- Open Access
Surfactant mediated liquid phase exfoliation of graphene
© Narayan and Kim. 2015
- Received: 25 March 2015
- Accepted: 18 May 2015
- Published: 8 October 2015
Commercialization of graphene based applications inevitably requires cost effective mass production. From the early days of research on graphene, direct liquid phase exfoliation (LPE) of graphite has been considered as the most promising strategy to produce high-quality mono or few-layer graphene sheets in solvent dispersion forms. Substantial success has been achieved thus far in the LPE of graphene employing numerous solvent systems and suitable surfactants. This invited review article principally showcase the recent research progress as well as shortcomings of surfactant assisted LPE of graphene. In particular, a comprehensive assessment of the quality and yield of the graphene sheets produced by different categories of the surfactants are summarized. Future direction of LPE methods is also proposed for the eventual success of commercial applications.
Graphene has been the most sensational material discovery over the past decades along with its unprecedented material properties such as ultrahigh tensile strength (~1TPa), high thermal conductivity of (5,000 W m−1 K−1), large specific surface area (2,630 m2 g−1), ballistic electron mobility (250,000 cm2V−1 s−1) and optical transparency (97.7 %) [1–6]. As a result of the worldwide boom in graphene research, a wide range of applications have been explored, including flexible/stretchable devices [7–9], high-frequency transistors [10, 11], energy storage/conversion , sensors , biomedical applications , and composites . Despite numerous research efforts, nonetheless, the discovery still seems far from commercial reality, which is principally due to the limited scalability and high cost of currently available graphene production methods.
Graphene production methods can be classified into top-down and bottom-up approaches. Well-known top-down methods include (i) mechanical exfoliation (Scotch tape method) historically used in the first discovery of graphene by Geim and Novoselov , (ii) chemically converted graphene (reduction of graphene oxide) , (iii) electrochemical exfoliation , (iv) liquid phase exfoliation (LPE) in the presence/absence of surfactants  and so on. Bottom-up approaches synthesize mono or few layer graphene structures from small molecule organic precursors by catalytic chemical vapour deposition (CVD) or organic synthesis or epitaxial growth on SiC and so on. Presently, reduction of chemically exfoliated graphene oxide is the most popular strategy for bulk graphene production among the aforementioned various approaches. Unfortunately, post-reduction methods cannot completely cure the structural defects introduced by the strong oxidation process. Thus, the band structure and electronic properties unique to graphene are severely deteriorated.
From early days of graphene research, LPE has been anticipated as the most desirable mass-production method for graphene. The principal attraction of this method is that, it is a straightforward and scalable process where pristine graphite or expandable graphite (obtained by thermal or microwave expansion of graphite intercalation compounds) is directly subjected to a solvent treatment to weaken the van der Waals attractive forces between graphene interlayers. External driving force such as ultrasonication, electric field or shearing can be applied to facilitate the spontaneous exfoliation into graphene sheets. Another significant advantage of this method is the production of exfoliated graphene sheets in the form of solvent suspension that allows an immediate utilization for spin-coating, spray painting or any other solution processing. For instance, simple vacuum filtration of the as-obtained graphene suspensions can be used for the fabrication of thin films with high conductivities . Novel graphene/polymer composites can be easily prepared by direct solution mixing. As such, LPE method addresses all crucial prospects for viable industrial applications.
Graphene is known to suffer from only a limited solvent dispersibility even for its good solvents, such as DMF or NMP, which is due to the small mixing entropy gain and strong intersheet π-π attraction of the generic two-dimensional structure. Moreover, those good solvents are toxic, expensive and not so volatile such that solution processing from those solvents is practically challenging. Alternative route is to employ an appropriate surfactant, which can mediate dispersion in water or any other mild volatile solvents. To date, a variety of surfactants belonging to different categories, including ionic /non-ionic, aromatic/non-aromatic, polymeric etc. have been investigated. However, these researches require further optimization for practical use and it is highly recommended to understand surfactant-solvent interaction in a more systematic way. To this end, this review article is motivated to offer an overview on the state-of art of LPE of graphene with the prime focus on surfactant-assisted exfoliation. In the first part of this article, we will briefly discuss the key parameters involved in the optimization of a fruitful LPE recipe. The subsequent sections will provide a systematically categorized comprehensive discussion on the recent progress in the surfactant promoted LPE of graphene.
2.1 Dispersing medium : solvent
where ∆Hmix is the enthalpy of mixing, Vmix is the volume of the mixture, TNS the thickness of graphene nanosheet, ESS and ESG are the surface energies of solvent and graphene, respectively, ɸG is the volume fraction of graphene dispersed. Accordingly, solvents belonging to this category, including N-methylpyrrolidone (NMP) (γ = 40 mJ m−2), N,N’-dimethylformamide (DMF) (γ = 37.1 mJ m−2) and ortho-dichlorobenzene (o-DCB) (γ = 37 mJ m−2) have been widely employed for LPE of graphene.
Ortho-dichlorobenzene (o-DCB) was shown to be another fair solvent for graphite exfoliation giving a dispersibility range of 0.03 mg/mL . Following the trend, Bourlinos et al. in 2009 explored a series of electron deficient perfluorinated aromatic solvents such as hexafluorobenzene(C6F6), octafluorotoluene (C6F5CF3), pentafluorobenzonitrile (C6F5CN), and pentafluoropyridine (C5F5N) to exfoliate fine graphite powder within relatively short sonication period of 1 h. Maximum dispersion concentration upto 0.1 mg/mL were obtained with pentafluorobenzonitrile, whereas the poorest yield of 0.05 mg/mL was measured for octafluorotoluene as well as pentafluoropyridine , Inspired by Coleman’s approach, Tagmatarchis and co-workers accomplished efficient exfoliation of graphite flakes in benzylamine solvent for prolonged sonication periods of 4–6 h leading to improved few-layer graphene dispersion concentration ~ 0.5 mg/mL . Further increase of the sonication period beyond 10 h did not seem to cause any increase in dispersion concentration. In a very recent study, to overcome the low yield and poor exfoliation issues, Sun et al. introduced four amine based organic solvents, namely 3,30-iminobis (N,Ndimethylpropylamine) (DMPA), N-[3-(dimethylamino)propyl]methacrylamide (DMAPMA), 2-(tert-butylamino) ethyl methacrylate (BAEMA) and 2-(dimethylamino) ethyl methacrylate (MAEMA), which challenge to outperform the previously known the best solvent, NMP, and other LPE systems with surfactants, including sodium cholate (SC), sodium taurodeoxycholate (STC) and polyvinylpyrrolidone(PVP) . In their control experiments, in particular DMPA exhibited 1.5 times higher dispersing capacity than NMP. Further optimization of the process was done using pre-exfoliated graphene as a starting material, obtained from 12 h bath sonication in isopropanol. This promoted the final graphene concentration up to ~1.4 mg/mL with a yield of 14 %. Spontaneous exfoliation of HOPG in chlorosulfonic acid was achieved by Behabtu et al. to produce a high concentration dispersion of monolayer sheets upto 2 mg/mL .
Majority of the above discussed solvents, even though successful to large extent, have significant drawbacks that limit the scalability for industrial manufacture. Solvents like NMP, DMF etc. are very expensive as well as highly toxic. In particular, NMP is regarded as a potential human reproductive hazard, which is easily absorbed through skin. Moreover, these solvents have high boiling points (NMP, 203 °C), making it difficult to deposit the exfoliated graphene flakes onto a target substrate. This would be a critical drawback in the fabrication of graphene transparent conductor for solar cells , field effect transistors , photodetectors  and so on. As those solvents take significant time for evaporation, re-aggregation of exfoliated graphene sheets may easily occur. Therefore, it is of paramount significance to explore more volatile and less toxic solvents along with the superior dispersing capability. To this end, attempts had been made to transfer graphene dispersions in NMP to low boiling solvents like ethanol via solvent exchange, noteworthy the sample showed 20 % sedimentation within one week . Nonetheless, direct graphene exfoliation in a single low boiling solvent is always preferable owing to the simplicity of process. Catheline et al. applied volatile THF (tetrahydrofuran) to produce graphenide solutions (solutions of negatively charged graphene flakes) by dissolution of graphite intercalation compound (GIC) KC8 . Severely crumpled graphene sheets were obtained that made it difficult to determine the precise thickness. A solvothermal-assisted exfoliation of expanded graphite in acetonitrile was attempted by Hou et al. utilizing the dipole-induced dipole interactions between graphene and polar acetonitrile . Coleman et al. investigated some common volatile solvents like chloroform, isopropanol and acetone as exfoliating media for graphene, but longer sonication times around 360 h were required to produce dispersions with the concentrations of 0.4 and 0.5 mg/mL from chloroform and isopropanol respectively .
2.2 External forces : ultrasonication/shear mixing
Recently, Coleman et al. reported high-shear mixing as a scalable alternative to sonication for the LPE of untreated graphite crystals. They demonstrated the scalability of the method to industrial manufacture level (Fig. 2(c)) . Once the local shear rate exceeds 104 s−1, exfoliation could produce large quantities (production rate as high as 0.4 g h−1) of defect-free, unoxidized graphene as indicated by the XPS and Raman spectroscopy.
2.3 Purification: centrifugation
In many cases, it is difficult to decouple the effect of area and thickness polydispersity, which makes sedimentation-based centrifugal separation less useful. Under these conditions Green and Hersam succeeded in isolating monodisperse graphene dispersions according to their buoyant densities using density gradient ultracentrifugation (DGU) . These thickness controlled graphene fractions were generated from sodium cholate encapsulated aqueous graphene dispersions, similar to that used for DGU separation of carbon nanotubes . In DGU separation, the graphene dispersion is introduced to a density gradient designed with matching buoyant density distribution. These density gradients upon ultracentrifugation, moves the graphene sheets to their isopycnic points, where the buoyant density of graphene matches with that of the medium. Consequently visible bands appear in the centrifuge tube (Fig. 3(e)), signature of successful isopycnic separations. A monotonic increase in the thickness of the graphene with increasing buoyant density was observed from AFM measurements (Fig. 3(f-g)) along with selective enrichment of 1–4 layered graphene sheets. Samples with ∼ 85 % monolayer graphene have been produced using this process. In this approach, nonetheless, the density of the environment has to precisely match with that of the flake, which in turn would depend on both the thickness and lateral size of the flakes.
As mentioned in the introduction part, use of surfactants in the LPE of graphene is principally motivated to explore water as an exfoliating medium. By adding suitable surfactants, the high surface energy of water (72.8 mJ m−2) could be reduced and optimized to make a feasible interaction with highly hydrophobic graphitic surfaces. The first aqueous surfactant based exfoliation was reported by Lotya et al. using sodium dodecyl benzene sulfonate (SDBS) . Following researches proved that surfactant assisted exfoliation can promote the stabilization of suspended graphene sheets against re-aggregation in organic solvents as well. A wide variety of ionic as well as non-ionic surfactants have been explored including both small molecules and polymers. Using non-covalent interactions, these surfactants interact with graphene surface by surface adsorption, micelle formation and/or π-π stacking. Ionic surfactants adsorbed onto graphene impart an effective charge, providing electrostatic repulsion to prevent re-aggregation of graphene sheets; meanwhile non-ionic surfactants provide the stabilization via steric interactions. We classified the entire range of surfactants into four main categories; (1) Aromatic and (2) Non-aromatic small molecules, (3) Ionic liquids and (4) Polymers, and discussed individually in the subsequent sections.
3.1 Aromatic small molecule surfactants
3.1.1 Aromatic ionic surfactants
Aromatic small molecules can act as highly efficient surfactants because of their hydrophobic surfaces similar graphene and the strong π-π interactions between them can facilitate LPE process. SDBS, the first surfactant tested for graphite exfoliation, is also an aromatic ionic molecule with a polar sulfonate group and hydrophobic dodecyl chain attached to benzene ring . A mixture of water, pristine graphite and SDBS were sonicated for 30 min, followed by centrifugation at 500 rpm for 90 min to produce 0.002 - 0.05 mg/mL suspensions. Small quantities (~3 %) of monolayer and large quantities (~43 %) of multi-layer (<5 layers) sheets were observed from the TEM and AFM analysis. Thin films prepared by the vacuum filtration of the as-obtained graphene suspensions showed a high sheet resistance (~970 kΩ/□) and conductivity (35 S/cm).
Hou et al. prepared aromatic anionic TCNQ (7,7,8,8-tetracyano-quinodimethane) coated graphene sheet suspensions in water as well as organic solvents . The expanded graphite was mixed with TCNQ with a few drops of DMSO and the subsequent exfoliation was carried out in water in the presence of KOH to facilitate the reduction of TCNQ to harmful TCNQ anion. The exfoliated graphene sheets were principally 2–3 layer thick and lateral dimensions ranged from hundreds of nanometres to few micrometres. Notably, the Raman analysis of TCNQ adsorbed graphene showed an increased ID/IG value compared with starting expanded graphite, which was attributed to the structural defects arising from the increased boundary edges of exfoliated sheets.
Charge transfer interactions between aromatic coronene salt and graphene were demonstrated by Rao et al. to exfoliate few layer graphene sheets prepared from thermally exfoliated graphite oxide (EG) and arc evaporated graphite in hydrogen atmosphere (HG) . The starting materials EG/HG were mixed with the coronene surfactant and heated to 100 °C for 24 h, followed by a sonication at 70 °C for 2 h. Stable graphene suspensions with majority mono- and few-layer sheets were revealed by microscopic studies. Another aromatic amphiphilic molecule, Rose Bengal with a hydrophilic carboxylate group and hydrophobic aromatic framework was also found to be useful for exfoliation of microwave expanded graphite in 10 % DMA (N,N-dimethyl acetamide) aqueous solution . More than 6 h bath sonication produced a mixture of mono- and few layer graphene dispersion with 12 wt.% yield and thin film prepared by vacuum filtration showed a high electrical conductivity of 12280 S/cm. Recently, Chen et al. showed direct exfoliation of HOPG (highly oriented pyrolytic graphite) using pyridinium tribromide (Py + Br3-) in 1:1 ethanol-water mixtures to give around 75 % monolayer sheets, which were stable over an year without any agglomeration . In particular, the exfoliated flakes contained no significant defects as it was indicated by the absence of D-peak in the Raman spectra and exhibited notably high conductivity value of 5100 S/cm.
In recent years, commercially available pyrene derivatives with suitable polar functional groups have been used by large number of research groups, as stabilizers in graphene exfoliation. Commercial availability and high exfoliation efficiency compared to traditional surfactants are the principal motivations. Almost 90 % yield of monolayered graphene sheets was achieved by Dong et al. in 2009, by exfoliation of graphite powders with tetrasodium salt of 1,3,6,8-pyrenetetrasulfonic acid (Py-4SO3) . In 2010, Zang et al. also reported aqueous phase exfoliation of graphite using 1-pyrenemethylamine hydrochloride (Py-NH3 +) and 1,3,6,8-pyrenetetrasulfonic acid (Py-4SO3-) tetrasodium salt hydrate . Fairly good quality few-layer graphene sheets with total oxygen content of 8.5 % and 16 % were obtained for Gr-Py-NH2 and Gr-Py-4SO3 hybrids, respectively, with nearly 50 % yield. In both the dispersions, positive and negative charges of the respective pyrene molecules adsorbed onto graphene surface provided static repulsive forces stabilizing the exfoliated sheets. More importantly, the pyrene derivatives acted as healing agents or electric “glue” during subsequent thermal annealing, where ID/IG value of Raman spectroscopy changed from 0.64 to 0.46. Consequently, a high conductivity of 181200 S/m (778 Ω/□) and a light transmittance greater than 90 % were exhibited by the as-prepared graphene films, which is the highest conductivity value ever achieved for graphene films prepared by LPE (note that graphene films fabricated by the CVD method can reach 200 Ω/□ at 80 % transparency) . Again in 2010, Kar and co-workers reported 1-pyrenecarboxylic acid (PCA) molecule assisted LPE of graphite powder, which had been commonly used to debundle single wall carbon nanotubes . Graphite powder and PCA in methanol/water mixtures were sonicated for more than 24 h. Methanol was added to aid complete dissolution of amphiphilic PCA molecule. The non-covalent interaction of π-clouds produced graphene-PCA complex in 1 wt % yield, where the concentration of graphene in the final dispersions were around 0.01 mg/mL. The exfoliated graphene was a mixture of mono- and multilayer flakes. Nonetheless, the authors demonstrated highly sensitive and selective conductometric sensor application (whose resistance rapidly changes >10 000 % in saturated ethanol vapor), and ultracapacitors with extremely high specific capacitance (∼120 F/g), power density (∼105 kW/kg), and energy density (∼9.2 Wh/kg). In 2011, Rangappa and Honma et al. used 1-pyrene sulfonic acid sodium salt (Py-1SO3) in a novel one-pot in-situ supercritical fluid exfoliation of graphite in ethanol-water mixtures . The presence of Py-1SO3 was shown to increase the mono- to bilayer graphene yield up to 60 % and also an increased Li-ion storage capacity was demonstrated compared to pure graphite materials.
A bunch of different pyrene derivatives were compared by Green and co-workers as stabilizers for expanded graphite exfoliation, which included pyrene (Py), 1-aminopyrene (Py–NH2), 1-aminomethyl pyrene (Py–Me–NH2), 1-pyrenecarboxylic acid (Py-COOH), 1-pyrenebutyric acid (Py-BA), 1-pyrenebutanol (Py-BuOH), 1-pyrenesulfonic acid hydrate (Py-SAH), 1-pyrenesulfonic acid sodium salt (Py–1SO3) and 1,3,6,8-pyrenetetrasulfonic tetra acid tetra sodium salt (Py–4SO3) . For all those pyrene derivatives the final graphene concentration increased initially with the addition of stabilizers and then decreased or remained constant (Fig. 5c); the highest yield obtained with Py-1SO3 which was around 0.8-1 mg/mL, whereas Py-4SO3 assisted exfoliation produced only 0.04 mg/mL few-layer graphene dispersion. Dispersions from pyrene stabilizers with sulfonyl functional groups also exhibited high temperature stability, hence promising for high temperature processing. Notably, the TEM images of Py-1SO3/Gr dispersion showed multi-layers and no information provided regarding the shelf-life of the dispersions.
Comparison of different aromatic ionic surfactants for producing colloidal dispersions of graphene
Flake lateral size
Graphite powder Sigma/Water
Low power bath sonication (Branson 1510E-MT) 30 min
Majority less than 5 layers. Exact value not given
35 % stable over 30 days
Sonication time 90 min.; type not mentioned.
100 nm –few μm
Majority 2-3 layers
Thermally exfoliated graphite oxide (EG)(5L±1)/water
Heating Gr/CS mixtures at 100 oC for 24 hrs. Sonication time 2 hrs at 70 oC; type not mentioned.
HG-CS yield given 0.15mg/mL. EG-CS yield not mentioned
0.5-1 nm thick 1-2layer flakes
Arc evaporated graphite in hydrogen atmosphere (HG)(3L±1)/water
Expanded Graphite by microwave assisted heating/10 % Dimethyl-acetamide aqueous solution
Bath sonication 250W/6-10 hrs.
12 wt %
>80 %,2-3layer flakes
Bath type sonicator(Branson® 3510R-DTH)/45 min
sub μm to several μms
Average thickness 174±105 nm. 75 % single layer
Graphite powder (Alfa Aesar)/ DMF, Water
Sonication time 30 min; type not mentioned
2-4 layers majority
More than 3 weeks
Graphite powder (Alfa Aesar)/ DMF, Water
Time 24 hrs
No exfoliation at all.
Graphite powder (Sigma)/ Methanol-water (1:4)
Bath sonicator (Branson 5510) 45 min sonication in MeOH, 24 hrs sonication in MeOH/H2O.
100 nm to few μm
Less than 10 nm thick few layers.
Synthetic graphite (<20 μm) (Sigma)/Water
Bath Sonicator (Sonics VX-130, 130W, 45 % power)ice bath, 2hrs
Average thickness 0.9±3 nm
Synthetic graphite (<20 μm) (Sigma)/water
Less than 2 hrs
Average thickness 1.3 -2.6 nm
Graphite powder /Ehtanol-water (5:1)
Bath sonication (US-4R, 40KHz, 10W)/30 min, followed by heating at 450 oC for 2h with SCF shaking.
0.6-2 nm 60 % 1-2layers.
Expanded Graphite (Asbury Carbons CAS 7782-425 ,GRADE-3805)/DI-water
Tip sonication(Misonix-XL2000, 7W)/1hr.
Graphite powder (NGS-Germany)/D2O solvent
70 W Probe sonicator(pulse mode in ice bath)/2hrs
1.29-1.65 nm 90 % single layer
3.1.2 Aromatic non-ionic surfactants
3.1.3 Non-aromatic surfactants
Samori et al. recently demonstrated a long chain aliphatic fatty acid, arachidic acid that exhibits a high selectivity to graphene surface attachment, so as to act as dispersion-stabilizing compound for LPE . High concentration conductive graphene ink was prepared following this supramolecular strategy and, thus, opened up new avenues for cost effective technological applications. Relevant reports motivated from this work are rapidly growing with many suggestions for the potential surfactants for low cost exfoliation, some of which include Gum Arabic , organosilanes , cellulose nanocrystals  etc.
3.1.4 Ionic liquids
Very recently, Texter and co-workers developed two excellent water stabilizers for graphene viz., triblock (TB) copolymer and copolymer nanolatex (NL) (Fig. 8(c)) based on a reactive IL acrylate surfactant 1-(11-acrylyoyloxyundecyl)-3-methyl imidazolium bromide (ILBr) . Surprisingly, this method claim essentially complete exfoliation without the need of centrifugation to eliminate any undispersed contents and could produce graphene aggregates in water at concentrations upto 5 w %. They demonstrated that these graphene dispersions were rheo-optical fluids and simple Couette shear fields could align submicron-micron sheets over macroscopic areas indicating its bright future for surface coating applications. Moreover, the work also illustrated the transfer of graphene sheets in water to non-aqueous media with the aid of stimuli responsiveness to various anions. Despite all these advantages, the procedure adopted high power and remarkably long sonication time upto 113 h, which has led to dramatically reduced flake dimensions, as confirmed by SEM. Nevertheless, given the very high graphene concentrations obtained by this protocol, ILs deserve more detailed investigation for LPE, even though the yield of monolayers seem to be unclear yet.
3.1.5 Polymeric surfactants
Researches on polymer stabilized LPE has expanded realms such that it is impossible to consider all of them in this confined discussion. It is noteworthy that the resulting graphene/polymer composites commonly exhibit novel synergistic properties, which are unknown in the individual components. In this section, we will provide only a brief discussion on some of the most highlighted investigations.
There are many studies on the exfoliated graphene composites based on a wide range of polymers, for instance, polystyrene (PS) , poly(styrene-co-butadiene-co-styrene) , poly methyl methacrylate (PMMA) , polyetherimide (PEId) , polylactide (PLA) , polypropylene , cellulose acetate , hyperbranched polyethylene (HBPE)  and so on. Since graphene is highly hydrophobic in nature, organic solvents are much more compatible for LPE, but water appears to be a more appealing choice when it comes to a cheaper and non-toxic green solvent for scalable processing. Such a hydrophobic to hydrophilic switching of graphite surface was achieved by Bourlinos et al. without any oxidation or damage to the sp2 carbon framework of graphene . They chose polyvinylpyrrolidone (PVP) (Fig. 9(a)), a non-ionic and biocompatible polymer surfactant for the straightforward LPE of graphene in aqueous phase under mild sonication for about 9 hrs. Specifically, PVP was chosen owing to its high solubility in water and great affinity to graphite surface; another reason was that PVP contains N-substituted pyrrolidone ring structure similar to NMP solvent, an efficient graphene exfoliant. Stable aqueous dispersions of the hydrophilic polymer coated graphene monolayers were obtained in 10 - 20 % yield, as confirmed by the AFM, TEM and Raman spectroscopy. The colloidal stability of the exfoliated graphene layers in water was suggested to be conferred by steric or/and depletion stabilization by the non-ionic yet largely hydrophilic polymer. Tagmatarchis and c-workers applied another trick to switch the solubilty of graphene from organic to water phase . They exfoliated graphene sheets in organic solvents such as NMP and o-DCB. Subsequent treatment of the exfoliated sheets with an acidic solution of poly[styrene-b-(2-vinylpyridine)] (PS-b-P2VP) (Fig. 9(c)) or poly(isoprene-b-acrylic acid) (Fig. 9(d)) (PI-b-PAA) block copolymers switched the dispersability into aqueous solutions.
Efficient exfoliation of graphene in a non-traditional solvent, ethanol was achieved by Hersam and Liang, by the addition of ethyl cellulose (Fig. 9(b)) as a stabilizing polymer . The post sedimentation graphene concentration in ethanol was found to increase from 1.6 to 122.2 μg/mL after 3 h sonication in the presence of ethyl cellulose. In an attempt to increase the dispersibility even further, the authors also developed an iterative solvent exchange using terpineol, ultimately yielding stable graphene inks to a level exceeding 1 mg/mL. Highly aligned graphene-polymer composites solution-cast from these inks demonstrated outstanding processability, and transparent conductive graphene thin films were also successfully prepared. In a rigorous study, Guardia et al. compared a wide range of ionic and non-ionic surfactants including polymers . Their findings signalled that non-ionic surfactants especially polymers outperformed the ionic counterparts for the high yield production of defect-free graphene. (Fig. 9(f)) The highest concentration of ~1 mg/mL was achieved by sonicating graphite with a triblock copolymer, Pluronic®P-123 (0.5 % w/v) for just 2 hrs and extending sonication time to 5 hrs afforded 1.5 mg/mL dispersions (Fig. 9(g)). AFM images of the graphene samples on SiO2/Si showed an average flake thickness of 1.0 - 3.0 nm. Defect-free basal planes of the vacuum filtrated graphene films were revealed by STM imaging and these films exhibited high conductivities (1160 S/m) as well. Notley, in a similar study, compared pluronic non-ionic surfactants, F108 (molecular weight ~ 14.6 kDa) and F127 (molecular weight ~ 12.5 kDa) with some ionic surfactants such as CTAB (hexadecyltrimethylammonium bromide), TTAB (tetradecyltrimethylammonium bromide), DTAB (dodecyltrimethylammonium bromide) and SDS (sodium dodecylsulfate,) . Interestingly, there was a key difference in the exfoliation procedure adopted by Notley compared to other procedures. A continuous surfactant addition method was employed during the sonication rather than adding all the surfactant at once before sonication. The idea was to continually maintain optimum surface tension of the surfactant/graphene solution by replacing the depleted surfactant that goes adsorbed on to graphene surface, throughout the sonication period. Graphene suspensions with very high concentrations of up to 1.5 % w/w (15 mg/mL) were achieved by the continuous addition of a highly concentrated aqueous solution of Pluronic F108 to graphite/water mixtures.
Highly conductive and transparent graphene films were fabricated by Jo et al. from direct exfoliation of graphite using a non-ionic semiconducting polymer quinquethiophene-terminated PEG (5TN-PEG) (Fig. 10(g)) as a surfactant in ethanol solution . Washing off the excess surfactants by THF from the vacuum filtered films, followed by chemical treatment with nitric acid and thionyl chloride, resulted in a very low sheet resistance of 0.3 kΩ/□ with 74 % transmittance at 550 nm. This is one of the lowest values of sheet resistance among graphene films prepared by top-down fabrication.
It is now well-recognized that one critical bottleneck standing in front of commercial utilization of graphene is the lack of a reliable mass production method for high quality graphene. In this context, LPE has long been considered as one of the most promising and versatile approach. In this review article, we highlighted the recent research progress in the production of high quality graphene by LPE, with a particular emphasis on the versatile role of different categories of surfactants.
LPE of graphene was initially developed with specific surface energy matching solvents (without surfactant). Relevant crucial processing factors such as solvents, external forces like ultrasonication/shear and purification methods by centrifugation have been discussed in detail in association with their influences on the exfoliation results. Significantly, most of the solvents used in the initial studies had revealed significant drawbacks, such high toxicity, high boiling point etc. that prompted the re-direction of research into environment benign less toxic solvents like water. Unfortunately, the surface energy of pure water is too high for graphene exfoliation such that a variety of surfactants have been introduced thus far. We categorized the large spectrum of surfactants in accordance to their structural functionalities into aromatic, non-aromatic, ionic liquids and polymers. Innumerable surfactants have been studied in this regard and many of them appeared highly promising LPE results.
For the further progress of surfactant assisted LPE, several shortcomings must be overcome: (1) The overall yield of LPE is still low; (2) Good exfoliating solvents are expensive and harmful; (3) Sonication/Shearing commonly lead to the drastic reduction in the size of exfoliated graphene sheets; (4) Residual surfactants are difficult to remove; (5) Typical surfactants are electrically insulators, which may significantly deteriorate the electrical connectivity among graphene layers; (6) All LPE methods produce graphene sheet with a high polydispersity in terms of lateral size as well as thickness. The future of real-life graphene applications strongly depends on how materials scientists address these formidable challenges and establish ideal large-scale LPE process for high quality graphene sheets. It is also highly required to attain more fundamental and systematic understanding of the exfoliation mechanism for innovative design of LPE schemes.
This work was financially supported by Institute for Basic Science (IBS) [CA1301-02] and the Asian Office of Aerospace Research and Development (AOARD FA2384-14-1-4013).
- KS Novoselov, AK Geim, SV Morozov, et al. Science 306, 66–669 (2004).Google Scholar
- E Fitzer, KH Kochling, HP Boehm, H Marsh, Pure Appl Chem 67, 473–475 (1995)View ArticleGoogle Scholar
- C Lee, X Wei, JW Kysar, J Hone, Science 321, 385–388 (2008)View ArticleGoogle Scholar
- AA Balandin, S Ghosh, W Bao, Nano Lett 8, 902–907 (2008)View ArticleGoogle Scholar
- A Peigney, C Laurent, E Flahaut, RR Bacsa, A Rousset, Carbon 41, 507–514 (2001)View ArticleGoogle Scholar
- M Orlita, C Faugeras, P Plochocka et al., Physical Review Lett 101, 267601 (2008)View ArticleGoogle Scholar
- FN Xia, T Mueller, YM Lin, A Valdes-Garcia, P Avouris, Nat Nanotechnol 4, 839–843 (2009)View ArticleGoogle Scholar
- T Mueller, FNA Xia, PA Vouris, Nat Photonics 4, 297–301 (2010)View ArticleGoogle Scholar
- G Konstantatos, M Badioli, L Gaudreau, J Osmond, M Bernechea, FPG De Arquer, F Gatti, FHL Koppens, Nat Nanotechnol 7, 363–368 (2012)View ArticleGoogle Scholar
- KS Novoselov, VI Fal’ko, L Colombo, PR Gellert, MG Schwab, K Kim, Nature 490, 192–200 (2012)View ArticleGoogle Scholar
- KS Kim, Y Zhao, H Jang, SY Lee, JM Kim, JH Ahn, P Kim, JY Choi, BH Hong, Nature 457, 706–712 (2009)View ArticleGoogle Scholar
- Y Huang, J Liang, Y Chen, Small 8, 1805–1808 (2012)View ArticleGoogle Scholar
- D Chen, H Feng, J Li, Chem Rev 112, 6027–6053 (2012)View ArticleGoogle Scholar
- C Chung, YK Kim, D Shin, SR Ryoo, BH Hong, DH Min, Acc Chem Res 46, 2211–2224 (2013)View ArticleGoogle Scholar
- X Sun, H Sun, H Li, H Peng, Adv Mater 25, 5153–5176 (2013)View ArticleGoogle Scholar
- D Li, MB Müller, S Gilje, RB Kaner, GG Wallace, Nat Nanotech 3, 101–105 (2008)View ArticleGoogle Scholar
- K Parvez, R Li, SR Punireddy, Y Hernandez, F Hinkel, S Wang, X Feng, K Mullen, ACS Nano 7, 3598–3606 (2013)View ArticleGoogle Scholar
- JN Coleman Adv. Funct.Mater. 19, 3680–3695(2009)Google Scholar
- Y Hernandez, V Nicolosi, M Lotya, FM Blighe, Z Sun, S De, IT McGovern, B Holland, M Byrne, YK Gunko, JJ Boland, P Niraj, G Duesberg, S Krishnamurthy, R Goodhue, J Hutchison, V Scardaci, AC Ferrari, JN Coleman, Nat Nanotechnol 3, 563–568 (2008)View ArticleGoogle Scholar
- P Blake, PD Brimicombe, RR Nair, TJ Booth, D Jiang, F Schedin, LA Ponomarenko, SV Morozov, HF Gleeson, EW Hill, AK Geim, KS Novoselov, Nano Lett 8, 1704–1708 (2008)View ArticleGoogle Scholar
- CE Hamilton, JR Lomeda, Z Sun, JM Tour, AR Barron, Nano Lett 9, 3460–3462 (2009)View ArticleGoogle Scholar
- AB Bourlinos, V Georgakilas, R Zboril, TA Steriotis, AK Stubos, Small 5, 1841–1845 (2009)View ArticleGoogle Scholar
- SP Economopoulos, G Rotas, Y Miyata, H Shinohara, N Tagmatarchis, ACS Nano 4, 7499–7507 (2010)View ArticleGoogle Scholar
- Z Sun, X Huang, F Liu, X Yang, C Roesler, RA Fischer, M Muhler, W Schuhmann, Chem Commun 50, 10382 (2014)View ArticleGoogle Scholar
- N Behabtu, J Lomeda, M Green, A Higginbotham, A Sinitskii, D Kosynkin, D Tsentalovich, A Parra-Vasquez, J Schmidt, E Kesselman, Y Cohen, Y Talmon, J Tour, M Pasquali, Nat Nanotechnol 5, 406–411 (2010)View ArticleGoogle Scholar
- X Wang, LJ Zhi, K Mullen, Nano Lett 8, 323–327 (2008)View ArticleGoogle Scholar
- CA Di, DC Wei, G Yu, YQ Liu, YL Guo, DB Zhu, Adv Mater 20, 3289–3293 (2008)View ArticleGoogle Scholar
- Y Cao, ZM Wei, S Liu, L Gan, XF Guo, W Xu, ML Steigerwald, ZF Liu, DB Zhu, Angew. Chem Int Ed 49, 6319–6323 (2010)View ArticleGoogle Scholar
- XY Zhang, AC Coleman, N Katsonis, WR Browne, BJ vanWees, BL Feringa, Chem Commun 46, 7539–7541 (2010)View ArticleGoogle Scholar
- A Catheline, L Ortolani, V Morandi, M Melle-Franco, C Drummond, C Zakria, A Penicaud, Soft Matter 8, 7882–7887 (2012)View ArticleGoogle Scholar
- W Qian, R Hao, YL Hou, Y Tian, CM Shen, HJ Ga, XL Liang, Nano Res 2, 706–712 (2009)View ArticleGoogle Scholar
- K Chatakondu, MLH Green, ME Thompson, KS Suslick, J. Chem. Soc. Chem Commun 3, 900–901 (1987)View ArticleGoogle Scholar
- L Spanu, S Sorella, G Galli, Phys Rev Lett 103, 196401–196404 (2009)View ArticleGoogle Scholar
- U Khan, A O’Neill, M Lotya, S De, JN Coleman, Small 6, 864–871 (2010)View ArticleGoogle Scholar
- U Khan, P May, A O’Neill, JN Coleman, Carbon 48, 4035–4041 (2010)View ArticleGoogle Scholar
- KR Paton et al., Nature Mater. 13, 624–630 (2014)Google Scholar
- U Khan, A O’Neill, H Porwal, P May, K Nawaz, JN Coleman, Carbon 50, 470–475 (2012)View ArticleGoogle Scholar
- AA Green, MC Hersam, Nano Lett 9, 4031–4036 (2009)View ArticleGoogle Scholar
- AA Green, MC Hersam, Mater Today 10, 59–60 (2007)View ArticleGoogle Scholar
- M Lotya, Y Hernandez, PJ King, RJ Smith, V Nicolosi, LS Karlsson, FM Blighe, S De, Z Wang, IT McGovern, J Am Chem Soc 131, 3611–3620 (2009)View ArticleGoogle Scholar
- R Hao, W Qian, L Zhang, Y Hou, Chem Commun 6, 6576–6578 (2008)View ArticleGoogle Scholar
- A Ghosh, KV Rao, SJ George, CNR Rao, Chem Eur J 16, 2700–2704 (2010)View ArticleGoogle Scholar
- GS Bang, HM So, MJ Lee, CW Ahn, J Mater Chem 22, 4806–4810 (2012)View ArticleGoogle Scholar
- I-WP Chen, C-Y Huang, S-HS Jhou, Y-W Zhang, Sci Rep 4, 3928 (2014)Google Scholar
- S Sampath, AN Basuray, KJ Hartlie, T Aytun, SI Stupp, JF Stoddart, Adv Mater 25, 2740–2745 (2013)View ArticleGoogle Scholar
- XC Dong, YM Shi, Y Zhao, DM Chen, J Ye, YG Yao, F Gao, ZH Ni, T Yu, ZX Shen, YX Huang, P Chen, LJ Li, Phys Rev Lett 102, 135501 (2009)View ArticleGoogle Scholar
- M Zhang, RR Parajuli, D Mastrogiovanni, B Dai, P Lo, W Cheung, R Brukh, PL Chiu, T Zhou, Z Liu, E Garfunkel, H He, Small 6, 1100–1107 (2010)View ArticleGoogle Scholar
- KS Kim, Y Zhao, H Jang, SY Lee, JM Kim, JH Ahn, P Kim, JY Choi, BH Hong, Nature 457, 706–710 (2009)View ArticleGoogle Scholar
- X An, T Simmons, R Shah, C Wolfe, KM Lewis, M Washington, SK Nayak, S Talapatra, S Kar, Nano Lett 10, 4295–4301 (2010)View ArticleGoogle Scholar
- J-H Jang, D Rangappa, Y-U Kwonc, I Honma, J Mater Chem 21, 3462–3466 (2011)View ArticleGoogle Scholar
- D Parviz, S Das, HST Ahmed, F Irin, S Bhattacharia, MJ Green, ACS Nano 6, 8857–8867 (2012)View ArticleGoogle Scholar
- A Schlierf, H Yang, E Gebremedhn, E Treossi, L Ortolani, L Chen, A Minoia, V Morandi, P Samorı, C Casiraghi, D Beljonne, V Palermo, Nanoscale 5, 4205–4216 (2013)View ArticleGoogle Scholar
- H Yang, Y Hernandez, A Schlierf, A Felten, A Eckmann, S Johal, P Louette, J-J Pireaux, X Feng, K Muellen, V Palermo, C Casiraghi, Carbon 53, 357–365 (2013)View ArticleGoogle Scholar
- JM Englert, J Rehrl, CD Schmidt, R Graupner, M Hundhausen, F Hauke, A Hirsch, Adv Mater 21, 4265–4269 (2009)View ArticleGoogle Scholar
- J Geng, BS Kong, SB Yanga, HT Jung, Chem Commun 46, 5091–5093 (2010)View ArticleGoogle Scholar
- RD Costa, J Malig, W Brenner, N Jux, DM Guldi, Adv Mater 25, 2600–2605 (2013)View ArticleGoogle Scholar
- J Malig, N Jux, D Kiessling, JJ Cid, P V’azquez, T Torres, DM Guldi, Angew Chem Int Ed 50, 3561–3565 (2011)View ArticleGoogle Scholar
- J Malig, AW Stephenson, P Wagner, GG Wallace, DL Officer, DM Guldi, Chem Commun 48, 8745–8747 (2012)View ArticleGoogle Scholar
- D Kiessling, RD Costa, G Katsukis, J Malig, F Lodermeyer, S Feihl, A Roth, L Wibmer, M Kehrer, M Volland, P Wagner, GG Wallace, DL Officer, DM Guldi. Chem Sci 4, 3085–3098 (2013)View ArticleGoogle Scholar
- A Roth, ME Ragoussi, L Wibmer, G Katsukis, G Torre, T Torres, DM Guldi, Chem Sci 5, 3432–3438 (2014)View ArticleGoogle Scholar
- R Kabe, X Feng, C Adachi, K Mullen, Chem Asian J 9, 3125–3129 (2014)View ArticleGoogle Scholar
- S Bose, T Kuila, AK Mishra, NH Kim, JH Lee, Nanotech. 22, (405603) 1–7 (2011)Google Scholar
- DW Lee, T Kim, M Lee, Chem Commun 47, 8259–8261 (2011)View ArticleGoogle Scholar
- S Vadukumpully, J Paul, S Valiyaveettil, Carbon 47, 3288–3294 (2009)View ArticleGoogle Scholar
- (a) S De, PJ King, M Lotya, A O’Neill, EM Doherty, Y Hernandez, GS Duesberg, JN Coleman, Small 6, 458–464 (2010). (b) M Lotya, PJ King, U Khan, S De, JN Coleman, ACS Nano 4, 3155–3162 (2010).Google Scholar
- RJ Smith, M Lotya, JN Coleman, New J Phys 12, 125008–125018 (2010)View ArticleGoogle Scholar
- A Ciesielski, S Haar, ME Gemayel, H Yang, J Clough, G Melinte, M Gobbi, E Orgiu, MV Nardi, G Ligorio, V Palermo, N Koch, O Ersen, C Casiraghi, P Samor, Angew Chem Int Ed 53, 10355–10361 (2014)View ArticleGoogle Scholar
- V Chabot, B Kim, B Sloper, C Tzoganakis, A Yu, Sci Rep 3, 1378 (2013)View ArticleGoogle Scholar
- D Nuvoli, V Alzari, R Sanna, S Scognamillo, M Piccinini, L Peponi, JM Kenny, A Mariani, Nanoscale Res Lett 7, 674 (2012)View ArticleGoogle Scholar
- PM Carrasco, S Montes, I Garcia, M Borghei, H Jiang, I Odriozola, G Cabanero, V Ruiz, Carbon 70, 157–163 (2014)View ArticleGoogle Scholar
- T Welton, Chem Rev 99, 2071–2084 (1999)View ArticleGoogle Scholar
- W Zheng, A Mohammed, LG Hines Jr, D Xiao, OJ Martinez, RA Bartsch, SL Simon, O Russina, A Triolo, EL Quitevis, J Phys Chem B 115, 6572–6584 (2011)View ArticleGoogle Scholar
- XQ Wang, PF Fulvio, GA Baker, GM Veith, RR Unocic, SM Mahurin, MF Chi, S Dai, Chem Commun 46, 4487–4489 (2010)View ArticleGoogle Scholar
- D Nuvoli, L Valentini, V Alzari, S Scognamillo, SB Bon, M Piccinini, J Illescas, A Mariani, J Mater Chem 21, 3428–3431 (2011)View ArticleGoogle Scholar
- D Ager, VA Vasantha, R Crombez, J Texter, ACS Nano 8, 11191–11205 (2014)View ArticleGoogle Scholar
- E-Y Choi, TH Han, J Hong, JE Kim, SH Lee, HW Kim, SO Kim, J Mater Chem 20, 1907–1912 (2010)View ArticleGoogle Scholar
- SH Lee, DR Dreyer, J An, A Velamakanni, RD Piner, S Park, Y Zhu, SO Kim, CW Bielawski, RS Ruoff, Macromol Rapid Commun 31, 281–288 (2010)View ArticleGoogle Scholar
- AS Patole, SP Patole, H Kang, J-B Yoo, T-H Kim, J-H Ahn, J Coll Inter Sci 350, 530–537 (2010)View ArticleGoogle Scholar
- YT Liu, XM Xie, XY Ye, Carbon 49, 3529–3537 (2011)View ArticleGoogle Scholar
- M Cardinali, L Valentini, JM Kennya, I Mutlay, Polym Int 61, 1079–1083 (2012)View ArticleGoogle Scholar
- H Wu, B Rook, LT Drzal, Polym Composites 34, 426–432 (2013)View ArticleGoogle Scholar
- X Li, Y Xiao, A Bergeret, M Longerey, J Chen, Polym Composites 35, 396–403 (2014)View ArticleGoogle Scholar
- MA Milani, D González, R Quijada, NRS Basso, ML Cerradad, DS Azambuja, GB Galland, Compos Sci Technol 84, 1–7 (2013)View ArticleGoogle Scholar
- P May, U Khan, JM Hughes, JN Coleman, J Phys Chem C 116, 11393–11400 (2012)View ArticleGoogle Scholar
- ZB Ye, SY Li, Macromol React Eng 4, 319–332 (2010)View ArticleGoogle Scholar
- AB Bourlinos, V Georgakilas, R Zboril, TA Steriotis, AK Stubos, C Trapalis, Solid State Commun 149, 2172–2176 (2009)View ArticleGoogle Scholar
- T Skaltsas, N Karousis, H-J Yan, C-R Wang, S Pispas, N Tagmatarchis, J Mater Chem 22, 21507–21512 (2012)View ArticleGoogle Scholar
- YT Liang, MC Hersam, J Am, Chem Soc 132, 17661–17663 (2010)View ArticleGoogle Scholar
- L Guardia, MJ Fernandez-Merino, JI Paredes, PS Fernandez, S Villar-Rodil, A Martinez-Alonso, JMD Tascon, Carbon 49, 1653–1662 (2011)View ArticleGoogle Scholar
- SM Notley, Langmuir 28, 14110 − 14113 (2012)Google Scholar
- X Zheng, Q Xu, J Li, L Lia, J Wei, RSC Adv 2, 10632–10638 (2012)Google Scholar
- Z Liu, J Liu, L Cui, R Wang, X Luo, CJ Barrow, W Yang, Carbon 51, 148–155 (2013)View ArticleGoogle Scholar
- F Liu, JY Choi, TS Seo, Chem Commun 46, 2844–2846 (2010)View ArticleGoogle Scholar
- MS Kang, KT Kim, JU Lee, WH Jo, J Mater, Chem C 1, 1870–1875 (2013)Google Scholar
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