650 microcylinders. 25
Counting is done with top-view optical images, thus only side-
way oriented cylinders are counted (the majority of the
cylinders). The 21% of aligned microcapsules counted in section
2.5 are accepted only if at least 75% of the diameters are
overlapping, which is the minimum for liquid encapsulation. 30
5. Conclusion
Directional face-wise FSA in water of 100-µm-sized SU-8 bulk
and hollow cylinders into pairs is demonstrated. Two distinct
cases are presented: one occurring at the water surface, where
surface tension dominates, the other occurring underwater, where 35
hydrophobic effects do. In the first case, assembly control is
enabled via geometrical design and shape recognition. While
regular cylinders (both bases flat) assemble in chains of up to 4
units, cylinders with one rounded base assemble nearly
exclusively into pairs. In the second case, self-assembly is 40
favored via face-selective hydrophobicity contrast.
In addition, the pairwise self-assembly is applied to half-
capsules that encapsulate a functional liquid while self-
assembling. The hydrophobicity contrast is in this case
engineered through a lift-off-like process of a hydrophobic SAM 45
before developing the SU-8. After self-assembly and co-
encapsulation of liquid, changing medium allows to reduce the
adhesion between the half-capsules and thus to release the
entrapped liquid via self-disassembly. As a proof of concept,
water soluble colored inks are first enclosed inside the capsules 50
and later released in isopropanol.
This work presents a fluidic path for the assembly of two-
component polymeric microcapsules fabricated in SU-8 by
photolithography. It is compatible with MEMS technology and
scalable to massively parallel assembly. The presented novel 55
encapsulation method may open new routes for smart
microcapsules with potential applications for health care, drugs
delivery, food market, information technology, and local
distributed sensing for civil and environmental engineering.
Acknowledgements 60
L. Jacot-Descombes and Dr. C. Martin-Olmos contributed
equally to this work. We acknowledge Nano-Tera.ch and the
project “SELFSYS” for funding the work presented here. We
thank Ikjoo Byun and Prof. Beom Joon Kim of Tokyo University
(Japan) for fruitful discussions. We also thank Dr. Sebastien 65
Jiguet, from Gersteltec (CH) for providing us the blue colored
SU-8 as well as Prof. Philippe Renaud from the Laboratory of
Microsystems for sharing experimental tools and advices. We
finally express our gratitude to the Center of Micro-
Nanotechnology (CMi) of EPFL for the support during the 70
microfabrication.
Notes and references
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R. Gullo, Dr. L. G. Villanueva, Dr. M. Mastrangeli, Prof. J. Brugger,
Microsystems Laboratory, Ecole Polytechnique Fédérale de Lausanne 75
(EPFL), CH-1015 Lausanne (Switzerland), E-mails: loic.jacot-
[email protected], [email protected] b Dr. G. Mermoud, Dr. M. Mastrangeli, Prof. A. Martinoli , Distributed
Intelligent Systems and Algorithms (DISAL) Laboratory, ENAC, Ecole
Polytechnique Fédérale de Lausanne (EPFL), CH-1015 Lausanne 80
(Switzerland), E-mail: [email protected]
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