Investigation of the Reduction of Graphene Oxide by Lithium Triethylborohydride

Abstract

The chemical reduction of a wet colloidal suspension of graphene oxide is a cost-effective and adaptable method for large scale production of "quasi" graphene for a wide variety of optoelectronic applications. In this study, modified Hummers' procedure was used to synthesize high quality graphene oxide at 50°C. This modified protocol thus eliminates the potentially hazardous second high-temperature step in Hummers' method for the production of GO. Furthermore, the reduction of graphene oxide by lithium triethylborohydride is demonstrated for the first time. According to FT-IR, UV-Vis, TGA, Raman, SEM/EDS, and AFM results, the reduced graphene oxide (LiEt3BH-RGO) has properties comparable to other reduced graphene oxide products reported in the literature.

Guangyuan Xu 1,2,3 and Jenny Malmström 1,2,3 and Neil Edmonds 1 and Neil Broderick 4 and Jadranka Travas-Sejdic 1,2,3 and Jianyong Jin 1,2

Academic Editor:Alessandro Pegoretti

1, School of Chemical Sciences, University of Auckland, 23 Symonds Street, Auckland 1142, New Zealand
2, The MacDiarmid Institute for Advanced Materials and Nanotechnology, Wellington 6140, New Zealand
3, Polymer Electronics Research Centre (PERC), School of Chemical Sciences, University of Auckland, 23 Symonds Street, Auckland 1142, New Zealand
4, Department of Physics, University of Auckland, 23 Symonds Street, Auckland 1142, New Zealand

Received 30 August 2015; Revised 7 December 2015; Accepted 16 December 2015

This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

1. Introduction

Since its discovery and successful isolation by Novoselov et al. [1] in 2004, graphene and its related carbon materials have been extensively studied and have become an important materials research platform, potentially having a high impact on many areas of nanotechnology and material science in the 21st century [2]. Graphene possesses tremendous mechanical, thermal, and electronic properties, which can be attributed to their large in-plane π -conjugation, nanoscale thickness and two-dimensional structure [3, 4]. A wide range of applications can be found in the fields of lithium-ion batteries [5, 6], super capacitors [7], solar cells [8], polymer nanocomposites [9] and even as sea water desalination membranes [10, 11].

Among all methods of graphene preparation, "bottom-up" methods such as chemical vapour deposition (CVD) [12] and the epitaxial growth method [13] demand significant capital investment which could translate to high production costs for scale-up of graphene production. Alternatively, the "top-down" strategy is promising to achieve inexpensive large scale synthesis of graphene. The common approaches include micromechanical exfoliation of graphite [1], liquid-phase exfoliation of graphite [14], and the most popular wet chemistry method via a graphene oxide (GO) "intermediate." The reduction of GO can be achieved by chemical reducing agents [15], photo and thermal reduction [16], and bacterial reduction [17].

Dozens of chemical reducing agents have been reported to eliminate oxygen containing functional groups on GO and restore sp² carbon networks. The list includes hydrazine [18], carbon monoxide [19], hydriodic acid [15], SOCl₂ [20], alcohol [21], Na-NH₃ solution [22], aluminum powder [23], NaOH [24], thiourea [25], ascorbic acid [26], glucose [27], p-phenylenediamine [28], NaBH₄ [29], and lithium aluminum hydride [30]. Several previously reported reducing agents have some limitations such as high toxicity or weak reducing power; therefore, efforts are being made to identify new reduction routes. In this paper, a new reduction approach for GO using lithium triethylborohydride (LiEt₃ BH, also known as super hydride) is investigated. From the literature [31, 32], lithium triethylborohydride is assumed to be a powerful agent to reduce carboxylic acids, carbonyl groups, and epoxy groups. One of the additional advantages for LiEt₃ BH reduction is that it is less toxic than lithium aluminum hydride. The rGO by lithium triethylborohydride will be abbreviated as LiEt₃ BH-RGO. In addition, in this work, the GO was prepared at a reaction temperature of 50°C, the original Hummers' method used 35°C [33]; therefore, 50°C is designated as medium temperature Hummer GO (MTH-GO). This method importantly removes the undesirable high-temperature step (98°C) of the potentially explosive reaction mixture used. A series of techniques including solid state Nuclear Magnetic Resonance (ssNMR), Fourier Transform Infrared (FTIR) spectroscopy, ultraviolet-visible spectroscopy (UV-Vis), Raman spectroscopy (Raman), X-ray Photoelectron Spectroscopy (XPS), Thermal Gravimetric Analysis (TGA), Atomic Force Microscopy (AFM), Scanning Electron Microscopy (SEM), and energy-dispersive X-ray spectroscopy (EDS) were applied to characterize the synthesized MTH-GO and LiEt₃ BH-RGO.

2. Experimental Details

2.1. Materials

Graphite powder (average particle size <45 μ m, Catalogue #496596) and lithium triethylborohydride (LiEt₃ BH, 1 M in THF solution, Catalogue #179728) were purchased from Sigma Aldrich. Concentrated sulphuric acid (H₂ SO₄ , ACS grade, 98%) and hydrochloric acid (HCl, ACS grade, 36.5-38%) were purchased from J. T. Baker. Potassium permanganate (KMnO₄ , AR grade) and 35% hydrogen peroxide (H₂ O₂ , LR food grade) were purchased from ECP. Sodium nitrate (NaNO₃ , AR grade) was purchased from UNIVAR.

2.2. Synthesis of MTH-GO

Graphite (2.0 g, 0.1667 mol) was firstly microwaved in 1000 W microwave oven for 10 s to expand the layers, the graphite turned red during this treatment [34]. The graphite and NaNO₃ (2.0 g, 0.0235 mol) were then added to the concentrated H₂ SO₄ (120 mL) and the mixture was magnetically stirred together in an ice water bath. KMnO₄ (12.0 g, 0.0759 mol) was then added to the suspension very slowly with vigorous stirring for 15 minutes. As shown in Figure 1(a), the color of the mixture became dark green. The mixture was then transferred to a preheated oil bath at 50°C to react for 24 hours. As the oxidation proceeded, the suspension became a very thick paste where the color changed from dark green to brownish purple (Figure 1(b)); this is similar to the color reported in the literature [33].

Figure 1: (a) Reaction suspension in sulfuric acid; (b) reaction paste after 24 h oxidation at 50°C; (c) the reaction mixture quenched with ice; (d) final reaction mixture after H₂ O₂ addition.

(a) [figure omitted; refer to PDF]

(b) [figure omitted; refer to PDF]

(c) [figure omitted; refer to PDF]

(d) [figure omitted; refer to PDF]

After oxidation under the medium temperature was completed, the mixture was quenched with 100 g of ice (made from distilled water). As the addition of ice progressed, the color of the mixture slowly turned to bright purple (Figure 1(c)). Finally, 35% H₂ O₂ (12 mL) was added in the suspension to consume the residual permanganate. If the synthesis is successful [33], the final graphite oxide mixture should be bright yellow as shown in Figure 1(d).

2.3. Purification of MTH-GO

37% HCl (100 mL) was added to the product mixture and centrifuged at 8000 rpm for 10 min. The clear supernatant was discarded and the precipitate was washed with 100 mL of ethanol followed by 100 mL of distilled water. The resulting graphite oxide solid was dialyzed (molecular weight cut-off = 1000 Da, Spectra/Por) for four days until the conductivity decreased to 10 μ S/cm to ensure the complete removal of ionic impurities. To obtain the graphene oxide, the graphite oxide product was exfoliated in an ultrasound bath (100 watts) for 2 hours as a 1000 mL aqueous dispersion.

The graphene oxide suspension was concentrated by rotoevaporation at 50°C, and approximately 800 mL water was removed. The concentrated graphene oxide suspension was ultrasonicated again for 30 mins and centrifuged at 8000 rpm for 5 min, and the sediment (assumed to be less exfoliated graphite oxide) was discarded. The supernatant was kept and dried in vacuum at 50°C for five days to obtain high quality MTH-GO (0.6 g, 30% yield).

2.4. Synthesis of LiEt₃ BH-RGO

Dry MTH-GO powder (30 mg) was added to anhydrous THF (40 mL) and ultrasonicated for two hours to form a relatively uniform dispersion; lithium triethylborohydride solution (LiEt₃ BH) (30 mL, 1 mol/L in THF) was then added dropwise at 0°C. Bubbles were observed initially and to complete the reaction the suspension was refluxed overnight under nitrogen at 66°C. The unknown amount of unreacted LiEt₃ BH was quenched with ethanol (10 mL) and deionized water (10 mL) at 0°C. The LiEt₃ BH-RGO product (14.6 mg) was isolated by filtration under slightly acidic pH condition and washed with acetone and deionized water three times and dried at 80°C under vacuum for five days (48% yield).

2.5. Characterization Techniques

¹³ C solid state NMR analyses were carried out on a dry sample using a Bruker Avance 300 standard bore magnet system operating at 300.13 MHz proton frequency (7.05 T). The spectra were obtained by using SPE HPDEC (single pulse excitation with high power decoupling) technique. The magic angle was adjusted by maximizing the sidebands of the ⁷⁹ Br signal of a KBr sample. Atomic Force Microscopy (AFM) was performed using an Asylum Research Cypher ES instrument (Oxford Instruments, US). Images were acquired in air using tapping mode with a gold coated NSG 10 probe (resonance frequency 255 kHz) from NT-MTD (Russia). The cantilever was driven using blueDrive photothermal excitation. During the postprocessing of images, the background of the images was flattened, while the features were preserved by masking. Scanning Electron Microscopy (SEM) and energy-dispersive X-ray spectroscopy (EDS) analysis were conducted using a Quanta 200F (FEI, US) operating in variable pressure ESEM mode. It is equipped with an EDAX brand EDS detector with a SiLi Lithium Drifted Super Ultrathin Window. The samples were coated with a Quorum Q150RS sputter coater to provide platinum coating. The XPS data were collected on a Kratos Axis Ultra DLD equipped with a hemispherical electron energy analyzer. Spectra were excited using monochromatic Al Kα X-rays (1486.69 eV) with the X-ray source operating at 150 W. This instrument illuminates a large area on the surface and then using hybrid magnetic and electrostatic lenses collects photoelectrons from the desired location on the surface. In this case, the analysis area was 300 by 700 μ m spot (=hybrid/slot). Data evaluation and peak fitting were performed using the CasaXPS software. Thermal Gravimetric Analysis (TGA) were performed using a TGA-50 (Shimadzu, Japan) under argon (flow rate of 50 mL/min) at a heating rate of 1°C/min from 30 to 800°C for graphene oxide and a heating rate of 5°C/min from 30 to 800°C for reduced graphene oxide. The Raman spectra were recorded on a Renishaw 1000 Raman Imaging Microscope consisting of a single grating spectrograph with holographic notch filter to remove Rayleigh scattered light, Leitz microscope, and air-cooled CCD array detector. The excitation laser was a Spectra-Physics Air-Cooled Argon ion laser with a blue emission line at 488 nm at 25 mW in combination with 2400 lines/mm grating. Fourier Transform Infrared (FTIR) analyses were performed using the Smart Orbit Diamond Attenuated Total Reflection (ATR) single reflection accessory of a Thermo Electron Nicolet 8700 FTIR spectrometer. The signals were processed using the OMNIC spectroscopic software.

3. Results and Discussion

3.1. Synthesis and Processing of MTH-GO

The oxidation temperature is the most critical parameter in graphite oxidation. Generally, the temperature of 35°C is used in the original Hummers' method. In this study, a reaction temperature of 50°C was used and the postheating step (98°C for 15 min) was eliminated. Increasing the reaction temperature to 50°C could enhance the rate and degree of oxidation. In Tour's improved method [35], 50°C was also shown to be an effective reaction temperature for the oxidation of graphite. However, the appropriate safe temperature should never exceed 55°C as manganese heptoxide (Mn₂ O₇ ) is explosive at temperatures above that. For the reader's benefit, the colour changes during the synthesis are illustrated in Figures 1(a)-1(d). As shown in Figure 2, the MTH-GO can be used to prepare partially transparent and free-standing membranes using vacuum filtration [36], with excellent mechanical properties including flexibility (Figures 2(a) and 2(b)). The Tyndall effect can be observed by the laser scattering in the fine colloidal MTH-GO aqueous suspension (Figure 2(c)). Finally, MTH-GO can be coated onto polyethylene terephthalate ( PET) films for laser inscription (Figure 2(d)).

Figure 2: (a) Partially transparent MTH-GO membrane; (b) free-standing and flexible MTH-GO membrane; (c) Tyndall effect of MTH-GO dispersion in water; (d) MTH-GO coating on PET film.

(a) [figure omitted; refer to PDF]

(b) [figure omitted; refer to PDF]

(c) [figure omitted; refer to PDF]

(d) [figure omitted; refer to PDF]

3.2. Chemical Reduction by Lithium Triethylborohydride (LiEt₃ BH)

In the "tool box" of organic chemistry, the reduction using hydrides is well understood [37]. Sodium borohydride (NaBH₄ ) is a common reducing agent in synthetic chemistry. When used in the presence of carbonyl groups, the borohydride can carry out a hydride transfer reaction to form an oxyanion and BH₃ molecule. However, the reduction of borohydride is limited by the types of carbonyl. Gao and coauthors [38] reported a complete reduction process using NaBH₄ as the first step of a three-step synthesis. After treatment of sulfuric acid and thermal annealing, the π -conjugated structure was effectively restored. Only less than 0.5 wt% of nitrogen and sulfur was left, which was more effective than other reduction methods.

Another common hydride is lithium aluminium hydride (LAH), one of the strongest reducing agents in organic synthetic chemistry. Ambrosi et al. [30] recently reported using lithium aluminum hydride to reduce graphene oxide and achieve a C/O ratio of 12.

Krishnamurthy and Brown [32] suggested that LiEt₃ BH is a strong reducing agent available for unselectively reducing carboxylic acids, carbonyls, and epoxy groups to corresponding hydroxyl groups. LiEt₃ BH has recently been reported in the production of thermally exfoliated graphene-Li₂ S nanocomposite, where sulfur loaded graphene was chemically modified using LiEt₃ BH to form uniformly dispersed Li₂ S nanoparticles [39]. Here, we show results from the chemical reduction of graphene oxide using this unselective reducing agent.

3.3. Characterization of MTH-GO and LiEt₃ BH-RGO

A variety of techniques were employed to identify MTH-GO's chemical structure and composition. Firstly, the solid state ¹³ C NMR result is illustrated in Figure 3, the major peak representing epoxide groups (C-O-C) is located at 61 ppm. The carbon adjacent to hydroxyl groups (C-OH) was shifted to 70 ppm; this peak only appears as a small shoulder embedded within dominant epoxide groups [38, 40]. Other carbonaceous signals can also be distinguished and stand for lactol groups (O-C-O) at 101 pm, lactol carbonyls, and esters near 164 ppm and ketone carbonyl groups at 191 ppm. The remaining broad peak at 130 ppm was designated to the sp² carbon from original graphitic structure. Those findings are consistent with the results reported in the literature [38, 40].

Figure 3: Solid state ¹³ C NMR spectrum of MTH-GO sample.

[figure omitted; refer to PDF]

Due to the limited solubility of graphene oxide, quantifying the C/O ratio using standard techniques (such as solution NMR) is not possible. Therefore, XPS was used to measure the chemical state of the element carbon at the graphene oxide surface. The C1s spectrum of MTH-GO (Figure 4) revealed five peaks, by deconvoluting that corresponds to the following functional groups including sp² carbon (C=C, 283.4 eV), sp³ carbon (C-C, 284.4 eV), epoxy/hydroxyls (C-O, 286.4 eV), carbonyl (C=O, 287.4 eV), and carboxylates (O-C=O, 288.5 eV). The higher energy peak at [approximate]292 eV is attributed to [figure omitted; refer to PDF] shakeup satellite of the sp² carbon. The binding energies of these functional groups were consistent with literature results [30]. Overall, the integration of combined oxidized carbon and that of graphitic carbon (both sp² and sp³ carbons) gives a ratio of oxidized to nonoxidized carbon species of approximately 1.6; that is, 60% of the carbon is in a oxidized form (in agreement with the overall O/C ratio of 0.6 derived from the survey spectra), which is similar to the reported degree of oxidation by other methods [35]. Near edge X-ray absorption fine structure (NEXAFS) measurements were also recently employed to compare the properties of graphene oxide produced by Hummers' and Tour methods, indicaing a higher incidence of C-OH and C=O functional groups in the material prepared by Tours' method [41].

Figure 4: C1s XPS spectra of MTH-GO.

[figure omitted; refer to PDF]

The morphology of both MTH-GO and LiEt₃ BH-RGO was investigated using AFM and SEM. For AFM imaging, a very dilute solution of MTH-GO or LiEt₃ BH-RGO was transferred onto a freshly cleaved mica. As shown in Figure 5, layers of MTH-GO are clearly visible at the surface, some overlapping each other and some curling up [35].

Figure 5: Tapping mode AFM image (a) shows the topography of MTH-GO and its height profile in (b). After LiEt₃ BH reduction, LiEt₃ BH-RGO sheets were diluted and ultrasonicated in water. Image (c) shows the topography of LiEt₃ BH-RGO suspension on mica and its cross-section analysis in (d).

(a) [figure omitted; refer to PDF]

(b) [figure omitted; refer to PDF]

(c) [figure omitted; refer to PDF]

(d) [figure omitted; refer to PDF]

The monolayer nature of graphene oxide and reduced graphene oxide was confirmed by AFM (Figure 5). The thickness of both MTH-GO and LiEt₃ BH-RGO was measured from section analysis to be in the range of 1.1-1.5 nm (data from several images, example shown in Figure 5), with LiEt₃ BH-RGO displaying more flexible/folded sheets. The LiEt₃ BH-RGO flakes (shown in Figure 5(c)) display numerous hole defects. The formation of holes may be caused by the removal of oxygen groups from the carbon lattice during the reduction resulting in vacancies forming on monolayer graphene sheets [42].

SEM was also performed to give further insight into the morphology and to compare the O/C ratio for MTH-GO and LiEt₃ BH-RGO (Figure 6 shows two different magnifications for each sample type). The SEM has shown an apparent change to a more wrinkled morphology after the reduction, resembling a very thin curtain, consistent with AFM.

Figure 6: SEM images of MTH-GO before (a-b) and after (c-d) LiEt₃ BH reduction with a low magnification of 1000x (top row) or high magnification of 25000x (bottom row).

[figure omitted; refer to PDF]

EDS (energy-dispersive X-ray spectroscopy) was used to characterize the elemental composition of MTH-GO and LiEt₃ BH-RGO. The atomic ratio of carbon to oxygen in MTH-GO was ~3.7 which increased to ~10.8 after the reduction. This is consistent with values reported previously (~8.8-12.5) [43] in the case of using reducing agent for reduction of MTH-GO. In addition, ~1.7 At % of sulfur was detected in MTH-GO, which may be residual sulfuric acid from the Hummer based preparation method. The sulfur content was significantly reduced in the LiEt₃ BH-RGO (~0.22 At %).

The UV-Vis characterization of MTH-GO and LiEt₃ BH-RGO (Figure 7) shows a prominent peak at 228 nm with shoulder band around 300 nm, this mostly originates from the conjugated structures of unoxidized graphitic domains (sp² C=C bond) [35, 44]. The shoulder peak originates from [figure omitted; refer to PDF] transitions of the carbonyl groups; these were clearly observed which is an excellent indication of the high degree of oxidation in the MTH-GO sample [44]. The absorption peak of LiEt₃ BH-RGO dispersion was shifted to ~260 nm from 228 nm after the chemical reduction. This could suggest that the LiEt₃ BH reduction is able to restore the electronic conjugation structure, as expected [44].

Figure 7: The UV-Vis spectra show the absorption change of MTH-GO and LiEt₃ BH-RGO after LiEt₃ BH reduction.

[figure omitted; refer to PDF]

Figure 8 compares the FTIR spectra of MTH-GO and LiEt₃ BH-RGO. For MTH-GO, a very broad, composite peak between 3000 and 3600 cm^-1 was observed due to the stretching vibration of hydroxyl group and physisorbed water. The secondary characteristic absorbance peaks from MTH-GO include a peak at 1736 cm^-1 corresponding to the C=O stretching vibration from the carboxyl group at the periphery of GO sheets and a band at around 1220 cm^-1 assigned to the C-O-C stretching vibration from epoxy groups on the basal plane. The FTIR spectrum of MTH-GO also displayed the presence of a peak at 1633 cm^-1 , attributed as an additive peak of both the bending mode of associated water and the contribution from the C=C (sp² ) bonds (seen as a shoulder around 1580 cm^-1 ). The contribution from the C=C (sp² ) modes is seen to vastly increase upon the reduction to LiEt₃ BH-RGO as expected. The FTIR-ATR characterization of MTH-GO was consistent with graphene oxide prepared by other methods [35]. After LiEt₃ BH chemical reduction, all absorbance intensities associated with oxygenous functional groups (carbonyl, epoxide, and hydroxyl, etc.) were decreased dramatically, showing that the MTH-GO was reduced to the LiEt₃ BH-RGO. The relative strong band at 1586 cm^-1 is the C=C stretching of sp² carbon from graphitic structures, with the water mode at 1633 cm^-1 present in MTH-GO being significantly reduced [27, 45]. The methyl and ethyl C-H stretching vibrations are seen to arise at 2800 cm^-1 -3000 cm^-1 as the functional groups in MTH-GO are reduced. The absorbance between 3100 cm^-1 and 3500 cm^-1 has been significantly diminished and corresponds to any residual hydroxyl groups or physisorbed water.

Figure 8: FTIR-ATR spectra of MTH-GO and LiEt₃ BH-RGO.

[figure omitted; refer to PDF]

To probe more information on the quality of the LiEt₃ BH-RGO by our lithium triethylborohydride method, Raman spectra of MTH-GO and LiEt₃ BH-RGO (Figure 9) were also collected and compared. The Raman spectrum of graphene is dominated by two features: the G mode ([approximate]1575 cm^-1 ) and the D mode ([approximate]1350 cm^-1 ), where the D mode relates to disorder in the sp² hybridized carbon system [27]. Both samples investigated here displayed two main absorbance peaks around 1355 cm^-1 and 1600 cm^-1 , corresponding to the D and G bands, respectively. The D band displays a shift from 1353 cm^-1 to 1359 cm^-1 after the reduction. This correlates to the loss of associated water in-between the layers of sp² hybridized carbon. In terms of peak intensity, the D band increased with concomitant decrease of the G band after lithium triethylborohydride reduction. Clearly, the reduction process transformed the structure of MTH-GO and produced domains of chemically reduced graphene. The [figure omitted; refer to PDF] ratio of LiEt₃ BH-RGO was about 1.06, while [figure omitted; refer to PDF] of MTH-GO is 0.85, indicating a more disordered structure. This result is consistent with other reduction methods, such as alumina powder [23], hydriodic acid [15], and hydrothermal "green" approaches [46].

Figure 9: Raman spectra of MTH-GO and LiEt₃ BH-RGO using 488 nm laser.

[figure omitted; refer to PDF]

The successful reduction of MTH-GO with LiEt₃ BH was further supported by TGA results as shown in Figure 10. The major weight loss of MTH-GO took place at three temperature zones. Approximately 10% of weight loss occurred between 30°C and 100°C and was due to the evaporation of absorbed water. The labile oxygenous functional groups (about 25 wt%) were eliminated between 140°C and 190°C with releasing CO₂ and other small molecules. The third significant mass loss occurred from 500°C to 600°C, which could be the pyrolysis of residual debris. Ultimately, all components were nearly gone resulting in less than 20% char yield. The TGA characterization of MTH-GO was consistent with the result reported by Stankovich et al. [18]. The thermal decomposition graphene oxide usually releases gas vigorously. During a fast heating process, rapid thermal expansion could occur, potentially leading to mass loss as well as instrument damage [18]. Therefore, here we chose a relatively slow heating rate (1°C/s) to analyse MTH-GO's thermal decomposition [18].

Figure 10: TGA investigation of decomposition behavior of MTH-GO with a heating rate of 1°C/min and LiEt₃ BH-RGO with the heating rate of 5°C/min (both under argon).

[figure omitted; refer to PDF]

In comparison, the TGA thermogram of LiEt₃ BH-RGO shows significantly improved thermal stability compared to MTH-GO. Interestingly, while the remainder of the reduced graphene oxide gave featureless and progressive weight loss [18, 22], the LiEt₃ BH-RGO had a noticeable weight loss which took place between 300 and 350°C as a result of the remaining oxygenous species. The overall weight loss of LiEt₃ BH-RGO from room temperature to 800°C is around 30%.

4. Conclusions

In conclusion, the main objectives for the new oxidation temperature to prepare high quality graphene oxide and a new chemical reduction reagent of lithium triethylborohydride (LiEt₃ BH) were achieved. Based on Hummers' method, the graphite oxidation temperature could be increased from 35°C to 50°C, and the second high-temperature step could be completely removed. As with other preparation methods, the synthesized MTH-GO contains different types of functional groups consisting of hydroxyl, carbonyl, and epoxide groups. Lithium triethylborohydride was demonstrated as an effective alternative reagent for graphene oxide chemical reduction as demonstrated through AFM, SEM/EDS, UV-Vis, FTIR, Raman, and TGA characterization.

Highlights

Note the following highlights:

(i) increased temperature (50°C) for Hummers' method to synthesize graphene oxide;

(ii) spectral analysis on the graphene oxide by different methods;

(iii): a new procedure for the reduction of graphene oxide by lithium triethylborohydride shown to be effective.

Acknowledgments

Jianyong Jin and Neil Broderick would like to thank The University of Auckland Faculty Research Development Fund (FRDF) Project no. 3702174 for their financial assistance. Jenny Malmström acknowledges the financial support from the MacDiarmid Institute for Advanced Materials and Nanotechnology. Guangyuan Xu is also grateful to Dr. Zoran Zujovic for assistance on solid state ¹³ C NMR, Dr. Michel Nieuwoudt for Raman, Ms. Catherine Hobbis for SEM/EDS, Dr. Xiaobo Ding, and Mr. Radesh Singh. All the authors thank their colleagues, Walt Wheelwright, Velram Balaji Mohan, Christopher Wilcox, Hong Kang, Alissa Hackett, Eddie Chan, Jian Zhang, James Wu, Zhixiu Wu, and Chao Liang, for their kind help.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

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