This protocol demonstrates a method for electrochemical roughening of thin-film platinum electrodes without preferential dissolution at grain boundaries. The electrochemical techniques of cyclic voltammetry and impedance spectroscopy are demonstrated to characterize these electrode surfaces.
This protocol demonstrates a method for electrochemical roughening of thin-film platinum electrodes without preferential dissolution at grain boundaries of the metal. Using this method, a crack free, thin-film macroelectrode surface with up to 40 times increase in active surface area was obtained. The roughening is easy to do in a standard electrochemical characterization laboratory and incudes the application of voltage pulses followed by extended application of a reductive voltage in a perchloric acid solution. The protocol includes the chemical and electrochemical preparation of both a macroscale (1.2 mm diameter) and microscale (20 µm diameter) platinum disc electrode surface, roughening the electrode surface and characterizing the effects of surface roughening on electrode active surface area. This electrochemical characterization includes cyclic voltammetry and impedance spectroscopy and is demonstrated for both the macroelectrodes and the microelectrodes. Roughening increases electrode active surface area, decreases electrode impedance, increases platinum charge injection limits to those of titanium nitride electrodes of same geometry and improves substrates for adhesion of electrochemically deposited films.
Nearly five decades ago, the first observation of surface enhanced Raman spectroscopy (SERS) occurred on electrochemically roughened silver1. Electrochemical roughening of metal foils is still attractive today because of its simplicity over other roughening methods2,3 and its usefulness in many applications like improving aptamer sensors4, improving neural probes5, and improving adhesion to metal substrates6. Electrochemical roughening methods exist for many bulk metals1,5,7,8,9,10. Until recently, however, there was no report on the application of electrochemical roughening to thin (hundreds of nanometers thick) metal films6, despite the prevalence of microfabricated thin-film metal electrodes in a number of fields.
Established methods to roughen thick platinum (Pt) electrodes5,8 delaminate thin-film Pt electrodes6. By modulating the frequency of the roughening procedure and the electrolyte used for the for the roughening, Ivanovskaya et al. demonstrated Pt thin-film roughening without delamination. That publication focused on using this new approach to increase the surface area of platinum recording and stimulation electrodes on microfabricated neural probes. The roughened electrodes were demonstrated to improve recording and stimulation performance and improve adhesion of electrochemically deposited films and improve biosensor sensitivity6. But this approach also likely improves surface cleaning of microfabricated electrode arrays and enhances the capabilities of thin-film electrodes for other sensor applications (e.g., aptasensors) as well.
The approach to roughen thin-film macroelectrodes (1.2 mm diameter) and microelectrodes (20 µm diameter) is described in the following protocol. This includes preparation of the electrode surface for roughening and how to characterize the roughness of the electrode. These steps are presented along with tips on how to optimize the roughening procedure for other electrode geometries and the most important factors to ensure an electrode is roughened nondestructively.
CAUTION: Please consult all relevant safety data sheets (SDS) before use. Several of the chemicals used in this protocol are acutely toxic, carcinogenic, oxidizing and explosive when used at high concentrations. Nanomaterials may have additional hazards compared to their bulk counterpart. Please use all appropriate safety practices when carrying out this protocol including the use of engineering controls (fume hood) and personal protective equipment (safety glasses, gloves, lab coat, full length pants, closed-toe shoes).
1. Cleaning the Pt electrode(s) before initial characterization and surface roughening
2. Electrochemical characterization of the electrode surface before roughening
3. Electrochemical roughening of a macroelectrode
NOTE: Electrochemical roughening is driven by series of oxidation/reduction pulses that result in oxide growth and dissolution. In the case of a weakly adsorbing anion (like HClO4), this dissolution is accompanied by Pt crystallite redeposition while in the case of strongly adsorbing anions (like H2SO4) this process results in preferential intergrain Pt dissolution that creates microcracks in the electrode surface6. Therefore, usage of high purity HClO4 electrolyte is essential to prevent microcracks in the electrode surface.
4. Electrochemical roughening of a microelectrode
5. Characterization of electrode surface after roughening
A schematic showing the voltage application for roughening both macroelectrodes and microelectrodes is shown in Figure 2. Optical microscopy can be used to visualize the difference in the appearance of a roughened macroelectrode (Figure 3) or microelectrode (Figure 4). In addition, electrochemical characterization of the Pt surface using impedance spectroscopy and cyclic voltammetry can readily show the increased active surface area of a roughened macroelectrode (Figure1) and microelectrode (Figure 5). The relationship between surface roughness and the number of roughening pulses applied (pulsing duration) is shown for macroelectrodes in Figure 4. For each new electrode geometry, within both the macroelectrode and microelectrode regimes, optimization of roughening parameters will likely be needed to obtain the ideal roughened surface for different applications. Table 1 presents an example of different roughening parameters to maximally increase electrode active surface area for different electrode geometries.
Figure 1. Roughened Pt macroelectrode electrochemical characterization. (A) Roughness factor as a function of pulse duration during roughening of macroelectrodes (1.2 mm diameter) in 0.5 M HClO4 with Vmax= 1.9 V and Vmin= -0.15 V, 250 Hz pulses applied for differing durations. (B) Cyclic voltammetry (scan rate of 100 mV/s) of a Pt macroelectrode roughened in 0.5 M HClO4 with Vmax= 1.9 V pulse amplitude, 250 Hz 300 s pulsing resulting in a 44x area increase measured in 0.5 M HClO4 before (blue) and after (red) roughening. Please click here to view a larger version of this figure.
Figure 2. Schematic of voltage pulsing paradigm for electrode roughening. Roughening begins with a series of oxidation/reduction pulses between a reductive, typically negative potential (Vmin) and an oxidative, typically positive potential (Vmax) immediately followed by a prolonged, constant application of a reductive potential to fully reduce any oxides produced by pulsing and stabilize the chemistry of the electrode surface. Please click here to view a larger version of this figure.
Figure 3. Optical microscopy images of Pt macroelectrodes. Electrode surface (A) as sputtered before roughening and (B) after roughening in perchloric acid solution. Parameters for roughening are found in Table 1. Each electrode is 1.2 mm in diameter. SEM of the electrode surfaces can be seen in Ivanovskaya, et al.6. Please click here to view a larger version of this figure.
Figure 4. Optical microscopy images of Pt microelectrodes roughened in perchloric acid solution. Parameters for roughening are found in Table1 with the amplitude of Vmax as the only difference between the electrodes shown here. From left to right Vmax = (A) 1.2, (B) 1.3, (C) 1.4 (V vs Ag|AgCl). Each electrode is 20 µm in diameter. SEM of the electrode surfaces can been seen in Ivanovskaya, et al.6. Please click here to view a larger version of this figure.
Figure 5. Roughened Pt microelectrode electrochemical characterization. (A) Impedance of roughened Pt microelectrode (20 µm disk) in PBS. The measured impedance (black circle) over the frequency range of 10 Hz – 100 kHz is shown overlaid by the modelled impedance (red x) from the equivalent circuit model. (B) Cyclic voltammetry (scan rate of 500 mV/s) of Pt microelectrode roughened in 0.5 M HClO4 with Vmax= 1.4 V pulse amplitude measured before (blue) and after (red) roughening. The roughened electrode has a 2.6x increased active surface area calculated from a ratio of roughness factors described in step 2.1.3 (surface roughness before = 1.48, surface roughness after = 3.8). Please click here to view a larger version of this figure.
Potential Pulses | Constant | Roughness factor (a) estimated from CV (b) estimated from EIS |
||||||
Potential | ||||||||
Electrode Geometry | Vmin | Vmax | Frequency (Hz) | Duty cycle | Duration (s) | Potential | Duration (s) | |
(V) | (V) | (V) | ||||||
1.2 mm diameter Pt disk | -0.15 | 1.9 – 2.1 | 250 | 1:1 | 10-300 | -0.15 | 180 | 44 (a) |
20 µm diameter Pt disk | -0.25 | 1.2 – 1.4 | 4000 | 1:3 | 100 | -0.25 | 180 | 2.6 (a) 2.7 (b) |
10 µm diameter Pt disk | -0.25 | 1.1 | 4000 | 1:3 | 100 | -0.25 | 180 | 2.2 (b) |
Table 1. Optimized parameters for roughening of different electrode geometries.
The electrochemical roughening of thin-film macroelectrodes and microelectrodes is possible with oxidation-reduction pulsing. This simple approach does require several key elements to nondestructively roughen thin-film electrodes. Unlike foils, roughening of thin metal films may lead to sample destruction if parameters are not properly chosen. Critical parameters of the roughening procedure are pulse amplitude, duration and frequency. Additionally, ensuring electrode cleanliness and perchloric acid purity prior to the procedure are critical to prevent electrode damage. The presence of organics or contaminates from the microfabrication process can contribute to destruction of the electrode via corrosion or delamination. Therefore, it is critical to ozone clean and solvent soak the device as well as to electrochemically prepare the electrode surface before the roughening begins.
Electrochemical roughening is driven by series of oxidation/reduction pulses that result in repetitive oxide growth and dissolution. In the case of a weakly adsorbing anion (like HClO4), this process is accompanied by Pt crystallite re-deposition. But, in the case of a strongly adsorbing anion (like H2SO4), this process results in microcrack formation due to preferential intergrain Pt dissolution6. The presence of chloride can also cause the destruction of the electrode during the roughening process. For this reason, it also critical to use high purity perchloric acid, a chloride free (or leakless) reference electrode and eliminate any other potential sources of chloride contamination.
If using impedance to estimate the surface area of microelectrodes (step 2.1.4), keep these things in mind. The impedance spectra of a clean Pt electrode in PBS under open circuit conditions should result in a linear Nyquist plot. This linearity indicates a purely capacitive response. Significant bending or deviations from linearity would indicate charge transfer due to the slow kinetics of dissolved oxygen reduction6. In the impedance analysis software, an equivalent circuit model is used to fit curves to this Nyquist plot. This equivalent circuit model consists of ohmic resistance (R) in series with a constant phase element (CPE), where R is composed of the device trace electrical resistance and ionic resistance of the solution and the CPE represents the double layer capacitance at the electrode-solution interface. The CPE parameters of double layer capacitance (Q) and exponent (α) are extracted from fitting the impedance spectra. Typically observed Q values for clean, sputtered Pt in PBS are close to 50 µF/ sα1 cm2 (in good agreement with the range 10-60 µF/cm2 observed on smooth metal electrodes in similar tests6,12).
The electrodes here were all discs of 250 nm thick sputtered Pt, fabricated flush with the flexible polyimide material that insulates the array6,13,14. The roughening parameters will be different for different electrode geometries within the macroelectrode and microelectrode scales (shown in Table1) and will need optimization for new electrode geometries. While not investigated here, there may also be differences in the parameters needed to roughen electrodes of the same geometry based on their topography (e.g., how recessed into the insulating substrate the electrode sits or if the electrode is created through evaporation instead of sputtering). Optimal roughening parameters may depend on the thin-film fabrication techniques used to create the device because the way a film is created may influence grain size and the preferential orientation of Pt crystalline domains in the Pt which may alter the metal reactivity.
With this roughening approach, larger electrodes can withstand a greater Vmax. This larger pulse amplitude enables 10x greater increases in the roughness factor of macroelectrodes compared to microelectrodes. This limits the applicability of the technique for roughening of microelectrodes if a more than 10x increased roughness is needed. Roughened 1.2 mm diameter macroelectrodes with a 44x increase in surface area showed charge injection limits of 0.5 – 1.39 mC/cm2, which are comparable to titanium nitride and carbon nanotube materials and 2 – 4 times greater than untreated platinum samples6.
In addition to the Nyquist plots shown in Figure 5A to characterize roughening's effect on microelectrodes, Bode plots for the impedance of roughened macroelectrodes and microelectrodes are shown in Ivanovskaya, et al6. From these Bode plots, the impedance at 1 kHz for an optimally roughened macroelectrode is 2.5x lower than the electrode before roughening (208.7 kΩ for untreated to 83.7 kΩ for the roughened electrode). And for microelectrodes, the impedance at 1 kHz was lowered ~2x (from 672 kΩ untreated to 336 kΩ for the roughened electrode).
Critical protocol parameters are pulse amplitude, duration and frequency and they need adjustment depending on the electrode size and morphology. When optimizing the roughening parameters for a new electrode type, start with the parameters in Table1 and begin varying Vmax. Fine tuning of the roughness factor (or a desired surface area) can then be achieved by varying pulse duration. While the specific pulsing parameters may need slight modification depending on the electrode geometry, topology and Pt composition, this roughening technique can be used to improve adhesion of electrodeposited films and improve electrode characteristics such as impedance, charge injection limits and charge storage capacity as demonstrated in Ivanovskaya, et al.6.
Recipes for electrochemical roughening of metal foils have existed for nearly five decades1 and electrochemical roughening of metal is still attractive because of the approach's simplicity and utility. But, use of this simple approach to roughen thin-film electrodes was not as straight forward and there was little information available on the procedure to successfully roughen thin metal films. With the approach described here, thin-film electrodes can now be easily electrochemically roughened. These roughened electrodes can be used to improve recording and stimulation electrodes in neural probes, improve adhesion of electrochemically deposited films to substrates, improve biosensor sensitivity, improve thin-film based aptasensor sensitivity, or to clean electrode arrays after fabrication.
The authors have nothing to disclose.
The authors would like to thank Lawrence Livermore National Laboratory's Center for Bioengineering for support during the preparation of this manuscript. Professor Loren Frank is kindly acknowledged for his collaborations with the group that have enabled fabrication and design of the thin-film Pt microarrays discussed in the above work. This work was performed under the auspices of the U.S. Department of Energy by Lawrence Livermore National Laboratory under Contract DE-AC52-07NA27344 and funded by Lab Directed Research and Development Award 16-ERD-035. LLNL IM release LLNL-JRNL-762701.
Acetone | Fisher Scientific, Sigma Aldrich or similar | n/a | Laboratory grade |
EC-Lab Software | Bio-Logic Science Instruments | n/a | For instrument control and data analysis |
Leakless Silver/Silver Chloride Reference | eDAQ Company, Australia | ET069-1 | Free from chloride anion contamination (or other type of chloride free electrode e.g. Mercury sulfate electrode) |
Mercury Sulfate & Acid Electrode Kit | Koslow, Scientific Testing Instruments | 5100A | glass, 9mm version |
Milipore DI water | MilliporeSigma | n/a | Certified resistivity of 18.2 MΩ.cm (at 25°C) |
Perchloric acid, 99.9985% | Sigma Aldrich | 311421 | High Purity |
Phosphate-buffered saline | Teknova | P4007 | 10mM PBS with 100mM NaCl, pH 7 or similar product from elsewhere |
Platinum Wire Auxiliary Electrode (7.5 cm) | BASi | MW-1032 | Counter electrode |
Pt macroelectrodes | Lawrence Livermore National Laboratory | n/a | 1.2 mm diameter, 250 nm thick Pt disc electrodes insulated in polyimide. More information in Reference 9. |
Pt microelectrode arrays | Lawrence Livermore National Laboratory | n/a | 20 µm diameter 250 nM thick Pt disc electrodes insulated in polyimide. More information in Reference 9. |
Sulfuric acid, 99.999% | Sigma Aldrich | 339741 | High Purity |
UV & Ozone Dry Stripper | Samco | UV-1 | for cleaning electrodes |
VersaSTAT 4 Potentiostat | AMETEK, Inc. | n/a | Good time resolution for pulsing tests |
VersaStudio Software | AMETEK, Inc. | n/a | For instrument control |
VMP-200 Potentiostat | Bio-Logic Science Instruments | n/a | Low current resolution option is preferable for measurements with microelectrodes |