Dušan K.
Božanić
a,
Adriaan S.
Luyt
b,
Lidija V.
Trandafilović
a and
Vladimir
Djoković
*a
aVinča Institute of Nuclear Sciences, University of Belgrade, P.O. Box 522, 11001 Belgrade, Serbia. E-mail: djokovic@vinca.rs
bDepartment of Chemistry, University of the Free State (Qwaqwa campus), Private Bag X13, Phuthaditjhaba 9866, South Africa
First published on 11th April 2013
Hybrid nanosystems composed of glycogen biopolymers and gold nanoparticles were prepared by an in situ non-toxic synthetic procedure. Transmission electron microscopy (TEM) and various spectroscopic methods (optical absorption, X-ray photoelectron and photoluminescence spectroscopy) were used for the characterization of the obtained bioconjugates. The gold nanoparticles formed in the presence of glycogen were spherical in shape and approximately 15 nm in diameter. The TEM micrographs show that the nanoparticles aggregated on the surface of the glycogen biomolecules. This effect induced a shift of the surface plasmon resonance band towards higher wavelengths on an increase in gold ion concentration. Effective medium theory calculations were carried out in order to explain the observed redshift of the plasmon band in the absorption spectra of the Au–glycogen colloids. The interactions of the gold nanoparticles with glycogen strongly affected the photoluminescence of the glycogenin protein incorporated into its structure. The Au–glycogen hydrocolloids exhibited good chemical stability in the presence of saline, phosphate buffered saline, alanine, histidine and D-glucose.
The application of the above-mentioned systems depends significantly on the type of biomolecule used as well as on the morphology and arrangement of the nanoparticles. All of these factors affect the surface plasmon resonance (SPR), the resonant absorption and the scattering of light that occurs due to the excitation of coherent electron oscillations at the surface of the particle.6 For this reason, the absorption spectrum can also provide, in combination with theoretical models, certain information about the size, shape and environment of the gold nanostructures. In the case of small spherical gold nanoparticles in water, the surface plasmon resonance occurs at approximately 525 nm, but nonspherical nanostructures or aggregates of nanoparticles15 exhibit absorption bands which are shifted to higher wavelengths. On the other hand, tuning the plasmon resonance via controlled aggregation and/or the self-assembling of nanoparticles holds great promise for many practical applications.16,17 The control of the resonant absorption of the gold nanostructures might also be of importance in photothermal cancer therapy.18 It was found that the nanoparticle-induced conversion of light into heat, and the consequent heat transfer to a malignant tissue, would be facilitated by an increase in the resonance wavelength due to the larger penetration depth of the incident radiation. In this study, we report on the preparation of bioconjugates, which allow the tunable positioning of the absorption band, that comprise gold nanoparticles and the carbohydrate polysaccharide glycogen.
Carbohydrates, along with proteins and amino acids, are essential components in a variety of metabolic processes. In nanotechnology, they have applications as reducing and templating agents for noble metal nanoparticles,19–21 while the preparation of functional glyconanoparticles has enabled the improved analysis of carbohydrate-based interactions with proteins.3,22,23 Polysaccharides (starch, chitosan, alginate, gum arabic, glycogen, etc.) are of particular interest and are the most-studied biomolecules for this purpose. Because of the large number of functional groups, these biopolymers have proved to be good environments for the growth of metal,19,24–36 semiconductor27,37–39 and oxide40,41 nanoparticles. Recently, they have been used as effective plasmonic platforms for SERS detection and tagging,32 and catalysis.33 In addition, the inherent biocompatibility of polysaccharides and the possibility of using green processing methods19 in the preparation of the nanoparticles are advantages in the medical applications of the obtained materials.34
Glycogen is a highly branched polymer of glucose which serves as the main glucose storage component in animal cells. Macromolecules of this polysaccharide are spherical structures, 20–40 nm in size, which are called β-particles. The well-defined morphology of glycogen is a consequence of the repetitive and uniform branching and linking of 13 glucose unit-long A-type and B-type polymer chains.42 According to the model proposed by Melendez-Hevia and co-workers,43,44 the structure of glycogen is optimal for the maximum glucose storage in the smallest possible volume, the maximum portion of the monosaccharide which can be released from the β-particles prior to debranching, and the efficient release of glucose. The dendrimer-like structure of glycogen also provides a large number of functional hydroxyl groups on its surface per volume unit of biopolymer, leading to as much as 34% of the glucose residues in the outermost layer of glycogen.44 Due to this highly developed surface, glycogen presents a convenient nanoreactor for the growth of metallic nanoparticles,28 and can act as a probe material for glucan–protein interactions.22,23 In our previous paper,28 we showed that glycogen–Ag nanoparticle conjugates can be successfully used as antimicrobial materials. Here we show that gold nanoparticles interact with glycogen molecules in a completely different way, which enables the control of the position of the SPR band.
Glycogen is native to human hepatic cells and using this biopolymer in biomedical applications can address the problems of biocompatibility and toxicity which sometimes arise in the applications of synthetic dendrimers.45 Furthermore, we used an in situ non-toxic chemical synthetic method for the preparation of the glycogen and gold nanoparticle hybrid nanosystems. The obtained hybrids were investigated by microscopic, structural and optical methods. The stability of the Au–glycogen colloids was tested in the presence of saline, phosphate buffered saline (PBS), alanine, histidine and D-glucose.
X-ray photoelectron spectroscopy (XPS) experiments were performed on a Physical Electronics Quantum 2000 instrument using Al Kα radiation (1486.6 eV). Prior to the analysis, the samples were sputtered by a 2 keV argon ion beam. The C 1s, O 1s, and Au 4f core levels were recorded at a 29.35 eV pass energy and a 55° take-off angle. The peak shift due to charge accumulation was corrected using the C 1s level at 284.44 eV as an internal standard.46 The XPS peaks were assumed to be linear combinations of Lorentzian and Gaussian line shapes and were resolved into individual components after the proper subtraction of the baseline, using the Shirley background subtraction method. The samples were prepared by the deposition of aqueous Au–glycogen solutions on the flat silicon wafers. They were subsequently dried in a vacuum at 40 °C.
A Nicolet 380 spectrophotometer was used for the FTIR spectroscopic analyses of the pure glycogen and glycogen–gold bioconjugates. The FTIR analyses were performed at room temperature in the spectral range of 4000–400 cm−1, with a resolution of 4 cm−1. The datasets were averaged over 200 scans.
The UV-vis absorption measurements of the Au–glycogen solutions were performed on a Thermo Evolution 600 spectrophotometer over a wavelength range of 200–900 nm.
The photoluminescence measurements of the pure glycogen and Au–glycogen aqueous solutions were performed on a Perkin-Elmer LS45 fluorescence spectrophotometer. For these analyses, we used a reference glycogen solution with the same concentration of biopolymer and pH values as the Au–glycogen colloids. The photoluminescence emission (PL) spectra were recorded in the wavelength range of 330–550 nm using an excitation wavelength λexc = 280 nm. The photoluminescence excitation (PLE) measurements were carried out at two emission wavelengths: λem = 360 nm and λem = 440 nm. The spectra were recorded over 250 nm–330 nm and 250 nm–400 nm intervals, respectively. The synchronous luminescence (SL) spectra were recorded over an excitation range of 240–500 nm and synchronous wavelength intervals (Δλ) from 30–140 nm. All of the measurements were performed in the right angle geometry with a scan speed of 100 nm min−1 and a slit size of 10 nm.
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Fig. 1 (a) TEM image of uranyl-stained glycogen; (b) TEM image and (c) corresponding particle size distribution of the [Au] = 3.0 × 10−5 M Au–glycogen sample; (d) TEM image of the [Au] = 9.0 × 10−5 M Au–glycogen sample. |
X-ray photoelectron spectroscopy was used to determine the composition and chemical environment of the elements present in the material. An XPS survey scan (not shown) revealed the presence of carbon, oxygen and gold core levels (hydrogen, although present in the biomolecule, is not detectable by XPS). Fig. 2 shows the high-resolution XPS spectrum of the Au 4f core level of the sample prepared with an initial Au ion concentration of 4.5 × 10−5 M. Two distinct lines separated by 3.67 eV were observed, namely the Au 4f5/2 and Au 4f7/2 lines, which occur because of the spin–orbit splitting of the Au 4f level.49 The positions of these lines, estimated after the correction due to charge accumulation, were 87.91 eV and 84.24 eV, respectively. In comparison to the reference value of bulk metallic gold of 84.04 eV49 (the vertical line in Fig. 2), the Au 4f7/2 line was shifted towards higher binding energies by 0.2 eV. A shift of this type was also observed in the case of starch and polyvinyl pyrrolidone-capped silver nanoparticles,29,30,50 and was attributed to the cumulative effects of the adsorption of the polymer onto the nanoparticles and the higher number of surface atoms due to the nanoparticles’ small size.50
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Fig. 2 XPS spectrum of the Au 4f level of glycogen-stabilized gold nanoparticles ([Au] = 4.5 × 10−5 M). The vertical line corresponds to the reference value for the Au 4f7/2 level of bulk gold (84.04 eV). |
The interaction between the glycogen biomacromolecules and gold nanoparticles was also investigated by FTIR spectroscopy, and no apparent differences were observed between the IR spectra of the pure glycogen and glycogen–Au conjugates. The former result implies that the biomolecule and the nanoparticles probably interact via OH groups.19,51
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Fig. 3 (a) UV-vis absorption spectra of the glycogen-stabilized gold nanoparticle colloids; (b) the dependence of the position of the absorption maxima on the initial gold ion concentration, and the linear fit. |
The observed differences in the band positions in the samples with different gold ion concentrations are a consequence of the interaction of individual glycogen molecules with multiple gold nanoparticles (see Fig. 1d). In particular, due to the nanometer size of the glycogen particles, the distances between the neighboring gold nanoparticles will be sufficiently small that the dipole–dipole interactions between them become significant. These interactions reduce the symmetry of the absorbers (with respect to that of the isolated spherical Au nanoparticles), which results in the appearance of additional modes at higher wavelengths53 and, consequently, results in the red shift of the absorption band of the colloid. At higher gold concentrations, the average number of nanoparticles per glycogen molecule increases and, due to smaller inter-particle distances, there is a further shift of the plasmon band towards higher wavelengths. It is worth mentioning that in a study on gold nanoparticles stabilized with poly(amidoamine) dendrimers, Srivastava et al.17 also managed to tune the position of the plasmon resonance by controlling the distance between the gold nanoparticles. However, instead of changing the concentration of the gold ions as in our case, the inter-particle distance was controlled by using different dendrimer generations (dendrimer sizes). The observed absorption behavior of the Au–glycogen colloids is closely related to the dendrimer-like structure of the glycogen β-particles and their nanometer size. To justify the former conclusion, we have prepared soluble starch-stabilized gold nanoparticles using the same synthetic procedure. The molecular structure of soluble starch is identical to that of glycogen, but its macromolecules are predominantly linear or have a lower extent of branching.40 In this case, it was found that the position of the absorption bands of the Au–starch colloids was not affected by the change in the gold ion concentration (see Fig. S2, ESI†). The concentration-dependent optical properties observed in Fig. 3 are also in agreement with the resonant light scattering study of Xiang et al.22 on glycogen–gold nanoparticle systems. They showed that the mixing of glycogen and a separately-prepared gold colloid resulted in the aggregation of the gold nanoparticles.
In order to confirm whether the proposed mechanism of interaction of the gold nanoparticles with glycogen molecules can indeed explain the changes in the plasmon absorption, we performed a series of calculations based on the effective medium theory. The employed theoretical method is based on the approach suggested by Schatz and co-workers54 in their investigations of the optical properties of nanoparticle aggregates. As a starting element in the present calculations, we considered a single glycogen molecule (represented by a sphere of diameter 2Rg = 40 nm) covered with N gold nanoparticles of diameter 2a = 15 nm. The dipole polarizability αag of such an aggregate is54
![]() | (1) |
![]() | (2) |
![]() | (3) |
The value of the filling factor f represents the volume fraction of the Au nanoparticles in the aggregate and is represented by
![]() | (4) |
Obviously, for given values of a and Rg, the factor f depends solely on the number of particles N attached to the glycogen outer layer. The values of f are limited by percolation effects, i.e. by the maximum number of gold nanoparticles that can be positioned on the biomolecule surface without being in mutual contact. The experimental absorption spectra can be qualitatively compared to the theoretically estimated absorption coefficients Aabs(λ) by
![]() | (5) |
By changing the values of the filling factor f, it is possible to change the positioning of the band maxima of the Aabs(λ) curves until they match the positions of the experimental bands. These curves and their corresponding f-values are presented in Fig. 4. The calculations suggest that an increase in the initial gold concentration is followed by an increase in the filling factor. According to eqn (4), this means that, on average, a larger number of gold particles will be attached to each glycogen molecule. In the case of the colloid with the lowest concentration, we found N to be 1.9, and for the highest concentration, [Au] = 9.0 × 10−5 M, N to be 8.9. A schematic illustration of the changes in N with the change in gold concentration is shown in the insets of Fig. 4. It should be noted that the values of N are not absolute due to a number of other factors that were not included in the calculations. Nevertheless, the presented theoretical analysis clearly suggests a possible mechanism of gold nanoparticle–glycogen interaction which results in the red shift of the absorption maximum. The trend of the increase in the number of nanoparticles attached to the glycogen molecules with an increase in [Au] is in agreement with the TEM observations (Fig. 1).
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Fig. 4 Comparison of the experimental (black) and theoretical (red) absorption spectra for the Au–glycogen colloids. Schematic representations of nanoparticle aggregates are provided in the insets. |
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Fig. 5 (a) Photoluminescence emission spectra (λexc = 280 nm) of glycogen (black line) and Au–glycogen (I: 0.03 mM Au, II: 0.06 mM Au and III: 0.09 mM Au) aqueous solutions. Photoluminescence excitation spectra (λem = 360 nm and 440 nm) of the glycogen solution are shown in the inset. (b) Synchronous photoluminescence emission spectra of glycogen (black line) and 0.045 mM Au–glycogen (red line) solutions for Δλ = 70 nm and 30 nm. The numbers in (b) correspond to the wavelengths of the emission maxima. |
The influence of gold on the PL emission of glycogen was further investigated by synchronous luminescence (SL) spectroscopy, since SL spectra provide information regarding the environment around the fluorophore functional groups.64 The surface plot of the SL data of glycogen-stabilized Au nanoparticles (concentration 4.5 × 10−5 M) shows different features to the spectrum of the glycogen solution (see Fig. S3, ESI†). The SL spectra of glycogen and Au–glycogen solutions obtained at scanning intervals of Δλ = 70 nm and 30 nm are shown in Fig. 5b. For these particular values of Δλ, the SL spectra reveal additional information about the effect of the nanoparticles on the emission of the tryptophan and tyrosine residues.64 In the Δλ = 70 nm case, a decrease in intensity and a red shift of the dominant band at λexc = 277 nm (λgm = 347 nm) in the presence of the gold nanoparticles was observed. This band corresponds to the fluorescence of tryptophan, and its shift towards higher wavelengths indicates that the nanoparticles induce an increase in the polarity of the environment around the tryptophan residues. The interaction of the gold nanoparticles with the glycogen leads to disaggregation of the hydrophobic cavities, thus forming a looser glycogenin structure. Fig. 5b also shows that the emission maximum (λem = 314 nm) from the tyrosine amino acid (Δλ = 30 nm) was not affected by the introduction of the nanoparticles, suggesting that the polarity of the environment around these residues did not change significantly. Similar effects were observed in the case of the SL spectra of human serum albumin treated with glycyrrhetinic acid.64 On the other hand, Kathiravan et al. showed that the conformational changes of bovine serum albumin induced by colloidal AgTiO2 particles should be associated with tyrosine and not with the tryptophan regions.65 The SL spectrum of the Au–glycogen sample for Δλ ≈ 100 nm, characteristic for fluorophores that produce peak B, did not show any additional features compared to the spectrum of the glycogen solution.
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Fig. 6 Changes to the gold plasmon resonance position and width, of the glycogen-stabilized gold nanoparticles, with time, in the presence of saline (black squares), PBS (squares), 0.2 M alanine (black triangles), 0.2 M histidine (triangles) and 0.1 M D-glucose (black diamonds). The reference sample (circles) was prepared by diluting the initial colloid solution ([Au] = 4.5 × 10−5 M) with water. |
It should be noted that Kattumuri et al.25 performed a similar procedure to test the chemical stability of the gold nanoparticles stabilized by the polysaccharide gum arabic. After seven days of monitoring the absorption properties of this system in the presence of 35% saline solution, they noticed a 15 nm red shift of the Au plasmon maximum and an increase in the band's width by approximately 10 nm. Also, the mixing of the Au–gum arabic bioconjugate with a 0.2 M histidine solution induced the broadening of the resonance band by nearly 25 nm.25 A comparison of these results with the results presented in Fig. 6 suggests that the stabilization of the gold nanoparticles by glycogen molecules results in the excellent chemical stability of the synthesized colloids.
The aggregation of the gold nanoparticles is related to the glycogen morphology (nanometer size of the β-particles), and has a profound influence on the absorption properties of these hybrid systems. Increasing the concentration of gold ions results in an increase in the number of nanoparticles per glycogen molecule and consequently there is a decrease in the distance between the nanoparticles. Since changes to the inter-particle distance induce a shift in the plasmon band, this effect can be used to control the position of the maximum absorption by changing the initial concentration of the gold ions. The gold–glycogen nanostructures studied here could be of interest in biomedical applications, particularly in photothermal cancer therapy. The good chemical stability of this colloidal system and the inherent biocompatibility of the glycogen biomolecules are certainly an advantage. However, for their successful application, further investigations are necessary, particularly on the influence of the nanoparticle size and loading capacity of the glycogen molecules on the position of the absorption band, as well as on the specific types of interaction which lead to their assembly.
Footnote |
† Electronic supplementary information (ESI) available: TEM images of the Au–glycogen samples, as well as the UV-vis and SL spectra of the Au–glycogen and Au–starch solutions. See DOI: 10.1039/c3ra40189h |
This journal is © The Royal Society of Chemistry 2013 |