Open Access Article
This Open Access Article is licensed under a Creative Commons Attribution-Non Commercial 3.0 Unported Licence

Reduced graphene oxide-polyaniline film as enhanced sensing interface for the detection of loop-mediated-isothermal-amplification products by open circuit potential measurement

Vu Thi Thuab, Bui Quang Tiencd, Dau Thi Ngoc Ngaab, Ly Cong Thanhce, Le Hoang Sinhf, Tu Cam Leg and Tran Dai Lam*bc
aUniversity of Science and Technology of Hanoi (USTH), Vietnam Academy of Science and Technology (VAST), 18 Hoang Quoc Viet, Cau Giay, Hanoi, Vietnam
bCenter for High Technology Development (HTD), Vietnam Academy of Science and Technology (VAST), 18 Hoang Quoc Viet, Cau Giay, Hanoi, Vietnam. E-mail: trandailam@gmail.com
cGraduate University of Science and Technology (GUST), Vietnam Academy of Science and Technology (VAST), 18 Hoang Quoc Viet, Cau Giay, Hanoi, Vietnam
dMilitary Academy of Logistics, Ngoc Thuy, Long Bien, Hanoi, Vietnam
eHanoi University of Pharmacy, 15-17 Le Thanh Tong, Hoan Kiem, Hanoi, Vietnam
fDuy Tan University, 03 Quang Trung, Da Nang, Vietnam
gSchool of Engineering, RMIT University, GPO Box 2476, Melbourne, VIC 3001, Australia

Received 12th May 2018 , Accepted 11th July 2018

First published on 16th July 2018


Abstract

The development of low cost, portable diagnostic tools for in-field detection of viruses and other pathogenic microorganisms is in great demand but remains challenging. In this study, a novel approach based on reduced graphene oxide-polyaniline (rGO-PANi) film for the in situ detection of loop-mediated-isothermal-amplification (LAMP) products by means of open circuit potential measurement is proposed. The pH-sensitive conducting polymer PANi was electro-deposited onto rGO coated screen printed electrodes and tuned to be at the emeraldine state at which the pH sensitivity was maximized. By combining PANi and rGO, the pH sensitivity of the system was modulated up to about −64 mV per pH unit. This enabled the number of amplified amplicons resulting from the isothermal amplification process to be monitored. The sensor was then examined for monitoring LAMP reactions using Hepatitis B virus (HBV) as a model. This simple, low-cost, reproducible and sensitive interfacing layer is expected to provide a new possibility for designing point-of-care sensors under limited-resource conditions.


Introduction

There is currently a great need for developing portable diagnostic tools for in-field detection of viruses and other pathogenic microorganisms in resource-limited settings. These platforms offer many advantages for detection of various pathogens including portability, automation, speed, cost, and efficiency.1 In order to achieve highly sensitive and early target detection, the molecular amplification technologies should be integrated onto such diagnostic tools. Loop-mediated isothermal amplification (LAMP) is one of the most advanced genetic techniques that can provide extremely fast sequential progression (less than 1 hour)2 and relatively high selectivity (100-fold greater than conventional PCR3). Using this technique, the gene amplification is performed under isothermal conditions within a short diagnostic time using six gene regions, and only one type of enzyme (Bst polymerase).4,5 To monitor the amplification process in LAMP reactions, optical aids such as turbidity, fluorescence, and pH sensitive dyes, using which the by-product of LAMP reactions (magnesium pyrophosphate) can be recorded, are employed to determine the amplification degree.6,7 Several works have also reported the use of the electrochemiluminescence technique for quantification of LAMP products.8,9 Nevertheless, the use of such optical detectors seems to be not suitable to comply with requirements of in-field diagnostic microchips such as low-cost, flexibility, portability and integration ability.

During the last decade, a number of LAMP-based microchips with electrochemical analysis of amplicons has been reported. Several works described the electrochemical record of the LAMP reaction process by monitoring the intercalation of DNA-binding redox reporter molecules (i.e., methylene blue10) into newly formed amplicons. Other research groups have demonstrated the voltammetric detection of the amount of deoxynucleotide triphosphates (dNTPs) consumed during reaction.11 Recently, the pH decrease caused by pyrophosphated protons released during LAMP reaction has also been utilized as an indicator for electrochemical analysis of amplicons. For instance, Gosselin et al. has developed potentiometric sensor based on polyaniline film to continuously monitor the pH of the solution during the LAMP amplification.12 The linear calibration of the potentiometric pH measurement, with a slope of −83 mV per pH unit was reported. In previously reported electrochemical detection methods, the output signals are strongly affected by the precipitation of by-products during LAMP reactions. In some cases, different redox molecules must be put in the reaction solution. This can lead to certain side-effects which inhibit sequential process. Therefore, monitoring the number of amplicons using pH change during LAMP reactions is more advantageous.

To sense the pH of the reaction solution, a pH-sensitive thin film should be used. In the case of electrochemical sensing of pH, this thin film must satisfy two critical requirements: high sensitivity to H+ or OH ions; and high conductivity. The pH-sensitive conducting polymer (i.e. polyaniline) meet these criteria.12,13 In the literature, it is well-known that polyaniline is a pH-sensitive film with the response of about several tens millivolts per pH unit at room temperature. The pH sensitivity of polyaniline is due to the proton doping (protonation) and dedoping (deprotonation) of the conducting oxidative state, namely emeraldine. It was reported that polyaniline has the highest potentiometric response to pH variation compared to other conducting polymers.14 Our research group has demonstrated the use of polyaniline films to monitor ion concentrations in different sensing configurations and as a pH-sensitive matrix for immobilizing enzymes.15 Lalit Kumar et al. deposited polyaniline films on flexible substrates for ammonia gas sensor16 while a high-performance flexible pH sensor based on polyaniline nanopillar array defined by soft lithography was reported by Yoon et al.17 However, polyaniline is more conductive at pH less than 5.0 and become less conductive at higher pH range.

To improve the conductivity of polyaniline film at pH range of LAMP reactions (7.0–9.0), carbonaceous materials are top candidates. With their specific electronic structures, graphene and its derivatives offer a superior conductivity and mechanical flexibility that are often required for disposable electrochemical sensing systems. In addition, these materials are biocompatible. A potentiometric pH sensor based on carbon-polyaniline composite was recently developed using direct laser writing for wearable point-of-care applications.18 Compared to graphene, reduced graphene oxide has similar behaviors including high conductivity, large surface area, and easy functionalization. They can be easily produced via chemical routes with low-cost and high yield.19 The reduced form of graphene oxide (rGO) also has abundant oxygen moieties and can improve the pH sensitivity of polyaniline film.20 A pH sensor based on polyaniline functionalized by reduced graphene oxide (PANi-rGO) for monitoring microbial fermentation process has been reported.21 PANi-rGO composite was also shown to have high electrical conductivity and capacitance for efficient electrochemical supercapacitors.22

In this work, we demonstrate the use of the highly-sensitive PANi and highly-conductive rGO films to fabricate the device for monitoring pH changes during genetic amplification in LAMP reactions. The film was first fabricated through electrochemical reduction of drop-casted graphene oxide, and followed by electro-deposition of PANi in acidic solution. The Open Circuit Potential (OCP) measurements were utilized for end-point detection of number of amplified amplicons. It should be emphasized that the measurement of the OCP is highly sensitive and reproducible. Indeed, although such a detection of LAMP products has been shown previously with potentiometric measurement,12 however, this method could trigger significant oxidation state change of PANi during current/potential imposition measurement, leading to inaccurate signals. By contrast, our OCP technique should provide a simpler and more accurate detection procedure since it can be done without any application of neither potential nor current to the system. Thus, subsequent and multiple measurements could be assured and unambiguously interpreted, without film damage.

Experimental

Chemicals

Graphene oxide (GO) was prepared from graphite powder using a modified version of the Hummer's method. Aniline (C6H5NH2) was purchased from Sigma Aldrich (USA). Phosphate buffered saline (PBS, pH 7.4) buffer was employed as the supporting electrolyte. All chemicals were of analytical grade and used without further purification, and redistilled water was used throughout. Screen printed carbon electrodes (SPE) with a three-electrode setup (diameter of working electrode is 3 mm) were purchased from Quasense (Thailand). LAMP amplification reagent (Loopamp DNA amplification kit) was provided by Eiken (Japan).

A set of six primers was designed according to literature to specifically target HBV in human blood. The primer set consisted of two outer primers (F3, B3), two inner primers (FIP, BIP), and two loop primers (LF, LB).23 All primers were commercially synthesized by Macrogen (Seoul, Korea).

Preparation of rGO/PANi films

The pH-sensitive sensor based on rGO-PANi was prepared on SPE electrode. Firstly, the graphene oxide (1 mg ml−1) was drop-casted onto the electrode. After that, the film was electrochemically reduced by cyclic voltammetry method with potential ranging from 0 V to −1.2 V for several cycles. Finally, polyaniline was electro-deposited by sweeping SPE‖rGO electrode in 0.5 M H2SO4 solution containing 0.3 M aniline for 10 cycles from −200 mV to +900 mV.

The surface morphology of the electrodes was characterized using a Hitachi S-4800 field emission scanning electron microscopy (FE-SEM) at acceleration voltage of 5 kV. Attenuated total reflectance Fourier transform Infrared Spectra (ATR-FTIR) of the samples were examined using IR-Tracer 100 (Shimadzu, Japan) and the samples were scanned between 500 and 4000 cm−1. The crystallinity of the prepared samples were determined by Raman spectroscopy in the spectral range 300–3500 cm−1 using 532 nm excitation source on a Horiba spectrometer.

pH test

The pH calibration measurements were conducted using PBS buffers with adjusted pH of 6.0–9.0. These buffers were used to measure the open circuit voltage (OCP) variation of the working electrode vs. Ag/AgCl reference electrode due to the pH change. All experiments were conducted at room temperature. All measurements were conducted on a PC-controlled Metrohm Autolab PGSTAT 302N electrochemical workstation (Metrohm Co., Ltd., Switzerland).

LAMP reaction

The LAMP mixture was prepared as described in our previous work.23 The phage DNA was diluted with PBS buffer (pH 7.4) to the concentration of 10 ng μl−1. A reaction mixture (25 μl) is consisted of 1.6 μM of the FIP and BIP primers, 0.8 μM of each outer primer (F3 primer and B3 primer), 0.8 μM of each loop primer (LPF primer and LPB primer), reaction mix (12.5 μl), Bst DNA polymerase (1 μl), and 5 μl sample. The LAMP reaction was conducted at 65 °C and then stopped at 84 °C after several intervals of time (0, 10, 20, 30, 40, 60 min). The number of amplified amplicons was recorded using OCP measurements in which no current occurred in the electrochemical cell. The LAMP products were also analyzed qualitatively by gel-electrophoresis technique in a 2% agarose gel. The exact concentration of DNA at every reaction step was determined using Nanodrop after the purification of DNA solution.

Results and discussion

Preparation of rGO-PANi film

Electro-deposition provides an efficient and versatile route for the synthesis of nanostructured polymers and their composites.24 In this work, the rGO-PANi film was prepared by the electro-polymerization of aniline (0.3 M) in 0.5 M H2SO4 solution on the surface of the rGO modified SPE. As seen from Fig. 1(a) which shows reduction of drop-casted graphene oxide material, an intense reduction peak is present at around – 1000 mV with the onset potential of −900 mV during the 1st cycle of cyclic voltammetry of graphene oxide. In the subsequent cycles, the intensity of the reduction peak decreases dramatically (Fig. 1S). Meanwhile, there are no anodic peaks for all cycles. This demonstrates the irreversible transition in which graphene oxide was converted completely into its reduced form.21 The cyclic voltammograms recorded during the electrodeposition of PANi onto rGO film is shown in Fig. 1(b). The continuous increase of current density has indicated the growth of PANi over the rGO surface.24 The transition between different oxidation states of polyaniline was also observed during deposition process (more details in Fig. 2S). As seen on cylic voltammograms in Fig. 1b, the first anodic wave situated at +225 mV (vs. Ag/AgCl) indicates transition of leucoemeraldine form of polyaniline to emeraldine salt while the second anodic wave occurred at +565 mV (vs. Ag/AgCl) denotes formation of fully doped perningraniline salt.20 The final scan was stopped at 0 V to obtain emeraldine – the only conductive form of polyaniline.14,16
image file: c8ra04050h-f1.tif
Fig. 1 Preparation of rGO-PANi film. (a) Electro-reduction of graphene oxide coated SPE: the drop-casted graphene oxide film was electrochemically reduced by sweeping in PBS solution (pH 7.4) at scan rate of 50 mV s−1 for several scans. (b) Electro-deposition of polyaniline onto SPE/rGO: the SPE/rGO electrode film was electrochemically modified by sweeping in 0.5 M H2SO4 solution containing 0.3 M aniline at scan rate of 50 mV s−1 for ten scans.

Structure and morphology of rGO-PANi film

Surface morphology of the rGO film and rGO-PANi film were characterized by FE-SEM (Fig. 2). As can be seen from Fig. 2(a), the rGO ‘wrinkles’ are present with random distribution on the electrode surface. Meanwhile, the polyaniline film was found to be in a microporous interconnected network (Fig. 2(b)) which is beneficial for electron transport at the electrolyte–electrode interface.25,26 The size of micropores was in the range of 0.3–0.9 μm. The very thin graphitic layer was completely hidden by the relatively uniform and thick polymeric film (∼110 nm) and cannot be seen by electron microscopy. Therefore, ATR-FTIR and Raman techniques were used to confirm the formation of rGO-PANi film and provide deeper insights on the structure of the composite material.
image file: c8ra04050h-f2.tif
Fig. 2 SEM images of rGO (a) and rGO-PANi (b) films. The polyaniline film was found to be in a microporous interconnected network with the size of micropores was in the range of 0.3–0.9 μm. The very thin graphitic layer was completely hidden by the relatively uniform and thick polymeric film (∼110 nm) and cannot be seen by electron microscopy.

The ATR-FTIR spectrum of rGO (Fig. 3) reaveals the presence of C[double bond, length as m-dash]C stretching (1400–1600 cm−1) and the disappearance of –C[double bond, length as m-dash]O (∼1700 cm−1) and –C–O– (∼1010 cm−1) stretching of the carboxylic and epoxide group. This result indicates that most of oxygen containing groups on the drop-casted graphene oxide material were eliminated. At the same time, the characteristic bands of the emeraldine structure were clearly obtained on rGO/PANi film after electrodepositing process (Fig. 3): 1564 and 1491 cm−1 (C[double bond, length as m-dash]C stretch), 1298 cm−1 (C–N stretch), 1134 cm−1 (C[double bond, length as m-dash]N), 797 cm−1 (C–H).16


image file: c8ra04050h-f3.tif
Fig. 3 ATR-FTIR spectra of rGO (black) and rGO-PANi (red) films. For rGO: 1400–1600 cm−1 (C[double bond, length as m-dash]C stretching), 1010 cm−1 (–C–O–). For rGO/PANi: 1564 and 1491 cm−1 (C[double bond, length as m-dash]C stretch), 1298 cm−1 (C–N stretch), 1134 cm−1 (C[double bond, length as m-dash]N), 797 cm−1 (C–H).

Fig. 4 exhibits Raman spectra of rGO and rGO-PANi films. The peaks at 1335 cm−1, 1581 cm−1, 2686 cm−1 are ascribed to typical D, G, and 2D Raman bands of graphitic material, respectively.27 The D band is related to the defects, edges and structural disorders of solid carbon whilst the G band is associated with the first-order scattering of E2g mode of sp2 hybridized carbon. The intensity ratio ID/IG is an effective indicator of the transition between GO and rGO. Here, the Raman spectrum (Fig. 4(a)) of rGO after electrochemical reduction shows a ID/IG ratio of 0.946, significantly higher than that value for GO of 0.803. This indicates that there is an increase in the number of defect sites caused by the removal of the functional groups from GO,21 and the GO material was electrochemically reduced into rGO. When there is polyaniline electrodeposited on rGO, the positions of the above peaks (Fig. 4(b)) are slightly shifted to longer wavenumbers of 1337 cm−1, 1585 cm−1 and 2760 cm−1. The other Raman peaks located at 812, 1164, 1244, 1403, 1483 cm are consistent with amine deformation (benzoid), C–H in-plane bending (benzoid), C–N+ prontonated amine stretching (quinoid), C–C stretching (quinoid), and N–H bending (quinoid), respectively (Fig. 4(b)).24


image file: c8ra04050h-f4.tif
Fig. 4 Raman spectra rGO (a) and rGO-PANi (b) films.

pH test

The pH response for rGO/PANi film was tested by measuring the OCP potentials at different pH values (6.0–9.0) as depicted in Fig. 5(a). It was found that the OCP value decreased with increasing pH. Two linear regions were obtained at pH ranging from 6.0 to 7.5 and pH ranging from 7.5 to 9.0 with the following regression equations:
OCP = 389.8803 − 64.1524 × pH (R2 = 0.9831) (pH = 6.0–7.5)

OCP = 78.8339 − 23.1149 × pH (R2 = 0.9598) (pH = 7.5–9.0)

image file: c8ra04050h-f5.tif
Fig. 5 (a) pH calibration curve of SPE/rGO-PANi electrode. The equilibrium potential increases with decreasing pH due to the protontation of emeraldine base form of polyaniline. pH range 6.0–9.0 (buffered PBS solution). (b) Schematic diagram demonstrating the pH-sensitive mechanism of SPE/rGO-PANi electrode.

The voltage drift caused by pH change of rGO-PANi film is of −64 mV per pH unit which is comparable to those obtained from other polyaniline-based sensors in previously reported works.12,18,19 Depending on the fabrication process of the electrodes, the slope of the calibration curves ranges from −55 to −90 mV per pH unit. Compared to pristine polyaniline film (Fig. 4S), the composite rGO-PANi exhibits a steeper slope of OCP-pH response curve, probably resulting from high conductivity of rGO material. Indeed, the electron transfer was found be faster when rGO was deposited on the electrode (Fig. 5S). Further improvement in the slope of potential–pH curve can be performed with the use of derivatives of polyaniline.20

The pH response mechanism of polyaniline-based sensors depends on the transistion from the emeraldine salt to the emeraldine base as documentated in the literature.14 It is generally agreed that PANi exists in three different base forms: leucoemeraldine (colorless, fully reduced, poor conducting), emeraldine (green, half-oxidized, conducting), and pernigranline (dark, fully oxidized, poor conducting).20 The only electrically conducting form is the emeraldine which can suffer from reversible protonation process (Fig. 5(b)) and is therefore sensitive to the acidic/alkalic degree of the solution.28 This is also the reason why we stopped the electro-deposition of polyaniline film at 0 mV. As the pH increases, the ions in the top-layers of the polymer chains will be transferred to the electrolyte solution during deprotonation process (dedoping). In contrast, the anions in the electrolyte solution can act as charge compensating ions in the protonation process (doping) as the pH decreases. Consequently, the OCP will decrease with increasing pH and vice versa. This behavior was also found in other polymers but the highest potentiometric response was reported for polyaniline.16

Notably, the protonation and deprotonation processes in polyaniline are reversible.16 It means that one can easily tune the transition between the emeraldine salt and the emeraldine base by shifting the pH of the solution. On the other hand, this p-type conducting polymer with dual pH sensitivity is sensitive with both negative and positive ions. Thus, our sensor should be reusable in principle. Indeed, we tried to transform emeraldine salt into emeraldine base by sweeping the used electrodes (previously incubated in alkaline electrolytes) in acidic solution without monomer. The experimental results have demonstrated the successful reform of emeraldine base but with a hysteresis (Fig. 6S).

LAMP reaction

The detection of LAMP products was conducted on rGO-PANi interface, by means of OCP measurement. The detection mechanism relies on the pH decrease caused by hydronium ions released during the elongation of DNA in LAMP reaction. Fig. 6(a) shows the normalized variation of the measured potential associated with positive and negative LAMP reactions. It was demonstrated that the OCP value increases with reaction time (27 mV over 40 minutes), indicating the increase in the number of amplicons and released protons. Meanwhile, an ignorable decrease in OCP values was found for negative sample (Fig. 6(a)). This demonstrates the high specificity of the sensor.
image file: c8ra04050h-f6.tif
Fig. 6 LAMP reactions: OCP detection (a), gel-electrophoresis (b) and absorbance measurements (c) of LAMP products.

These results are in good agreement with gel-electrophoresis and absorbance measurements. In Fig. 6(b), positive LAMP sample shows multiple bands of different sizes upon agarose gel electrophoresis. This is caused by inverted-repeat structures of LAMP products. At the same time, the DNA concentration was found to be increased about 103 – fold (as determined from absorbance spectra (Fig. 6(c))).

Conclusions

The pH sensitivity of the rGO-PANi interface was investigated and successfully applied for the detection of LAMP reactions by means of OCP measurement. The rGO ad-layer with high conductivity and intrinsic pH sensitivity has contributed to the overall enhanced sensitivity of the sensing interface. A reduction in OCP value of 27 mV was found for 102-times genetic amplification. The incorporation of a microfluidic flow system and microarray configuration will be carried out in further works for simultaneous detection of multiplex pathogens in point-of-care devices.

Conflicts of interest

There are no conflicts to declare.

Acknowledgements

This work acknowledges financial support from National Foundation of Science and Technology Development project, code: NAFOSTED 104.04-2014.36 (T.D.L).

References

  1. M. Zarei, Biosens. Bioelectron., 2018, 106, 193 CrossRef PubMed.
  2. T. Notomi, H. Oayama, H. Masubuchi, T. Yonekawa, K. Wanatabe, N. Amoni and T. Hase, Nucleic Acids Res., 2000, 28, 63e CrossRef.
  3. Q. D. Zhang, G. March, V. Noel, B. Piro, S. Reisberg, L. D. Tran, L. V. Hai, E. Abadia, P. E. Nielsen, C. Sola and M. C. Pham, Biosens. Bioelectron., 2012, 32, 163 CrossRef PubMed.
  4. T. Notomi, Y. Mori, N. Tomita and H. Kanda, J. Microbiol., 2015, 53, 1 CrossRef PubMed.
  5. M. Safavied, M. K. Kanakasanapathy, F. Tarlan, M. U. Admed, M. Zourob, W. Asghar and H. Shafiee, ACS Biomater. Sci. Eng., 2016, 2, 278 CrossRef PubMed.
  6. N. Tomita, Y. Mori, H. Kanda and T. Notomi, Nat. Protoc., 2008, 3, 877 CrossRef PubMed.
  7. T. Yoshikawa, T. Matsuo, Y. Kawamura, M. Ohashi, T. Yonekawa, H. Kanda, T. Notomi and M. Ihira, J. Virol. Methods, 2014, 201, 65 CrossRef PubMed.
  8. S. Roy, S. X. Wei, J. L. Z. Ying, M. Safavied and M. U. Admed, Biosens. Bioelectron., 2016, 86, 346 CrossRef PubMed.
  9. N. F. N. Azam, S. Roy, S. A. Lim and M. U. Admed, Food Chem., 2018, 248, 29 CrossRef PubMed.
  10. K. Hsieh, A. S. Patterson, B. S. Ferguson, K. W. Plaxco and H. T. Soh, Angew. Chem., Int. Ed., 2012, 124, 4980 CrossRef.
  11. K. Qu, Q. Li, Z. Cui, J. Zhao and X. Sun, Electroanalysis, 2011, 23, 2438 CrossRef.
  12. D. Gosselin, M. Gougis, M. Baque, M. N. Belgacem, D. Chaussy, A. G. Bourdat, P. Mailey and J. Berthier, Anal. Chem., 2017, 89, 10124 CrossRef PubMed.
  13. C. O. Baker, X. Huang, W. Nelson and R. B. B. Kaner, Chem. Soc. Rev., 2017, 46, 1510 RSC.
  14. A. A. Karyakin, O. A. Bobrova, L. V. Lukachova and E. E. Karyakina, Sens. Actuators, B, 1996, 33, 34 CrossRef.
  15. T. T. Cao, H. B. Nguyen, V. T. Nguyen, T. T. Vu, B. Maxime, P. Mattieu, L. S. Jean, B. T. Phan, D. L. Tran, N. M. Phan and V. C. Nguyen, Sens. Actuators, B, 2018, 260, 78 CrossRef.
  16. L. Kumar, I. Rawal, A. Kaur and S. Annapoorni, Sens. Actuators, B, 2017, 240, 408 CrossRef.
  17. J. H. Yoon, S. B. Hong, S. O. Yun, S. J. Lee, T. J. Lee, K. G. Lee and B. G. Choi, J. Colloid Interface Sci., 2017, 490, 53 CrossRef PubMed.
  18. R. Rahim, O. Manuel, T. Ali, K. Shahla, K. Ali and Z. Babak, ACS Appl. Mater. Interfaces, 2017, 9, 9015 CrossRef PubMed.
  19. A. A. Ambrosi, K. C. Chun, N. M. Latiff, A. H. Loo, C. H. A. Wong, A. Y. S. Eng, A. Bonanni and Ma. Pumera, Chem. Soc. Rev., 2016, 45, 2458 RSC.
  20. T. Lindfors and A. Ivaska, J. Electroanal. Chem., 2002, 531, 43 CrossRef.
  21. S. Chinnathambi and G. J. W. Euverink, Sens. Actuators, B, 2018, 264, 38 CrossRef.
  22. N. A. Kumar, H. J. Choi, Y. R. Shin, D. W. Chang, L. Dai and J. B. Baek, ACS Nano, 2012, 6, 1715 CrossRef PubMed.
  23. Q. T. Bui, T. N. Nguyen, T. L. Nguyen, T. T. Vu and D. L. Tran, J. Electron. Mater., 2017, 46, 3565 CrossRef.
  24. R. Sha, K. Komori and S. Badhulika, Electrochim. Acta, 2017, 233, 44 CrossRef.
  25. X. Mengli, S. Yonghai, Y. Yihan, G. Coucong, S. Yuan, W. Linyu and W. Li, Sens. Actuators, B, 2017, 252, 1187 CrossRef.
  26. S. Liang, W. Xiaoying, Y. Baiqin, W. Qian, T. Qianqian, J. Zhanyou and Z. Jing, Electrochim. Acta, 2017, 255, 286 CrossRef.
  27. A. C. Ferrari, J. C. Meyer, V. Scardaci, C. Casiraghi, M. Lazzeri, F. Mauri, S. Piscanec, D. Jiang, K. S. Novoselov, S. Roth and A. K. Geim, Phys. Rev. Lett., 2006, 97, 187401 CrossRef PubMed.
  28. A. Lewenstam, J. Bobacka and A. Ivaska, J. Electroanal. Chem., 1994, 368, 23 CrossRef.

Footnote

Electronic supplementary information (ESI) available. See DOI: 10.1039/c8ra04050h

This journal is © The Royal Society of Chemistry 2018
Click here to see how this site uses Cookies. View our privacy policy here.