Open Access

High performance of carbon nanotubes/silver nanowires-PET hybrid flexible transparent conductive films via facile pressing-transfer technique

Nanoscale Research Letters20149:588

https://doi.org/10.1186/1556-276X-9-588

Received: 21 September 2014

Accepted: 18 October 2014

Published: 28 October 2014

Abstract

To obtain low sheet resistance, high optical transmittance, small open spaces in conductive networks, and enhanced adhesion of flexible transparent conductive films, a carbon nanotube (CNT)/silver nanowire (AgNW)-PET hybrid film was fabricated by mechanical pressing-transfer process at room temperature. The morphology and structure were characterized by scanning electron microscope (SEM) and atomic force microscope (AFM), the optical transmittance and sheet resistance were tested by ultraviolet-visible spectroscopy (UV-vis) spectrophotometer and four-point probe technique, and the adhesion was also measured by 3M sticky tape. The results indicate that in this hybrid nanostructure, AgNWs form the main conductive networks and CNTs as assistant conductive networks are filled in the open spaces of AgNWs networks. The sheet resistance of the hybrid films can reach approximately 20.9 to 53.9 Ω/□ with the optical transmittance of approximately 84% to 91%. The second mechanical pressing step can greatly reduce the surface roughness of the hybrid film and enhance the adhesion force between CNTs, AgNWs, and PET substrate. This process is hopeful for large-scale production of high-end flexible transparent conductive films.

Keywords

Flexible transparent conductive filmCNTs/AgNWsAdhesionPressing-transfer

Background

Flexible transparent conductive films (FTCFs) have received much attention because of their electrical and optical properties and their feasibility in bending, folding, and mounting to a surface, which have a great potential to be applied in a large-area display, touch screen, light-emitting diode, solar cell, semiconductor sensor, etc. [17]. Indium tin oxide (ITO) as a traditional transparent conductive material has been widely used for organic solar cells and light-emitting diodes; however, it cannot meet the market demand of FTCF due to its rising cost and brittleness and hence it has limited applicability in flexible electronic devices [810]. Carbon nanotubes (CNTs) [11, 12], graphene [13, 14], or a hybrid of them [15] have attracted significant interest and have been successfully used as transparent conductive materials on flexible substrates in organic light-emitting diodes and solar cells. However, their performance in terms of sheet resistance and transparency is still inferior to ITO. Metal nanowires (MNWs) are a promising replacement of ITO, CNTs, or graphene because of their high dc conductivity and optical transmittance [16, 17]. Gold nanowire (AuNW) [18], silver nanowire (AgNW) [1923], copper nanowire (CuNW) [2427], aluminium nanowire (AlNW) [28], and hybrid [29, 30] films have been demonstrated to have optical transmittance comparable to an ITO film at the same sheet resistance. Especially MNWs on a plastic substrate can have better mechanical properties than ITO.

Nevertheless, researchers found that MNW films have electrically nonconductive open spaces (approximately 200 to 1,000 μm), and the open spaces become bigger for sparser networks [31, 32], and some applications require continuously conductive or low nonconductive regions. The large openings in a MNW network could be problematic for some device applications when the charge diffusion path length is less than the hole size. One strategy to overcome the defect of MNW films is to fill components such as graphene [3234], CNTs [35], conductive polymers [3639], or metal oxides [40], but these reported methods may cause processing and cost problems. Increasing the density of MNWs may also reduce the open spaces and the sheet resistance, but the optical transmittance may also be greatly affected. Meanwhile, the price of MNWs, especially AuNWs and AgNWs, is still too high to be heavily used for decreasing manufacturing cost. Significant improvement is needed for new materials or processes which can bring cost-effective and reliable transparent conductive films.

In this work, we attempted to mix and use CNTs and AgNWs as conductive materials and transfer CNT/AgNW hybrids on flexible polyethylene terephthalate (PET) film and then form CNT/AgNW-PET films by a facile two-step mechanical pressing technique. In this design, AgNWs were the main conductive networks, and CNTs as the assistant conductive networks were filled in the open spaces of the AgNW networks; both of them had good connections, which made the CNT/AgNW-PET films possess low sheet resistance and high optical transmittance.

Methods

The silver nanowires with a diameter of approximately 50 to 90 nm and a length of approximately 10 to 20 μm and the multi-walled carbon nanotubes with a diameter of approximately 20 to 50 nm and a length of approximately 5 to 15 μm used during the fabrication of the films were purchased from Nanjing Xianfeng Tech Co., Ltd (Nanjing, Jiangsu, China) and supplied with a concentration of 10 and 2 mg/mL in alcohol, respectively. The suspensions were further diluted to a concentration of 0.1 and 0.01 mg/mL, respectively, in alcohol which was subsequently used in all the transfer processes.The schematic representation of the preparation process of CNT/AgNW-PET films is shown in Figure 1a. First, the hybrid suspensions of CNTs/AgNWs with different ratios (mL/mL approximately 0.5/2, 1/2, 2/2, 4/2, 2/1, 2/3, 2/4) were obtained by direct mixing of CNT and AgNW suspensions, diluting to a volume of 10 mL and then supersonic dispersing treatment for 30 min. Then, the hybrid suspension was vacuum filtered by using a polyvinylidene fluoride (PVDF) filter membrane (Φ5 cm, hole diameter of 0.2 μm). Third, the hybrid CNT/AgNW film was transferred onto a PET substrate by pressing the filter membrane using a stainless steel plate and a press machine at a pressure of 3 MPa for 10 s. Then, the CNT/AgNW-PET film was obtained after lifting the pressure and removing the PVDF filter membrane slowly. When the semi-finished product was dried at room temperature for more than 30 min, to enhance the adhesion of CNT/AgNW networks on the PET substrate and reduce the junction resistance between CNTs and AgNWs, a second pressing at a pressure of 10 MPa for 30 s was implemented using a bare glass plate as a counter. As a comparison, a hybrid film was heated to 120°C for 30 min to test the effect of heating on the optical transmittance and sheet resistance.
Figure 1

Transfer preparation of CNT/AgNW-PET films (a) and suspensions (b); SEM pictures of AgNWs (c) and CNTs (d).

Optical transmittance (T) was obtained using a Beijing PGeneral TU-1900 ultraviolet-visible spectroscopy (UV-vis) spectrophotometer (Beijing Purkinje General Instrument Co., Ltd., Beijing, China) with a blank PET as the reference. The surface morphology and structural pictures were obtained using a JEOL JSM-7001 field emission scanning electron microscope (SEM; JEOL Ltd., Tokyo, Japan) and Shanghai Zhuolun MicroNano D3000 atomic force microscope (AFM; Shanghai Zhuolun MicroNano Instrument Co., Ltd., China). Sheet resistance (Rs) was measured using four-point probe technique by depositing silver paint with a thickness more than 80 nm at the corners in a square shape with sides of approximately 3 mm and at least ten locations across the sample, and the values reported in this work are the mean value obtained across the entire film. The adhesion test was carried out by observing the remaining nanowires adhering to the PET substrate and measuring the Rs and T of films when the 3M sticky tape was peeled off.

Results and discussion

Figure 1a shows the schematic representation of the transfer process of CNT/AgNW networks onto the PET substrate. It can be found that this process has several distinguishing features. The entire process is implemented at room temperature and takes only several minutes. It is very critical for actual production due to avoiding the disadvantages from high temperature and complicated process. The process is also easy to control and adjust. First, the measured amount of CNTs and AgNWs are mixed in alcohol and sonicated for 30 min without adding any surface active agent that is enough to guarantee that the suspension is stable for more than 12 h, and the suspension and SEM pictures of AgNWs and CNTs are shown in Figure 1b,c. The nanowires can be dispersed very well by this method. Then, the suspension is filtered on a commercially available PVDF filter membrane to obtain a uniform film of CNTs/AgNWs. Whereafter, the PVDF membrane bearing the CNTs/AgNWs is pressed against the PET substrate at a moderate pressure of 3 MPa, because we found that in our experiments the sheet resistance of AgNW film has little change when pressed at a pressure of more than 3 MPa, so 3 MPa is enough for a AgNW film to reduce resistance. When the pressure is released after a few seconds and the PVDF membrane is peeled off slowly from the substrate, the CNT/AgNW film is entirely transferred onto the substrate. The size of the hybrid film is limited only by the size of the starting PVDF filter membrane. We note that the static pressing step can be replaced by rolling pressing to realize massive production. In the last step, a high pressure of 10 MPa is needed to enhance the junction between CNTs and/or AgNWs. Actually, the high pressure treatment is also very important to reduce surface roughness and adhesion of films that will be mentioned in the later section. In brief, these above-mentioned features are beneficial for the large-scale production of flexible transparent conductive films.Figure 2 shows the SEM pictures of CNT/AgNW films at different ratios on PET substrates fabricated with the mechanical pressing-transfer process. From Figure 2a, it can be seen that the transfer process is extremely uniform over the entire area of the film leading to a uniform density of nanowires everywhere on the substrate. With the different ratios of CNTs/AgNWs shown in Figure 2b,c,d,e,f, the AgNWs form the main conductive networks, and CNTs as the assistant conductive networks are filled in the open spaces of the AgNWs networks; both of them have good connections. The difference between them is the density of CNT networks due to the different addition amount of CNTs.
Figure 2

SEM pictures of CNT/AgNW films at different ratios. The different ratios are (a) and (b) 1:10, (c) 2:10, (d) 0.5:10, (e) 0.25:10, and (f) 1:15.

The corresponding optical transmittance and sheet resistance of CNT/AgNW-PET films of several different ratios are shown in Figure 3. It can be seen that most of the films have a constant transmittance from 400 to 900 nm and low sheet resistance. When the adding amount of CNTs to AgNWs is approximately 0.25 to 2, the sheet resistance of hybrid films can reach approximately 20.9 to 53.9 Ω/□ with the optical transmittance of approximately 84 to 91% at λ = 550 nm (T550). Too much addition of CNTs or AgNWs would affect the sheet resistance and transmittance of hybrid films because of the absorption of visible light by CNTs and reflection by AgNWs [31]. Meanwhile, we note that when the amount of AgNWs is fixed and with the increase of CNTs from 0.5 to 2, the optical transmittance and sheet resistance of AgNW film have a relatively small change, while the amount of CNTs is fixed and with the increase of AgNWs from 5 to 20, the optical transmittance and sheet resistance of AgNW film have a distinct decrease simultaneously, so it can be concluded that the AgNW network plays a major part for the optical transmittance and sheet resistance of CNT/AgNW-PET films, while the CNT network just plays an assistant role.
Figure 3

Optical transmittance and sheet resistance of CNT/AgNW-PET films by pressing-transfer process, a blank PET substrate was the reference.

For practical applications such as displays and solar cells, low roughness and enhanced adhesion are also always required [4145]. In our study, these requirements were realized by second mechanical pressing at room temperature. Figure 4a shows the SEM image of a CNT/AgNW-PET film after pressing at 10 MPa for 30 s. The compressed, closely contact points between CNTs and/or AgNWs can be seen distinctly, and it will be beneficial for strong adhesion, low roughness, and junction resistance. As a consequence, the AFM images of the CNT/AgNW-PET film before and after second pressing in Figure 4b,c show that the surface roughness decreases greatly from 97.6 to 28.1 nm after second mechanical pressing. Adhesion tests were implemented by 3M sticky tape. Although it is enough for the hybrid film to reduce the junction resistance under 3 MPa, and second mechanical pressing has little effect on the transmittance and sheet resistance of the hybrid film as shown in Figure 5, we note that comparing with those without second pressing the hybrid film after second mechanical pressing has stronger adhesion to the PET substrate, and we tried to peel off the CNT/AgNW film from the PET substrate using 3M sticky tape by firmly attaching it on the surface of the CNT/AgNW film, but the film remained on the PET without visible change indicating its strong adhesion between CNTs/AgNWs and substrate. Meanwhile, from the results of Rs and T550 of the CNT/AgNW film before and after adhesion test, the Rs of the film without second pressing increases rapidly from 20.9 to 117 Ω/□; the T550 also changes from 87% to 91%. While with second pressing the Rs just increases from 20.4 to 22.3 Ω/□, the T550 changes from 85% to 85.5%. Therefore, we believe that the main role of the second mechanical pressing is reinforcing the adhesion force between CNTs, AgNWs, and PET substrate except for reducing surface roughness. To compare the effect of second pressing with traditional heating process [46], a film of pressing transfer without second pressing was heated at 120°C and also tested by 3M sticky tape as shown in film 2 of Figure 5. The Rs and T550 of film 2 by heating process decrease from 41 to 32 Ω/□ and 90% to 86%, respectively, while the Rs of the heated film after adhesion test rises dramatically to 198 Ω/□, which means that the heating process plays a role not as much as second mechanical processing for adhesion enhancement. Furthermore, comparing with other reported results, e.g., AgNW film with Rs approximately 20 Ω/□ and T550 approximately 80% prepared via meyer rod coating and pressing under 18 GPa by Cui's group [31], AgNWs film with Rs approximately 8.6 Ω/□ and T550 approximately 80% prepared via drop-coating and mechanical pressing under 25 MPa by Noji's group [45], and AgNW/CNT film with Rs approximately 17 Ω/□ and excellent stretchable property, but no T information prepared via vacuum filtration and plasmonic welding process by Woo and co-workers [35], our results and this simple technique have an obvious advantage and potential to be applied to practice from the economic and practical point of view.
Figure 4

SEM and AFM images of CNT/AgNW-PET film and CNT/AgNW network. (a) SEM image of CNT/AgNW-PET film pressed at 10 MPa for 30 s; AFM images of the CNT/AgNW network (b) before and (c) after second pressing.

Figure 5

R s and T 550 of CNT/AgNW films before/after second mechanical pressing, adhesion test (3M sticky tape), and heating (120°C).

Conclusions

CNT/AgNW-PET flexible transparent conductive films were fabricated by mechanical pressing-transfer process at room temperature. AgNWs form the main conductive networks, and CNTs as the assistant conductive networks are filled in the open spaces of the AgNWs networks; both of them have good connections, and the sheet resistance of the hybrid films reaches approximately 20.9 to 53.9 Ω/□ with the optical transmittance of approximately 84 to 91%. The second mechanical pressing step can greatly reduce the surface roughness of the hybrid film and reinforce the adhesion force between CNTs, AgNWs, and PET substrate. This process is more hopeful to be used in practical production of flexible transparent conductive films compared with traditional heating-treatment process.

Declarations

Acknowledgements

The authors wish to acknowledge the financial support of the Priority Academic Program Development of Jiangsu Higher Education(1033000003), the National Natural Science Foundation of China (51274106), the Science and Technology Support Program of Jiangsu Province (BE2012143, BE2013071), the Natural Science Research Program of Jiangsu Province Higher Education (12KJA430001, 14KJB430010), the Chinese Postdoctoral Foundation (2013 M531280), and the Talents Foundation of Jiangsu University (12JDG073).

Authors’ Affiliations

(1)
Institute for Advanced Materials, Jiangsu University

References

  1. Yim JH, Joe S, Pang C, Lee KM, Jeong H, Park JY, Yeong Ahn H, Mello JC, Lee S: Fully solution-processed semitransparent organic solar cells with a silver nanowire cathode and a conducting polymer anode. ACS Nano 2014, 8(3):2857–2863. 10.1021/nn406672nView ArticleGoogle Scholar
  2. Ham J, Kim S, Jung GH, Dong WJ, Lee JL: Design of broadband transparent electrodes for flexible organic solar cells. J Mater Chemist A 2013, 1: 3076–3082. 10.1039/c2ta00946cView ArticleGoogle Scholar
  3. Mayousse C, Celle C, Moreau E, Mainguet JF, Carella A, Simonato JP: Improvements in purification of silver nanowires by decantation and fabrication of flexible transparent electrodes. Application to capacitive touch sensors. Nanotechnology 2013, 24(21):215501. 10.1088/0957-4484/24/21/215501View ArticleGoogle Scholar
  4. Ham J, Lee JL: ITO breakers: highly transparent conducting polymer/metal/dielectric (P/M/D) films for organic solar cells. Adv Energy Mater 2014, 4: 11–15.Google Scholar
  5. Li XS, Zhu YW, Cai WW, Borysiak M, Han BY, Chen D, Piner RD, Colombo L, Ruoff RS: Transfer of large-area graphene films for high-performance transparent conductive electrodes. Nano Lett 2009, 9(12):4359–4363. 10.1021/nl902623yView ArticleGoogle Scholar
  6. Wu J, Agarwal M, Becerril HA, Bao Z, Liu Z, Chen Y, Peumans P: Organic light-emitting diodes on solution processed graphene transparent electrodes. ACS Nano 2010, 4: 43–48. 10.1021/nn900728dView ArticleGoogle Scholar
  7. Yu Z, Zhang Q, Li L, Chen Q, Niu X, Liu J, Pei Q: Highly flexible silver nanowire electrodes for shape-memory polymer light-emitting diodes. Adv Mater 2011, 23: 664–668. 10.1002/adma.201003398View ArticleGoogle Scholar
  8. Noh YJ, Kim SS, Kim TW, Na SI: Cost-effective ITO-free organic solar cells with silver nanowire–PEDOT:PSS composite electrodes via a one-step spray deposition method. Solar Energy Mater Solar Cells 2014, 120: 226–230.View ArticleGoogle Scholar
  9. Noh YJ, Kim SS, Kim TW, Na SI: Effect of sheet resistance of Ag-nanowire-based electrodes on cell-performances of ITO-free organic solar cells. Semicond Sci Technol 2013, 28: 125008. 10.1088/0268-1242/28/12/125008View ArticleGoogle Scholar
  10. Minami T: Transparent conducting oxide semiconductors for transparent electrodes. Semicond Sci Technol 2005, 20: S35-S44. 10.1088/0268-1242/20/4/004View ArticleGoogle Scholar
  11. Oliva J, Papadimitratos A, Rosa E, Zakhidov A: Semi-transparent polymer light emitting diodes with multiwall carbon nanotubes as cathodes. Physica status solidi A in press in pressGoogle Scholar
  12. Hu LB, Hecht DS, Gruner G: Carbon nanotube thin films: fabrication, properties, and applications. Chem Rev 2010, 110: 5790–5844. 10.1021/cr9002962View ArticleGoogle Scholar
  13. De S, Coleman JN: Are there fundamental limitations on the sheet resistance and transparent of thin graphene films? ACS Nano 2010, 4: 2713–2720. 10.1021/nn100343fView ArticleGoogle Scholar
  14. Zheng QB, Li ZG, Yang JH, Kim JK: Graphene oxide-based transparent conductive films. Progress in Mater Sci 2014, 64: 200–247.View ArticleGoogle Scholar
  15. Tung VC, Chen LM, Allen MJ, Wassei JK, Nelson K, Kaner RB, Yang Y: Low-temperature solution processing of graphene-carbon nanotube hybrid materials for high-performance transparent conductors. Nano Lett 2009, 9: 1949–1955. 10.1021/nl9001525View ArticleGoogle Scholar
  16. Wu H, Hu LB, Rowell MW, Kong DS, Cha JJ, McDonough JR, Jia Z, Yang Y, McGehee MD, Cui Y: Electrospun metal nanofiber webs as high-performance transparent electrode. Nano Lett 2010, 10: 4242–4248. 10.1021/nl102725kView ArticleGoogle Scholar
  17. Azulai D, Belenkova T, Gilon H, Barkay Z, Markovich G: Transparent metal nanowire thin films prepared in mesostructured templates. Nano Lett 2009, 9: 4246–4249. 10.1021/nl902458jView ArticleGoogle Scholar
  18. Lyons PE, De S, Elias J, Schamel M, Philippe L, Bellew AT, Boland JJ, Coleman JN: High-performance transparent conductors from networks of gold nanowires. J Phys Chem Lett 2011, 2: 3058–3062. 10.1021/jz201401eView ArticleGoogle Scholar
  19. Coskun S, Ates ES, Unalan HE: Optimization of silver nanowire networks for polymer light emitting diode electrodes. Nanotechnology 2013, 24: 125202. 10.1088/0957-4484/24/12/125202View ArticleGoogle Scholar
  20. Mahajan A, Francis L, Frisbie CD: Facile method for fabricating flexible substrates with embedded, printed silver lines. ACS Appl Mater Interfaces 2014, 6: 1306–1312. 10.1021/am405314sView ArticleGoogle Scholar
  21. Im HG, Jin J, Ko JH, Lee J, Lee JY, Bae BS: Flexible transparent conducting composite films using a monolithically embedded AgNW electrode with robust performance stability. Nanoscale 2014, 6: 711–715. 10.1039/c3nr05348bView ArticleGoogle Scholar
  22. Huang GW, Xiao HM, Fu SY: Paper-based silver-nanowire electronic circuits with outstanding electrical conductivity and extreme bending stability. Nanoscale 2014, 6: 8495–8502. 10.1039/C4NR00846DView ArticleGoogle Scholar
  23. Kumar ABVK, Bae CW, Piao LH, Kim SH: Silver nanowire based flexible electrodes with improved properties: high conductivity, transparency, adhesion and low haze. Mater Res Bulletin 2013, 48: 2944–2949. 10.1016/j.materresbull.2013.04.035View ArticleGoogle Scholar
  24. Sachse C, Weiß N, Gaponik N, Müller-Meskamp L, Eychmüller A, Leo K: ITO-free, small-molecule organic solar cells on spray-coated copper-nanowire-based transparent electrodes. Adv Energy Mater in press in pressGoogle Scholar
  25. Rathmell AR, Wiley BJ: The synthesis and coating of long, thin copper nanowires to make flexible, transparent conducting films on plastic substrates. Adv Mater 2011, 23: 4798–4803. 10.1002/adma.201102284View ArticleGoogle Scholar
  26. Li SJ, Chen YY, Huang LJ, Pan DC: Large-scale synthesis of well-dispersed copper nanowires in an electric pressure cooker and their application in transparent and conductive networks. Inorganic Chem 2014, 53: 4440–4444. 10.1021/ic500094bView ArticleGoogle Scholar
  27. Cheng Y, Wang S, Wang R, Sun J, Gao L: Copper nanowire based transparent conductive films with high stability and superior stretchability. J Mater Chem C 2014, 2: 5309–5316. 10.1039/c4tc00375fView ArticleGoogle Scholar
  28. Azuma K, Sakajiri K, Matsumoto H, Kang S, Watanabe J, Tokita M: Facile fabrication of transparent and conductive nanowire networks by wet chemical etching with an electrospun nanofiber mask template. Mater Lett 2014, 115: 187–189.View ArticleGoogle Scholar
  29. Eom H, Lee J, Pichitpajongkit A, Amjadi M, Jeong JH, Lee E, Lee JY, Park I: Ag@Ni core–shell nanowire network for robust transparent electrodes against oxidation and sulfurization. Small in press in pressGoogle Scholar
  30. Stewart IE, Rathmell AR, Yan L, Ye SR, Flowers PF, You W, Wiley BJ: Solution-processed copper–nickel nanowire anodes for organic solar cells. Nanoscale 2014, 6(11):5980–5988. 10.1039/c4nr01024hView ArticleGoogle Scholar
  31. Hu LB, Kim HS, Lee JY, Peumans P, Cui Y: Scalable coating and properties of transparent, flexible, silver nanowire electrodes. ACS Nano 2010, 4: 2955–2963. 10.1021/nn1005232View ArticleGoogle Scholar
  32. Kholmanov IN, Domingues SH, Chou H, Wang XH, Tan C, Kim JY, Li HF, Pine R, Zarbin AJG, Ruoff RS: Reduced graphene oxide/copper nanowire hybrid films as high-performance transparent electrodes. ACS Nano 2013, 7: 1811–1816. 10.1021/nn3060175View ArticleGoogle Scholar
  33. Hsiao ST, Tien HW, Liao WH, Wang YS, Li SM, Ma CC, Yu YH, Chuang WP: A highly electrically conductive graphene–silver nanowire hybrid nanomaterial for transparent conductive films. J Mater Chem C 2014, 2: 7284–7291. 10.1039/C4TC01217HView ArticleGoogle Scholar
  34. Tien HW, Hsiao ST, Liao WH, Yu YH, Lin FC, Wang YS, Li SM, Ma CCM: Using self-assembly to prepare a graphene-silver nanowire hybrid film that is transparent and electrically conductive. Carbon 2013, 58: 198–207.View ArticleGoogle Scholar
  35. Woo JY, Kim KK, Lee J, Kim JT, Han CS: Highly conductive and stretchable Ag nanowire/carbon nanotube hybrid conductors. Nanotechnology 2014, 25: 285203. 10.1088/0957-4484/25/28/285203View ArticleGoogle Scholar
  36. Choi DY, Kang HW, Sung HJ, Kim SS: Annealing-free, flexible silver nanowire-polymer composite electrodes via a continuous two-step spray-coating method. Nanoscale 2013, 5: 977–983. 10.1039/c2nr32221hView ArticleGoogle Scholar
  37. Kiran Kumar ABV, Jiang JW, Bae CW, Seo DM, Piao LH, Kim SH: Silver nanowire/polyaniline composite transparent electrode with improved surface properties. Mater Res Bulletin 2014, 57: 52–57.View ArticleGoogle Scholar
  38. Amjadi M, Pichitpajongkit A, Lee S, Ryu S, Park I: Highly stretchable and sensitive strain sensor based on silver nanowire-elastomer nanocomposite. ACS Nano 2014, 8: 5154–5163. 10.1021/nn501204tView ArticleGoogle Scholar
  39. Kim YS, Chang MH, Lee EJ, Ihm DW, Kim JY: Improved electrical conductivity of PEDOT-based electrode films hybridized with silver nanowires. Synthetic Metals 2014, 195: 69–74.View ArticleGoogle Scholar
  40. Morgenstern FSF, Kabra D, Massip S, Brenner TJK, Lyons PE, Coleman JN, Friend RH: Ag-nanowire films, coated with ZnO nanoparticles as a transparent electrode for solar cells. Appl Phys Lett 2011, 99: 183307. 10.1063/1.3656973View ArticleGoogle Scholar
  41. Park J, Kim M, Shin JB, Choi KC: Transparent chromatic electrode using the mixture of silver nanowire and silver nanoprism. Current Appl Phys 2014, 14: 1005–1009. 10.1016/j.cap.2014.05.006View ArticleGoogle Scholar
  42. Khaligh HH, Goldthorpe IA: Hot-rolling nanowire transparent electrodes for surface roughness minimization. Nanoscale Res Lett 2014, 9: 310. 10.1186/1556-276X-9-310View ArticleGoogle Scholar
  43. Lee J, Lee I, Kim TS, Lee JY: Efficient welding of silver nanowire networks without post-processing. Small 2013, 9: 2887–2894. 10.1002/smll.201203142View ArticleGoogle Scholar
  44. Hauger TC, Al-Rafi SMI, Buriak JM: Rolling silver nanowire electrodes: simultaneously addressing adhesion, roughness, and conductivity. ACS Appl Mater Interfaces 2013, 5(23):12663–12671. 10.1021/am403986fView ArticleGoogle Scholar
  45. Tokuno T, Nogi M, Karakawa M, Jiu JT, Nge TT, Aso Y, Suganuma K: Fabrication of silver nanowire transparent electrodes at room temperature. Nano Res 2011, 4(12):1215–1222. 10.1007/s12274-011-0172-3View ArticleGoogle Scholar
  46. Madaria AR, Kumar A, Ishikawa FN, Zhou CW: Uniform, highly conductive, and patterned transparent films of a percolating silver nanowire network on rigid and flexible substrates using a dry transfer technique. Nano Res 2010, 3: 564–573. 10.1007/s12274-010-0017-5View ArticleGoogle Scholar

Copyright

© Jing et al.; licensee Springer. 2014

This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly credited.

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