Huajun
Qiu
*ac,
Liang
Li
b,
Qiaolin
Lang
b,
Feixue
Zou
a and
Xirong
Huang
a
aSchool of Chemistry and Chemical Engineering, Shandong University, Jinan, 250100, China
bQingdao Institute of Bioenergy and Bioprocess Technology, Chinese Academy of Sciences, Qingdao, 266101, China
cSchool of Chemical and Biomedical Engineering, Nanyang Technological University, 70 Nanyang Drive, Singapore 637457. E-mail: qiuhuajun@gmail.com
First published on 6th February 2012
We, the named authors, hereby wholly retract this RSC Advances article. Signed: Huajun Qiu, Liang Li, Qiaolin Lang, Feixue Zou and Xirong Huang, China, September 2012. Retraction endorsed by Sarah Ruthven, Managing Editor. Retraction published 26 September 2012.
Metal nanorods/nanowires (especially aligned nanorods/nanowires with hollow interiors or tailored porosity) have attracted wide interest due to their intriguing physicochemical properties, and are applicable in important fields including catalysis,23 biological labeling,24 surface-enhanced Raman scattering,25–27 electrogenerated chemiluminescence,28,29etc. For the fabrication of these one-dimensional nanostructures, template-based synthesis is one of the most widely used routes.30–33 For example, AuAg alloy nanorods have been prepared by electrodeposition using porous alumina as the template, and then the AuAg nanorods are chemically/electrochemically dealloyed to obtain nanoporous gold nanorods.30,33 The same strategy has also been used for the fabrication of nanoporous PtCo and PtNi nanowires.23,34 In another fabrication strategy, dispersed (not aligned) nanoporous gold nanowires can be obtained by galvanic replacement reaction between Ag nanowires and HAuCl4 at a high temperature of 100 °C.35 However, these methods require template preparation and removal (porous alumina template) or the excessive use of surfactants and high temperatures (Ag nanowire template). Moreover, these methods are not quite suitable for large scale fabrication.
Recently, dealloying, which refers to selective dissolution of one or more components out of an alloy, has been demonstrated to be an ideal method to fabricate three-dimensional (3D) nanoporous metals with bicontinuous ligament/pore structure.36–42 Nanoporous metals prepared by dealloying have some unique properties such as adjustable pore/ligament size, excellent electron conductivity, extremely clean ligament surface, etc. and have been widely investigated in applications such as catalysis, sensing, SERS, and so forth.25,27,38,43–52 It is generally recognized that ideal bicontinuous nanoporous structures are obtained from dealloying binary alloys with a single phase solid solubility across all compositions (like AuAg alloy).36 In comparison with the single phase alloy system, less attention has been paid to the dealloying of two-phase or multiphase alloy systems and the resulting products. In theory, for a two-phase system, if one phase can be dealloyed and another not, a two phase alloy can be used to fabricate porous/nonporous metal composites. If the two phases can be separately dealloyed, then nanoporous metal composite with two kinds of nanoporous metals or two different pore size distributions can be obtained. For example, by dealloying AuAl alloy which contains Al2Au and AlAu phases, nanoporous gold with two pore size distributions can be obtained.42 If one phase is entirely removed and another is dealloyed, the dealloying of the two phase alloy leads to nanoporous metals with bimodal channel/pore size distributions.40 The big channels are formed by the entire removal of one metal phase; while, the small channels/pores result from the selective dissolution of an alloy phase. However, what can we obtain if multiphase alloy systems are dealloyed? The multiphase system may contain metal phase which can be completely removed and different alloy phases which can be selectively dealloyed. In the present work, we report that by one-step dealloying PtNiAl ternary alloy containing multiple alloy phases in NaOH solution, aligned np-PtNi alloy nanorod-like structures can be successfully fabricated. The mechanism of the formation of aligned nanorods is discussed. Moreover, the aligned np-PtNi nanorods have greatly enhanced electrocatalytic activity and sensing performance towards some small molecules such as alcohols and hydrogen peroxide. After being loaded with glucose oxidase (GOx), a sensitive glucose biosensor is also fabricated.
XRD is used to examine the phase structures of the PtNiAl ternary alloy and the dealloyed sample (Fig. S2, ESI†). For the ternary alloy, due to the large content of Al, a pure Al phase exists. The other diffraction peaks are complex and can be ascribed to different Al-based alloy phases such as Al3Ni, Al6Pt, Al3Ni2, etc. indicating the existence of multiple alloy phases in the precursor alloy. However, it is interesting to find that after the 24 h dealloying, accompanied with the complete removal of Al, a uniform PtNi alloy structure is obtained. One can see from Fig. S2 (ESI†) that the dealloyed sample shows a set of three diffraction peaks which are assigned to the (111), (200), (220) reflections of face-centered cubic structure. No peaks from pure Ni (or its oxides) as well as Pt-Ni ordered alloy phase are observed, which suggests the formation of disordered single-phase PtNi alloy. As compared with the standard diffraction pattern of Pt, all diffraction peaks for the dealloyed sample shift to higher angles due to the substitution of smaller Ni atoms in Pt crystal lattice. Notably, the diffraction peak from (111) diffraction are more pronounced, while those from (200) and (220) diffraction are so weak that they are barely discernible. This indicates that the PtNi alloy is primarily dominated by (111) facets.
Fig. 1a and 1b show the plan-view and section-view, respectively, of SEM images of the dealloyed sample. It can be observed that the resulted sample consists of well-aligned nanorod-like structures with a diameter of 200–500 nm (Fig. 1a) and a length of over 1 μm (Fig. 1b). Fig. 1c is the enlarged SEM image of the nanorods, which shows bicontinuous ligament-pore structure with the ligament size of ∼3 nm. The clear contrast between the dark skeletons and inner bright pores in the TEM image (Fig. 1d) further indicates the formation of an open interconnected network structure within each nanorod. HRTEM image (Fig. 1e) provides more details for this structure, in which the continuous lattice fringes are well resolved around the whole pore, indicating the formation of single-crystalline interconnected ligaments. It is noted that most of the exposed facets are along (111) planes with the lattice spacing measured to be 0.215 nm which is in accordance with the value calculated by Vegard's law. The result that most exposed facets are along (111) planes is also in excellent agreement with that obtained from the XRD study.
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Fig. 1 SEM images of np-PtNi nanorod-like structure [plan-view, (a); section-view, (b); enlarged SEM image, (c)], TEM (d) and HRTEM (e) images of the sample. |
XPS is further used to examine the surface properties of np-PtNi. Fig. S3a in the ESI† shows the Ni 2p spectrum of np-PtNi nanorods. The spectrum shows the presence of metal Ni as well as Ni oxide and hydroxides (NiO, Ni(OH)2, and NiOOH). The Ni 2p spectrum shows a complex structure with an intense satellite signals at high binding energy adjacent to the main peaks, which can be attributed to multielectron excitation.5 The Ni 2p XPS peaks at the binding energies of 852.7, 853.8, 855.6, and 857.3 eV correspond to Ni0, NiO, Ni(OH)2, and NiOOH, respectively 5. Fig. S3b in the ESI† presents the XPS spectra of the Pt 4f region for the np-PtNi nanorods. The two peaks can be ascribed to metal Pt and no signals related to oxidized Pt species are observed. The electronegativity difference between Ni and Pt (1.9 and 2.2, respectively) implies an electron-withdrawing effect of Pt from the neighbouring Ni atoms, which makes the latter more difficult to reduce.
It is very interesting to find that by a simple dealloying of PtNiAl alloy, aligned nanoporous nanorod-like structure with uniform PtNi alloy ligament can be successfully fabricated. The dealloying process has been widely studied in previous work. Most of these studies are focused on dealloying of binary alloy such as AgAu alloy for the preparation of nanoporous gold (NPG).54 The formation mechanism has been discussed according to corrosion disordering/diffusion reordering model, dynamic roughening transition model and kinetic Monte Carlo model.55,56 However, in the present case, for the PtNiAl ternary alloy with multiple alloy phases, the dealloying process and formation mechanism of the aligned nanoporous nanorod-like structure are obviously more complicated. We assume that the dealloying of the ternary alloy started firstly with the pure Al phase (the most active component). The removal of pure Al phase would result in the formation of the large channels in the alloy. The formed large channels also facilitate the diffusion of the dealloying solution and the further dealloying of AlNi and AlPt alloy phases. Accompanied with the removal of Al in the AlNi and AlPt alloy phases, the remaining Ni and Pt adatoms on the alloy/solution interface will interdiffuse to form PtNi alloy ligaments and nanopores. It is reasonable to believe that these different Al-based alloy phases should be very close to each other and the interdiffusion and interaction between the left Pt and Ni must be very strong, which results in the formation of uniform PtNi alloy instead of hybrid of nanoporous Pt and nanoporous Ni. To explain the formation of nanorod-like structures, due to the coexistence of multiple alloy phases, it is assumed that as the pure Al phase is etched away the remaining Al-based alloy phases might also go through a fast self-assembly process to form aligned nanorod-like structures. On the other hand, it is quite possible that in the precursor PtNiAl alloy, these Al-based alloy phases exist in the form of nanorods and after the dealloying, the nanorod-like structure is maintained. The exact mechanism still needs further investigation.
Fig. 2a shows the cyclic voltammograms (CVs) of np-PtNi and Pt/C catalyst in 0.5 M H2SO4 + 1.0 M ethanol solution. It is observed that the anodic peak in the forward scan locate at 0.90 V for np-PtNi, which is much lower than that of the Pt/C catalyst (0.95 V), indicating more favorable ethanol oxidation on the alloy nanorod electrode. More importantly, the specific current density of np-PtNi is about 2.5 times that of Pt/C. To explain the enhanced electrocatalytic activity of np-PtNi, the presence of Ni oxygenated species on np-PtNi surface would provide rich oxygen source for COads oxidation during alcohol electrooxidation and leave the active sites of Pt for further reaction (i.e., bifunctional mechanism).5 The electronic structure modification of Pt by the interaction with Ni (demonstrated by the XPS study) should also contribute to the enhancement. Moreover, compared with Pt/C catalyst, the 3D bicontinuous spongy structure within each nanorod provides good transport channels for electrons and small molecules, which should effectively facilitate the reaction kinetics on the nanoporous nanorod electrode.
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Fig. 2 CVs of np-PtNi and Pt/C electrodes in 0.5 M H2SO4 + 1.0 M C2H5OH solution, scan rate: 50 mV s−1 (a); current responses of np-PtNi and Pt/C electrodes on successive addition of C2H5OH in 0.5 M H2SO4 solution at 0.9 V (b); inset of (b) is plots of current at 0.9 V versus C2H5OH concentrations. |
For ethanol electro-oxidation, two anodic peaks are observed in one potential cycle. The anodic peak in the forward scan is ascribed to the oxidation of freshly adsorbed ethanol molecules on the electrode surface, and usually used for the evaluation of catalyst activity. However, there are still controversies about the origin of the oxidation peak during the backward scan. Some thought that the anodic peak in the backward scan was attributed to the oxidation of incompletely oxidized carbonaceous intermediates accumulated on the catalyst surface during the forward scan.7 While others believed that the reverse current peak cannot be ascribed to the intermediate species removal, and should originate from the oxidation of the fresh molecules on reduced (re-activated) Pt surface because they experimentally demonstrated that most intermediates are removed when the potential is over 0.6 V vs. RHE (using methanol as model).6 Here, we observe that by increasing the scan rates, the ratio of the forward anodic peak current (If) to the backward anodic peak current (Ib) decreases (If/Ib is 0.67 at 100 mV s−1 and 0.94 at 10 mV s−1, Fig. S4†). It is known that in the forward scan, a faster scan rate usually causes insufficient molecule oxidation producing more intermediates, thus the decreased If/Ib with increasing scan rates might be due to more intermediate oxidation in the backward scan. Therefore, the reverse current peak might be indeed related to the oxidation of intermediates. However, the large peak current density in the backward scan cannot exclude the oxidation of fresh alcohol molecules on re-activated Pt surface. It is possible that both the oxidation of intermediates and fresh molecules attribute to the large reverse peak current.
To get more insights into the enhanced electrocatalytic activity of np-PtNi, CO electro-stripping experiment was carried out. As shown in Fig. S5 (ESI†), the CO stripping peak on np-PtNi locates at 0.74 V, which is greatly negatively shifted (by ∼100 mV) compared with that on Pt/C (0.83 V). The current density for CO electro-oxidation on np-PtNi is also smaller than that on Pt/C. These results indicate that the CO adsorption is much weaker on the np-PtNi than on Pt/C. In other words, the np-PtNi is much more tolerant to CO poisoning. The weak CO adsorption should be due to the electronic modification of Pt through interaction with Ni and the existence of surface Ni oxygenated species.
The analytical performance of np-PtNi is evaluated by recording its amperometric response to successive addition of ethanol into the electrolyte (Fig. 2b). The two electrodes respond quickly and sensitively to each addition of ethanol. The np-PtNi exhibits a much higher sensitivity and wider linear range (up to 16 mM, R = 0.997) with the detection limit of ∼20 μM (inset in Fig. 2b). The enhanced electroanalytical performance of the np-PtNi is clearly due to its higher electrocatalytic activity and better resistance to CO poisoning. This linear range is wider than those of some alcohol dehydrogenase (ADH)-based electrochemical ethanol sensors such as ADH/NPG (1.0–8.0 mM),43 ADH/carbon nanotubes (CNT) (0.5–5.0 mM)58 and ADH/ reduced graphene oxide (0.9–10 mM).59
In addition to the remarkably increased electrocatalytic activity towards ethanol oxidation, np-PtNi also exhibits enhanced electrocatalytic activity towards the oxidation/reduction of H2O2, an essential mediator in food, pharmaceutical, clinical and enzymatic reaction. Fig. 3 shows CVs of np-PtNi and Pt/C electrodes in 0.1 M PBS (pH 7.0) in the presence and absence of 10 mM H2O2. It is observed that compared with Pt/C electrode (Fig. 3b), the np-PtNi electrode exhibits both higher oxidation current starting from ∼0.25 V during the forward scan and higher reduction current starting at ∼0.53 V during the backward scan in the presence of 10 mM H2O2 (Fig. 3a). In particular, it is noted that on Pt/C electrode, the current for H2O2 reduction starts at ∼0.42 V which is ∼0.11 V negatively shifted compared with that on np-PtNi. The more positive onset potential and much higher current density for H2O2 reduction on np-PtNi indicate that the as-prepared nanoporous alloy nanorods have greatly enhanced electrocatalytic activity towards H2O2 reduction.
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Fig. 3 CVs of np-PtNi (a) and Pt/C (b) electrodes in PBS (0.1 M, pH 7.0) with and without 10 mM H2O2, scan rate: 50 mV s−1. |
Fig. 4 shows the amperometric responses of the two electrodes on successive addition of H2O2 into the stirring PBS at 0.1 V. As observed, the two electrodes respond rapidly to the addition of H2O2 and reach the maximum steady-state currents within 4 s. The np-PtNi electrode has a higher current response compared with Pt/C electrode. This result is also in good agreement with the results obtained from the CV study. As shown in the inset of Fig. 4, np-PtNi electrode exhibits linear response to H2O2 concentration up to ∼2.0 mM (R = 0.996) with a detection limit of 0.5 μM, which is lower than certain horseradish peroxidase (HRP) and carbon nanotube (CNT)-based biosensors.60–62 The reproducibility of the np-PtNi electrode has also been studied. For the same electrode, the relative standard deviations (RSD) for 0.4 mM H2O2 are 3.6% for five measurements. For five np-PtNi electrodes, the RSD is 4.6%. The nanoporous nanorod electrode also shows good long-term stability. The electrode was tested for the detection of 1.0 mM H2O2 every three days for one month and the current response retained ∼95% of the initial value.
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Fig. 4 Amperometric current responses of np-PtNi and Pt/C electrodes on successive addition of H2O2 into the stirring PBS (0.1 M, pH 7.0); applied potential: 0.1 V; inset is plots of current versus H2O2 concentrations. |
The stability of electrocatalysts under long-term electrochemical operation conditions is important for their practical applications as both fuel cells and electrochemical sensors. The structure stability of np-PtNi under long-term continuous potential cycling from 0.6 V to 0.9 V in 0.5 M H2SO4 solution was studied by monitoring the change of its EASA (Fig. S6 in ESI†). It is observed that the EASA of Pt/C suffers a significant loss (∼75% remained) after 5000 cycles, while that of the np-PtNi nanorod retains more than 90% of its initial value, indicating that alloying Pt with Ni greatly improves the structure stability.
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Fig. 5 Amperometric current responses of GOx/np-PtNi and GOx/Pt/C electrodes on successive addition of glucose into the stirring PBS (0.1 M, pH 7.0); applied potential: 0.1 V; inset is plots of current versus glucose concentrations. |
The much higher current response on the GOx/np-PtNi is obviously due to the higher electrocatalytic activity of np-PtNi towards H2O2 reduction. Moreover, np-PtNi with bimodal porosity, i.e., big channels obtained from the removal of pure Al phase and nanopores obtained from the selective dealloying alloy phases, is more favorable for both GOx immobilization in the big channels and the free mass transfer of small molecules (e.g. substrates and products of GOx) through the nanopores. Note that the small nanopore size (4–6 nm) would be not possible for GOx (∼8 nm in diameter)64 getting into the inner pore the nanorods.65
To evaluate the practical application of the np-PtNi-based biosensor, two real samples (liquor and glucose injection) were tested. The results obtained with this biosensor are in good agreement with the values certified by the manufacturers (Table S1, ESI†) indicating that this biosensor is accurate for real sample determination.
Footnote |
† Electronic supplementary information (ESI) available: See DOI: 10.1039/c2ra01308h |
This journal is © The Royal Society of Chemistry 2012 |