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
First published on 16th July 2018
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.
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.
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).
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.
The ATR-FTIR spectrum of rGO (Fig. 3) reaveals the presence of CC stretching (1400–1600 cm−1) and the disappearance of –CO (∼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 (CC stretch), 1298 cm−1 (C–N stretch), 1134 cm−1 (CN), 797 cm−1 (C–H).16
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
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) |
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†).
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))).
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c8ra04050h |
This journal is © The Royal Society of Chemistry 2018 |