R. Poplausksa,
U. Malinovskisa,
J. Andzanea,
J. Svirkstsab,
A. Viksnaab,
I. Muiznieksc and
D. Erts*a
aInstitute of Chemical Physics, University of Latvia, Riga, Latvia. E-mail: donats.erts@lu.lv
bDepartment of Chemistry, University of Latvia, Riga, Latvia
cDepartment of Biology, University of Latvia, Riga, Latvia
First published on 24th September 2014
Electrochemical etching of metal wires is widely used to fabricate sharp probes for use in scanning tunnelling microscopy. In this work an electrochemical fabrication method for sharp aluminium probes coated with nanoporous anodised aluminium oxide (AAO) layer is described. The method presented here involves simultaneous anodisation and etching of aluminium wires. The probe apex radius as well as the nanopore length and diameter depend on the etching mode, which could be direct current (DC), alternating current (AC), or pulsed voltage mode (PVM). The probes, coated with a nanoporous AAO layer, were used to demonstrate addressed DNA delivery.
In this paper we present an electrochemical method for fabricating sharp Al probes coated with a nanoporous anodised aluminium oxide (AAO) layer.8 It is one of the most popular and promising materials for template assisted growth of nanostructures9 and for other applications (such as for catalysts, immobilisation enzymes,10 DNA hybridisation and filtration,11,12 sensors,13 and nano-tips14,15). We also demonstrate the application of AAO coated nanoprobes to addressed DNA delivery into the cytoplasm of selected plant cells.
The etching and anodisation was performed at room temperature using three different regimes: alternating current (AC), direct current (DC), and pulse voltage mode (PVM). A homemade two-electrode electrochemical cell and a programmable (±30 V range) voltage source was used to generate rectangular pulses with duration from 10 μs to 1 s, which were applied to the electrodes, the aluminium wire, and a sheet of platinum, which had ∼10 times larger surface area than the aluminium surface. The electrodes were placed inside a 50 mL beaker filled with the electrolyte solution. The immersion depth of the aluminium wire was 2–3 mm. The electrolyte was not stirred during the etching/anodising process in order to reduce the risk of probe apex damage during fabrication. The etching/anodising process was controlled by visual observation under an optical microscope and stopped when the length of the immersed aluminium wire decreased to 0.5–1 mm. After the etching/anodising, the probes were immediately withdrawn from the electrolyte, rinsed with deionised water and allowed to dry naturally at room temperature. The structure of the fabricated probes was investigated by a scanning electron microscope (Hitachi S 4800).
DNA transportation experiments with AAO probes were done using a homebuilt system, which consists of a 3D micromanipulator (SIGNATONE 96MW-MML) placed on an epifluorescent inverted microscope (OLYMPUS IX-71) with a long working distance (10 × 0.3 NA) objective lens. Such a system allowed direct and simultaneous observation of the positioning of the whole probe as well as the DNA sorption/desorption process on the surface of the probe. Detection of the DNA movement into and out of the porous AAO was based on the observation of the colour and intensity of the fluorescence from the whole probe surface. However, this system did not allow precise quantification of the sorbed/desorbed DNA solution. A quartz tuning fork (TF) with an attached probe was mounted on a micromanipulator and used to control the distance between the apex of the probe and the counter electrode/cell surface. The TF oscillation frequency and amplitude were registered and managed using an AFM controller (Nanonis OC4).
Lambda bacteriophage DNA was cut with restriction endonuclease Eco130I (Fermentas), precipitated with isopropanol, dissolved in TE buffer (10 mM TRIS, 1 mM EDTA, pH 8) and labelled with the intercalating dye ethidium bromide (Abmax300 and 360 nm, Emmax 590 nm). The quality and concentration of the DNA achieved from the above process were determined by agarose gel electrophoresis and UV spectrophotometry (Amersham Ultraspec 3110). Single stranded DNA with 6-carboxyfluorescein (Abmax 495 nm, Emmax 520 nm) attached to the 5′ end (5′FAM – GAGATCGGATTGAGGAGGTC, green fluorescent dye) from MWG-Biotech AG was dissolved in TE buffer.
A significant improvement could be achieved using concentrated acid solutions and rapid switching between the etching and anodising processes. This solution provided a surface anodising process, intensive oxide dissolution, and the formation of the probe apex. Experiments showed that probes coated with an AAO layer could be obtained using electrolytes composed of a mixture of 98% H2SO4, 85% H3PO4, and H2O with a volume ratio in the range of 1:
0–2
:
0.5–4 and a voltage interval of 19–35 V for the DC and 11–18 V at 50 Hz for the AC regimes. Phosphoric acid was added to the etching electrolyte solution on purpose to increase the AAO etching rate. The formation of an AAO layer in the phosphoric acid electrolyte occurs at a bias voltage starting from 80 V.17,18 At our applied voltage of 10–35 V DC it worked just like an AAO dissolving agent. We found that the optimal electrolyte to obtain probes of the best quality is a mixture of sulphuric and phosphoric acids with water in a ratio of 1
:
1.2
:
2. Depending on the required probe parameters, which are the probe apex radius, the pore length and the pore diameter, several electrochemical etching modes could be used to obtain the required result.
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Fig. 2 SEM images of (a) an aluminium probe with AAO coating fabricated by the DC mode at a constant current of 100 mA and (b) apex of the same probe. |
The cross-section structure of the DC-etched probes was investigated to find the pore length and test for the presence of a metal core inside the probe. Fig. 3 shows SEM images of the cross-sections of the DC-etched probes. The probes for the cross-section investigation were randomly selected. In both samples a metal core was present (Fig. 3a and b). The observed pore length can reach 4000 nm at a distance of 50 μm from the probe apex (Fig. 3a) and approx. 1000 nm at a distance of 10 μm from the probe apex (Fig. 3b). The cross-section images also demonstrate that a thick AAO layer formed along the straight planes instead of forming radially along the Al wire surface. Such AAO layer formation results in its splitting between the different planes (Fig. 3a) due to mechanical stress between the straight planes formed on the conical surface.19 The cracked areas at the aluminium surface were covered with a thin, porous AAO layer (Fig. 3c).
The drawback of the DC etching method was aluminium surface passivation, which results in an untimely termination of the probe etching process. The process could be re-established by increasing the applied voltage to the probe. In such cases the etching and anodising process was reinitiated spontaneously and with very high intensity. The average yield of good quality probes fabricated by the DC method was about 10%.
When pore lengths below 150 nm were required, it was preferable to use the AC etching mode, which enables alternating anodising and cathodising processes at the aluminium surface. The cathodising process caused by the negative half-period of the AC bias resulted in intensive etching of the probe surface in addition to the primary etching by phosphoric acid. Cathodising could be explained as a partial etching of an AAO layer previously formed during the positive half-period of the AC voltage cycle as a result of an increase in the concentration of hydrogen ions next to the AAO surface as a result of water hydrolysis:21
Al2O3 + 6H+ → 2Al3+ + 3H2O | (1) |
It was found that a nanoporous layer formed at the probe surface when the applied AC bias was between 11 and 18 V. The best quality probes were obtained at 14–15 V AC bias (Fig. 4a). Probes fabricated in the AC mode had a pronounced conical apex structure. Investigation of the cross-section of randomly chosen probes showed that the nanopore length was approximately 150 nm (Fig. 4b) and apex radii varied in the range of 250–1000 nm.
The width of the positive pulse was selected based on the data from the kinetic curve of the electrical current density for the anodising process of planar surfaces in a standard (20 V DC, 0.3 M H2SO4) electrolyte solution20–22 (Fig. 5 inset). This kinetic curve depicts the time intervals during which the bottom AAO barrier layer of the pores (I) and the base of the pores (II) were formed. Region (III) of the curve indicates the process of pore growth and the increase of the coating thickness.
For the sharp probe apex formation to occur, the speeds of the anodising and etching processes must be balanced. The width of the positive pulses was controlled in real time to mimic the current changes of the kinetic curve to be equal to the length of region I, which stops at the lowest point of the kinetic curve in the inset of Fig. 5. At that point, the pulse polarity was switched to negative. Switching from positive to negative pulses occurred in the automatic regime if the current remained constant or increased during three successive measurements (the time interval of one measurement was 2.5 ms). If the positive pulses were wider, the kinetic process would move to region II, pores would start to be formed, and the AAO layer would grow in thickness and reduce the speed of the probe apex etching.
The best quality probes were obtained using a mixture of sulphuric and phosphoric acids with water in a 1:
1.2
:
2 ratio as electrolyte and a the positive pulse amplitude between 10 and 25 V. At higher pulse amplitudes intensive side reactions (release of gases) started impeding the formation of the pores. At lower positive pulse amplitudes it was not possible to obtain sharp probe apexes.
The cathodising process occurred during the negative pulse and, similarly to the AC regime, (1) resulted in partial or full dissolution of the AAO barrier layer formed during the time of the previous positive pulse. As can be observed from the current–time curve (Fig. 5), the electrical current during the negative pulse was higher than during the positive pulse of the same value. This observation corresponds to partial etching of the AAO layer during the negative pulse. This process promotes further the probe apex etching reaction. The optimal amplitude and width of the negative pulse were chosen experimentally based on the quality of the obtained probes. The amplitudes of the negative pulses were between 5 and 12 V. The reduction of the current amplitude during the positive pulse after 46 seconds of anodising/etching (Fig. 5) is caused by a decrease of the probe surface and indicates that the probe formation has finished, and the etching/anodising process should be interrupted.
The negative pulse current decrease was accompanied by current fluctuations (Fig. 5) whose nature is not understood yet.
The control of the proportion of negative and positive pulses during etching/anodising process in the PVM mode allowed obtaining sharper probe apexes than in the AC or DC modes. It was possible to obtain probes with apex radii down to 80 nm (Fig. 6).
A drop of ethidium-bromide-labelled Eco130I-digested λ bacteriophage DNA solution (1 μL, 10 ng μL−1) was deposited on ITO glass. To check the ability of the probe to transfer and deliver the DNA molecules, the probe was immersed into this drop (Fig. 7, position 1). For the DNA electrophoretic sorption, a positive voltage of 0.5 V was applied between the probe and the ITO substrate. Then the nanoporous probe filled with the DNA molecules was withdrawn from the DNA solution drop and moved into the TE buffer solution drop (Fig. 7, position 2) for the DNA desorption process. The DNA sorption and desorption processes were visually detected by observing the colour and intensity of the fluorescence of the probe (Fig. 8).
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Fig. 8 Process of sorption (a–c) and desorption (d–f) of DNA molecules marked with ethidium bromide to- and from- the pores of a fabricated probe. |
The absorption process of the DNA substance could be controlled by varying the sorption time (Fig. 8). At the beginning of the DNA sorption process, the probe fluorescence colour was blue, which corresponds to the AAO fluorescence (Fig. 8a). Thirty seconds after the beginning of the DNA sorption process, the probe fluorescence colour turned to orange (Fig. 8b), and its intensity increased with time (Fig. 8c). The orange colour matched the fluorescence colour of the ethidium-bromide-marked, double-stranded DNA molecules used for this test and established the DNA sorption by the pores of the probe. For the DNA desorption from the pores, the voltage applied between the probe and the ITO substrate was switched from positive to negative of the same magnitude (−0.5 V). Fig. 9d–f illustrate the DNA desorption from the probe when the fluorescence colour changed from orange to blue as the DNA molecules were desorbed from the pores.
To test the AAO probe's suitability for DNA delivery into plant cells, Allium cepa (onion) epidermal cells were used. 5′-FAM-labelled, single-stranded DNA dissolved in TE buffer solution (DNA concentration 10 μM) was used for the delivery into the A. cepa cells. A freshly prepared A. cepa cell monolayer was placed on a clean ITO slide serving as electrode (Fig. 7, position 3). To prevent drying of the cells, they were continuously moisturised using filter paper strips saturated with buffer solution. For the DNA delivery, the probe was positioned above the chosen cell. The probe position was defined, and the probe was moved to the drop with DNA molecules (Fig. 7, position 1) and immersed into it for 5 minutes for the DNA electrophoretic sorption. After the DNA sorption process was finished, the probe was returned to the previously defined position above the selected cell and lowered until it penetrated the cell. When the plant cell wall and plasma membrane were pierced, the DNA molecules were desorbed from the probe pores into the cytoplasm of the cell.
Fig. 9 illustrates the delivery of the DNA molecules into the cell: Fig. 9a and b show the surface of the cell monolayer respectively before and after the penetration by the probe followed by the DNA desorption. In Fig. 9b the footprint of the probe surrounded by a bright fluorescent spot of delivered DNA molecules is clearly seen, indicating that the DNA molecules were successfully delivered into the cytoplasm of the cell.
The fabricated probes were used to demonstrate addressed delivery of DNA molecules into the cytoplasm of plant cells. Further development of the experimental setup for the addressed DNA delivery is required to enable accurate dosage of the delivered DNA solution. An improvement of this experimental setup could include direct (detection of fluorescence) and indirect (e.g., quantitative polymerase chain reaction) methods for the precise quantification of sorbed/delivered DNA.
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