Gold Nanoparticles/Carbon Nanotubes and Gold Nanoporous as Novel Electrochemical Platforms for L-Ascorbic Acid Detection: Comparative Performance and Application

: Herein, the effects of nanostructured modiﬁcations of a gold electrode surface in the development of electrochemical sensors for L-ascorbic acid detection have been investigated. In particular, a bare gold electrode has been modiﬁed by electrodeposition of gold single-walled carbon nanotubes (Au/SWCNTs) and by the formation of a highly nanoporous gold (h-nPG) ﬁlm. The procedure has been realized by sweeping the potential between +0.8 V and 0 V vs. Ag/AgCl for 25 scans in a suspension containing 5 mg/mL of SWCNTs in 10 mM HAuCl 4 and 2.5 M NH 4 Cl solution for Au/SWCNTs modiﬁed gold electrode. A similar procedure was applied for a h-nPG electrode in a 10 mM HAuCl 4 solution containing 2.5 M NH 4 Cl, followed by applying a ﬁxed potential of − 4 V vs. Ag/AgCl for 60 s. Cyclic voltammetry and electrochemical impedance spectroscopy were used to characterize the properties of the modiﬁed electrodes. The developed sensors showed strong electrocatalytic activity towards ascorbic acid oxidation with enhanced sensitivities of 1.7 × 10 − 2 µ A µ M − 1 cm − 2 and 2.5 × 10 − 2 µ A µ M − 1 cm − 2 for Au/SWCNTs and h-nPG modiﬁed electrode, respectively, compared to bare gold electrode (1.0 × 10 − 2 µ A µ M − 1 cm − 2 ). The detection limits were estimated to be 3.1 and 1.8 µ M, respectively. The h-nPG electrode was successfully used to determine ascorbic acid in human urine with no signiﬁcant interference and with satisfactory recovery Nanoporous gold ﬁlms The self-templating a combined time saving electrochemical-templating two steps: gold electrodeposition and hydrogen bubbling at the electrode, as a self-template, realized by applying a negative potential, lower In this work, we describe two nano-structured electrochemical sensors for AA detection based on the modiﬁcation of a bare gold electrode with electrodeposited Au/SWCNTs and self-templating h-nPG, respectively, as represented in Scheme 1. The morphology of the electrodes has been characterized through scanning electron microscopy (SEM), energy dispersive X-ray spectroscopy (EDX), Raman spectroscopy and electrochemical impedance spectroscopy (EIS). The electrochemical characterization of the two sensors has been reported and the analytical performances were compared. Moreover, the potential application of the h-nPG based sensor for testing AA in human urine samples was also investigated.


Introduction
L-Ascorbic Acid (AA) or vitamin C is a very important compound, that is abundant in many fruits, vegetables and humans [1]. An appropriate amount of this vitamin is especially important for maintaining a healthy immune system. It also plays an important role in wound healing, keeping your bones strong, enhancing brain function and preventing cancer and other diseases, thanks to its antioxidant properties [2][3][4]. For this reason, the AA content is used as a health indicator [5]. AA cannot be synthetized by the human body, as humans can take AA only from food and integrators. One of the most common reasons people take vitamin C supplements is because, historically, there have been suggestions of the effectiveness of this vitamin to prevent the common cold [6,7]. Moreover, it is known that deficiency of AA can cause scurvy, anemia and premature ageing [8]. European studies have also shown a negative correlation between vitamin C plasma levels and all-cause of cardiovascular mortality [9]. In recent years, emerging literature suggests the role of vitamin C in the treatment of a variety of viral infections [10]. Preliminary Nanoporous gold films are generally fabricated using the following methods: dealloying, electrochemical deposition and templating [50,51]. The self-templating method is a combined time saving electrochemical-templating method involving two steps: gold electrodeposition and hydrogen bubbling at the electrode, as a self-template, realized by applying a negative potential, usually lower than −3 V vs. SCE [52][53][54][55].
In this work, we describe two nano-structured electrochemical sensors for AA detection based on the modification of a bare gold electrode with electrodeposited Au/SWCNTs and self-templating h-nPG, respectively, as represented in Scheme 1. The morphology of the electrodes has been characterized through scanning electron microscopy (SEM), energy dispersive X-ray spectroscopy (EDX), Raman spectroscopy and electrochemical impedance spectroscopy (EIS). The electrochemical characterization of the two sensors has been reported and the analytical performances were compared. Moreover, the potential application of the h-nPG based sensor for testing AA in human urine samples was also investigated.
Chemosensors 2021, 9, x 3 of 20 the electrode surface, thus avoiding the drawback of an undesirable loss of material from the surface, as is the case for gold nanoparticles. Nanoporous gold films are generally fabricated using the following methods: dealloying, electrochemical deposition and templating [50,51]. The self-templating method is a combined time saving electrochemical-templating method involving two steps: gold electrodeposition and hydrogen bubbling at the electrode, as a self-template, realized by applying a negative potential, usually lower than −3 V vs. SCE [52][53][54][55].
In this work, we describe two nano-structured electrochemical sensors for AA detection based on the modification of a bare gold electrode with electrodeposited Au/SWCNTs and self-templating h-nPG, respectively, as represented in Scheme 1. The morphology of the electrodes has been characterized through scanning electron microscopy (SEM), energy dispersive X-ray spectroscopy (EDX), Raman spectroscopy and electrochemical impedance spectroscopy (EIS). The electrochemical characterization of the two sensors has been reported and the analytical performances were compared. Moreover, the potential application of the h-nPG based sensor for testing AA in human urine samples was also investigated. Scheme 1. Schematic representation of the Au/SWCNTs (Method 1) and h-nPG (Method 2). modified gold sensor for ascorbic acid detection.
Electrochemical impedance (EIS) was utilized to characterize the different modifications of the Au electrode surface. EIS experiments were carried out at equilibrium potential called open circuit potential (OCP) without bias voltage in the frequency range of 0.1-10 3 Hz using an ac signal of 10 mV amplitude at a formal potential of the redox probe (0.22 V vs. Ag/AgCl), using Autolab Potentiostat/Galvanostat (Eco Chemie, Utrecht, The Netherlands). Three-electrode cell configuration with Ag/AgCl as reference electrode and the glassy carbon rod as a counter electrode was used for measures. EIS measurements were carried out using 10 mL of PBS buffer solution containing mixture of 5 mM Fe(CN) 6 3− /Fe(CN) 6 4− , as electrochemical probe.

Preparation of Gold Modified Electrodes
Au/SWCNTs classical and SPE gold electrodes were modified according to a similar procedure developed in our previous work for MWCNTs, by electrodeposition of Au/SWCNTs sweeping the potential between +0.8 V and 0 V vs SCE for 25 scans at 0.05 Vs −1 in a suspension containing 5 mg/mL of SWCNTs in 10 mM HAuCl 4 containing 2.5 M NH 4 Cl [56,57].
The h-nPG classical and SPE gold electrodes were modified by electrodeposition of h-nPG by initially sweeping the potential for 25 scans between +0.8 V and 0 V vs. Ag/AgCl at 50 mV s −1 in a 10 mM HAuCl 4 solution containing 2.5 M NH 4 Cl. Successively, a fixed potential of −4 V vs. Ag/AgCl was applied to the modified electrode for 60 s in the same solution, in order to allow the formation of pores, due to hydrogen bubbling. Finally, the electrodes were further activated in 0.5 M H 2 SO 4, by running CVs between 0 and +1.7 V versus Ag/AgCl at a scan rate of 100 mV s −1 for 25 cycles, until a well-defined CV was obtained [58].

SEM Experiments
A high-resolution field emission scanning electron microscopy (SEM) (HR FESEM, Zeiss Auriga Microscopy, Jena, Germany) was used to investigate the morphology of the modified screen-printed electrodes. All samples were prepared using gold plates (25 Å~25 Å~1 mm, ALS Co. Ltd., Tokyo, Japan) instead of gold electrodes.
In order to evaluate the Au content of the h-nPG modified screen-printed electrode, energy dispersive X-ray spectroscopy (XPS) (Zeiss Auriga Microscopy, Jena, Germany) measurements were performed. The EDX spectrum and data were collected during sample surface scanning by SEM electron probe.

Raman Spectroscopy
Raman spectra were recorded at room temperature, in back-scattering geometry, with an inVia Renishaw micro-Raman spectrometer (Wotton-under-Edge, Gloucestershire, UK), using the 514.5 nm emission line from an Ar ion laser. The power of the incident beam was about 5 mW. Repeated accumulations (20 scans × 20 s) were acquired on different sample regions using a 50× objective to check sample homogeneity. The spectra were calibrated using the 520.5 cm −1 line of a silicon wafer.

SEM Characterization
SEM experiments were carried out to investigate the morphology of the Au bare and the Au/SWCNTs and h-nPG modified screen-printed electrodes (Figure 1, panels A-C). In the case of the Au/SWCNTs electrode, it is possible to clearly note the presence of clusters of AuNPs, with a distribution of nanoparticles in the range 50-250 nm diameter, onto the Au electrode surface (Figure 1, panel B). The presence of SWCNTs has been confirmed by Raman spectroscopy (see Section 3.2). The initial reduction of Au 3+ to Au 0 with the formation of AuNPs probably facilitated the entrapment of the SWCNTs, allowing a good electrode nanocoating.
As for the h-nPG modified electrode, the honeycomb-like feature with evenly distributed micropores of approximately 10-25 µm in diameter is clearly observed (Figure 1, panel C). The magnified SEM image shows a highly porous branched structure with smaller pores with a diameter of a few hundred nanometers ( Figure 1, panel D). The porous structure permeates the gold electrode surface generating the typical sponge-like appearance. It is interesting to note that a negative potential of −4 V vs. Ag/AgCl was necessary for the formation of nucleation centers for the deposition of Au atoms and for the simultaneous evolution of hydrogen bubbling, needed for pore formation. The deposition time of 60 s is quite short compared to a similar method proposed by Kumar et al. [54], where the optimum deposition time was found to be 400 s at the same applied potential, probably thanks to the previous step of potential sweeping, not used in the other work.
In addition, SEM-EDX microanalysis was conducted to support the information obtained with SEM images obtained for the h-nPG film. It shows the presence of only Au element uniformly distributed in the nanoporous structure, indicating the successful formation of the h-nPG film on the surface of the gold electrode ( Figure 1, panels D and E).

SEM Characterization
SEM experiments were carried out to investigate the morphology of the Au bare and the Au/SWCNTs and h-nPG modified screen-printed electrodes (Figure 1, panels A-C). In the case of the Au/SWCNTs electrode, it is possible to clearly note the presence of clusters of AuNPs, with a distribution of nanoparticles in the range 50-250 nm diameter, onto the Au electrode surface (Figure 1, panel B). The presence of SWCNTs has been confirmed by Raman spectroscopy (see Section 3.2). The initial reduction of Au 3+ to Au 0 with the formation of AuNPs probably facilitated the entrapment of the SWCNTs, allowing a good electrode nanocoating.
As for the h-nPG modified electrode, the honeycomb-like feature with evenly distributed micropores of approximately 10-25 μm in diameter is clearly observed ( Figure  1, panel C). The magnified SEM image shows a highly porous branched structure with smaller pores with a diameter of a few hundred nanometers ( Figure 1, panel D). The porous structure permeates the gold electrode surface generating the typical sponge-like appearance. It is interesting to note that a negative potential of −4 V vs. Ag/AgCl was necessary for the formation of nucleation centers for the deposition of Au atoms and for the simultaneous evolution of hydrogen bubbling, needed for pore formation. The deposition time of 60 s is quite short compared to a similar method proposed by Kumar et al. [54], where the optimum deposition time was found to be 400 s at the same applied potential, probably thanks to the previous step of potential sweeping, not used in the other work.
In addition, SEM-EDX microanalysis was conducted to support the information obtained with SEM images obtained for the h-nPG film. It shows the presence of only Au element uniformly distributed in the nanoporous structure, indicating the successful formation of the h-nPG film on the surface of the gold electrode ( Figure 1, panels D and E).

Raman Characterization
Raman spectroscopy was utilized to demonstrate the presence of SWCNTs onto the Au/SWCNTs modified electrode. The spectra clearly identified the presence of carbon nanotubes (CNTs). Similar spectral profiles were observed in several surface spots, shown in Figure 2. Signals at ~1358, ~1581 and at ~2710 cm −1 correspond to the D-(defect, photondefects interaction), G-(graphite, E2g stretching mode of carbon atoms, and G'-bands (second-order overtone of D band), respectively [59]. The absence of radial breathing modes (RBM) in the range 130-400 cm −1 , a characteristic of singled-walled carbon nanotubes (SWCTs), could be ascribed to the sharp increase of the background obscuring the low intensity modes. No significant variations of the D-band to the G-band intensity ratios (ID/IG, a measure of the structural disorder of the carbon material,) were observed on the spectra of the samples with respect to those of pristine SWCNTs indicating that the dispersion process did not yield an increase of defects.

Raman Characterization
Raman spectroscopy was utilized to demonstrate the presence of SWCNTs onto the Au/SWCNTs modified electrode. The spectra clearly identified the presence of carbon nanotubes (CNTs). Similar spectral profiles were observed in several surface spots, shown in Figure 2. Signals at~1358,~1581 and at~2710 cm −1 correspond to the D-(defect, photondefects interaction), G-(graphite, E 2g stretching mode of carbon atoms, and G'-bands (second-order overtone of D band), respectively [59]. The absence of radial breathing modes (RBM) in the range 130-400 cm −1 , a characteristic of singled-walled carbon nanotubes (SWCTs), could be ascribed to the sharp increase of the background obscuring the low intensity modes. No significant variations of the D-band to the G-band intensity ratios (I D /I G , a measure of the structural disorder of the carbon material,) were observed on the spectra of the samples with respect to those of pristine SWCNTs indicating that the dispersion process did not yield an increase of defects.

Electrochemical Characterization
The electrochemical behavior of both Au bare and Au-modified electrodes was studied using two electrochemical techniques, cyclic voltammetry (CV) and electrochemical impedance spectroscopy (EIS), able to characterize the reversibility of the electron transfer process and the charge transfer resistance at the electrode-solution interface, respectively. The redox couple Fe(CN)6 3−/4− was used as anionic electrochemical probe for examining the different platforms [58,61].

Cyclic Voltammetry Characterization
The unmodified and modified Au electrodes were electrochemically characterized by using cyclic voltammetry experiments in a solution containing 5 mM [Fe(CN) 6 ] 3−/4− and 0.1 M KCl, at a scan rate of 50 mV s −1 . Figure 3 shows the CV profiles of the bare, Au/SWCNTs and h-nPG gold electrodes, respectively. All CVs show a couple of redox peaks with a large increase of the anodic and cathodic peak currents and a decrease of the peak-to-peak separation (ΔEp), after electrode modifications, due to the increase of the electroactive surface area and reversibility of the systems, in both cases. The highest anodic and cathodic peak currents were observed with h-nPG electrode, together with the lowest ΔEp value of about 87 mV, close to the theorical ΔEp value (59 mV), typical of a monoelectronic reversible mediator.
In addition, the effect of the scan rate on the current responses of the h-nPG electrode has been evaluated. Figure 4 shows the CVs corresponding to different scan rates from 5 to 500 mV s −1 and the linear relationship between the peak current values and the square root of the scan rate. The corresponding linear equations for the anodic and cathodic peak currents are Ipa (A) = −3.02 × 10 −5 + 3.67 × 10 −4 v 1/2 (V·s −1 ) with the square of correlation coefficient R 2 = 0.994, and Ipc (A) = 3.20 × 10 −5 + 3.76 × 10 −4 v 1/2 (V·s −1 ) with R 2 = 0.992. These results attest a diffusion-controlled mass transfer process at the solution/h-nPG interface.
All electroanalytical parameters before and after electrode modifications, such as ΔEp, electroactive areas (Ae), ρ values and the heterogeneous electron transfer rate

Electrochemical Characterization
The electrochemical behavior of both Au bare and Au-modified electrodes was studied using two electrochemical techniques, cyclic voltammetry (CV) and electrochemical impedance spectroscopy (EIS), able to characterize the reversibility of the electron transfer process and the charge transfer resistance at the electrode-solution interface, respectively. The redox couple Fe(CN) 6 3−/4− was used as anionic electrochemical probe for examining the different platforms [58,61].

Cyclic Voltammetry Characterization
The unmodified and modified Au electrodes were electrochemically characterized by using cyclic voltammetry experiments in a solution containing 5 mM [Fe(CN) 6 ] 3−/4− and 0.1 M KCl, at a scan rate of 50 mV s −1 . Figure 3 shows the CV profiles of the bare, Au/SWCNTs and h-nPG gold electrodes, respectively. All CVs show a couple of redox peaks with a large increase of the anodic and cathodic peak currents and a decrease of the peak-to-peak separation (∆E p ), after electrode modifications, due to the increase of the electroactive surface area and reversibility of the systems, in both cases. The highest anodic and cathodic peak currents were observed with h-nPG electrode, together with the lowest ∆E p value of about 87 mV, close to the theorical ∆E p value (59 mV), typical of a monoelectronic reversible mediator.
In addition, the effect of the scan rate on the current responses of the h-nPG electrode has been evaluated. Figure 4 shows the CVs corresponding to different scan rates from 5 to 500 mV s −1 and the linear relationship between the peak current values and the square root of the scan rate. The corresponding linear equations for the anodic and cathodic peak currents are I pa (A) = −3.02 × 10 −5 + 3.67 × 10 −4 v 1/2 (V·s −1 ) with the square of correlation coefficient R 2 = 0.994, and I pc (A) = 3.20 × 10 −5 + 3.76 × 10 −4 v 1/2 (V·s −1 ) with R 2 = 0.992. These results attest a diffusion-controlled mass transfer process at the solution/h-nPG interface.
to the nano-structuration obtained with carbon nanotubes and to the 3D-network of the h-nPG, which improves the electron transfer rate between the electrode surface and the bulk solution. Consequently, the roughness factors ρ values reported in Table 1 increased accordingly.    accordingly.   All electroanalytical parameters before and after electrode modifications, such as ∆E p , electroactive areas (A e ), ρ values and the heterogeneous electron transfer rate constants (k 0 ) of the bare and the modified electrodes are reported in Table 1. In particular, the electroactive area (A e ) of Au/SWCNTs and h-nPG electrodes resulted to be about 14 and 20 times larger than that reported for the bare electrode. This behavior can be ascribed to the nano-structuration obtained with carbon nanotubes and to the 3D-network of the h-nPG, which improves the electron transfer rate between the electrode surface and the bulk solution. Consequently, the roughness factors ρ values reported in Table 1 increased accordingly. The A e values have been evaluated using the Randles-Sevcik equation [60], which for a reversible process is as follows: Ip = 2.686 × 10 5 n 3/2 A e D 0 1/2 C 0 υ 1/2 (1) where I p is the voltammetric peak current (A), n the number of electrons (n = 1), A e the electroactive area (cm 2 ), D 0 the diffusion coefficient (7.6 × 10 −6 cm 2 s −1 for ferricyanide), C 0 the concentration (mol cm −3 ), and υ the scan rate (Vs −1 ). In particular, the A e values were calculated by using the slope of the plot I p vs υ 1/2 for each electrode. The heterogeneous electron transfer rate constant (k 0 ) values were calculated using the extended method obtained by merging Klingler-Kochi and Nicholson-Shain methods, for totally irreversible and reversible systems, respectively [62][63][64][65], and the roughness factors (ρ) from the ratio of the electroactive (A e ) to the geometric area (A g ) of each electrode.
It is interesting to note that the k 0 value obtained in the case of Au/SWCNTs and h-nPG electrodes resulted to be about four and five times higher than that obtained with Au bare electrode, respectively, showing a relatively faster electron transfer kinetics, thanks to the high conductivity of the gold nanostructures. Compared to the 20-times increase in the electroactive area obtained with h-nPG electrode, the corresponding increase in the k 0 value is quite limited. This can be ascribed to the fact that the [Fe(CN) 6 ] 3−/4− redox probe has a fast kinetics and therefore its concentration at the outerpore rapidly drops to zero without leaving to the redox probe enough time to reach the inner pore surface which is not "utilized".

Electrochemical Impedance Spectroscopy Characterization
EIS measurements were carried out for further characterization of the modified electrodes. Figure 5 shows the Nyquist plots for the Au bare and the modified Au/SWCNTs and h-nPG electrodes in 0.1 M KCl containing 5.0 mM Fe(CN) 6 3−/4 . It is known that the Nyquist plot consists of a semi-circular part at high frequencies, which diameter represents the charge transfer resistance R ct , and a linear part at low frequencies, indicative of systems with diffusion-controlled current [64]. The semicircle diameter depends on the dielectric and insulating features at the electrode-electrolyte interface and can reveal its properties. The EIS data were fitted and the corresponding equivalent circuits are reported in Figure 6. A classical Randles circuit was successfully applied to fit Au bare ( Figure 6, circuit (b)), while circuit (a) was proposed for better fitting both h-nPG and Au/SWCNTs modified electrodes.
As can be seen in Figure 5, the largest semicircle was obtained with the Au bare electrode, which corresponds to a R ct value of 1540 Ω (Figure 3, panel a). The R ct value progressively decreases with electrode modification, obtaining a R ct value of 92 Ω with Au/SWCNTs (panel b) and of 1 × 10 −6 Ω with h-nPG electrode (panel c), indicating a higher electron transfer rate in the redox probe, thanks to the conductivity of the gold nanostructures. This effect is particularly evident with the h-nPG modified electrode in the low-frequency region, probably because of the interconnected nanoporous structure, suitable for facile electron transport.
The results of the electrochemical fitting by the equivalent circuits are reported in Table 2. Moreover, the kinetic parameters i 0 (exchange current) and k 0 (electron transfer rate constant) have been also determined by EIS measurements [64], using the equations R ct = RT/nF i 0 and i 0 = nFAk • C, where C is the concentration of the redox probe (mol cm −3 ) and A the electrode area (cm 2 ). These results are in perfect agreement with the kinetic parameters obtained by cyclic voltammetry discussed in the previous paragraph. It is interesting to note that with this method the k 0 value for the h-nPG electrode was not evaluated, being the process diffusion-controlled only ( Figure 5, panel c).

L-Ascorbic Acid Sensor
The electrochemical response of AA in 0.1 M phosphate buffer pH = 7.0 has been investigated by cyclic voltammetry at bare and modified gold electrodes, as reported in Figure 7. All CVs show an irreversible reaction without the cathodic peak in the reverse scan, according to the following reaction mechanism, which involves the release of two electrons and two protons [27]:  It appears evident that both peak current and peak position of AA oxidation change with the modification of the electrode surface. Anodic peak currents obtained with Au/SWCNTs and h-nPG modified electrodes exhibit higher peak currents and less positive peak potentials than observed at bare electrode. In particular, the peak current potential of AA oxidation at a bare Au electrode occurs at about 0.55 V vs Ag/AgCl (Figure 7, panel a), decreasing to 0.45 V at Au/SWCNTs electrode (panel b) and to 0 V in the case of h-nPG electrode (panel c). The positive potential shifts accompanied by an increase in the peak currents of AA oxidation show that the modified electrodes have a catalytic effect towards AA oxidation, being the catalytic effect of h-nPG electrode stronger than Au/SWCNTs electrode. This result is consistent with the "discriminative amplification" described by Park et al. [47], which occurs at nanoporous electrodes. The AA exhibits a slow kinetics [66,67] and therefore the AA concentration at the outerpore does not fall to zero and the AA oxidation takes place deeper inside the nanopores. Moreover, structural defects and the low index crystalline faces in inner surface of the pores play a dominant role in enhancing the electron transfer rate [50,68,69]. These effects can explain the improved electron transfer kinetics with the marked shift of the anodic peak potential towards more negative values.
As the oxidation reaction of AA is accompanied by a two-proton transfer (reaction 1) [68], which is facilitated at higher pH values, it is possible that an increase in the pH value would increase the peak currents and shift the peak potentials towards more negative values, as already reported by some authors [40,[70][71][72]. Nevertheless, a pH value of 7.4 in 0.1 M phosphate buffer has been chosen in this study, as it is closer to physiological conditions. Figure 8 shows the linear part of the calibration curves of the modified AA sensors (curves B and C). The calibration curve of the bare Au sensor was reported as comparison The three electrodes showed the same linear range between 5 and 400 µM, with a detection limit (S/N = 3) of 3.8, 3.1 and 1.8 µM for the bare, Au/SWCNTs and h-nPG modified electrode, respectively. The linear range is relatively extended, but it covers the normal range of AA concentration in human urine. The sensitivity resulted strongly enhanced with both nanostructured modified electrodes compared to bare electrode, resulting to be 1.7 × 10 −2 µA µM −1 cm −2 and 2.5 × 10 −2 µA µM −1 cm −2 for Au/SWCNTs and h-nPG, respectively, about 2 times higher values than that determined for the bare gold electrode (1.0 × 10 −2 µA µM −1 cm −2 ).
The h-nPG based sensor showed the highest sensitivity and was therefore chosen for further characterization. The more sensitive differential pulse voltammetry (DPV) technique was also performed with the h-nPG modified electrode. DP voltammograms are reported at different concentration of AA in Figure S1 (Supplementary Materials). The electrode sensitivity resulted to be higher with a linear range linear fitted by equation: I (mA) = 0.01 [AA] (mM) + 11, R 2 = 0.991 between 2 and 800 µM.
It is interesting to underline that very few nPG based sensors have been reported in literature for AA detection. El-Said and Qiu [73,74] used an electrochemical deposition and dealloying method, respectively, for the fabrication of nPG sensors for dopamine (DA) detection in the presence of AA. Differential pulse voltammetry experiments showed two well-separated oxidation peaks, allowing the selective determination of DA in the presence of AA with both sensors, but the aim of these works was the detection of DA, being AA studied only as a possible interferent at a fixed concentration. The h-nPG based sensor showed the highest sensitivity and was therefore chosen for further characterization. The more sensitive differential pulse voltammetry (DPV) technique was also performed with the h-nPG modified electrode. DP voltammograms are reported at different concentration of AA in Figure S1 (Supplementary Materials). The electrode sensitivity resulted to be higher with a linear range linear fitted by equation: I (mA) = 0.01 [AA] (mM) + 11, R 2 = 0.991 between 2 and 800 μM.
It is interesting to underline that very few nPG based sensors have been reported in literature for AA detection. El-Said and Qiu [73,74] used an electrochemical deposition and dealloying method, respectively, for the fabrication of nPG sensors for dopamine (DA) detection in the presence of AA. Differential pulse voltammetry experiments showed two well-separated oxidation peaks, allowing the selective determination of DA in the presence of AA with both sensors, but the aim of these works was the detection of DA, being AA studied only as a possible interferent at a fixed concentration.
Most sensors for AA detection recently reported in literature have been realized through the development of efficient strategies for the modification and/or functionalization of novel electrochemical platforms, based on conductive polymers, metal oxides, metallic nanoparticles and other nanomaterials, such as carbon nanotubes and graphene, or on their combination for a synergistic effect, as reported in Table 3. The proposed h-nPG sensor shows a clear enhancement of the electrochemical performances, in terms of lower detection limit, extended linear range and better stability, compared to other h-nPG based AA sensors reported in literature, as reported in the first three rows of Table 3. Nevertheless, it exhibits a lower sensitivity and a higher LOD value when compared to classical glassy carbon electrodes modified with metal nanocomposite materials [75][76][77][78][79][80][81]. On the other hand, these sensors have known drawbacks, such as long Most sensors for AA detection recently reported in literature have been realized through the development of efficient strategies for the modification and/or functionalization of novel electrochemical platforms, based on conductive polymers, metal oxides, metallic nanoparticles and other nanomaterials, such as carbon nanotubes and graphene, or on their combination for a synergistic effect, as reported in Table 3. The proposed h-nPG sensor shows a clear enhancement of the electrochemical performances, in terms of lower detection limit, extended linear range and better stability, compared to other h-nPG based AA sensors reported in literature, as reported in the first three rows of Table 3. Nevertheless, it exhibits a lower sensitivity and a higher LOD value when compared to classical glassy carbon electrodes modified with metal nanocomposite materials [75][76][77][78][79][80][81]. On the other hand, these sensors have known drawbacks, such as long and complex synthesis of metal nanoparticles, drop casting of the nanomaterial onto the electrode surface, resulting in different loading causing poor reproducibility and stability, and electrode surface biofouling. Conversely, the h-nPG based electrodes have the advantage to show strong antibiofouling features [32] and to be prepared by a simple, fast and reproducible electrodeposition method. List of abbreviations: AuE = gold electrode; PVP = polyvinylpyrrolidone; GCE = glassy carbon electrode; rGO = reduced graphene oxide; HP-ß-CD = hydroxypropyl-b-cyclodextrin; P(Arg) = poly(L-arginine); GO = graphene oxide; AgNPs = silver nanoparticles; Au-PDNs = gold decorated-polydopamine nanospheres; SPCE = screen-printed carbon electrode; AgNC = silver nanocube; PDA-NS = polydopamine nanospheres; poly(PR) = Procion Red MX-5B; TmPO 4 = thulium phosphate; poly-TB = poly-Trypan Blue.

Reproducibility and Stability
The reproducibility of the h-nPG sensor was evaluated and expressed as relative standard deviation (RSD) for n = 8, where n represents the number of sensors used for the test of 10 µM of AA. The RSD value was found 2.54%, attesting that the highly reproducibility of the method.
The stability of the proposed sensor was also studied by measuring the anodic peak current variations of each sensor when stored in pH 7.4 PBS for 1 month at 4 • C. The anodic peak current retained about 98% of its initial value.

Interference Studies
The selectivity of the h-nPG sensor was tested by evaluating the effects of several interfering compounds present in biological fluids on the determination of 100 M AA. Initially, the interference of dopamine (DA) and uric acid (UA) were investigated, as they frequently coexist in biological systems. They are easily oxidized at most conventional electrodes at closed potentials, showing overlapping voltammetric signals. The anodic peaks of AA, DA and UA overlapped at about 0.5 V vs. Ag/AgCl at bare gold electrodes (curves not shown), while at h-nPG electrode the anodic peaks appear well resolved with peak potentials at 0, 0.20 and 0.32 V vs. Ag/AgCl, respectively, as reported in Figure 9, thus not affecting the AA detection. The anodic shift of the peak potentials of AA, DA and UA, which allows their selective determination, can be explained by taking into account that, AA, DA and UA show slow electron transfer reactions [32,47,66]. The concentration of their oxidized forms at the outerpore does not fall to zero, meaning that the reduction of the oxidized species takes place deeper inside the nanopores. This "nanoconfinement effect" results in an improvement of the electron transfer kinetics with a concomitant anodic shift of the peak potentials. urea, and citric acid were checked by adding equal quantities of the interferent and AA. The results are shown in Table 4. No significant influence was observed for all interferences with a relative error lower than 5%.

Real Samples Analysis
The feasibility of the proposed h-nPG sensor for clinical applications was tested by detecting the AA concentration in human urine samples by using the low cost and easyto-use SPEs. The only sample pretreatment required was a proper dilution (1:10 3 ) of the urine samples using 0.1 M PBS pH = 7 in order to fit the linear range of the sensor. Different concentrations of AA were added to three human urine samples supplied from laboratory co-workers. All measurements were performed on a triplicate basis and the results were Successively, other possible interfering species such as glucose, L-cysteine, L-lysine, urea, and citric acid were checked by adding equal quantities of the interferent and AA. The results are shown in Table 4. No significant influence was observed for all interferences with a relative error lower than 5%.

Real Samples Analysis
The feasibility of the proposed h-nPG sensor for clinical applications was tested by detecting the AA concentration in human urine samples by using the low cost and easy-touse SPEs. The only sample pretreatment required was a proper dilution (1:10 3 ) of the urine samples using 0.1 M PBS pH = 7 in order to fit the linear range of the sensor. Different concentrations of AA were added to three human urine samples supplied from laboratory co-workers. All measurements were performed on a triplicate basis and the results were compared with those obtained with a standard spectrophotometric method, by following the absorbance at 570 nm. As shown in Table 5, the results obtained with the two methods resulted in a very good agreement and allowed to ascertain the practical utility of the proposed sensor for the detection of AA in human urine samples.

Conclusions
Two novel electrochemical sensors based on gold electrodes modified with Au/SWCNTs and h-nPG have been realized and utilized for the detection of AA. Both CV and EIS experiments confirmed the high electrochemical performances of the modified electrodes, compared to the bare gold electrode. AA was determined in the linear range 5-400 µM with detection limits of 3.1 and 1.8 µM, with Au/SWCNTs and h-nPG modified sensor, respectively. The higher sensitivity showed by the h-nPG electrode over the bulk gold and Au/SWCNTs electrodes can be attributed to the unique, highly curved morphology that permeates the material, exhibiting a high density of steps and holes, which can facilitate the electron transfer of AA.
Another strength of the proposed h-nPG electrode is its easy preparation method, by a self-templated electrodeposition technique, compared to the dealloying methods reported in literature for the fabrication of h-nPG electrodes for AA detection [32,74,80,81] which means the harsh conditions needed for chemical dealloying can be avoided.
Moreover, the h-nPG sensor was successfully tested with disposable SPEs, properly modified, for accurate detection of AA in human urine samples, with satisfactory results, showing high recovery values. For these reasons, the proposed sensor may have promising potential applications for non-invasive, reliable, fast, cheap and accurate monitoring of AA at the POC.