Jin-Kyung Lee,
Heejung Kang,
Sanghwa Lee,
Inho Choi and
Byeong-Hyeok Sohn*
Department of Chemistry, Seoul National University, Seoul 151-747, Korea. E-mail: bhsohn@snu.ac.kr
First published on 28th August 2014
We demonstrated the fabrication of fluorophore-functionalized nanopatterns with topographic features. To obtain fluorescent nanopatterns, diblock copolymers having fluorophores in one of the blocks were synthesized by the reversible addition fragmentation chain transfer polymerization and were annealed by solvent vapor, resulting in perpendicular or parallel cylindrical nanopatterns functionalized with fluorophores, depending on the annealing solvent. Then, by etching one of the copolymer blocks, we were able to produce fluorescent topographic nanopatterns. Furthermore, Au nanorods selectively loaded in the nanometer-sized valley of the pattern effectively altered the fluorescence of the topographic nanopattern.
As an alternative or a complimentary method to top-down lithographic techniques for nanoscale patterns, utilization of self-assembled nanostructures of block copolymers has been considered. Block copolymers, consisting of two or more polymers covalently connected, spontaneously assemble into various nanostructures including spheres, cylinders, and lamellae, of which sizes are typically in the range of a few tens of nanometers.16,17 Thus, nanostructures of block copolymers can be applied to efficient generation of functional nanopatterns without heavy lithographic tools.18,19
In this work, we first demonstrated the creation of fluorescent nanopatterns because top-down lithography or bottom-up assembly alone cannot efficiently produce fluorescent patterns in the nanometer range. For effective production of fluorescent nanopatterns without a lithographic tool, we synthesized diblock copolymers having fluorophores in one of the blocks by the reversible addition fragmentation chain transfer (RAFT) polymerization. Since fluorophores are covalently linked to one of the blocks, they assembled only in the nanodomains of that block by solvent vapor annealing, resulting in hexagonal or linear fluorescent nanopatterns. However, these fluorescent nanodomains are embedded in the matrix of the other block of copolymers. Thus, by etching the matrix block selectively, we finally obtained pure fluorescent nanopatterns with topographic features. In addition, we were able to modify fluorescence of the nanopattern by placing Au nanorods in the nanometer-sized valley of the pattern. This result implies a potential application in detection of nanometer-sized objects with fluorescent topographic nanopatterns.
000 g mol−1 with PS standards and 141
000 g mol−1 with PMMA standards. The polydispersity index is 1.08 (GPC with PS standards, ESI, Fig. S1†). To synthesize poly(methylmethacrylate)-b-poly(styrene-r-(4-vinylbenzylchloride)) (PMMA-b-P(S-r-4VBC)) diblock copolymers, the PMMA macro chain transfer agent (1.0 g, 0.0079 mmol), AIBN (0.3 mg, 0.00079 mmol), styrene (8.72 g, 8.4 mmol), and 4-vinylbenzyl chloride (1.28 g, 0.84 mmol) were added together in a Schlenk tube. Oxygen was exchanged by argon in three freeze–thaw cycles and polymerization was carried out at 70 °C for 22 h. Copolymers were purified by precipitation in methanol three times. To remove unlinked P(S-r-4VBC) polymers, Soxhlet with cyclohexane was performed and then 1.7 g of PMMA-b-P(S-r-4VBC) in pale pink powder was obtained. The number average molecular weight is 263
000 g mol−1 and the polydispersity index is 1.13 (GPC, ESI, Fig. S1 and NMR, ESI, Fig. S2†).
:
4. A thin film was exposed to saturated vapor of acetone or chloroform in a closed glass jar at room temperature for 1 h (acetone) or 13 h (chloroform). After annealing, the sample was removed to ambient atmosphere and dried. PMMA domains in annealed films were etched by oxygen plasma (80 W, 38 mTorr) for 10 s (an acetone-annealed film) and 13 s (a chloroform-annealed film).
000 g mol−1 and 1.13, respectively (ESI, Fig. S1†). The mole ratio between two blocks is 1
:
1 (ESI, Fig. S2†). The NMR result also confirmed 10.4 mol% of 4VBC in the PS block (ESI, Fig. S2†). Since benzyl chloride can react with primary amine,20,21 rhodamine 110, which shows absorption at 496 nm and emission at 520 nm (ESI, Fig. S3†), was selected as a representative fluorophore and covalently linked to the P(S-r-4VBC) block as shown in Fig. 2. We confirmed that 7.8 mol% of rhodamine 110 was attached to the P(S-r-4VBC) block (ESI, Fig. S4†). This fluoropore-functionalized diblock copolymers synthesized by RAFT enable the fabrication of a fluorescent nanopattern without a lithographic tool because fluorophores covalently linked to one of the blocks can spontaneously assemble only in the nanodomain of that block by solvent vapor annealing.
To produce fluorescent nanopatterns, we first annealed a thin film of PMMA-b-P(S-r-4VBC-r-Rho) by acetone vapor, instead of thermal annealing, to avoid undesirable changes of fluorophores at high temperatures. Since we employed a relatively large molecular weight (264
000 g mol−1) of the fluorophore-functionalized copolymer, PMMA-b-PS with a low molecular weight (10
000 g mol−1) was mixed with the copolymer to promote evolution of nanostructures during the solvent annealing as demonstrated in the literature.22
In Fig. 3, we can find a hexagonally ordered nanopattern in an acetone-annealed PMMA-b-P(S-r-4VBC-r-Rho) thin film. In the TEM image (Fig. 3a), dark gray dots and white regions between them correspond to P(S-r-4VBC-r-Rho) and PMMA, respectively, because PMMA generally appears bright in TEM images due to thinning by the electron beam.23 In the AFM image (Fig. 3b), bright nanopatterns are also discernible, which are perpendicular cylinders of the P(S-r-4VBC-r-Rho) block in a hexagonal array, embedded in the matrix of the PMMA block. The diameter and center-to-center distance (domain spacing) of these cylindrical nanostructures are ∼62 nm and ∼83 nm, respectively.
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| Fig. 3 PMMA-b-P(S-r-4VBC-r-Rho) thin film after acetone vapor annealing: (a) TEM image; (b) AFM image. The scale bars are 500 nm. | ||
Acetone can selectively swell the PMMA block of PMMA-b-P(S-r-4VBC-r-Rho) copolymers so that the formation of cylindrical nanostructures of the P(S-r-4VBC-r-Rho) block in the PMMA matrix is reasonable even though the mole ratio between two blocks is 1
:
1. Perpendicular cylinders are typically obtained in a thin film of diblock copolymers when the film thickness is smaller than a half of the domain spacing.24 Thus, the perpendicular cylinders in Fig. 3 can be understood because the film has a smaller thickness (∼32 nm) than a half of the domain spacing (∼41.5 nm). Therefore, we produced a nanopattern of hexagonally ordered cylinders, which are functionalized with red-emitting fluorophores, by acetone vapor annealing on a thin film PMMA-b-P(S-r-4VBC-r-Rho) copolymers as shown in the schematic illustration in Fig. 3b.
To generate a topographic nanopattern, we removed the PMMA matrix, in which the fluorophore-functionalized cylinders are hexagonally arranged, in a thin film of PMMA-b-P(S-r-4VBC-r-Rho) copolymers. Oxygen plasma etching was performed directly on the thin film, which etched the PMMA block faster than the other block, resulting in a topographic nanopattern of cylinders functionalized with red-emitting fluorophores (Fig. 4). The height of cylinders becomes ∼8 nm, indicating that most of PMMA domains were removed when the film thickness before etching (∼32 nm) is considered. We confirmed red-color emissions from the topographic nanopattern as shown in the PL spectrum of Fig. 4b. Thus, we generated a fluorescent topographic nanopattern from a thin film of PMMA-b-P(S-r-4VBC-r-Rho) copolymers which is illustrated in Fig. 4a. We note that UV irradiation followed by washing with acetic acid can selectively remove PMMA domains in a diblock copolymer containing a PMMA block without scarifying the film thickness.25 However, this process, particularly UV irradiation, can damage fluorescent characteristics of fluorophore-functionalized copolymers.
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| Fig. 4 Fluorescent topographic nanopattern from acetone-annealed PMMA-b-P(S-r-4VBC-r-Rho) after etching the PMMA matrix: (a) AFM image; (b) PL spectrum. The scale bar is 500 nm. | ||
By annealing a thin film of PMMA-b-P(S-r-4VBC-r-Rho) copolymers with chloroform instead of acetone, we obtained a fluorescent nanopattern consisting of fluorophore-functionalized cylinders parallel to the film plane as shown in Fig. 5. In both TEM and AFM images, we can find parallel cylinders with the diameter of ∼61 nm and the center-to-center distance of ∼84 nm, which are almost identical to those of perpendicular cylinders in Fig. 3. In general, cylindrical nanostructures are oriented parallel to the substrate in thin films of diblock copolymers by solvent vapor annealing with the film thickness greater than a half of the domain spacing.24 The film thickness (∼48 nm) in Fig. 5 is larger than a half of the domain spacing (∼42.5 nm). In addition, chloroform can dissolve both blocks of PMMA-b-P(S-r-4VBC-r-Rho) but prefer the PMMA block to the other block.24 These conditions can explain cylindrical nanostructures parallel to the film plane in a thin film of PMMA-b-P(S-r-4VBC-r-Rho) annealed by chloroform. Thus, we generated a nanopattern of fluorophore-functionalized cylinders oriented parallel to the substrate as shown in the schematic illustration in Fig. 5b.
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| Fig. 5 PMMA-b-P(S-r-4VBC-r-Rho) thin film after chloroform vapor annealing: (a) TEM image; (b) AFM image. The scale bars are 500 nm. | ||
As the previous case of cylindrical nanostructures in hexagonal order, we produced a topographic nanopattern by removing the PMMA matrix in a thin film of PMMA-b-P(S-r-4VBC-r-Rho) copolymers after chloroform vapor annealing. By oxygen plasma etching, we obtained a topographic nanopattern of parallel cylinders functionalized with red-emitting fluorophores as shown in the AFM image of Fig. 6, in which the thickness of each cylinder is ∼16 nm. We also confirmed red-color emissions from this topographic nanopattern as shown in the PL spectrum of Fig. 6b. Therefore, by chloroform annealing, a fluorescent topographic nanopattern of parallel cylinders was created (schematic illustration in Fig. 6a), whereas that of hexagonally ordered cylinders was obtained by acetone annealing (schematic illustration in Fig. 4a), using the same fluorophore-functionalized copolymer.
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| Fig. 6 Fluorescent topographic nanopattern from chloroform-annealed PMMA-b-P(S-r-4VBC-r-Rho) after etching the PMMA matrix: (a) AFM image; (b) PL spectrum. The scale bar is 500 nm. | ||
To examine a value of a fluorescent topographic nanopattern, we introduced Au nanorods on the fluorescent nanopattern of parallel cylinders with and without a topographic feature. We employed Au nanorods having the diameter of ∼33 nm and the length of ∼96 nm (ESI, Fig. S5†), which can be fit into the valley of the topographic nanopattern because the diameter is smaller than the width of the valley (∼44 nm). In the AFM images of Fig. 7, most of Au nanorods are aggregated on a thin film of PMMA-b-P(S-r-4VBC-r-Rho) without a topographic feature, whereas Au nanorods exist individually and many of them follow the cylindrical line on the topographic nanopattern. From the height profile of single nanorod on the film without a topographic pattern (Fig. 7a), the thickness of a nanorod (∼31 nm) is almost the same as its diameter (∼33 nm), indicating that the nanorod resides on the top of the film. In contrast, the thickness of the nanorod on the topographic pattern (∼17 nm) is close to a half of its diameter, which confirms that the nanorod fits into the valley of the topographic pattern. These Au nanorods in the valleys of the topographic pattern increased emissions of the fluorescent nanopattern (Fig. 8b) due to the near-field scattering effect of Au nanorods26 which exist very next to the fluorophore-functionalized cylinders. However, no enhancement of the emission was observed in the case of Au nanorods on the top of the fluorescent nanopattern without a topographic feature (Fig. 8a). When a spacer layer of poly(acrylic acid) (8000 g mol−1) with the thickness of 7.2 nm was inserted between Au nanorods and the fluorescent nanopattern, no enhancement of the emission was observed (ESI, Fig. S6†), implying that the distance between Au nanorods and the fluorescent nanopattern is crucial for near-field effects of Au nanorods. Thus, a fluorescent topographic nanopattern can find a potential application of detection or sensing with nanometer-sized objects. We note that the nanopatterns with or without Au nanorods did not show enough absorption in UV-Vis spectroscopic measurements because they were too thin.
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| Fig. 8 PL spectra of PMMA-b-P(S-r-4VBC-r-Rho) thin films with Au nanorods (solid line) and without Au nanorods (dashed line): (a) without topographic pattern; (b) with topographic pattern. | ||
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c4ra06139j |
| This journal is © The Royal Society of Chemistry 2014 |