solvent-infiltration imprint lithography: a novel method to prepare large area...
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Cite this: J. Mater. Chem., 2012, 22, 21154
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Solvent-infiltration imprint lithography: a novel method to prepare large areapoly(3-hexylthiophene) micro/nano-patterns
Jinhe Wang,*a Guoquan Min,b Zhitang Song,c Xiuyuan Ni,d Weimin Zhou,b Jing Zhan,b Yanping Zhang,b
Jianping Zhanga and Liyi Shi*a
Received 31st July 2012, Accepted 21st August 2012
DOI: 10.1039/c2jm35086f
A new method is developed in this work to fabricate large area poly(3-hexylthiophene) (P3HT) micro/
nano-patterns. The method is based on solvent-infiltration imprint lithography (SIIL). P3HT micro/
nano-patterns, including micro-prism arrays, nano-grating and nano-hole arrays, have been
successfully prepared with features ranging from 400 nm to 3 mm. The regularity of the patterns was
studied by SEM and the morphology of the pattern surfaces was investigated by atomic force
microscope (AFM). The solidification mechanism of this method is based on solvent infiltration instead
of external UV or heat to form the polymer pattern. This mechanism makes SIIL more universal, of
lower cost than hard-mold imprint lithography, and more efficient than capillary force based
lithography since high glass transition temperature (Tg) polymers or even polymer/nano-particle blends
can be patterned quickly. Polymer solar cells with nano-hole arrays and nano-grating are prepared
using SIIL, respectively, and the power conversion efficiency is improved compared with traditional
film-structure polymer solar cells.
1 Introduction
Conjugated polymers are considered as organic semiconductor
materials that could lead to the next generation of electronic and
optical devices. Conjugated polymers have many advantages
over inorganic semiconducting materials, such as low cost and
flexibility of use. Poly(3-hexylthiophene) (P3HT) is an important
conjugated polymer that has been widely used in solar cells,1–4
organic transistors,5–7 and polymer light-emitting diodes
(LEDs).8,9 In order to improve performance, micro or nano
patterns are usually required in these devices.10 For example,
micro-textures are employed in solar cells to improve sun light
absorption,11–13 where micro-arrays are used in organic thin film
transistors to increase carrier mobility,14–16 and photo crystals are
fabricated on the surface of LEDs to improve the light
output.17–19
Up to now, photolithography with subsequent dry and wet
etching processes, is the most common micro-pattern fabrication
method in the state-of-the-art semiconducting industry.
aResearch Center of Nano-science and Nano-technology, ShanghaiUniversity, Shangda Road 99, Shanghai, 200444, P. R. China. E-mail:[email protected] Promotion Center, Jiachuan Road 245, Shanghai 200237,P. R. ChinacLaboratory of Nanotechnology, Shanghai Institute of Microsystem andInformation Technology, Chinese Academy of Sciences, Changning Road865, Shanghai 200050, P. R. ChinadPolymer Department of Fudan University, Handan Road 220, Shanghai200433, P.R. China
21154 | J. Mater. Chem., 2012, 22, 21154–21158
However, this method is hardly applicable to conjugated poly-
mers because the polymer will be significantly damaged or have
its intrinsic properties altered under the harsh patterning
conditions. Some other non-destructive patterning methods,
including the anodic aluminum oxide (AAO) template
method,20,21 dip-pen nanolithography22,23 and nanoimprint
lithography24–27 have been used to fabricate micro/nano-patterns
of polymers.28–30 However, these methods usually rely on
expensive state-of-the-art equipment or cannot fabricate patterns
over large areas.31 Take nanoimprint lithography for example,
the conjugated polymer is heated above its glass transition
temperature (Tg) and is then imprinted by a hard master which
has been patterned previously. Once the temperature drops back
below the Tg, the conjugated polymer is solidified again and the
pattern is transferred from the hard master to the conjugated
polymer. This nanoimprint process is usually carried out on
expensive equipment which can provide high temperatures (50–
100 �C above the Tg of the polymer), high pressures (ca. 40 bar, 1
bar ¼ 100 000 Pa) and full area contact at the same time.32,33
Even so, some high Tg polymers are hard to imprint using this
process. Many papers have aimed at solving this problem. One
method is by using solvent vapor to lower the Tg of the polymer
and reduce the imprint temperature and pressure,32,34 but this
method usually requires long times (for example 3–6 hours) to
swell the polymer film, which will reduce the process efficiency
inevitably.
In this paper we report a novel imprint lithography method,
solvent infiltration imprint lithography (SIIL), by combining the
This journal is ª The Royal Society of Chemistry 2012
Fig. 1 Schematic of SIIL. (a) Spin-coating substrate with P3HT solu-
tion. (b) Imprint P3HT solution film with PDMS mold. (c) Solvent
infiltrates through the PDMS mold. (d) P3HT pattern formed on
substrate.
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essential feature of nanoimprint lithography—imprinting a
polymer film—with the key element of soft lithography—
molding a prepolymer or polymer solution with an soft stamp.
This idea is similar to capillary force lithography (CFL), which
was developed by simply combining nanoimprint and soft
lithographies.35 The differences between SIIL and CFL are (1)
the resist layer, which for the soft mold in SIIL is a polymer
solution or polymer paste rather than solid polymer film. So
heating is not needed to ‘‘melt’’ the polymer and the filling time is
much reduced. (2) The solidification of the polymer in SIIL is
achieved by solvent infiltration into the soft mold instead of
waiting for the temperature to drop below the polymer Tg or
chemical cross-linking reactions. So the heating or UV is not
necessary in SIIL. It combines the wide adaptability of nano-
imprint lithography and the low cost of soft lithography and can
pattern polymers or polymer/particle blends without heating or
UV radiation. Using this method, micro/nano-patterns of P3HT
and P3HT/PCBM polymer solar cells with nano-grating and
nano-hole arrays were fabricated.
2 Experimental
2.1 Materials
Poly(3-hexylthiophene) (P3HT, green power,Mw: approximately
55–60 kg mol�1, regioregular >95%, metal content <0.02%) and
[6,6]-phenyl-C61-butyric acid methyl ester (PCBM) (black
powder) was purchased from Luminescence Technology Corp.
1,2-Dichlorobenzene was obtained from Shanghai Guoyao
Corp. Poly(ethylenedioxythiophene) doped with poly-
(styrenesulfonate) (PEDOT:PSS) was purchased from Sigma-
Aldrich. Polydimethylsiloxane (PDMS) Sylgard 184 and its
curing agent were purchased from Dow Corning Corp. Two
nano-patterned polycarbonate masters were provided by
Shanghai Institute of Optics and Fine Mechanics. The micro-
structure master is fabricated by photolithography following dry
and wet etching processes.
2.2 Replication of the PDMS soft mold
Replication of the PDMS mold was processed as follows: PDMS
and its curing agent 30 g (10 : 1 by weight) was mixed and
degassed. The mixture (1 g) was diluted with toluene (60 wt%) to
decrease the viscosity. The diluted mixture was spin coated at
3000 rpm for 30 s on the master. Then, the rest of the mixture was
carefully poured onto the surface, followed by curing at 80 �C for
120 min. After that, the soft PDMSmold was peeled off carefully
from the master. The detailed experimental process can be found
in the work of Zhou et al.36
Fig. 2 SEM images of patterned P3HT film fabricated by solvent-infil-
tration nanoimprint lithography. (a) Six-sided cylinder array with sides of
3 mm and a period of 15 mm. (b) Four-sided cylinder array with sides of
3 mm and a period of 10 mm. (c) Tri-prism array with sides of 3 mm and a
period of 15 mm. (d) Quadrilateral sink with sides of 10 mm and a depth of
about 700 nm. (e) Nano-hole array with diameters of 400 nm and a period
of 800 nm. (f) Nano-grating with a line width of 400 nm and a period of
800 nm.
2.3 Solvent-infiltration imprint micro/nano patterns of P3HT
P3HT solution in 1,2-dichloriobenzene (50 mg ml�1) was spin-
coated (500 rpm) on ITO glass. The imprinting process was
carried out immediately. Imprint parameters were a temperature
of 25 �C, imprinting pressure of 0.3 bar and imprinting time of
3 min. A schematic of the entire solvent-infiltration imprinting
process is shown in Fig. 1.
This journal is ª The Royal Society of Chemistry 2012
2.4 Polymer solar cells fabrication
An approximately 40 nm thick layer of PEDOT:PSS was spin-
coated on ITO and annealed at 120 �C for 15 min to remove
water. P3HT and PCBM (weight ratio of 1 : 1) was dissolved in
chlorobenzene at a concentration of 20 mg ml�1. The P3HT/
PCBM solution was filtered using 0.45 mm syringe filter before
spin-coating on the PEDOT:PSS layer, then, the SIIL was
carried out to fabricate the nano-grating and nano-hole patterns,
followed by with annealing at 120 �C for 15 min. To complete the
device fabrication, 1 nm of LiF, 30 nm of Al and 70 nm of Ag
were evaporated in order onto the patterns under high vacuum
through a shadow mask. The active device area was measured to
be 0.1 cm2. A blank solar cell was fabricated under the same
conditions, except the SIIL step.
J. Mater. Chem., 2012, 22, 21154–21158 | 21155
Fig. 3 AFM images of PDMSmolds and corresponding P3HT patterns.
(A) Six-sided cylinder mold of PDMS; (a) six-sided cylinder of P3HT. (B)
Four-sided cylinder mold of PDMS; (b) four-sided cylinder of P3HT. (C)
Tri-prism mold of PDMS; (c) tri-prism of P3HT.
Fig. 4 Cross-section curves of different shape molds and corresponding
P3HT structures.
Fig. 5 AFM images of PDMS mold and P3HT with concentric circles.
Fig. 6 Cross-section curves of PDMSmold and P3HT concentric circles
fabricated with different concentrations of P3HT solution.
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2.5 Measurement and characterization
The imprinted patterns were measured by FE SEM (Hitachi S-
4800). The morphologies of the imprinted patterns were inves-
tigated by atomic force microscope (Veeco, Dimension 3100) in
tapping mode. The J–V curve was tested by East China Normal
University with a PVIV-412V solar cell test system.
3 Results and discussion
SIIL successfully produced various P3HT micro/nano-structure
patterns on ITO glass without hot embossing or reactive ion
etching, as shown in Fig. 2. A six-sided cylinder (Fig. 2a), four-
sided cylinder (Fig. 2b), tri-prism (Fig. 2c), quadrilateral sink
21156 | J. Mater. Chem., 2012, 22, 21154–21158
(Fig. 2d), nano-hole (Fig. 2e), and nano-grating (Fig. 2f) with
figure sizes ranging from 400 nm to 3 mm are visible over the large
area. The details of these micro/nano-structures are given in the
figure captions. These figures indicate that highly uniformed
micro/nano-structures can be fabricated on large areas through
SIIL.
This journal is ª The Royal Society of Chemistry 2012
Fig. 7 Cross-section of the nano-grating polymer solar cell.
Fig. 8 J–V curves of polymer solar cells.
Table 1 Characteristics of the three polymer solar cells
Solar cells Voc (V) Jsc (mA cm�2) FF PCE (%)
Film structure 0.57 8.07 46.31 2.13Nano-grating 0.58 9.05 44.37 2.31Nano-hole array 0.61 8.87 53.86 2.93
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In order to study the pattern transfer fidelity of SIIL, AFM
was used to test the surfaces of the PDMS mold and fabricated
P3HT micro/nano patterns. Fig. 3(A)–(C) shows the AFM
images of the three PDMS molds which have different hole-
shapes and hole-size, but the same hole-depth. The AFM images
of the three corresponding P3HT patterns are also shown in
Fig. 3(a)–(c). A cross-section was made in each graph and the
position of the cross-section was shown in each 2D image. The
cross-section curve of each structure was also given below each
graph. These 2D images of the mold and the corresponding
P3HT patterns show that the shapes of the three micro-structures
are transferred very well. The cross-section curves of each
structure were intercepted (between the two vertical broken lines
of each cross-section curve) to compare the mold and the cor-
responding P3HT structure further (Fig. 4, the cross-section
curves of molds are inverted for convenient comparison). This
figure shows that the mold and the corresponding P3HT
structure match each other very well. The height of each
This journal is ª The Royal Society of Chemistry 2012
micro-structure is lower than the depth of each PDMS mold,
which results from the infiltration of the solvent.
The influence of the polymer solution concentration on the
fidelity of SIIL was also studied. The AFM images of the PDMS
mold with concentric circles and one of the P3HT concentric
circles are shown in Fig. 5. The cross-section curves of the PDMS
mold and P3HT concentric circles fabricated with different
concentrations of P3HT solution are shown in Fig. 6. This figure
shows that as the concentration of the polymer solution
decreases the P3HT structure becomes smaller and the meniscus
becomes more obvious. This phenomenon can be used to fabri-
cate small size polymer structures with relatively large-size
molds, which we will study next.
3.1 The properties of polymer solar sells
The aim of a micro/nano-structure fabrication method is to
fabricate micro/nano-structures which can be used in optical,
photovoltaic or biochip devices. In this work, we used SIIL in
polymer solar cells. Fig. 7 is the SEM image of the cross-section
of the nano-grating P3HT/PCBM polymer solar cell after the Al
cathode layer had evaporated. The thickness of the active layer is
in the range of 70–110 nm and the Al layer is about 30 nm. The
nano-grating structure is still visible.
To investigate the effect of the nano-structures on the
performance of the polymer solar cells, photocurrent density–
voltage (J–V) curves were measured (Fig. 8) and the values of
short circuit current densities (Jsc), fill factors (FF), open circuit
voltage (Voc) and power conversion efficiency (PCE) are shown
in Table 1. The increase of Jsc can be attributed to light
diffraction in the nano-structures of the active layer and light
reflection on the nano-texturing Al rear electrode, which
improves light trapping within the active layer.
4 Conclusions
In summary, we have demonstrated an extremely simple, highly
efficienct, universal method for fabricating high Tg polymer
micro/nano patterns, including micro-prism arrays, nano-grating
and nano-hole arrays over large areas. In the proposed method,
the P3HT structure is formed by imprinting the P3HT solution
and solvent infiltration, rather than by heating the polymer
beyond its glass transition temperature or by chemical cross-
linking reactions. The transfer fidelity of SIIL depends on the
concentration of the polymer solution. When the concentration
of the P3HT solution is 50 mg ml�1, the lateral fidelity of SIIL is
good and the height of the P3HT structures are smaller than the
PDMS mold resulting from the solvent infiltration. Lower
concentrations of P3HT solution can be used to fabricate smaller
P3HT structures using the same PDMS mold. SIIL can be used
in P3HT/PCBM polymer solar cells, and the nano-grating and
nano-hole arrays improve the PCE of the polymer solar cell.
Acknowledgements
This work was China Postdoctoral Science Foundation funded
project and supported by Shanghai Postdoctoral Science Foun-
dation (11R21420900) and Natural Science Foundation of
Shanghai (no. 11ZR1432100).
J. Mater. Chem., 2012, 22, 21154–21158 | 21157
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