A highly sensitive gold nanoparticle bioprobe based electrochemical immunosensor using screen printed graphene biochip

Syazana Abdullah Limac, Hiroyuki Yoshikawab, Eiichi Tamiyab, Hartini Mohd Yasinc and Minhaz Uddin Ahmed*c
aEnvironmental and Life Sciences Programme, Faculty of Science, Universiti Brunei Darussalam, Jalan Tungku Link, Gadong, BE 1410, Brunei Darussalam
bNanobioengineering Laboratory, Department of Applied Physics, Graduate School of Engineering, Osaka University, 2-1 Yamada-oka, Suita, Osaka 565-0871, Japan
cBiosensors and Biotechnology Laboratory, Chemical Science Programme, Faculty of Science, Universiti Brunei Daruusalam, Jalan Tungku Link, Gadong, BE 1410, Brunei Darussalam. E-mail: minhaz.ahmed@ubd.edu.bn; minhazua@gmail.com; Tel: +673 888 4752

Received 24th September 2014 , Accepted 29th October 2014

First published on 29th October 2014


Abstract

This study describes a highly sensitive electrochemical immunosensor for the detection of human chorionic gonadotropin (hCG) that uses gold nanoparticles (AuNP) as the electrochemical label and graphene as electrode material. The primary antibody was first immobilized on the graphene working electrode surface by physical adsorption. Antigen hCG was then added and sandwiched with a secondary antibody labelled with AuNPs. After this, a series of sandwich-type immunoreactions were performed on the electrode, AuNPs were quantified by subjecting the immunocomplex to a preoxidation process of high potential at 1.2 V for 40 s and immediately reduced and scanned by differential pulse voltammtery (DPV). Electrodeposition of gold during the reduction stage of the redox reaction was determined by cyclic voltammetry (CV) that showed a linear relationship with the different hCG concentrations. In this study, a linear relationship between reduction peak current signals and hCG concentration from 0 to 500 pg mL−1 (correlation coefficient of 0.97351) with a detection limit of 5 pg mL−1 was obtained.


Introduction

Electrochemical devices are the most used sensing elements in biosensor development due to inherent small size, their high sensitivity, low cost and their compatibility with advanced microfabrication technologies.1–3 Analytical work of immunosensors is based on the principle that a stable complex forms as a result of specific molecular recognition by antibodies of antigens.4 The binding of an antigen to its specific antibody is identified and quantitated by coupling the immunochemical reaction to the surface of a transducer. Electrochemical immunosensors have gained momentum across the globe in the research and development departments of various industries such as agriculture, food safety, medical diagnostics, quality control, environmental and industrial monitoring,5 to name a few.

Human chorionic gonadotropin (hCG) is a glycoprotein hormone made up of an α-subunit and a β-subunit joined together by hydrophobic and ionic noncovalent interactions. While the α-subunit can also be found in other glycoprotein hormones such as luteinizing hormone, follicle stimulating hormone, and thyroid stimulating hormone, the β-subunit is unique to hCG.

Hydatidiform moles and choriocarcinoma cells produce β-subunit in excess and consequently these are secreted as free β-subunit. The free β-subunit may be used as cancer biomarker as it acts as an autocrine in cancer cells, promotes cell growth, invasion, and metastases.6,7 Having closely linked to gestational trophoblastic disease, germ cell tumours, non-trophoblastic gynaecological cancers and common epithelial tumours, observing hCG levels in blood serum and urine is essential to cancer monitoring and relapse detection in patients.8

Graphene is a two-dimensional planar sheet of sp2 bonded carbon atoms that are tightly packed in a honeycomb lattice structure.9 Graphene forms a basis for other carbon allotropes such as single-walled carbon nanotube that could be envisioned as a single graphene sheet wrapped around to form a cylinder whereas multi-walled carbon nanotube consists of multiple layers of graphene sheets rolled to form a cylinder.10 Graphene possess extraordinary properties for instance, double surface area than that of single walled carbon nanotubes, ultra-high mechanical strength, a tunable electronic band gap, excellent thermal conductivity, room-temperature Hall effect, and ultra-high elasticity.11 These excellent features are attributed to sp2 bonds and electron configuration of graphene that makes it an ideal material for potential electronic and electrochemical sensing applications.12

The use of highly sensitive tags are imperative in immunosensor work to amplify signal response and lower the detection limits. Metal nano-size tags are shown to be more advantageous in comparison to traditional enzymatic and organic fluorescent dye signal tags as single nano-size tag contains large number of signal molecules thus emitting much higher signal than the conventional single tag containing only one or several signal molecules.13

Particularly, gold nanoparticles (AuNPs) have gained immense attention from researchers due to their unique characteristics owing to the remarkable electronic configuration, high ratio of surface atoms to bulk atoms, strong localised surface plasmon resonance band that allows electromagnetic confinement through interaction with optical wave, quantum effects and other traits resulting from their extremely small sizes.14 AuNPs are also mostly used as signal probe owing to the their ease of fabrication and functionalization; and high stability.15–17 An example of using nanoparticles to load large amount of signal molecules was a study by Omidfar et al.18 Upon conjugation of AuNPs with anti-human serum albumin (HSA), a competitive immunoreaction was performed. Then, oxidation of AuNPs was carried out in 0.1 M HCl at high potential of 1.3 V for 80 s followed by reduction of AuCl4 to Au0 in differential pulse voltammetry (DPV) mode to produce the electrochemical signals. This approach is based on the oxidoreduction properties of the AuNPs in acidic medium where target analyte in sample is detected through the quantification of nanoparticles. A decrease in DPV responses was observed with increasing concentrations of HSA in standard and real samples. In optimal conditions, this immunosensor based on MCM-41–PVA nanocomposite film could detect HSA in a high linear range (0.5–200 ng mL−1) with a low detection limit of 1 ng mL−1. Lai et al.19 based their work on the principle of utilizing nanoparticles to induce deposition of metal for further amplification with streptavidin-functionalized silver-nanoparticle-enriched carbon nanotube (CNT/AgNP) served as trace label for sensitive detection of carcinoembryonic antigen (CEA) and α-fetoprotein (AFP). This group chose silver nanoparticles (AgNPs) in their investigation as these nanoparticles can be oxidized at more negative potential with a relatively sharp peak thus eliminating the interference of reducing species and improving the detection precision and sensitivity. Through a sandwich-type immunoreaction on the immunosensor array, numerous AgNPs are captured onto every single immunocomplex and are further amplified by a subsequent AgNP-promoted deposition of silver from a silver enhancer solution to obtain the sensitive electrochemical-stripping signal of the AgNPs. The amplified AgNPs showed well-defined anodic stripping peak in 1.0 m KCl solution. Both the high content of AgNPs on the synthesized tag and the following silver enhancement greatly amplified the detection signal, which led to a detection limit down to 0.093 and 0.061 pg mL−1 for CEA and AFP respectively. However, this procedure suffered from the disadvantages of complicated fabrication and instability of AgNP probe. To circumvent these problems, another group17 used gold nanoparticles (AuNPs) synthesized in situ to catalyze the deposition of silver labeled to the signal antibody. They designed a triple signal amplification strategy combining the AuNPs-catalyzed Ag deposition after sandwich-type immunoreaction to amplify the anodic stripping signal with graphene for rapid electron transfer and microbead carried AuNPs. The triple signal amplification greatly enhanced the sensitivity for CEA detection with a linear range of 0.5 pg mL−1 to 0.5 ng mL−1 and a detection limit down to 0.12 pg mL−1.

The outstanding signal enhancement potential of AuNPs and their ability to form bioconjugated molecules, together with the remarkable sensitivity of graphene, have become the basis of this study to design a highly sensitive electrochemical biosensor. Our signal amplification strategy involved physical immobilization of primary antibody onto disposal graphene-modified screen-printed carbon electrode (SPCE) or graphene biochip. Antigen hCG was then added and sandwiched with a secondary antibody labelled with AuNPs. This was then subjected to a high potential of 1.2 V for 40 s in 0.5 M HCl and immediately followed by voltammetric measurement (Fig. 1).


image file: c4ra11066h-f1.tif
Fig. 1 Schematic illustration of the electrochemical immunosensor system. (a) The primary antibody was immobilized onto the graphene working electrode by physical adsorption. Bovine serum albumin (BSA) was applied to block uncoated surface of the electrode. A sandwich-type immunoreaction was then performed. (b) Redox reaction was carried out at a high potential of 1.2 V for 40 s (termed as preoxidation) in 0.5 M HCl to oxidize the AuNPs which were immediately reduced and (c) scanned by DPV from 1 V to 0 V.

Materials and methods

Reagents and materials

Monoclonal anti-human α-subunit of follicle-stimulating hormone (Mab-FSH) and monoclonal anti-human chorionic gonadotropin (Mab-hCG), with affinity constants of 2.4 × 109 M−1 and 4.4 × 109 M−1 respectively, were obtained from Medix Biochemica (Finland). The molecular weight hCG (Abdserotec, UK) was stated to be 39.5 kD by SDS PAGE. Colloidal solution of Au nanoparticles with diameter of 40 nm of optical density 10 was purchased from BBI solutions (UK). Bovine serum albumin (BSA), sodium azide (NaN3), HCl, Na2HPO4, NaH2PO42H2O, polyethylene glycol (PEG), and KH2PO4 were purchased from Sigma-Aldrich (USA). All solutions were prepared and diluted using double distilled water.

Instrumentations

Cyclic voltammetry (CV) and Differential Pulse Voltammetry (DPV) were performed using a Autolab PGSTAT101 III (Metrohm, Netherlands) working together with its Nova 1.10 software. The screen-printed electrodes (SPEs) were purchased from DropSens (Spain) and consisted of a graphene modified working electrode, a carbon counter-electrode, and silver reference electrode. All measurements were made at room temperature (21 ± 1 °C).

Preparation of graphene biochip

Immobilization of primary antibody was carried out by dropping 6.68 μL of Mab-FSH solution (100 μg mL−1) in 50 mM phosphate buffered saline (PBS, pH 7.4) onto the surface of working electrode and incubated overnight at 4 °C. After incubation, excess antibodies were rinsed with PBS. Following rinsing, 50 μL of blocking solution (1% BSA in PBS) was added onto the electrode surface to prevent non-specific binding and incubated at 4 °C for another 12 h. The blocking solution was then washed with PBS. The Mab-FSH-immobilized immunosensor was stored at 4 °C until needed.

Bioconjugation of gold nanoparticle to hCG antibody (Au–Mab-hCG)

A mixture of 100 μL of Mab-hCG solution (50 μg mL−1 in 5 mM KH2PO4, pH 7.5) and 900 μL of 0.1% Au nanoparticle solution was prepared and kept for 10 min at room temperature. To block any uncovered surface on the AuNPs, 50 μL of 1% PEG in 50 mM KH2PO4 solution (pH 7.5) and 100 μL of 10% BSA in 50 mM KH2PO4 solution (pH 9.0) were added. The Au nanoparticle-conjugated Mab-hCG (Au–Mab-hCG) was then collected through centrifugation (8000g for 15 min at 4 °C). Au–Mab-hCGs were suspended in 1 mL of preservation solution (1% BSA, 0.05% PEG 20[thin space (1/6-em)]000, 0.1% NaN3 and 150 mM NaCl in 20 mM tris–HCl buffer, pH 8.2), and centrifuged again to collect the Au–Mab-hCGs. Au–Mab-hCGs were then suspended in the preservation solution and stored as stock solution.

Sandwiched immunocomplex reaction procedure

Antigen hCG was prepared at various concentrations (between 0 and 500 pg mL−1) with 1% BSA in PBS. Then, 6.68 μL of these antigen hCG solutions were added onto the Mab-FSH-immobilized immunosensor and left to incubate for 30 min at room temperature with moderate shaking allowing for the antigen–antibody reaction. Au–Mab-hCG stock solution was diluted to 10 fold and 6.68 μL of this diluted solution was applied onto the rinsed surface. After incubation for another 30 min at room temperature, the surface was washed with blank PBS.

Preoxidation of AuNPs and signal measurement

A direct redox reaction was carried out using 50 μL of 0.5 M HCl covering the entire three-electrode zone of the SPE at room temperature. The analytical procedure was based on the following process on the electrode surface: the preoxidation of the colloidal gold was performed at constant potential of 1.2 V for 40 s producing AuCl4 ions absorbed on graphene electrode surface:
Au + 4Cl → AuCl4 + 3e

AuCl4 ions were immediately reduced20 to Au at 0.35 V and the reduced ions were scanned in the potential range from 1 V to 0 V with a step potential of 4 mV, a modulation amplitude of −50 mV, a modulation time of 50 s and an interval time of 200 ms. The potentials were obtained against the Ag/AgCl reference electrode printed within the SPE.

Results and discussion

Mab-AuNP conjugation characterization

Conjugation of antibody to AuNP was confirmed by UV-Vis measurements because AuNPs and protein have different absorbance wavelength of A525 and A280 respectively.21 Prior to the addition of antibody, the absorption value of colloidal gold was observed at 528 nm. After addition of antibody, bonds were formed between AuNPs and the amino groups of the antibody causing the absorbance maximum value shifted to 550 nm due to a change in refractive index as a consequence of the attachment of antibody layer on AuNPs thus confirming the antibody conjugation to gold.22

Electrochemical characterization of immunosensor

To investigate the reduction properties of Au ions to Au in HCl, comparison work was carried out between carbon SPE and graphene-modified SPCE. Fig. 2 displays CV graphs of bare and AuNPs-incubated graphene (graph A) and carbon (graph B) electrodes in the potential range from −0.8 V to 1.3 V. The reduction signal of AuNPs for both electrodes could be observed at the potential of 0.36 V. By comparing the current signals for both electrodes, it was revealed that graphene (curve 2A(b)) exhibited a more prominent reduction peak (19 μA) as compared to carbon (curve 2B(d) with reduction peak of 1.7 μA). This demonstrated that graphene promotes the reduction of AuNPs better than carbon due to not only the high surface area of graphene but also its outstanding electron transfer attribute.23 Kampouris and Banks24 reported that enhanced electron transfer of graphene occur primarily at the edge of the graphene rather than at the basal.
image file: c4ra11066h-f2.tif
Fig. 2 The cyclic voltammograms of bare (a) and AuNPs immobilised (b) on graphene SPE (A) electrode at 100 mV s−1 in 0.5 M HCl. The cyclic voltammograms of bare (c) and AuNPs immobilised (d) on SPCE (B) at 100 mV s−1 in 0.5 M HCl.

DPV graphs presented in Fig. 3 are obtained from Au–Mab-hCG immobilised immunosensor with hCG concentrations varying from 0 to 500 pg mL−1 in PBS. The reduction signal was observed at 0.35 V and the peak current intensified in correlation with the increasing hCG concentrations.


image file: c4ra11066h-f3.tif
Fig. 3 DPV of the Au–Mab-hCG on graphene electrodes.

The formation of different layers on the working graphene electrode surface was characterized by CV using Fe(CN)63−/Fe(CN)64− as a redox probe after each assembly step. As shown in Fig. 4, cyclic voltammogram on the bare and Au–Mab-hCG immobilized SPEs were obtained with a reversible redox peak of 10 mM Fe(CN)63−/Fe(CN)64− with oxidation and reduction peaks of bare electrode observed at 0.2 V and 0 V respectively (curve a). Upon immobilization of primary antibody (Mab-FSH) on the electrode surface, an insulating layer was formed in which redox probe could not reach and this subsequently decreased rate of current transfer (curve b).25 After adding antigen hCG (curve c) and Au–Mab-hCG (curve d), interestingly no further significant decrease in redox peaks were seen. This could be due to protein fouling caused by the immobilized antibody molecules and/or at pH values greater than the isoelectric point of antibody, electrostatic interactions between the anionic Fe(CN)63−/Fe(CN)64− and the negatively charged antibody molecules could occur.26 Then, after redox electrochemical reactions of various concentrations of hCG in 0.5 M HCl were performed, the response current in Fe(CN)63−/Fe(CN)64− significantly decreased (curve e). The decrease in current response was due to a layer of Au being electrodeposited on the graphene electrode when Au ions were reduced during the redox reaction process in HCl27 that further hinder electrons reaching the electrode surface.


image file: c4ra11066h-f4.tif
Fig. 4 Cyclic voltammograms of 10 mM Fe(CN)63−/Fe(CN)64− solution in 50 mM phosphate buffer (pH 7) at (a) a bare graphene electrode, (b) Mab-FSH-modified graphene electrode, (c) after adding antigen hCG hormone, (d) after adding Au–Mab-hCG and (e) after electrochemical redox reaction of 1000 pg mL−1 hCG hormone in 0.5 HCl. Potential range from −0.5 to 0.9 V with scan rate of 100 mV s−1.

In order to establish the relationship upon electrochemical redox reaction of different hCG concentrations in 0.5 M HCl and oxidation peak current signals measured in 10 mM Fe(CN)63−/Fe(CN)64− solution, a calibration graph was plotted. As shown in Fig. 5, the oxidation peak current response of 10 mM Fe(CN)63−/Fe(CN)64− solution depended linearly on the concentration of hCG hormone with correlation coefficient of 0.9974 with linear range from 50 to 1000 pg mL−1. This phenomenon was due to the layering of Au that was produced when Au ions were reduced to form Au. This result also served as evidence that at higher hCG concentrations more attachment of Mab-hCG–AuNPs to hCG occurred and more formation of antigen–antibody–AuNPs complexes which subsequently deposit thicker layer of Au onto the graphene electrode surface after electrochemical redox process in 0.5 M HCl. This led to lower current signal as Au acts as a barrier that impedes electron transfer between the redox probe and the electrode surface.


image file: c4ra11066h-f5.tif
Fig. 5 Calibration plots that illustrate the relationship between the hCG concentrations (after redox reaction in 0.5 M HCl) and the oxidation peak current signals measured in 10 mM Fe(CN)63−/Fe(CN)64− solution in 50 mM phosphate buffer pH 7. The limit of detection of 50 pg mL−1 of hCG was obtained.

Electrochemical optimization of the immunosensor

The preoxidation potential was optimized in this study by assigning potentials of 1.20, 1.40 and 1.60 V vs. Ag/AgCl with a pre-oxidation time of 40 s using 250 pg mL−1 of hCG and the respective reduction peak current responses were investigated. Fig. 6 shows that increasing the pre-oxidation potential has resulted in decreasing reduction peak current intensity which suggested more Au ions are lost at higher pre-oxidation potential.28 Maximum reduction peak was discerned at 1.20 V with peak disappearing at 1.40 V. Hence, 1.20 V was chosen to be the optimum pre-oxidation potential used throughout this study.
image file: c4ra11066h-f6.tif
Fig. 6 DPV graphs of Au–Mab-hCG on graphene modified SPCE in 0.5 M HCl at hCG concentration of 250 pg mL−1. Different pre-oxidation potentials (1.20 V, 1.40 V and 1.60 V) were used after the immunocomplexes formation with pre-oxidation time set at 40 s.

Analytical performance of electrochemical system

The principle of our detection system was based on the peak current intensities of Au ions reduced in 0.5 M HCl by DPV. Different concentrations of hCG ranging from 0 to 500 pg mL−1 was used to evaluate the analytical linear range and sensitivity of our immunosensor. Increasing the hCG concentrations also enhance the intensity of reduction peak current responses with correlation coefficient found to be 0.97351 (Fig. 7). This correlation coefficient value obtained in the DPV was attributed to the irreproducible deposition of Au onto the graphene biochips. In addition, DPV is more sensitive and gives higher resolution when compared to CV. A detection limit of 5 pg mL−1 was achieved for hCG under the optimum conditions.
image file: c4ra11066h-f7.tif
Fig. 7 Calibration curve for the detection of hCG established from peak current intensities of AuNPs.

Comparison of different studies for hCG detection using SPE

A comparison to determine hCG hormones using this method with different electrode materials published by other groups is displayed in Table 1. By far, our group achieved a lower detection limit by using graphene biochip in AuNPs redox in HCl signal amplification approach than the work by Idegami27 and Xuan Viet28 groups that used carbon SPE and single-walled carbon nanotube-modified carbon SPE which were reported to be 36 pg mL−1 and 13 pg mL−1 respectively for the detection of hCG. It is important to highlight that the SPE used in this study comprised of inert carbon counter electrode that is advantageous over platinum counter electrodes. In acidic solution, platinum dissolved and formed platinum ions which may affect the activity of reaction on the working solution.29 The lower detection limit in our work might be associated to, as discussed earlier, the large surface area and outstanding electron transfer performance of graphene due to the presence of more sp2-like planes and various edge defects present on its surface.30 Lu et al.31 and Yang et al.32 demonstrated the superiority of graphene as a sensing material in similar studies but employing the catalytic reaction of hydrogen peroxidase towards the reduction of hydrogen peroxide where they achieved low detection limits of 2.6 pg mL−1 for the detection of hCG and 50 pg mL−1 for human IgG respectively.
Table 1 Comparison of different studies for the determination of hCG hormone using SPCEs
Methods Working electrode Limit of detection Reference
DPV SPCE 36 pg mL 27
DPV Single walled carbon nanotube-modified SPCE 13 pg mL 28
DPV Graphene-modified SPCE 5 pg mL This work


Conclusions

The combined merits of AuNPs and graphene were explored in this study. To the best of our knowledge, this is the first study that uses graphene-modified carbon SPEs or graphene biochip for the detection of hCG using AuNPs redox in HCl signal enhancement strategy and we have achieved a LOD of 5 pg mL−1 for the detection of hCG hormone. Our work with graphene produced the best LOD over other SPEs and this paves ways for more graphene-related work in our laboratory to detect other cancer biomarkers in the future.

Acknowledgements

S.A. Lim would like to thank the Ministry of Education, Brunei Darussalam for the opportunity given to undertake a Ph.D programme at Universiti Brunei Darussalam (UBD). The authors also acknowledge Nur Syakimah Ismail from Department of Applied Physics, Graduate School of Engineering, Osaka University and Kisan Koirala from Chemical Science Programme, Faculty of Science, UBD for their kind assistance and helpful discussion in this work.

References

  1. D. R. Thévenot, K. Toth, R. A. Durst and G. S. Wilson, Pure Appl. Chem., 1999, 71, 2333–2348 CrossRef.
  2. M. U. Ahmed, I. A. Saaem, P. C. Wu and A. Brown, Crit. Rev. Biotechnol., 2014, 34, 180–196 CrossRef PubMed.
  3. M. U. Ahmed, M. M. Hossain and E. Tamiya, Electroanalysis, 2008, 20, 616–626 CrossRef CAS.
  4. R. P. Ekins, J. Clin. Ligand Assay, 1999, 22, 61–77 Search PubMed.
  5. S. Ripp, M. L. Diclaudio and G. S. Sayler, Biosensors as Environmental Monitors, in Environmental Microbiology, ed. R. Mitchell and J.-D. Gu, Wiley-Blackwell, 2nd edn, 2010, ch. 9 Search PubMed.
  6. K. Visconti and N. Zite, Clin. Obstet. Gynecol., 2012, 55, 410–417 CrossRef PubMed.
  7. L. A. Cole, Placenta, 2007, 28, 977–986 CrossRef CAS PubMed.
  8. P. Kassanos, R. K. Iles, R. H. Bayford and A. Demosthenous, 13th International Conference on Electrical Bioimpedance and the 8th Conference on Electrical Impedance Tomography, IFMBE Proceedings, 2007, 17, pp. 620–623 Search PubMed.
  9. Y. C. Lin and P. W. Chiu, in Graphene: Properties, Preparation, Characterisation and Devices, ed. V. Skakalova and A. Kaiser, 2014, pp. 265–291 Search PubMed.
  10. K. Dasgupta, J. B. Joshi and S. Banerje, Chem. Eng. J., 2011, 171, 841–869 CrossRef CAS PubMed.
  11. A. K. Geim, Science, 2009, 324, 1530–1534 CrossRef CAS PubMed.
  12. D. Chen, L. H. Tang and J. H. Li, Chem. Soc. Rev., 2010, 39, 3157–3180 RSC.
  13. J. U. HuangXian, Sci. China: Chem., 2011, 54, 1202–1217 CrossRef PubMed.
  14. C. Louis and O. Pluchery, Gold nanoparticles for physics, chemistry and Biology, World Scientific Publisher, 2012, ISBN: 978-1-84816-806-0 Search PubMed.
  15. L. Ding, A. M. Bond, J. Zhai and J. Zhang, Anal. Chim. Acta, 2013, 797, 1–12 CrossRef CAS PubMed.
  16. V. K. K. Upadhyayula, Anal. Chim. Acta, 2012, 715, 1–18 CrossRef CAS PubMed.
  17. D. Lin, J. Wu, M. Wang, F. Yan and H. Ju, Anal. Chem., 2012, 84, 3662–3668 CrossRef CAS PubMed.
  18. K. Omidfar, H. Zarei, F. Gholizadeh and B. Larijani, Anal. Biochem., 2012, 421, 649–656 CrossRef CAS PubMed.
  19. G. Lai, J. Wu, H. Ju and F. Yan, Adv. Funct. Mater., 2011, 21, 2938–2943 CrossRef CAS.
  20. Z. P. Chen, Z. F. Peng, P. Zhang, X. F. Jin, J. H. Jiang, X. B. Zhang, G. L. Shen and R. Q. Yu, Talanta, 2007, 72, 1800–1804 CrossRef CAS PubMed.
  21. J. W. Choi, D. Y. Kang, Y. H. Jang, H. H. Kim, J. Min and B. K. Oh, Colloids Surf., A, 2008, 313–314, 655–659 CrossRef PubMed.
  22. S. Thobhani, S. Attree, R. Boyd, N. Kumarswami, J. N. M. Szymanski and R. A. Porter, J. Immunol. Methods, 2010, 356, 60–69 CrossRef CAS PubMed.
  23. Y. Fang and E. Wang, Electrochemical Biosensors on Platforms of Graphene, Chem. Commun., 2013, 49, 9526 RSC.
  24. D. K. Kampouris and C. E. Banks, Chem. Commun., 2010, 46, 8986–8988 RSC.
  25. Q. Li, N. Li, P. Le Tissier, D. R. Grattan and K. Kerman, Electroanalysis, 2012, 24, 1272–1276 CrossRef CAS.
  26. J. A. Ho, H. C. Chang, N. Y. Shih, L. C. Wu, Y. F. Chang, C. C. Chen and C. Chou, Anal. Chem., 2010, 82, 5944–5950 CrossRef CAS PubMed.
  27. K. Idegami, M. Chikae, K. Kerman, N. Nagatani, T. Yuhi, T. Endo and E. Tamiya, Electroanalysis, 2008, 20, 14–21 CrossRef CAS.
  28. N. Xuan Viet, M. Chikae, Y. Ukita, K. Maehashi, K. Matsumoto, E. Tamiya, P. Hung Viet and Y. Takamura, Biosens. Bioelectron., 2013, 42, 592–597 CrossRef PubMed.
  29. C. Gu, B. C. Norrris, F. R. F. Fan, C. W. Bielawski and A. J. Bard, ACS Catal., 2012, 2, 746–750 CrossRef CAS.
  30. S. Alwarappan, A. Erdem, C. Liu and C. Z. Li, J. Phys. Chem. C, 2009, 113, 8853 CAS.
  31. J. Lu, S. Liu, S. Ge, M. Yan, J. Yu and X. Hu, Biosens. Bioelectron., 2012, 33, 29–35 CrossRef CAS PubMed.
  32. Y. C. Yang, S. W. Dong, T. Shen, C. X. Jian, H. J. Chang, Y. Li and J. X. Zhou, Electrochimica Acta, 2011, 56, 6021–6025 CrossRef CAS PubMed.

This journal is © The Royal Society of Chemistry 2014
Click here to see how this site uses Cookies. View our privacy policy here.