Oleksandr Smirnov*ab,
Volodymyr Dzhagancd,
Mariia Kovalenkoa,
Oleksandr Gudymenkoc,
Veronika Dzhagana,
Nazar Mazurc,
Oksana Isaievac,
Zoia Maksimenkoc,
Serhiy Kondratenkod,
Mykola Skorykde and
Volodymyr Yukhymchukc
aESC “Institute of Biology and Medicine”, Taras Shevchenko National University of Kyiv, Kyiv, Ukraine. E-mail: plantaphys@gmail.com
bInstitute of Plant Physiology and Genetics, National Academy of Sciences of Ukraine, Kyiv, Ukraine
cV. Lashkaryov Institute of Semiconductors Physics, National Academy of Sciences of Ukraine, Kyiv, Ukraine
dPhysics Department, Taras Shevchenko National University of Kyiv, Kyiv, Ukraine
eG.V. Kurdyumov Institute for Metal Physics, National Academy of Sciences of Ukraine, Kyiv, Ukraine
First published on 3rd January 2023
Fungi produce and excrete various proteins, enzymes, polysaccharides, and secondary metabolites, which may be used as media for the “green” synthesis of metal and semiconductor nanoparticles (NPs). ZnO NPs with a flower-like morphology were synthesized by an affordable colloidal route, using an aqueous extract of Ganoderma lucidum as a reducing agent and stabilizer. Each individual “flower” has a large effective surface, which is preserved when the particles are close packed into a dense film, which is advantageous for numerous applications. The phonon Raman spectrum and X-ray diffraction (XRD) pattern prove the high crystallinity of the NPs, with the distinct pattern of a hexagonal (wurtzite) lattice, negligible residual stress, and a crystallite size of 12–14 nm determined from the XRD. The photoluminescence (PL) spectrum of the as-synthesized ZnO NPs contains a structured defect-related feature in the violet-blue range, while the green PL, common for nanostructures synthesized by “green” routes, is very weak. By applying dimethylsulfoxide as an additional passivating agent, the excitonic (UV) PL band was activated without enhancement of the defect-related features. Ag NP-decorated ZnO flowers were synthesized by subsequent silver reduction by pepper extract. The ZnO/Ag NPs exhibited efficient surface-enhanced Raman scattering (SERS) of a standard dye analyte, rhodamine 6G, ensuring the feasibility of other applications that require close contact of ZnO/Ag to other nanostructures or molecules to realize the energy of the charge transfer.
This work is the first report on the synthesis of ZnO NPs using Ganoderma lucidum (G. lucidum) fruiting body extract as the bio-reducing and stabilizing agent. G. lucidum is a wood-degrading and traditional medical Basidiomycota (reishi mushroom), containing over 400 bioactive compounds with bioreductive properties, including different proteins, amino acids, polysaccharides, fatty acids, phenolic compounds, triterpenoids, steroids, and alkaloids.20,21 Therefore, the NPs synthesized have additional potential applications owing to the well-known medical properties of Ganoderma extracts.20 On the other hand, ZnO nanostructures with flower-like morphologies have attracted much attention recently, with a whole review paper devoted to them.22 The particular morphologies and other properties of the ZnO nanoflowers obtained in different works are shown to be quite different, primarily due to the different methods of their synthesis, such as chemical vapor deposition, facile hydrothermal synthesis, thermal evaporation, chemical reduction, bio-synthesis, and the solvothermal method. The range of demonstrated and prospective applications of ZnO and ZnO/Ag nanoflowers is also broad, including in biosensors, catalysts, bio-markers for the diagnosis of diseases and therapeutic processes, wastewater remediation and gas sensing.22 The decoration of the ZnO surface with Ag NPs is performed to improve catalytic and sensing applications, in particular, so the Ag NP plasmon can be used to enhance the Raman scattering of analyte molecules. For many of the applications an affordable, bio- and environmentally friendly, and scalable synthesis is preferred. Green synthesis from plant extracts is a suitable option, as highlighted in previous work.22 Both the bio-compatibility and flower-like morphology of the ZnO NPs synthesized in this work for the first time from (medical) fungi extract are consistent with the work described above. The large effective surface of the films prepared from these flower-shaped NPs is also advantageous for fabricating plasmonic nanostructures, which can be used as substrates for surface-enhanced Raman scattering (SERS) or other similar sensing applications, as demonstrated in this work (Fig. 1).
For the myco-synthesis of ZnO NPs, zinc acetate dihydrate (Zn(CH3COOH)2·2H2O) (1.095 g) was dissolved in deionized water (100 mL) by stirring at ambient temperature. Then, 10 (sample #1) or 5 mL (#2) of fungi extract was added, the pH of the obtained solution was adjusted to approx. 12 with 1.0 M NaOH, and the mixture was stirred for 3 hours at room temperature. Following this, the dispersion was centrifuged, and the solid precipitate was washed with deionized water and ethanol three times, respectively. The obtained white powder was dried for 10 hours at 60 °C.
For the synthesis of AgNP-decorated ZnO NPs, dried white ZnO NP powder (0.05 g) was dissolved in deionized water (100 mL) by stirring at ambient temperature. Then, to test the effectiveness of the synthesis of the AgNP-decorated ZnO NPs, four experimental mixtures were made: 2 mL of the ZnO NP solution was mixed with 2 mL of 0.001 M silver nitrate (AgNO3); 1 mL of the ZnO NP solution was mixed with 3 mL of 0.001 M silver nitrate (AgNO3); 3 mL of the ZnO NP solution was mixed with 1 mL of 0.001 M silver nitrate (AgNO3); and 2 mL of the ZnO NP solution was mixed with 2 mL of 0.001 M silver nitrate (AgNO3) and 1 mL of chili pepper (Capsicum annuum) fruit extract, which was pre-prepared according to the method described in ref. 23.
The size and morphology of the ZnO NPs were studied using scanning electron microscopy (SEM, Tescan Mira 3 MLU). The X-ray diffraction (XRD) study was performed using a Philips X'Pert PRO – MRD setup with a Cu Kαl line (λ = 0.15406 nm) in a symmetric (2Θ − ω) mode, with a scan step of 0.025°. Optical absorption spectra were recorded using a StellarNet Silver Nova 25 BWI6 spectrometer. PL spectra were measured with a Shimadzu RF-1501 spectrophotometer at a spectral resolution of 1 nm. For Raman spectra, a 532 nm solid-state laser was used for excitation, and a single-stage spectrometer RM1000 (Renishaw) equipped with a cooled CCD detector for acquisition. The laser power density on the samples was approx. 104–105 W cm−2 to preclude irreversible thermal or photo-induced modification of the samples. A spectral resolution of 1 cm−1 was determined from the Si phonon peak width of a single crystal Si substrate. The Si phonon peak position of 520.5 cm−1 was used as a reference for determining the positions of the Raman peaks.
Fig. 2 Representative SEM images of the ZnO NPs (#1) synthesized with G. lucidum aqueous extract, acquired with different magnifications: 182000 (a), 74000 (b), and 12600 (c). |
The NPs exhibit a distinct diffraction pattern of hexagonal ZnO of wurtzite-type structure (ICDD PDF No. 010-75-0576).24 The diffraction peaks of sample #1, synthesized with a concentration of the extract twice that of sample #2, are slightly stronger and narrower, and the contribution of the amorphous feature is weaker, indicating a higher crystallization degree in this sample.
From the angle positions and widths of the reflections 002\004 and 100\200, the crystallite sizes and residual deformations were calculated using the Williamson–Hall method (Table 1):
βcosθ = λ/D + 4εsinθ, |
Sample | Strain ε along a | D along a | Strain ε along c | D along a |
---|---|---|---|---|
1 | 1.4 10−3 | 12.3 | 1.0 10−3 | 14.3 |
2 | 3.4 10−3 | 12.7 | 2.3 10−3 | 13.3 |
The hexagonal type of structure and even the particular ratio of peak intensities observed for the ZnO flower-like particles in this work is very common for ZnO NPs synthesized using various other extracts.10,19,25 The particle morphology, on the contrary, is rather sensitive to the particular extract used.26 Particles with round shapes12 and hexagonal shapes,25 and only rarely particles with a developed morphology have been reported.16 The major difference in the XRD patterns in other works is the intensity of the 002 reflection (relative to the other peaks),17 which can be indicative of the different aspect ratios of the crystalline domains along the a and c axes of the hexagonal crystal structure, or some minor admixture of the zinc blende phase, which has its primary reflection close to the 002 peak of the wurtzite.27
Additional information on the internal structure of the ZnO-Gan NPs, as well as on the lattice vibration (phonon) properties, was obtained by Raman spectroscopy. The Raman scattering acquired with two different powers (5 × 10−4 W cm−2 and 10−5 W cm−2) of the excitation laser line (λexc = 532 nm) is presented in Fig. 3b. The few cm−1 downward shifting of the phonon peaks in the Raman spectra of the NPs and other nano-sized materials excited with a higher laser power/intensity is of thermal nature, i.e., the thermal energy generated in the NP is larger than that which can be dissipated into the environment and thus leads to an increased temperature in the NPs. Nevertheless, the spectrum acquired at a laser power of ten times higher contains more spectral features that are intense enough for analysis. Their spectral position needs to be corrected using the position of the peaks in the spectrum acquired at a lower laser power. The set of peaks observed for our ZnO (Fig. 3b) corresponds to the well-known pattern of nanocrystalline ZnO at off-resonant (sub-bandgap) excitation:28–32 Elow2 at 103 cm−1, Ehigh2 at 442 cm−1, Ehigh2 − Elow2 at 335 cm−1, ATO1 at 384 cm−1, and ALO1 at 587 cm−1, as well as the first overtone of the ALO1 at 1160 cm−1 (Fig. 3b). Several weaker features observed in our spectra are also present in the higher-power spectrum: the 205 cm−1 mode can be attributed to 2 × Elow2, and the 661 cm−1 one to TA + LO (TA stands for “transversal acoustical” and LO for “longitudinal optical” phonons).30–32 The shoulder (at about 535 cm−1) of the LO mode is characteristic of a nanostructure surface optical (SO) phonon mode.33,34 In microcrystalline ZnO the LO and its overtone peaks are very strong both in resonant (near- or above-bandgap) and off-resonant (e.g. green laser line) excitation.35 In the NPs, the LO peak and its overtones usually dominate the Raman spectrum under the resonant excitation with a 325 nm laser source.4,36,37 The moderate intensity of the LO and 2LO features and their comparable intensity in our non-resonant spectra are fully consistent with the 12–13 nm size of the nanocrystallites obtained from the XRD measurements.
ZnO NPs synthesized in water or under other mild conditions usually exhibit only a broad-band PL in the visible range, centered around 550 nm, attributed to defects such as oxygen vacancies (primarily on the NP surface).37,38 The excitonic PL (EPL) is more typical for NPs and polycrystalline films obtained at higher temperatures,36,39 while NPs synthesized under mild conditions also showed pronounced EPL in some previous work.37,40 The spectrum of the as-synthesized ZnO NPs in the present work exhibits distinct bands centered at 460 and 550 nm, and another band is seen as a shoulder at 415 nm (Fig. 4a). We labeled these bands as BPL (“blue PL”), DPL (defect PL, see above), and VPL (violet PL) bands, respectively. The PL features similar to BPL were attributed earlier to zinc interstitials41 or zinc vacancies.42,43 The origin of the VPL has been related in some previous work to unspecified intrinsic defects,44 although it also matches spectrally the range discussed by others concerning zinc vacancies44 and zinc interstitials.43 It should be noted that establishing the nature of the components of the PL spectrum requires tremendous research efforts and goes beyond the scope of the present paper.
Modifying the NP surface is a well-known approach to both modifying the properties of the NPs and clarifying the nature of some properties, particularly the origin of different PL bands.40,45,46 Dimethyl sulfoxide (DMSO), for instance, a very useful solvent, miscible with water, often used in biomedical applications and the synthesis of nanoparticles,47–49 was shown to be an efficient stabilizer of the ZnO colloidal NPs,37,38 ensuring a very high intensity of both surface-related (DPL)38,45 and excitonic (EPL)37,40 bands. Therefore, we investigated the influence of adding DMSO (after synthesis) on the PL spectrum of the present ZnO NPs. The evolution of the PL spectra of the ZnO NPs upon the addition of DMSO to the as-synthesized NP solution is shown in Fig. 4b. One can see that the DPL and BPL remain unaffected, while the VPL intensity increases dramatically, and the EPL band appears and evolves into a distinctly resolved feature at the highest DMSO content (ZnO:DMSO ratio 1:10, top spectrum). We varied the content of DMSO in a broader range, and subjected the mixture to ultrasound and heating at different temperatures (below 100 °C). All these changes did not cause much more quantitative or qualitative change in the spectra than that shown in Fig. 4b.
The experiment with DMSO addition demonstrates the high sensitivity of the PL spectrum of the synthesized ZnO NPs to the environment, indicating the high potential of these NPs in various sensing applications, not only optical, but also any other sensing applications that involve charge transfer between the NP (surface) and the environment.
The obtained hetero NPs were investigated as a substrate for surface enhanced Raman scattering using a standard analyte Rhodamine 6G (R6G). The advantage of these ZnO/Ag heteroNPs for SERS application is expected to be the combination of the enhancement stemming from the individual Ag NPs on each of the ZnO particles and the occurrence of so-called “hot spots” between the Ag NPs attached to different/neighboring ZnO particles. The flower-like morphology of the latter allows their close-packing into a dense film with a high probability of contact points between the “petals” of the neighboring ZnO/Ag particles.
Fig. 6 Raman spectra of Rhodamine 6G (10−5 M) with bare ZnO NPs (a), ZnO/Ag sample #1 (b), and ZnO/Ag sample #4 (c). |
An analogous series of experiments (Fig. 6b) performed for ZnO/Ag NP sample #1 (with the lowest amount of Ag) revealed no Raman peaks for the extract when only ZnO/Ag NPs were measured (black curves), and no R6G peaks when R6G was deposited on dried ZnO/Ag NPs (blue curves), while distinct analyte features could be registered when the analytes were mixed with ZnO/Ag NPs in the solution (green curves). This result indicates that mixing the analyte with the ZnO/Ag NPs in the solution may provide a higher probability/concentration of the analyte molecule occurring in the “hot spot” between the Ag NPs of the neighboring ZnO NPs. The same series of measurements performed for ZnO/Ag NP sample #4 (with the largest amount of Ag) is presented in Fig. 6c. Surprisingly, the increased amount of AgNPs in this sample compared to #1 did not cause an increase in the Raman intensity in the solution mixed approach (green curves), while a SERS signal at least 5 orders of magnitude stronger is observed in the case of the R6G solution deposited on the preliminarily dried ZnO NPs (blue curves). No Raman signal in this deposition mode was observed for the ZnO/Ag #1 NPs. To explain this observation, we can assume that in addition to the different morphological and optical properties of the individual ZnO/Ag NPs with different amounts of Ag, as well as possible differences in their aggregation properties (responsible for the interparticle contact), the mechanism of the analyte drying and finding of the hot spots may also be complex and dependent on the concentration of Ag NPs in the given system. In particular, the potential advantage of mixing solutions for placing R6G molecules in the hot spots at low Ag NP concentrations (sample #1 above) may turn out to be less critical when the Ag NP concentration is high (sample #4 above). In the latter case, the analyte molecules may better “find” the hot spots on the preliminarily dried ZnO NP layer because of a surface tension-driven accumulation of the molecules in the points of contact between the neighboring ZnO/Ag NPs.
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