Sensors and Actuators B 204 (2014) 211–217 Contents lists available at ScienceDirect Sensors and Actuators B: Chemical journal homepage: www.elsevier.com/locate/snb ZnO nanorods as immobilization layers for interdigitated capacitive immunosensors P. Sanguino a,∗ , Tiago Monteiro a,b , S.R. Bhattacharyya c , C.J. Dias b , Rui Igreja b,∗∗ , Ricardo Franco a a REQUIMTE, Departamento de Química, Faculdade de Ciências e Tecnologia Universidade Nova de Lisboa 2829-516, Caparica, Portugal CENIMAT/I3 N, Departamento de Ciência dos Materiais, Faculdade de Ciências e Tecnologia, FCT, Universidade Nova de Lisboa and CEMOP-UNINOVA 2829-516, Caparica, Portugal c Departamento de Física & ICEMS, Instituto Superior Técnico 1049-001, Lisbon, Portugal b a r t i c l e i n f o Article history: Received 27 January 2014 Received in revised form 20 May 2014 Accepted 30 June 2014 Available online 1 August 2014 Keywords: ZnO nanorods Interdigitated electrodes Capacitive immunosensor Biosensor Impedance spectroscopy a b s t r a c t ZnO nanorod structures were deposited on micrometer interdigitated Au electrodes to function as threedimensional matrixes for the immobilization of antibodies in a capacitive immunosensor format. As a proof of concept, anti-horseradish peroxidase (anti-HRP) antibodies were immobilized on the ZnO nanostructured surface by a crosslinking process. The ZnO nanorod layer allows distribution of antibodies across the entire region probed by the measuring electric field applied to the microelectrodes. This is an alternative approach to the use of more expensive nanometer electrodes necessary in the detection of smaller layers of antibodies. The new micrometer interdigitated capacitive immunosensor was able to discriminate between HRP antigen in buffer; a non-specific antigen in buffer; or buffer alone, as proven by capacitance measurements. Maximum response of the sensor was achieved in the 5–6 kHz frequency range, opening the possibility for a simplified single frequency detection system for direct antigen detection in complex biological samples. © 2014 Elsevier B.V. All rights reserved. 1. Introduction Impedance spectroscopy is a powerful tool to detect physical, chemical, or biochemical changes in a medium. In particular, in the last 30 years, this technique has been extensively used as a label free technique for the detection of biomolecular interactions in the vicinity of metal or semiconductive electrode surfaces [1]. The application of this capability in the biosensors field was first demonstrated in 1982 when Arwin et al. [2] showed that it was possible to detect enzyme activity by the adsorption of protein on the surface of an electrode. Later on, in 1986, Newman et al. [3] reported the use of interdigitated electrodes (IDE) to detect capacitive changes from the specific binding of antibodies to antigens. This affinity capacitive biosensor was built from two copper IDE with a width and spacing of 50 m which were covered with an insulating layer of parylene (1 m thick) to prevent Faradaic currents when measuring capacitance changes in a liquid environment. The ∗ Corresponding author. Tel.: +351 918 615 752. ∗∗ Corresponding author. Tel.: +351 212 948 562. E-mail addresses: pesang@sapo.pt (P. Sanguino), rni@fct.unl.pt (R. Igreja). http://dx.doi.org/10.1016/j.snb.2014.06.141 0925-4005/© 2014 Elsevier B.V. All rights reserved. specificity of the biosensor was achieved by immobilization of antigens on a SiO2 layer (0.3 m thick) deposited on top of the insulating polymer. The binding of the antibody to the immobilized antigen created a change in the capacitance of the biosensor due to changes on the permittivity of the small layer above the metal IDE. The smaller size of these microelectrodes is an advantage over macrosized traditional electrodes [4,5]. It allows for compactness, portability, simplicity, higher sensitivity, and less volume of target samples to be integrated in an immunosensor. However, these early micrometer spaced electrodes affinity biosensors were not able to create an appreciable impedance variation upon binding of the antibody–antigen pair. This is not surprising since, for micrometer IDE, the thickness of the layer probed by the fringing electrical field above the electrodes (in the micrometer range) is much larger than the sensing layer created by the immobilized antigens or antibodies (typically 10–100 nm). Therefore, this sensing layer, occupies just a fraction of the region measured by the electric field which results in the small binding event signal being masked by the much larger signal from the surrounding medium. This fact was confirmed by a theoretical calculation of the electric field between the IDE [6]. These authors showed that all the current between the electrodes flows in a 212 P. Sanguino et al. / Sensors and Actuators B 204 (2014) 211–217 Fig. 1. (a) Schematic representation of the proposed immunosensor with the ZnO nanorod matrix layer for antibody immobilization. (b) Partial cross section of the immunosensor. The ZnO nanorod layer is used to immobilize and distribute the antibody molecules across the region probed by the measuring electric field. layer, thinner than the IDE spatial wavelength IDE , which in turn is defined as 2 times the sum of electrode width W and electrode gap G (IDE = 2(W + G)). For IDE with an equal gap and spacing of 10 m this corresponds to a 40 m layer. In fact, 95% of the current goes through a layer of 20 m. More recently, Igreja and Dias [7–9] used conformal mapping techniques to develop analytical expressions for the capacitance of IDE. According to this model, the capacitance of the IDE reaches a saturation value at a layer thickness above the electrodes of IDE /2. For our IDE example with equal gap and spacing of 10 m this corresponds to 20 m layer. Any physical, chemical, or biochemical change occuring beyond this distance from the electrodes plane will have a negligible probability to be measured as a capacitance variation by the interdigitated electrode transducer. In order to overcome the small thickness problem of the immobilization layer, and to increase sensitivity, IDE immunosensors have been designed with nanometer electrode dimensions [6,10]. Ideal IDE values range from 20 to 200 nm. However, when compared to micrometer IDE, fabrication of nanometer electrodes requires complex and expensive production methods and facilities. Nevertheless, most research groups have been developing IDE immunosensors with dimensions of hundreds of nanometers which is clearly a compromise between cost and sensitivity of the biosensor [11–15]. Here, we investigated the use of ZnO nanorod structures deposited by the hydrothermal method on Au micro-IDE (W and G = 10 m) as a means of immobilization of antibodies that will function as probes to the target analyte of interest (Fig. 1a). The 3-dimensional matrix layer created by the ZnO nanorods allows the distribution of the probe molecules across the region where the fringing electric field penetrates. For our micro-IDE (W and G = 10 m) this region can spread to a distance of 20 m above the electrode plane (Fig. 1b). In this way, we expect these new immunosensors to mostly detect capacitance changes due to the binding affinity process and not to changes in the layer above the small immobilization region as is the case in a conventional IDE sensor where most of the probed region is air or liquid medium. Owing to a number of interesting properties, ZnO is an ideal candidate to be used as the material for the matrix layer. It has high mechanical strength, high thermal stability, and high oxidation resistance in harsh environment. Its biocompatibility and nontoxicity makes it a strong candidate to be used in the bio and chemical sensors field [16–20]. In addition, the fabrication of ZnO nanorod structures by the hydrothermal route is simple, fast, inexpensive, and can be performed at low temperature [21–23]. More recently, ZnO nanorods were used for enzyme immobilization in glucose sensors [24]. 2. Materials and methods 2.1. Materials and reagents The horseradish peroxidase (HRP) enzyme was from Sigma–Aldrich, and used without further purification. Polyclonal anti-HRP antibody was purchased from antibodies-online.com. Tween 20, phosphate buffered saline (PBS) buffer, bovine serum albumin (BSA), bicinchoninic acid (BCA), copper(II) sulfate, 2,2 -azino-bis(3-ethylbenzothiazoline-6-sulphonic acid) (ABTS), (3-mercaptopropyl)trimethoxysilane 2,2,4-trimethylpentane, (MPTMS), zinc nitrate hexahydrate (Zn(NO3 )2 ·6H2 O), and sodium hydroxide were from Sigma–Aldrich. Sulfo-MBS (mmaleimidobenzoyl-N-hydoxysuccinimide ester) was from Pierce Biotechnology. Hydrogen peroxide H2 O2 30% w/v and zinc acetate dihydrate (Zn(CH3 COO)2 ·2H2 O) were from Panreac. Water was Milli-Q quality. Amicon-ultra 500 (30 kDa) centrifugal filters were from Millipore. 2.2. IDE fabrication A double layer of Cr/Au (10/40 nm thickness) was deposited by e-beam on a substrate of borosilicate glass. The thin Cr layer promotes adhesion of the gold layer. Micrometer IDE were patterned according to standard photolithography and lift-off process. Fabricated microelectrodes had a width and gap of 10 m which resulted in a metallization ratio of 0.5 and a spatial wavelength IDE of 40 m. The area covered by the microelectrodes was 0.7 cm2 . 2.3. ZnO nanorod deposition Prior to deposition of the ZnO nanorods, the micro-IDE were cleaned for 15 min in ethanol, acetone, DI water, and finally blown dry with an Ar jet. The ZnO nanorod layer was deposited by the simple hydrothermal route in a two step process. In the first step, a seed layer was deposited by spincoating a solution of zinc acetate dihydrate (Zn(CH3 COO)2 ·2H2 O) in ethanol (5 mM) for 30 s at 2000 rpm. The coated microelectrodes were then dried with Ar jet, followed by annealing in air at 250 ◦ C for 30 min. The annealing process promotes the thermal decomposition of the zinc acetate to ZnO seeds according to the following equation: Zn(CH3 COO)2 → ZnO + CO2 + (CH3 )2 CO (1) For each interdigitated microelectrode, this step was repeated twice in order to increase the density of the nucleation layer. For the hydrothermal growth, the ZnO seeded microelectrodes were suspended in a 0.01 M aqueous solution of zinc nitrate P. Sanguino et al. / Sensors and Actuators B 204 (2014) 211–217 213 hexahydrate (Zn(NO3 )2 ·6H2 O) and 0.35 M NaOH. Separate solutions of zinc nitrate hexahydrate and NaOH were prepared in deionized water (Mili-Q). The solutions were then mixed in a glass beaker containing the suspended microelectrodes, by slowly adding the NaOH solution to the zinc nitrate hexahydrate solution. After vigorously stirring (700 rpm) the solution for 2 h at 25 ◦ C, the temperature was increased to 80 ◦ C and the stirring was reduced to 300 rpm. After 6 h of deposition, the ZnO coated microelectrodes (micro-IDEZnO ) were dried with an Ar jet followed by 30 min at 90 ◦ C for drying. Crystal growth orientation of ZnO nanorods was analyzed by X-ray diffraction in a –2 configuration equipped with a Cu source. 2.4. Antibody immobilization Attachment of the antibody probes to the ZnO nanorod structures was by cross-linking with Sulfo-MBS. This heterobifunctional crosslinker contains N-Hydroxysuccinimide (NHS) ester and maleimide groups that allow covalent conjugation with aminoacid side chains presenting amine and sulfhydryl groups. The antibody immobilization process is divided in 3 stages: silanization, conjugation and crosslinking. In the silanization step (Fig. 2(a)), the micro-IDEZnO transducers were submerged in a 2% (v/v) solution of MPTMS in 2,2,4-trimethylpentane for 1 h. To remove the unbounded MPTMS, the silanized transducers were then washed in the solvent and finally dried with an Ar jet. Attachment of the MPTMS molecules to the ZnO surface has been reported to be predominantly through the silane groups with the sulfhydryl groups molecularly oriented away from the surface [25]. Therefore, this stage makes sulfhydryl ( SH) groups available at the surface of the nanorods for further linking to maleimide groups of the crosslinker Sulfo-MBS. In the antibody conjugation stage (Fig. 2(b)), a PBS solution of anti-HRP antibody (0.5 mg/ml) and Sulfo-MBS crosslinker (13.8 g/ml) was incubated for 30 min at room temperature. The moderate 10-fold molar excess of crosslinker over antibody was selected in order to avoid deleterious effects to the antibody structure. Covalent conjugation is possible by the attachment of the NHS ester groups of Sulfo-MBS to the amine groups of the antibody antiHRP. The unbounded crosslinker, was removed by ultrafiltration with an Amicon-Ultra 500 (30 kDa) and centrifugation at 7500 × g, 15 min at 4 ◦ C. Finally, in the crosslinking stage (Fig. 2(c)), 50 l of the conjugated mixture were spread over the silanized IDEZnO transducer and left to incubate for 3 h at room temperature. During this process, the maleimide groups of the conjugate S-MBS/antiHRP bind to the sulphydryl groups present on the silanized surface of the ZnO. The prepared sensors were washed in PBS solution and dried with Ar jet. Following the immobilization of antibody, and in order to prevent non-specific binding, the sensors were covered with 50 l of 5% (w/v) BSA in PBS with 0.05% (v/v) Tween®-20 and left to incubate for 2 h. Finally, the mounted sensor set was washed 3 times for 5 min in plenty of fresh PBS. 2.5. Antigen sensor testing To test the IDEZnO immunosensor, we applied 50 l of PBS, HRP in PBS (6.7 M), and an unrelated and non-specific antigen (Plasmodium falciparum Heat shock protein 70 – PfHsp70) (6.7 M in PBS) on 3 identical immunosensors that were fabricated simultaneously. The testing solution was left on the sensors for 1 h at room temperature and then washed with PBS. In the following, SHRP , SPBS , and SPfHsp70 refer to sensors tested with HRP, PBS, and PfHsp70 solutions, respectively. On these tests, HRP is the specific antigen target and PfHsp70 the non-specific antigen. Fig. 2. Antibody immobilization on ZnO nanorods with S-MBS crosslinker. (a) Silanazation of the ZnO nanorod surface. (b) Conjugation of anti-HRP antibody with the crosslinking moiety. (c) Crosslinking of the conjugate to the silanized nanorods. 2.6. Measurements Capacitance (C) and loss tangent (tan ı) measurements were made with an Agilent 4294A precision impedance analyzer in the range of 40 Hz to 110 MHz. Measurements were performed after each fabrication and testing stage. To eliminate the influence of water (either in the liquid or vapor forms), sensors were dried for 30 min under vacuum. After reaching the base pressure of the system (1E−2 mbar), C values were recorded for all spectra. For each sensor, 3 measurements were taken where the electrical contacting probes were repositioned each time. 2.7. Horseradish peroxidase (HRP) enzymatic assay The presence of antigen (due to specific binding to the respective antibody) in the tested sensors was assessed by an enzymatic assay of horseradish peroxidase (HRP) using 2,2 -azino-bis(3ethylbenzothiazoline-6-sulphonic acid) (ABTS) as substrate. The three sensors, SHRP , SPBS , and SPfHsp70 , were placed inside a solution 214 P. Sanguino et al. / Sensors and Actuators B 204 (2014) 211–217 Fig. 3. Deposition of ZnO nanorods on Au micro-IDE. Density of ZnO nanorods clusters over the micrometer electrodes for deposition times of (a) 3, (b) 5, and (c) 7 h. Stability of ZnO nanorods: (d) before washing and (e) after washing twice with PBS. of ABTS + H2 O2 according to the Sigma–Aldrich enzymatic assay of peroxidase [26]. In brief, the amount of HRP enzyme present in the sensors is proportional to the amount of oxidized ABTS which can be determined by measuring the absorbance at 424 nm and visually confirmed by the development of a green color in solution. This color change was evaluated 3 min after submerging the sensors in the assay solution. 3. Results and discussion 3.1. ZnO nanorod layer The first step in the fabrication of the proposed immunosensor was the hydrothermal deposition of the ZnO nanostructures on top of the Au micro-IDE. Photoluminescence and photoconductivity measurements of nanorod structures obtained with this method have been previously reported [27]. Ideally, the 3-dimensional layer should have a high density of ZnO structures with sizes capable of including them well inside the measuring region of the probing electric field. The duration of the hydrothermal process is an important parameter for determining the size and coverage of ZnO structures deposited on the Au microelectrodes. In order to establish the deposition time to be used in the fabrication of the sensors, ZnO nanostructures were grown on Au micro-IDE for three different deposition times: 3, 5, and 7 h (Fig. 3). From Fig. 3(a) we can conclude that a deposition time of 3 h did not produce an acceptable coverage of the electrodes. On the other hand, for 5 h (Fig. 3(b)) and 7 h (Fig. 3(c)) of deposition, a much higher density of nanorod structures was observed. Apart from ZnO nanostructures density and size, the stability of ZnO nanostructures is paramount in the fabrication and testing of the proposed immunosensor. To determine this parameter, a micro-IDEZnO was washed with PBS to simulate the fabrication and testing procedures. After drying with an Ar jet, the washing procedure was repeated. Fig. 3(d) and (e) shows optical microscopy images of the micro-IDEZnO before and after washing twice with PBS, respectively, showing that ZnO nanorod structures remained attached to the surface of the microelectrode transducer. It can therefore be concluded that these 3-dimensional structures are optimal anchoring substrates for antibody probe immobilization on the immunosensor. In order to shorten sensor fabrication time as much as possible, not compromising the quality of the obtained sensors, we have decided for a deposition time of 6 h. In these conditions, we obtained ZnO nanorods with approximate lengths of 5 m and widths of 100 nm (Fig. 4(a)). The X-ray diffraction pattern of Fig. 4(b) shows that the deposited ZnO nanorods exhibit the wurtzite hexagonal crystal structure with preferential growth in Fig. 4. (a) SEM micrograph of the ZnO nanostuctured matrix layer. (b) –2 X-ray diffraction pattern for the deposited ZnO nanorods. The first peak, located at about 34.5◦ , can be assigned to the (0 0 2) crystallographic plane family in hexagonal ZnO. P. Sanguino et al. / Sensors and Actuators B 204 (2014) 211–217 Fig. 5. Evolution of the capacitance (at 10 kHz; log scale) for the three sensors during the various fabrication steps. The deposition of ZnO nanorods increases the capacitance of the micro-IDE by two orders of magnitude. During fabrication, changes in capacitance are identical for all the sensors. Sensors SHRP , SPf Hsp70 , and SPBS were tested with specific antigen, non-specific antigen and buffer, respectively. the (0 0 2) direction. This fact can be attributed to the low surface energy of the (0 0 2) crystal plane [28]. The XRD peak at 38.4 was assigned to Zn (1 0 0) according to the Joint Committee on Powder Diffraction Standards (JCPDS) card (no. 040831). 3.2. Sensor fabrication 215 Fig. 6. Confirmation of the presence of HRP in the immunosensor by an enzymatic assay of horseradish peroxidase (HRP) using ABTS as substrate. The sensor tested with HRP solution was able to oxidize ABTS as indicated by the green color change. Sensors tested with PBS and PfHsp70 were not able to promote this color change, confirming HRP absence. The response of the sensors to the testing solutions was determined by calculating the capacitance and phase shift variation from the measured capacitance and loss tangent spectra. Fig. 7 presents these variations when sensors are tested with the respective assay (HRP; specific antigen), or control (PfHsp70; non-specific antigen), and PBS solutions. When the immunosensor was tested with the solution containing the specific antigen (anti-HRP), a decrease in the capacitance Having determined the conditions for the hydrothermal deposition of ZnO nanostructures, three sensors (SHRP , SPBS , and SPfHsp70 ) were fabricated simultaneously as described in the materials and methods section. Briefly, the process can be divided into four stages: (1) deposition of ZnO nanostructures on the surface of the micro-IDE; (2) functionalization of the ZnO nanostructured electrodes with the organosilane MPTMS; (3) cross-linking of the SMBS/anti-HRP conjugate to the MPTMS treated electrodes; (4) blocking of the sensors with BSA, to prevent nonspecific binding. The capacitance of the three immunosensors was recorded after each fabrication step. As presented in Fig. 5, after deposition of the ZnO nanostructures (first step of the fabrication process), the capacitance of the micro-IDE increased by two orders of magnitude. This capacitance increase can be explained by the increased surface area provided by the ZnO nanostructures. After the silanization step, the capacitance increases again for all the sensors by almost one order of magnitude. However, a slight decrease of the capacitance takes place after the two following fabrication steps, namely, antibody crosslinking and BSA blocking. It is important here to notice that shifts in the capacitance after each fabrication step, are always in the same direction for all three sensors. This identical behavior attests the robustness of the fabrication procedure of the proposed immunosensors. 3.3. Sensor testing Finalized sensors, with a nominal capacitance of 10 nF (Fig. 5), were tested with the respective assay solutions: PBS only for the SPBS sensor; anti-HRP in PBS, for the SHRP sensor; and PfHsp70 in PBS, for the SPfHsp70 sensor. The presence of the antigen in the SHRP sensor was confirmed by an enzymatic assay of horseradish peroxidase (HRP) (see Section 2). The green color change, corresponding to ABTS oxidation and promoted by the presence of HRP in the sensors, was only seen in the sensor tested with HRP solution (Fig. 6). The sensors SPBS and SPfHsp70 that did not contain HRP, did not promote the oxidation of the ABTS solution and consequently, no green color was observed. Fig. 7. (a) Sensors capacitance (real part) and (b) phase shift variation spectra of the IDEZnO immunosensor when tested with an HRP antigen solution, PfHsp70 nonspecific antigen solution, and PBS buffer alone. 216 P. Sanguino et al. / Sensors and Actuators B 204 (2014) 211–217 was observed for all tested frequencies below 1 MHz (Fig. 7(a)). On the other hand, testing the sensor with the non-specific solutions (PBS only or PfHsp70 in PBS) resulted in the increase of the capacitance in the same frequency range. This opposite response confirms that the proposed immunosensor is able to discriminate between solutions containing the specific target (anti-HRP) and solutions that do not contain this HRP antibody-specific antigen. The buffer solution (PBS) in which the specific and non-specific antigens are diluted will affect the immunosensor response, increasing the capacitance. This is probably due to accumulation of Na+ and Cl− ions in the sensor matrix which in turn increases its permittivity. This could explain the positive variation of the immunosensor capacitance when tested with PBS and non-specific antigen solutions. After antigen-antibody bonding the medium permittivity will decrease which is attributed to a decrease in antibody polarization when bonded to the specific antigen. The same opposite response between controls and specific antigen is also obtained when plotting the phase shift variation below 8 kHz (Fig. 7(b)), but in this case, the response of the sensor to the specific antigen solution is positive, while the response to the non-specific solutions is negative. It is interesting to notice that the variation of the capacitance (Fig. 7(a)), when testing the immunosensor with the specific antigen (HRP), decreases for frequencies above 6 kHz. Based on the physical model described by Pethig and Kell [29], Gebbert et al. [30] calculated that the maximum excitation frequency at which an immobilized antibody–antigen complex (in a water medium) responds to changes in the electric field, is around 6 kHz. This is consistent with our data. Although our immunosensors are in a “dry” state during measurements, the water vapor present in the low vacuum chamber (10−2 mbar) is probably enough to keep a water envelope around the antibody–antigen complex, therefore validating the calculations for our case. The maximum variation of the capacitance in the 5–6 kHz frequency range allows for simplified single frequency probing in future practical applications. 4. Conclusions For the first time, we have used ZnO nanostructures as a sensitive layer coupled with interdigitated microelectrode transducers in an affinity immunosensor format. The addition of a 3-dimensional matrix, on top of the interdigitated microelectrodes, allowed distribution of antibody probes across the region probed by the fringing electric field. This setup opens the opportunity for the use of interdigitated electrodes with micrometer dimensions (10 m), an important advantage over nanometer interdigitated sensors for which more complex and expensive fabrication procedures are required. The new IDEZnO immunosensors were able to identify buffered aqueous solutions containing the target antigen (HRP), responding with a negative capacitance variation. Conversely, solutions without the specific antigen, produced an opposite variation in the capacitance of the immunosensors. The IDEZnO immunosensor response presented a maximum at the excitation frequency of 6 kHz which foresees the future sensor instrumentation particularly easy for practical applications. Acknowledgments This work was supported by Fundação para a Ciência e a Tecnologia, Portugal (Grants PEstC/EQB/LA0006/2013 to PS and RF; PTDC/CTM-NAN/112241/2009 to RF; post-doc grant SFRH/BPD/70803/2010 to PS; post-doc grant SFRH/BPD/ 66773/2009 to SRB; and the COMPETE Program). 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Comput. 2 (2013), ID-10. [28] S. Fujihara, C. Sasaki, T. Kimura, Appl. Surf. Sci. 180 (2001) 341–350. [29] R. Pethig, D.B. Kell, Phys. Med. Biol. 32 (1987) 933–970. [30] A. Gebbert, M. Alvarez-Icaza, W. Stocklein, R.D. Schmid, Anal. Chem. 64 (1992) 997–1003. Biographies Pedro Sanguino received his degree in Physics Engineering from Instituto Superior Técnico, IST, Lisbon, Portugal, in 1999 and the Ph.D. degree in Technological Physics Engineering from the same institution in 2005. Since 2011 he is a Postdoc in the Chemistry Department of Faculdade de Ciências e Tecnologia from the Universidade Nova de Lisboa (FCT-UNL). Dr. Sanguino has a solid background in the production and characterization of thin films and is currently working in the biosensors field. Tiago Monteiro received the degree in Molecular and Cellular Biology from Universidade Nova de Lisboa (UNL) in 2011. He is currently pursuing his M.Sc. Degree in Biotechnology at the same institution. Soumya Bhattacharyya was born in Kolkata/India in 1981. He completed his studies of Physics in 2004 and began his PhD in 2005 with a CSIR fellowship at the Jadavdur University. His thesis topic was “Synthesis and charaterization of Gallium Nitride films by sputtering technique”. He completed his PhD in 2009 and worked as a Postdoc fellow (FCT grant) at the Instituto Superior Técnico in Lisbon. He is currently an assistant professor at the physics department of Suri Vidyasagar College in India. His current research interests are wide band gap semiconductors and their device applications. C.J. Dias was born in Angola in 1959. He graduated in Engineering Physics from Universidade Nova de Lisboa (UNL) in 1982 and joined the Physics Department of the same University in 1985. He received the Ph.D. from University of North Wales (Bangor) in 1994 working on ferroelectric polymer–ceramic composites. Since then Prof. Dias has been auxiliary professor at UNL and is currently working in the Materials Science Department and is a full member of CENIMAT/I3N research associated laboratory in Nanostructures, Nanomodelation and Nanofabrication. His research P. Sanguino et al. / Sensors and Actuators B 204 (2014) 211–217 interests include characterization of dielectrics and their use in various applications such as sensors and actuators, acoustics and polymer materials for energy applications. Rui Igreja was born in Lisbon, Portugal in 1966. He graduated in Engineering Physics from Universidade Nova de Lisboa (UNL) in 1992 and joined the Physics Department of the same University in 1993. He obtained the M.Sc. degree in instrumentation, industrial maintenance and quality in UNL in 1998 and the Ph.D. in materials engineering (microelectronics and optoelectronics) (2006) in UNL. Prof. Igreja is currently an auxiliary professor at Materials Science Department at UNL and full member of CENIMAT/I3N research associated laboratory in 217 nanostructures, nanomodelation and nanofabrication. His research interests include solid state physics, dielectrics and chemical and biological sensors. Ricardo Franco (b. 1966) holds a degree in Applied Chemistry and Biotechnology (1989) and a Ph.D. in Bioinorganic Chemistry (1995), both by Universidade Nova de Lisboa, Portugal. Currently, he is an assistant professor of Biochemistry at the Faculdade de Ciências e Tecnologia, Universidade Nova de Lisboa, Portugal. Prof. Franco’s research activities focus on antibodies, protein and DNA interactions with nanoparticles and nanostructures of noble metals using spectroscopic techniques, for the development of nanobiosensors.