Zhenghong
Gao
a,
Chunyi
Zhi
b,
Yoshio
Bando
b,
Dmitri
Golberg
b,
Makoto
Komiyama
c and
Takeshi
Serizawa
*d
aDepartment of Advanced Interdisciplinary Studies, The University of Tokyo, 4-6-1 Komaba, Meguro-ku, Tokyo, 153-8904, Japan
bInternational Center for Materials Nanoarchitectonics (MANA), National Institute for Materials Science (NIMS), Namiki 1-1, Tsukuba, Ibaraki, 305-0044, Japan
cResearch Center for Advanced Science and Technology (RCAST), The University of Tokyo, 4-6-1 Komaba, Meguro-ku, Tokyo, 153-8904, Japan
dDepartment of Organic and Polymeric Materials, Tokyo Institute of Technology, 2-12-1-H121 Ookayama, Meguro-ku, Tokyo, 152-8550, Japan. E-mail: serizawa@polymer.titech.ac.jp
First published on 11th June 2012
We report that efficiently disentangled boron nitride nanotubes (BNNTs) can be obtained due to functionalization in an aqueous solution with a natural water-soluble polysaccharide, gum arabic (GA). An atomic force microscopy study showed excellent dispersion of GA-functionalized BNNTs in the aqueous phase. Fluorescent, ultraviolet, and infrared absorption spectroscopies revealed the strong interactions between GA and the sidewalls of BNNTs. Subsequently, several functional proteins were successfully immobilized onto the surfaces of GA-functionalized BNNTs via strong electrostatic interactions under suitable pH conditions.
Boron nitride nanotubes (BNNTs) are of increasing interest because of their peculiar shapes and unique physicochemical properties. In view of its molecular structure, BNNT is similar to carbon nanotubes (CNTs), and almost no changes in the tube's structural parameters are evident, except that B and N atoms alternatively substitute C atoms in a graphene-like network.9 However, the properties of BNNTs are dramatically distinctive from those of CNTs in many aspects.9 For example, the band-gap of BNNTs is independent of tube's chirality and geometry, while the corresponding properties of CNTs complicatedly correlate with those.10 The BNNT's resistance to oxidizing agents and robustness at high temperatures is also superior to those of CNTs. Because of these unique physiochemical properties, BNNTs are very promising nanomaterials in chemistry and physics, particularly for the development of new nanobiotechnologies.
In many cases, BNNTs factually exhibit superior performances over their C counterparts.10–12 For example, first, the highly thermostable nanoscale inner channels of BNNTs provide a perfect confined space for the controllable growth of semiconducting nanowires and the linear assembly of functional nanoparticles along the channels.13,14 Second, either B or N sites within BNNTs are available for selective chemical activation.15,16 These properties make BNNTs ideal candidates for use as cargo or vectors for massive loading of drugs or biomolecules on both their outer and inner sidewalls via diverse chemical methodologies. Moreover, a typical external multi-walled BNNT diameter ranges from several nanometers to around 80 nm.17 Such a polydispersed size of the material could increase the chance of immobilization since the nanostructures may select the nanotube of suitable diameter for making an ensemble.18
However, until now, many prospective applications of BNNTs are still hampered because of several issues. First, similar to their C analogs, BNNTs are insoluble in standard solvents, such as milli-Q and general buffers, but a good solubility is a basic requirement for the applications.19 Second, the sidewalls of pristine BNNTs are chemically inert, and they must primarily be activated for the following functionalizations in various useful bio-devices.20 Third, the poor biocompatibility of BNNTs is also needed to be improved for applying in vivo.21
In the case of CNTs, the sidewall functionalization with various biomolecules and biopolymers has paved an efficient pathway for solving the corresponding issues.22 However, the sidewall functionalization of BNNTs with similar techniques has just recently drawn attention. In our previous investigations, we have reported that peptides,23 single-strand DNA24 and nucleotides25,26 can work for the sidewall functionalization of multi-walled BNNTs, leading to excellent dispersions in aqueous solutions. However, these pathways are closely related to the organic syntheses, which are usually expensive, time-consuming, and extremely toxic. To facilitate and broaden the prospective applications of BNNTs in a more practical approach, new pathways for lower-cost, more efficient, and biocompatible sidewall functionalization are highly desired.
Natural polysaccharides are the most abundant biopolymers in nature. They are reasonably good candidates for functionalizing BNNTs because of their cheapness, good water solubility, and well-recognized biocompatibility. Among various natural polysaccharides, gum arabic (GA), which is found in exudates of Arabic Senegal and Acacia Seyal trees, is an abundant and renewable polysaccharide with highly branched complex molecular properties.27 Although properties of GA have been widely investigated, the precise chemical structure of GA is still not fully understood. The latest research has suggested that GA is composed of main three units (Scheme S1, ESI†).27 One major unit is a highly branched polysaccharide, which takes about 90 wt%. Another is high molecular weight arabinogalachan–protein complexes taking about 10 wt% of the total. The rest of the composition is around 1 wt% of the total. It is known that the major functional properties of GA are correlated with the arabinogalactan–protein complexes. The two kinds of molecular models for arabinogalactan–protein complexes have been proposed and well-established: the “wattle-blossom” and the “twisted hairy rope”.27 Very recently, the use of GA has started to be extended into the fields of nanoscience and nanotechnology. For example, GA can be capped onto the surface of inorganic quantum dots28 or magnetic nanoparticles,29 giving these nanoparticles excellent solubility and biocompatibility. It has also been reported as a suitable dispersant for the individual stabilization of single-walled CNTs in aqueous solutions.30
In this contribution, taking many of the outstanding advantages of GA into account, we performed the first trial to disentangle multi-walled BNNTs in the presence of GA in an aqueous solution. Meanwhile, we used dextran (DT), dextran sulfate (DS), and two starch compositions, such as amylose (AL) and amylopectin (AP), as references (Scheme S2, ESI†). The interactions between GA and BNNTs were investigated using fluorescence, Fourier transform-infrared (FT-IR), and ultraviolet-visible (UV-Vis) absorption spectroscopies. Subsequently, several model proteins with different biological functions, usually used in modern biotechnologies, were immobilized onto the GA-functionalized BNNT surfaces by utilizing the electrostatic interactions as a basic driving force by controlling pHs (Scheme 1). The functionalization of BNNT sidewalls with GA allows efficient disentanglement of GA-functionalized BNNTs. GA could increase the number of surface charges and the categories of functionalities of BNNTs, which is helpful for hierarchical functionalization and subsequent applications. GA-functionalized BNNTs offer great opportunities for studying the physiochemical properties of individual disentangled BNNTs. Meanwhile, considering the rapid advancements in the band-gap engineering of BNNTs,10–12 such BNNTs are promising for the construction of BNNT-based electronics and optics. On the other hand, the successful immobilization of proteins onto the surface of GA-functionalized BNNT is an important initial step towards the development of BNNT-based bio-devices, which are particularly meaningful for many bio-related technological applications.
Scheme 1 Schematic representation of disentanglement of multi-walled BNNTs via functionalization with GA for proteins immobilization. |
The FT-IR spectra were recorded using a Perkin-Elmer Spectrometer, 10 times for each sample, and were Fourier-transformed at a resolution of 4 cm−1. All spectra were corrected with a baseline supported by Perkin-Elmer software. All stock solutions were drop-casted onto a gold film substrate after drying completely under ambient conditions for the measurements. GA-functionalized BNNTs solution was purified by using a centrifugation-filter (Millipore Ireland Ltd. Amicon ultra-2 mL, 100 K centrifugal filter; regenerated cellulose 1000000 MWCO) under 3500 rpm for 30 min at 25 °C against milli-Q water for 4 to 6 runs for removal of free GA. The pristine BNNTs and GA powder were used to measure the FT-IR spectra of the original BNNTs and pure GA, respectively.
The fluorescence was measured with a JASCO FP-6500 spectrofluorometer by excitation at 214 nm with a scan rate of 100 nm s−1. The measurement temperature was controlled at 25 °C. The UV-Vis spectra were recorded by a JASCO V-670 spectrophotometer at the ambient temperature. For fluorescence and UV-Vis spectra measurements, a GA-functionalized BNNTs solution was purified using a procedure similar to that for the FT-IR measurements. The original BNNT samples were similarly prepared by the same dispersing procedure without GA for recording reference spectra.
Fig. 1 (a) UV-Vis absorption spectra of the as-prepared BNNT dispersions with and without GA; (b) comparative potential of GA, DT, DS, AL and AP for the disentanglement of BNNTs in an aqueous solution. All the concentrations are 0.15 mg mL−1. Absorbance at 500 nm was recorded for the comparison. |
Fig. 2 (a) Dependence of the amount of BNNTs on the concentration of GA, and (b) plots of BNNT amounts as a function of the concentration of GA. |
Fig. 3 (a) Dispersion of GA-functionalized BNNTs; (b) AFM image of GA-functionalized BNNTs on the mica surface; (c) statistic distribution of heights and (d) lengths of GA-functionalized BNNTs. |
We assumed that arabinogalactan–protein complexes contained in GA were critical for the functionalization, while referring to previous studies on the molecular structure of GA.32 The presence of arabinogalactan–protein complexes in GA is an apparent difference of GA from other polysaccharides used in this study. The arabinogalactan–protein complexes in GA could play the key role for the high potential of GA for dispersing BNNTs in water. The “wattle-blossom” structural model of arabinogalactan–protein complexes has been widely accepted because it can be applied for perfectly explaining the behavior of GA on oil–water interfaces.32 The sidewalls of BNNTs are superhydrophobic, therefore, it was imagined here that the “wattle-blossom” structural model is also appropriate for explaining the mechanism of the regarded functionalization. The hydrophobic part of the arabinogalactan–proteins complex is soft and can adjust its low-energy conformation for matching the physical geometry of BNNTs via strong hydrophobic interactions. In the meantime, the hydrophilic part of GA is exposed for interacting with water molecules. Thus, the strong steric forces among GA molecule chains absorbed on BNNT sidewalls can prevent BNNTs from aggregation. It thereby endows an excellent dispersion of BNNTs.
FT-IR is a potential technique for gaining an insight into the assumed mechanism. As shown in Fig. 4, the peaks corresponding to the original BNNTs appeared at 771 cm−1 and 1346 cm−1, which were assigned to respective E1u (TO) and E1u (LO) modes (TO: transverse optic; LO: longitudinal optic), while they appeared at 791 cm−1 and 1361 cm−1 for the GA-functionalized BNNTs. The broad peak corresponding to the stretching vibration mode of –NH of arabinogalactan–protein complexes appeared at ∼3328 cm−1, while it appeared at ∼3312 cm−1 for the GA-functionalized BNNTs.33 The other changes in the peaks (ν(C–OH): 1024 cm−1; δ(C–H): 1416 cm−1 and β(N–H): 1560 cm−1) corresponding to GA were also found. These obvious changes in the FT-IR absorption spectra additionally verified the presence of interactions between the arabinogalactan–protein complexes of GA and the hydrophobic BNNT surfaces.
Fig. 4 Comparative FT-IR spectra of purified GA-functionalized BNNTs, pure GA and the original BNNTs. |
It had been indicated that the arabinogalactan–protein complexes of GA could be degraded (primary structure breakdown) prior to carbohydrate components of GA by treating GA at the mild temperature (60 °C–100 °C) for less than 24 h.27 In order to further point out the importance of arabinogalactan–protein complexes of GA for the observed functionalization, GA was treated here by heating at 80 °C for 12 and 24 h to degrade arabinogalactan–protein complexes in GA. Then, resultant GA was applied for the BNNTs' functionalization. The amount of BNNTs functionalized with thermo-treated GA in solution was very much reduced (Fig. 5), as expected, further confirming that the arabinogalactan–protein complexes play an important role for interacting with the BNNT sidewalls.
Fig. 5 The effect of the heating treatment of GA on the potential for the disentanglement of BNNTs in an aqueous solution. Absorbance at 500 nm was recorded for the comparison. |
Fig. 6 Comparative fluorescence spectra of GA, original BNNTs and purified GA-functionalized BNNTs. |
UV-Vis absorption spectra were acquired to further explore the effect of GA on the electronic structure of BNNTs (Fig. 7). After removing free GA from the dispersion, a notable red shift of the UV-Vis absorption peak for the BNNTs was observed. A sharp peak assigned to the band-gap transition of BNNTs appeared at 200 nm for the original BNNTs, while it appeared at 205 nm for the GA-functionalized BNNTs. This shift evidenced that the electrical structure of BNNTs was significantly affected by the strong hydrophobic interactions between the BNNTs and GA, thereby resulting into the band-gap reduction. This observation indicated that GA on the BNNT surface may behave as a dopant. The same doping effects have also been observed previously in other organic molecule-functionalized BNNT systems.19,35 In addition, the apparent mountain-like absorption peak appeared at around 280 nm for the GA-functionalized BNNTs. The peak may originate from the arabinogalactan–protein complexes of GA absorbed on BNNTs, suggesting that GA is indeed covered over the hydrophobic sidewalls of BNNTs. It is important to note that the absorption peak at around 280 nm might be a result of the Van Hove singularities of BNNTs,34 which could be related to the emission at 330 nm.
Fig. 7 Comparative UV-Vis absorption spectra of GA, original BNNTs and purified GA-functionalized BNNTs. |
For the immobilization of proteins onto GA-functionalized BNNTs, the pHs of model protein solutions of SAv, BSA, Lyz, and IgG were adjusted to pH 3 or 4 (Table 1) using a universal Britton Robinson buffer. The pHs of the proteins solutions were controlled to be lower than the isoelectric points of these proteins (SAv: 6.8–7.5;44 BSA: 4.8–5.4;45 Lyz: 10.7–11.0;46 IgG: 5.0–8.5.47), allowing the positively charged proteins to be attracted electrostatically and interact with the negatively charged GA-functionalized BNNT surfaces, thus leading to the required immobilization. AFM was employed for imaging the proteins immobilized on the surface of GA-functionalized BNNTs. Fig. 8a and 8b show AFM images of GA-functionalized BNNTs without proteins; the surfaces were rather smooth. As shown in Fig. 8c–e, it is clear that many protein particles locate on GA-functionalized BNNT surfaces, whereas the background of the sample is much cleaner. The same results can also be further seen in the 3D AFM images, as shown in Fig. S2 (ESI†). The height profile of these proteins on GA-functionalized BNNTs is further roughly monitored by using AFM (Fig. S3, ESI†). The sizes of SAv and BSA on GA-functionalized BNNTs are averaged as 8.2 ± 0.8 nm and 6.8 ± 1.2 nm (Table 1), respectively. These sizes are close to those for original SAv48 of 4.2 × 5.6 × 5.6 nm3 and BSA49 of 4.0 × 4.0 × 14.0 nm3 used in these experiments (Table 1), implying a thin layer coverage of proteins molecules on GA-functionalized BNNTs. In the cases of Lyz and IgG, the sizes of these proteins on GA-functionalized BNNTs are averaged as 12.9 ± 1.3 nm and 32.2 ± 3.2 nm (Table 1), respectively. These sizes are larger than those for original Lyz50 of 4.5 × 3.5 × 3.5 nm3 and IgG38 of 14.5 × 8.5 × 4.0 nm3. This difference may primarily result from the changes of protein conformations induced by the large surface curvature of BNNTs. On the other hand, the densities of Lyz and IgG on BNNTs are pretty high, which resulted in difficulties and errors during AFM measurements. These investigations strongly support the fact that the proteins were successfully immobilized onto the surface of GA-functionalized BNNTs. The presented approach is more efficient compared with the previous reports, in which immobilization of proteins onto BNNTs had been achieved by means of functionalizing BNNT using 1-pyrenebutyric acid N-hydroxysuccinimide ester (PAHE) in solution. Using the former approach, it took at least 24 h to stir the mixture of proteins and PAHE-functionalized BNNTs for the immobilization.17 Furthermore, in the present study, almost all proteins have closely been arrayed along with the longitudinal direction of GA-functionalized BNNTs, confirming that GA-functionalized BNNTs are indeed efficiently workable for proteins immobilization. Although the precise biological activities of those proteins immobilized on GA-functionalized BNNTs are needed to be carefully investigated in the future, the present approach is envisaged to be the significant breakthrough aiming at promoting BNNT applications in nanotechnologies.
Fig. 8 (a, b) AFM images of GA-functionalized BNNTs; (c) SAv (d) BSA (d) Lyz and (e) IgG on GA-functionalized BNNTs. |
Protein | Molecular weight (kDa) | Isoelectric point | Size (nm3) | Immobilization pH | AFM height (nm) |
---|---|---|---|---|---|
SAv44,48 | 52.8 | 6.8–7.5 | 4.2 × 5.6 × 5.6 | 4.0 | 8.2 ± 0.8 |
BSA45,49 | 66.8 | 4.8–5.9 | 4.0 × 4.0 × 14.0 | 3.0 | 6.8 ± 1.2 |
Lyz46,50 | 14.7 | 10.7–11.0 | 4.5 × 3.5 × 3.5 | 4.0 | 12.9 ± 1.3 |
IgG47,38 | 150 | 5.0–8.5 | 14.5 × 8.5 × 4.0 | 4.0 | 32.2 ± 3.2 |
Footnotes |
† Electronic Supplementary Information (ESI) available: Schemes S1, S2 and Fig. S1–S3. See DOI: 10.1039/c2ra20765f/ |
‡ The difference in AFM size of BNNTs appearing in Fig. 3 and Fig. 8 originates from the AFM tip-broading effect which is generally caused by the non-perfect shape of the AMP tip and a notable dispersion in nanoobject sizes. |
This journal is © The Royal Society of Chemistry 2012 |