Low-Dimensional Carbon Nanomaterials 2012View this Special Issue
Research Article | Open Access
Matthew Cole, Pritesh Hiralal, Kai Ying, Chi Li, Yan Zhang, Kenneth Teo, Andrea Ferrari, William Milne, "Dry-Transfer of Aligned Multiwalled Carbon Nanotubes for Flexible Transparent Thin Films", Journal of Nanomaterials, vol. 2012, Article ID 272960, 8 pages, 2012. https://doi.org/10.1155/2012/272960
Dry-Transfer of Aligned Multiwalled Carbon Nanotubes for Flexible Transparent Thin Films
Herein we present an inexpensive facile wet-chemistry-free approach to the transfer of chemical vapour-deposited multiwalled carbon nanotubes to flexible transparent polymer substrates in a single-step process. By controlling the nanotube length, we demonstrate accurate control over the electrical conductivity and optical transparency of the transferred thin films. Uniaxial strains of up to 140% induced only minor reductions in sample conductivity, opening up a number of applications in stretchable electronics. Nanotube alignment offers enhanced functionality for applications such as polarisation selective electrodes and flexible supercapacitor substrates. A capacitance of 17 F/g was determined for supercapacitors fabricated from the reported dry-transferred MWCNTs with the corresponding cyclic voltagrams showing a clear dependence on nanotube length.
Carbon nanotubes, one-dimensional high aspect ratio carbon allotropes, have received significant interest in the past two decades as a viable candidate material to replace the industry pervading, and increasingly expensive, transparent conductor, indium tin oxide (ITO). Although highly transparent and highly conductive, ITO exhibits poor flexing performance due to microcrack formation. Carbon nanotube networks are extremely flexible [1–3], highly conductive [4–6] and offer impressive optical transparency [4, 7–9]. Nevertheless, in order to fully exploit these features, films must be free-standing or supported on substrates of similar opacity and flexibility, namely, polymers and elastomers. Little work on the direct deposition of aligned nanotubes onto polymers has been reported , and as a result few applications exploit the properties of pristine nanotubes. Direct nanotube deposition on polymers necessitates substantial reductions in growth temperatures. This most often results in the deposition of inflexible pyramidal carbon nanofibres  rather than highly graphitic and conductive nanotubes.
A variety of solution processes have been explored to produce nanotube thin films [5, 12–14]. Nevertheless, such detrimental chemi douche processing, employing aggressive sonication and costly acid treatments, ultimately degrades the nanotubes electronic properties. Nanotube alignment has been demonstrated in a number of ways [15–17] though solution processing produces isotropic networks lacking the advantageous structural anisotropy associated with the initial as-grown one-dimensional nanostructures. Consequently, a wet-chemistry-free, inexpensive, and facile transfer technique, that retains the nanotubes alignment, is necessary for applications such as flexible optoelectronic polarisers and supercapacitors for next-generation energy storage [18–21] and display technologies.
Carbon nanotube-based thin films offer extremely high surface areas which make them functionally desirable for high-density energy storage, though binderless processes that offer strong surface and intertube adhesion combined with excellent conductivities and nanotube alignment are advantageous traits. We herein report on the dry-transfer of multiwalled carbon nanotubes to polymer substrates and demonstrate control over the sheet resistance and optical transparency of the transferred thin films. Simple supercapacitor structures have also been demonstrated as one viable application of the proposed technique.
Multiwalled carbon nanotubes (MWCNTs) were synthesised by thermal chemical vapour deposition (CVD) in a commercially available cold-walled reactor (AIXTRON, Black Magic). Bilayer catalysts were prepared by RF sputtering 10 nm Al2Ox onto 200 nm thermally oxidised Si substrates which were subsequently exposed to ambient atmosphere and coated with 1 nm thermally evaporated Fe (0.2 Å/s). The chamber was prepressurised to 26 mbar with 8 sccm C2H2 diluted in 192 sccm H2. An ohmically heated graphite stage was ramped at 5°C/s to 700°C. Growth was repeatedly observed to initiate at ~520°C. Figures 1(a) and 1(b) show typical profile and areal scanning electron micrographs (SEMs) of an as-grown MWCNT forest. A high-resolution transmission electron micrograph (HR-TEM) of an individual MWCNT is given in the inset of Figure 1(b). The MWCNTs are formed from 2–5 graphitic walls, were(S.D) nm in diameter, and had an initial growth rate of ~0.8 μm/s that monotonically decreased over time. Figure 1(c) is the Raman spectra of the as-grown forest (Renishaw InVia, He-Ne source operating at 633 nm/3 mW). The spectra are characteristic of MWCNTs [22, 23] and were highly uniform across samples, highlighting process reproducibility.
Figure 2 illustrates the dry-transfer process. A polycarbonate (PC) destination substrate is angled toward the sources MWCNTs and is compressed using a quartz cylinder, rotated and sheared at ~1 cm/s. The MWCNTs readily de-bond from the source substrate and adhere to the PC. The dry-transfer process does not degrade the crystallographic order of the MWCNTs, as evidenced via Raman spectroscopy. A variety of destination substrates were considered, including poly(ethylene terephthalate), polycarbonate, and Al foil. In the latter case, when transferring extremely short nanotubes (<1 μm), self-assembled monolayer (SAM) adhesion promoters were necessary, such as poly(lysine) and aminopropyltriethoxy silane (APTES). Prior to SAM treatment MWCNTs did not adhere to the Al foil, whereas after treatment nearly 100% (by area) were successfully transferred.
Figure 3(c) shows a 900 nm × 900 nm AFM micrograph (Agilent) of a dry-transferred MWCNT film on a PC substrate demonstrating the high degree of alignment. An optical micrograph of poly(lysine)-treated Al foil with a dry-transferred MWCNT film is given in Figure 3(d). The inset depicts a schematic of the substrates cross-section.
MWCNT thin films were patterned by standard photolithography and O2 reactive ion etching (RIE: 0.2 mbar, 100 W, 120 s) (Figures 3(b) and 3(e)). Transparency control was demonstrated using RIE. The transparency between the polymer-protected 5, 20, and 50 μm dots was controlled, as illustrated in Figure 3(f). Transparency control was also demonstrated by adjusting the length of the MWCNTs prior to the dry-transfer, (by varying the CVD growth duration). In this instance, films were defined by patterning the bilayer catalyst prior to growth. A Mo catalyst-passivation process was used to prevent nanotube growth from particular areas. No nanotubes grew from those areas coated with Mo (20 nm). An inexpensive laser-jet patterning technique was employed to achieve this. Patterned MWCNT forests were then transferred, as afore mentioned. Repeatedly rolled films became sufficiently compacted such that they formed free-standing, pristine MWCNT “paper” that maintained structural integrity even under rigorous mechanical strain.
Uniaxial strain and bend radii measurements were performed using computer-controlled custom-built systems connected to a Keithley 6430 source-measure unit. Experiments were performed at room temperature and pressure.
3. Results and Discussions
Figure 4 shows optical micrographs of three prepatterned transferred samples of differing MWCNT length. The sheet resistance () and optical transmittance () were found to be strongly dependent on the MWCNT length. Figure 5(a) shows the UV-Vis-NIR transmittance of films fabricated from MWCNTs < 1 μm to 500 μm in length. For the most opaque and highly conductive films, ~1.2 Ω/sq. with ~9% transparency (550 nm). For nominally equivalent samples, two- and four-probe conductivity measurements yielded ~10.2 Ω/sq. and ~2.6 Ω/sq., respectively, evidencing a low contact resistance (7.6 Ω/sq). The most transparent films (85% for <1 μm long MWCNTs) had sheet resistances as low as 550–1000 Ω/sq. Reducing the nanotube length substantially increased the optical transmission whilst only increasing the sheet resistance by approximately one order of magnitude (Figure 5(b)). This observation can be explained in terms of the increased number of inter-nanotube junctions for films comprised of shorter nanotubes. Furthermore, one would expect longer nanotubes to increase the films conductivity as the rolling process produces substantially thicker films which offer lower bulk resistance. The DC conductivity in such films is primarily dependent on tunnelling between individual nanotubes. As a result, the conductivity is critically dependent on the number of conduction pathways, junctions, and the general network morphology—all of which can be varied by adjusting the nanotube length and degree of alignment. The films demonstrated optoelectronic characteristics nearing the ITO benchmark and superior characteristics to competing organic technologies such as TDA and PEG-enhanced PEDOT:PSS [24, 25].
The sheet resistance () and optical transparency at 550 nm (T) are related by [26–28]; where is the impedance of free space (377 Ω), is the optical conductivity, and is the direct current electrical conductivity. A viable transparent electrode must demonstrate low- and high- throughout the optical window (300–900 nm). For an ideal transparent conductor, . Fitting (1) gives . Graphite has a conductivity ratio of , whereas current driven applications require . The minimum industry standard for (brittle) transparent conductors, typical for display applications, is (>90% for <100 Ω/sq.) [26, 29]. The reported conductance ratio is someway off the industry standard but is nevertheless close to the state-of-the-art for thin films prepared from chemically modified graphene . Though the pristine thin films offer only modest performance, it is important to stress that these films are chemically untreated. The films have not been doped in anyway. Suitable doping will lead to conductivity enhancements, for a given transparency, thus allowing the films to compete with more traditional vacuum and spray processing, which intrinsically employ en route doping procedures.
The AC sheet resistance of the dry-transferred films was investigated at microwave frequencies using a technique described in detail in . The transmissive sheet resistances, in the 120–175 THz range, were found to be 0.3 and 640 Ω/sq., for nanotubes 500 μm and 1 μm long, and were broadly consistent with the DC measurements for films of similar optical characteristics discussed previously.
The uniaxial strain response of the dry-transferred MWCNTs and the primary competing technologies, namely CVD grown (2–4 layer) hot press laminated graphene (HPLG)  and commercially available PET-supported ITO, is shown in Figure 6(a). Samples were electrically contacted using mechanical clamps and conductive epoxy (inset Figure 6(a)). The maximum uniaxial tensile strain (), defined as the strain for which , of commercially available ITO was ~1.2%. HPLG samples failed at ~15% and showed excellent correspondence with the theoretical values for single graphene flake failure [32, 33]. The dry-transferred MWCNT thin films withstood strains of up to 140% (the limit of the apparatus) whilst showing only a minor reduction in conductivity (~5, where denotes the initial/relaxed sheet resistance). Similar performance has been reported elsewhere, though predominately only in the case of solution-processed single-walled carbon nanotube thin films . As the films become increasingly strained, the MWCNTs align. The individual MWCNTs observe negligible strain during this aligning stage. It is not until the film has maximised its degree of alignment that the MWCNTs undergo nanoscopic straining and eventually fail catastrophically. As a result, exceptionally high failure strains are possible owing to the networks porosity and anisotropy.
The cyclic strain performance is plotted in Figure 6(b). Under equivalent conditions, ITO/PET was strained to 1% and then relaxed. The resistivity of the ITO/PET was around 44% larger than the initial unstrained film. Straining irreversibly increased the sheet resistance of the ITO through microcrack formation. In contrast, dry-transferred films were strained (50%), then relaxed, and the process repeated. The initial strain (cycle 1) increased the sample resistance by approximately 42%; however each cycle thereafter the relaxed resistance repeatedly returned to this value. The long-term flexing stability of the dry-transferred thin films was considered by straining samples by 22%, over 100 cycles. The dry-transferred films showed a negligible increase in resistance over time. Figure 6(c) depicts a dependence on the electrode separation. Increasing the electrode separation (L) tended to increase the maximum attainable strain as this increased the amount of available material over which the strain was distributed. Figure 6(d) shows the variation in the normalised change in resistance as a function of the radius of curvature. The inset(s) depict the apparatus during a typical measurement. and was largely independent of the radius of curvature over the range considered. of the ITO samples increased by over three orders of magnitude for curvatures <9.5 mm. Similarly, HPLG samples showed a linear increase in for radius <5 mm.
A key feature of the reported technique is the ability to align the nanotubes during the inexpensive and rapid dry-transfer process. The degree of nanotube alignment is illustrated in Figure 7, which plots the Steridian 37 (Str37) function for a transferred sample, calculated using the SPIP image analysis software. Str37 is defined as the ratio of the in-plane distance between the real autocorrelation centre and the boundary at which the height of the image has decayed to 37% of the depth-range at this autocorrelation centre. An autocorrelation is applied to the images depth-range to infer the position. The decay in the depth-range in all directions is evaluated and the Str37 value is calculated [35, 36]. For perfectly aligned arrays Str37 = 0, whilst for disordered networks which exhibit no directional preference, Str37 = 1. Depending on the roll technique both well-aligned (Figures 7(a)–7(d)) and highly isotropic networks could be transferred (Figures 7(e) and 7(f)). Str37 = 0.26 for the aligned transfers and 0.60 for the compressed/isotropic transfers.
Aligned nanotube electrodes may find application as tunable optical polorisors and advanced electrode materials in next generation flexible display technologies. Figure 7(g) shows a fabricated bilayer structure. Here crossed and aligned structures, of controlled controlled pitch, were transferred to a PET substrate by successive rolls of pre-patterned forests to from optical polarisers that exploit the nanoscopic spacing of the nanotubes, and also the microscopic spacing of the patterned films.
To demonstrate one potential application of the dry-transferred thin films, two-electrode electric double-layer (EDLC) cells were constructed. Due to the films’ high conductivity, the MWCNTs functioned as both the active material and charge collector, reducing the overall material requirements therefore increasing the weight fraction of the active material in the device. The final EDLC was 10 mm × 10 mm (Figure 8(a)). An insulating porous separator (Celgard 2500) was sandwiched between two MWCNT electrodes soaked in electrolyte (1 M Tetraethylammonium tetrafluoroborate (Et4NBF4) in propylene carbonate, Sigma-Aldrich). Al tape was used to externally electrically contact the cell. Three different films, comprised of different MWCNT lengths, were considered. The nanotube lengths and active weights were 28.5 μm/0.6 mg·cm−2 (1 min growth), 96 μm/1.1 mg·cm−2 (5 min), and 235 μm/2.3 mg·cm−2 (10 min). Cells were charcaterised by galvanostatic charge/discharge (1 mA/cm2) and cyclic voltammetry (50 mV/s) measured using an Autolab PGSTAT302N potentiostat (Figure 8(b)).
Thicker films offered higher conductivities and longer nanotubes showed a higher capacitance per unit area as well as a lower equivalent series resistance (ESR), both of which are essential for high-power delivery. The capacitance of the two-electrode MWCNT EDLCs was estimated to be between 6 and 17 F/g, for cells biased to 1 V. This is roughly twice the capacitance reported for sprayed, solution-processed single-walled carbon nanotube devices under similar experimental conditions . The ESR decreases with increasing film conductivity and ranged from 1000 Ω (28.5 μm) to 44 Ω (235 μm) corroborating the sheet resistance estimates made previously. Nevertheless, the overall ESR is still somewhat higher than expected. This is most likely attributed to the relatively resistive Schottky barrier at the Al-MWCNT interface, the intrinsic resistivity of the electrolyte, as well as contributions from the multiple electrolyte/MWCNT interfaces. Thicker electrodes increase the energy density allowing the active material to occupy a greater volume ratio. However, this is offset by higher ion diffusion barriers in the inner regions of the electrode, resulting in substantial internal resistance and consequently reducing high-power performance. This limits the practical thickness of any nanostructured electrode. Thus, ideally thick electrodes that possess both high capacitance and that are operable at high power are desired. Up to the thicknesses studied, approximately constant power densities were observed (2.48 W/g), indicating that high permeability is maintained even for thicker electrodes.
We have reported the development of an MWCNT dry-transfer technique capable of transferring CVD-synthesised aligned MWCNTs to a variety of flexible substrates without chemically pre-treating the MWCNTs to enhance their adhesion. Accurate control over both the optical transparency and sheet resistance was shown to depend critically on the length of the as-grown MWCNTs. The dry-transferred MWCNT thin films showed a change in resistance as low as 5 for strains in excess of 140%, outperforming PET-supported ITO by two orders of magnitude and hot press laminated graphene by one order of magnitude. The alignment of the constituent MWCNTs was shown to be controllable and was demonstrated to offer a viable approach to the fabrication of flexible transparent polarisation selective electrodes for advanced display technologies. Double-layer supercapacitor cells were fabricated and showed a modest capacitance of up to 17 F/g. The results demonstrated that the dry-transferred MWCNT electrodes are excellent candidates for inexpensive, compact, high-energy-density storage and offer industry compatibility via a facile active material transfer approach.
This work was supported by the Schiff Studentship, Cambridge University. M. Cole acknowledges the support of St. John’s College Cambridge and St. Edmund’s College Cambridge. C. Li thanks the Scientific Research Foundation of Graduate School of Southeast University, China (Grant no. YBJJ0926). K. Teo acknowledges the support of the EC Grant TECHNOTUBE.
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