Liquid Exfoliation of Layered Materials

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Science  21 Jun 2013:
Vol. 340, Issue 6139, 1226419
DOI: 10.1126/science.1226419

Structured Abstract


Since at least 400 C.E., when the Mayans first used layered clays to make dyes, people have been harnessing the properties of layered materials. This gradually developed into scientific research, leading to the elucidation of the laminar structure of layered materials, detailed understanding of their properties, and eventually experiments to exfoliate or delaminate them into individual, atomically thin nanosheets. This culminated in the discovery of graphene, resulting in a new explosion of interest in two-dimensional materials.

Layered materials consist of two-dimensional platelets weakly stacked to form three-dimensional structures. The archetypal example is graphite, which consists of stacked graphene monolayers. However, there are many others: from MoS2 and layered clays to more exotic examples such as MoO3, GaTe, and Bi2Se3. These materials display a wide range of electronic, optical, mechanical, and electrochemical properties. Over the past decade, a number of methods have been developed to exfoliate layered materials in order to produce monolayer nanosheets. Such exfoliation creates extremely high-aspect-ratio nanosheets with enormous surface area, which are ideal for applications that require surface activity. More importantly, however, the two-dimensional confinement of electrons upon exfoliation leads to unprecedented optical and electrical properties.

Embedded Image

Liquid exfoliation of layered crystals allows the production of suspensions of two-dimensional nanosheets, which can be formed into a range of structures. (A) MoS2 powder. (B) WS2 dispersed in surfactant solution. (C) An exfoliated MoS2 nanosheet. (D) A hybrid material consisting of WS2 nanosheets embedded in a network of carbon nanotubes.


An important advance has been the discovery that layered crystals can be exfoliated in liquids. There are a number of methods to do this that involve oxidation, ion intercalation/exchange, or surface passivation by solvents. However, all result in liquid dispersions containing large quantities of nanosheets. This brings considerable advantages: Liquid exfoliation allows the formation of thin films and composites, is potentially scaleable, and may facilitate processing by using standard technologies such as reel-to-reel manufacturing.

Although much work has focused on liquid exfoliation of graphene, such processes have also been demonstrated for a host of other materials, including MoS2 and related structures, layered oxides, and clays. The resultant liquid dispersions have been formed into films, hybrids, and composites for a range of applications.


There is little doubt that the main advances are in the future. Multifunctional composites based on metal and polymer matrices will be developed that will result in enhanced mechanical, electrical, and barrier properties. Applications in energy generation and storage will abound, with layered materials appearing as electrodes or active elements in devices such as displays, solar cells, and batteries. Particularly important will be the use of MoS2 for water splitting and metal oxides as hydrogen evolution catalysts. In addition, two-dimensional materials will find important roles in printed electronics as dielectrics, optoelectronic devices, and transistors.

To achieve this, much needs to be done. Production rates need to be increased dramatically, the degree of exfoliation improved, and methods to control nanosheet properties developed. The range of layered materials that can be exfoliated must be expanded, even as methods for chemical modification must be developed. Success in these areas will lead to a family of materials that will dominate nanomaterials science in the 21st century.

Furthering Exfoliation

In addition to graphene, a wide range of layered materials, including oxides, chalcogenides, and clays are of interest because of their optical, electrical, and mechanical properties. While many methods can be used to cleave layered sheets from the bulk material, they are difficult to scale up. Liquid exfoliation routes may hold the best promise for making materials in large quantities. Nicolosi et al. (p. 1226419) review progress in developing exfoliation routes, both aqueous and nonaqueous for a wide range of starting materials.


Not all crystals form atomic bonds in three dimensions. Layered crystals, for instance, are those that form strong chemical bonds in-plane but display weak out-of-plane bonding. This allows them to be exfoliated into so-called nanosheets, which can be micrometers wide but less than a nanometer thick. Such exfoliation leads to materials with extraordinary values of crystal surface area, in excess of 1000 square meters per gram. This can result in dramatically enhanced surface activity, leading to important applications, such as electrodes in supercapacitors or batteries. Another result of exfoliation is quantum confinement of electrons in two dimensions, transforming the electron band structure to yield new types of electronic and magnetic materials. Exfoliated materials also have a range of applications in composites as molecularly thin barriers or as reinforcing or conductive fillers. Here, we review exfoliation—especially in the liquid phase—as a transformative process in material science, yielding new and exotic materials, which are radically different from their bulk, layered counterparts.

In 1824, Thomas H. Webb heated a mineral similar to mica and, by means of thermal exfoliation, transformed it into what is today a valuable commodity, with applications as an ion exchange resin, an insulating material, and a structural binder in cement. He named the mineral “vermiculite” for its wormlike appearance upon exfoliation (Fig. 1), from the Latin vermiculare meaning “to breed worms.” Almost 200 years later, in 2004, Geim and Novosolov showed that thin transparent adhesive tape could be used to exfoliate graphite into single atomic layers of graphene and demonstrated atomically thin devices (1). As a process, exfoliation of layered solids has had a transformative effect on materials science and technology by opening up properties found in the two-dimensional (2D) exfoliated forms, not necessarily seen in their bulk counterparts.

Fig. 1 Crystal structures, naturally occurring forms, and exfoliated products for four example layered materials.

(A) Graphite consists of alternating stacks of hexagonally arranged carbon atoms (black spheres), (B) is a naturally occurring mineral, and (C) exfoliates to single atomic layers of carbon called graphene. (D) Vermiculite is a layered silicate hydrate (typically Mg1.8Fe0.9Al4.3SiO10(OH)2•4(H2O) that (E) is found naturally as a mineral and (F) can be exfoliated,for example, upon heating. Silicon atoms are in blue, oxygen atoms are in red, Al/Mg/Fe atoms are in yellow, and interlayer counterions are in black (H and H2O not shown). (G) MoS2 is a layered arrangement of S and Mo atoms (chalcogen atoms are in yellow, and transition metal are in green) that (H) is found naturally as the mineral molybdenite and (I) can be exfoliated to MoS2 monolayers. (J) Layered manganese dioxide (manganese atoms are in yellow, oxygen is in red, and interlayer counterions are in black) occurs naturally (K) as birnessite and (L) can be exfoliated to give MnO2 nanosheets. (C), (I), and (L) are adapted from (48), (87), and (58), respectively. The layer spacings for each material are graphite, 0.35 nm; vermiculite, 1.5 nm; MoS2, 0.6 nm; and MnO2, 0.45 nm.

Layered materials are defined as solids with strong in-plane chemical bonds but weak out-of-plane, van der Waals bonds. Such materials can be sheared parallel or expanded normal to the in-plane direction. In the extreme limit, these processes yield nanometer-thin—even atomically thin—sheets that are not at all characteristic of the bulk precursor. This production of extremely thin sheets from layered precursors is known as exfoliation or delamination, although in this work we will use the former term. The sheets produced are generally referred to as nanosheets, where “nano” refers to the magnitude of the thickness. Although in the ideal case such nanosheets consist of single monolayers, they are often manifested as incompletely exfoliated flakes comprising a small number (<10) of stacked monolayers.

There are many types of layered materials, which can be grouped into diverse families (Fig. 1). The simplest are the atomically thin, hexagonal sheets of graphene (13) and hexagonal boron nitride (h-BN) (4). Transition metal dichalcogenides (TMDs) (such as MoS2 and WSe2) (5, 6) and metal halides (such as PbI2 and MgBr2) (7) have near-identical structures and consist of a plane of metal atoms sandwiched between planes of halide/chalcogen atoms. Layered metal oxides (such as MnO2, MoO3, and LaNb2O7) (811) and layered double hydroxides (LDHs) [such as Mg6Al2(OH)16] (8, 12) represent a diverse class of materials with a large variety of structures. Similarly, layered silicates, or clays, are minerals and exist as many different types, with well-known examples being montmorillonite or the micas (13, 14). Generally, oxides, LDH, and clay nanosheets are charged and are accompanied by charge-balancing ions (8, 14). Other interesting families are the layered III-VIs (such as InSe and GaS) (15), the layered V-VIs (such as Bi2Te3 and Sb2Se3) (16), the metal trichalcogenides, and metal trihalides. Although many other layered materials exist (Table 1), all share a planar, anisotropic bonding and therefore the potential to be exfoliated into nanosheets.

Table 1 Referenced table of families of layered compounds, including structures and information on exfoliation methods, potential applications, and availability.

This table is not exhaustive. Crystal structures were obtained from the CrystalMaker Library (

View this table:

One substantial advantage of layered materials is their diversity. Even before exfoliation, the many families of layered materials display a very broad spectrum of properties. For example, TMDs (5, 6) occur as more than 40 different types depending on the combination of chalcogen (S, Se, or Te) and transition metal (5, 6). Depending on the coordination and oxidation state of the metal atoms, or doping of the lattice, TMDs can be metallic, semimetallic, or semiconducting (6). In addition, these materials display interesting electronic behavior, such as superconductivity or charge-density wave effects (6). Similarly, the many different types of layered metal oxides have interesting electronic, electrochemical, and photonic properties (8). These materials have been fabricated into transistors, battery electrodes, and magneto-optic devices (810). Thus, even as bulk crystals, layered materials are an interesting and potentially useful material class. This makes them an exciting starting material for exfoliation into nanosheets. As we will see below, exfoliation dramatically enhances the range of properties displayed by an already diverse material type.

Why Exfoliate?

The simplest effect of exfoliation is to dramatically increase the accessible surface area of a material. For surface-active or catalytic materials, this can radically enhance their chemical and physical reactivity. The ion exchange ability of minerals such as vermiculite to purify water at 1000 meq/kg depends on its near 106-fold increase in surface area after expansion (13). In structural mechanics, the strength and stiffness of composites increase as the thickness of planar fillers, such as clay or graphite, decreases (17). When heat causes exfoliation, a layered material can be used as an intumescent (or thermally expansive) material. Hence, vermiculite and graphite are used for fire retardation in paints and firestop pillows because they reduce their density upon heating and produce an ash of low thermal conductivity.

As interest in nanotechnology has intensified in recent decades, another important advantage of exfoliation has emerged. In a layered crystal, the electronic wave function extends in three dimensions. However, after exfoliation electrons are constrained to adopt a 2D wave function, thus modifying the electronic band structure. Graphite can be transformed into a graphene monolayer after exfoliation, with electronic properties that differ greatly from any other material (1). These include an enormously high carrier mobility and other exciting properties, such as Klein tunnelling and the half-integer quantum Hall effect (1, 3). Likewise, the properties of MoS2 depend strongly on exfoliation state. The bandgap of MoS2 changes on exfoliation from 1.3 eV for the bulk crystal to 1.9 eV for an exfoliated nanosheet. Because the bandgap changes monotonically with number of monolayers per nanosheet, this allows the electronic response to be chosen at will (18). In addition, although multilayer MoS2 is not photoluminescent, exfoliation-induced changes in its electronic structure lead to photoluminescent behavior in exfoliated monolayers (19). Similar behavior is expected in other layered semiconductors (5).

Large-Scale Exfoliation in Liquids?

The exfoliation of graphite demonstrated by Geim and Novolosov was achieved essentially by rubbing graphite on a surface (1). Such mechanical exfoliation remains the source of the highest-quality graphene samples available and has resulted in some major advances (1). However, it suffers from low yield and a production rate that is not technologically scalable in its current form. One possible solution is the exfoliation of layered compounds in liquids to give large quantities of dispersed nanosheets. This should allow for methods to obtain sizable quantities of 2D materials that can be processed by using existing industrial techniques, such as reel-to-reel manufacturing. Here, we briefly outline the four main liquid exfoliation techniques for layered materials (schematics are provided in Fig. 2, and examples of exfoliated nanosheets are provided in Fig. 3).

Fig. 2 Schematic description of the main liquid exfoliation mechanisms.

(A) Ion intercalation. Ions (yellow spheres) are intercalated between the layers in a liquid environment, swelling the crystal and weakening the interlayer attraction. Then, agitation (such as shear, ultrasonication, or thermal) can completely separate the layers, resulting in an exfoliated dispersion. (B) Ion exchange. Some layered compounds contain ions between the layers so as to balance surface charge on the layers. These ions (red spheres) can be exchanged in a liquid environment for other, often larger ions (yellow spheres). As above, agitation results in an exfoliated dispersion. (C) Sonication-assisted exfoliation. The layered crystal is sonicated in a solvent, resulting in exfoliation and nanosheet formation. In “good” solvents—those with appropriate surface energy—the exfoliated nanosheets are stabilized against reaggregation. Otherwise, for “bad” solvents reaggregation and sedimentation will occur. This mechanism also describes the dispersion of graphene oxide in polar solvents, such as water. NB, solvent molecules are not shown in this figure.

Fig. 3 TEM images of liquid exfoliated nanosheets.

(A) A graphene nanosheet exfoliated by means of sonication in the solvent N-methyl-pyrrolidone (27). (B) A h-BN nanosheet exfoliated by means of sonication in the solvent isopropanol (29). (C) An MoS2 nanosheet exfoliated by means of sonication in an aqueous surfactant solution (58). (D) An MoS2 nanosheet exfoliated by means of Li ion intercalation (22). (E) A TiO2 nanosheet exfoliated by means of ion exchange (25). (F) Functionalized layered double hydroxide nanosheets exfoliated by means of sonication in ethanol (65). (G) Hydroxylated metal carbide nanosheets exfoliated by means of sonication in methanol (66). Where available, high-resolution images have been included as insets. All images were adapted from the sources as referenced.

One of the oldest methods of exfoliating layered crystals with low reductive potential is oxidation and subsequent dispersion into suitable solvents. The best example is that of graphite (20), in which treatment with oxidizers such as sulphuric acid and potassium permanganate results in addition of hydroxyl and epoxide groups to the basal plane. The resulting hydrophillicity allows water intercalation and large-scale exfoliation to yield graphene oxide upon ultrasonication. The dispersed flakes are predominantly monolayers, typically hundreds of nanometers across, and stabilized against reaggregation by a negative surface charge at concentrations of up to 1 mg/ml. Dispersed graphene oxide can be chemically reduced in the liquid phase but will then aggregate unless surfactant or polymer stabilizers are present. Although reduction removes most of the oxides, structural defects remain, rendering the properties of oxidatively produced graphene substantially different from pristine graphene.

Layered materials can also strongly adsorb guest molecules into the spacing between layers, creating what are called inclusion complexes. This forms the basis of another exfoliation method that is widely applied to layered materials, including graphite (21) and TMDs (22, 23). Intercalation, often of ionic species, increases the layer spacing, weakening the interlayer adhesion and reducing the energy barrier to exfoliation. Intercalants such as n-butyllithium (22, 23) or IBr (21) can transfer charge to the layers, resulting in a further reduction of interlayer binding. Subsequent treatment such as thermal shock (21) or ultrasonication (22, 23) in a liquid completes the exfoliation process. The exfoliated nanosheets can be stabilized electrostatically by a surface charge (23) or by surfactant addition (21). In the case of MoS2, this method tends to give highly exfoliated nanosheets (22). However, ion intercalation–based methods have drawbacks associated with their sensitivity to ambient conditions (2224).

Ion exchange methods take advantage of the fact that LDHs, clays, and some metal oxides contain an exchangeable interlayer of cationic counterions (8). For example, titanium dioxide (TiO2) layered crystals tend to be negatively charged (because of the presence of both Ti3+ and Ti4+ ions) and so contain counter-ions such as Cs+ between the layers to ensure charge neutrality (8, 25). Such ions can be exchanged for protons by soaking in acidic solutions. The protons can then be exchanged for bulky organic ions (for example, tetrabutylammonium cations), leading to substantial swelling. Alternatively, some clays containing small monovalent ions such as sodium swell from intercalation of water (13). In general, swelling facilitates exfoliation through ultrasonication or shear mixing to give negatively charged nanosheets (26).

A more recent strategy for exfoliation is to expose the layered material to ultrasonic waves in a solvent (27). Such waves generate cavitation bubbles that collapse into high-energy jets, breaking up the layered crystallites and producing exfoliated nanosheets. Modeling has shown that if the surface energy of the solvent is similar to that of the layered material, the energy difference between the exfoliated and reaggregated states will be very small, removing the driving force for reaggregation (28). Graphene, h-BN, TMDs, and some TMOs have been exfoliated in this way by using solvents such as N-methyl-pyrrolidone (28, 29). Similarly, ultrasonication in surfactant or polymer solutions gives nanosheets that are electrostatically or sterically stabilized (17, 30).


The exfoliation of layered compounds is an area of research that dates back several centuries. Modern research probably began with Webb and progressed via the work of chemists such as Schafhaeutl, Brodie, and Staudenmaier on the production of graphite intercalation compounds and graphite oxide in the mid-19th century (20). Although these early researchers knew of the laminar nature of graphite, the detailed structure was not known until the 1920s (28). Early attempts to understand exfoliated layered compounds used transmission electron microscopy (TEM) to image few- and possibly even mono-layer exfoliated graphene oxide as early as 1948. However, the limitations of available instrumentation made it impossible to verify whether monolayers were really observed (20, 31). The 1960s saw a flurry of activity on the cleavage (often using adhesive tape) of TMD crystals to produce nanosheets that approached monolayer thickness (32). This was complemented in 1967 by the demonstration that inorganic layered compounds—in this case, vermiculite clay—could be exfoliated in liquids by means of ion intercalation followed by shear mixing (26). In 1975, a similar technique was used to exfoliate TaS2, possibly producing monolayers (33). Subsequently, the availability of cheap ultrasonic agitators provided a more effective energy source for exfoliation, leading to the demonstration of ion intercalation–assisted exfoliation of TaS2, NbS2, and MoS2, as well as layered oxides (23, 34, 35). In these reports, TEM and x-ray diffraction suggested that monolayers had been produced. A decade later in 2000, the exfoliation of layered double hydroxides by means of ion exchange followed by stirring or reflux was demonstrated (36).

Much of this work has historically been limited by the instrumentation available. Early TEM characterization used techniques such as intensity analysis (34) or shadowing (32), which would not meet today’s standards of proof for imaging a single layer. However, the development of scanning tunnelling microscopy (STM) and atomic force microscopy (AFM) in the 1980s and recent advances in scanning TEM have changed this entirely. By the time Geim et al. produced nanosheets through mechanical exfoliation (1), a new generation of scientific instrumentation with atomic-scale resolution had emerged in order to fully analyze exfoliated materials with unprecedented precision. The result has been a renewed surge in interest in these exotic, molecular-scale materials.

Recent Advances in Liquid Exfoliation

Although the exfoliation of layered materials has a long history, it was interest in graphene that stimulated renewed curiosity in this area. For this reason, we outline the recent developments in the liquid exfoliation of layered crystals, using Geim and Novoselov’s 2004 paper describing the properties of exfoliated graphene as a starting point.

In a series of papers beginning in 2004 (1, 3, 37, 38), Geim, Novoselov, and collaborators showed that monolayers of graphene and other 2D materials could be removed from their parent crystals by means of mechanical exfoliation and placed on substrates of choice. This was somewhat surprising because theoretical studies had suggested that 2D materials should be intrinsically unstable after exfoliation (2). This apparent contradiction was later resolved with the suggestion that the exfoliated monolayers are stabilized by the formation of ripples that effectively extend the 2D material into the third dimension (39). However, the most exciting result of exfoliation was the demonstration that graphene displayed electronic, mechanical, and thermal properties not seen in any other material. For example, in addition to the previously undiscovered electronic properties described above, monolayer graphene displays the highest strength and the highest thermal conductivity ever recorded (13). Very soon, it became clear that such a material would be required in much larger quantities than mechanical cleavage could deliver. It was immediately obvious that such scalable production might be achieved through liquid exfoliation (40).

One of the first approaches to liquid exfoliation was the oxidization of graphite. In 2006, Ruoff et al. demonstrated platelets of graphite oxide with monolayer thickness (20). Now known as graphene oxide (GO), this material is electrically insulating, although it can be rendered conducting via reduction (20). The oxidation allows one to control the amount and type of attached oxides, potentially enabling control of electrical conductivity and luminescence (41). A disadvantage of this method is that it necessarily introduces chemical groups and defects that scatter electrons, giving relatively high resistivity. Graphene oxide exfoliation has been the subject of many papers and reviews (20).

Around the time of Geim’s seminal paper, McEwan et al. produced good-quality nano-graphite by sonicating graphite in the solvent dichlorobenzene (42). However, monolayer graphene was not observed in this work. It was not until 4 years later that liquid-exfoliated monolayer graphene was produced by ultrasonicating graphite in solvents such as N-methyl pyrrolidone and di-methyl formamide (27, 43). It was found that exfoliation was only achieved by using solvents with surface tension close to 40 mJ/m2. Theoretical modeling showed that for such solvents, the solvent-graphene interaction is optimized so that the energetic cost of exfoliation was minimized (27, 44, 45). This method resulted in low-concentration dispersions of small but high-quality, defect-free graphene flakes. Recent improvements have substantially enhanced both the dispersed concentration (up to 30 mg/ml), the nanosheet size (up to 5 μm), and the range of solvents (28, 4548). This method is promising for applications in which good electrical performance is required. For example, solvent-exfoliated graphene has been used to prepare transparent electrodes for liquid crystal devices (43). Recent results on printed electronic circuits have yielded mobility values of ~100 cm2/Vs (49), which are some of the highest for any chemically exfoliated graphenes. In addition, liquid exfoliation of graphene with minimal lattice defects allows the effective reinforcement of polymers (17).

Unfortunately, the most useful solvent of all, water, has a surface tension of 72 mJ/m2 and so cannot by itself exfoliate graphene. However, if graphite is ultrasonicated in aqueous surfactant solutions, graphene can be exfoliated and stabilized against reaggregation through electrostatic effects (30, 5053). Similarly, when ultrasonicated in polymer solutions, by using both water and organic solvents, graphene can be exfoliated and stabilized through steric effects (17, 54, 55). The latter method is particularly useful as a method for producing polymer-nanosheet composites (17).

Similar methods have recently been used to exfoliate both h-BN (4, 29, 56, 57) and a range of TMDs in both solvents and surfactant or polymer solutions (29, 54, 5861). Dispersions of TMDs such as MoS2, WS2, MoSe2, MoTe2, TaSe2, and NbSe2 (58) were obtained at concentrations as high as 40 mg/ml (61). As with graphene, dispersion works for solvents or solvent blends (62) with surface energies that minimize the energetic cost of exfoliation (29). TMDs prepared with this scalable method have attracted interest as composite fillers (63) and for energy storage (64). For example, Smith et al. have demonstrated solution-processed MoS2/nanotube composite cathodes for Li ion batteries with reversible capacities of >200 mA h g−1 (58). Chemical pretreatment also facilitates exfoliation by means of sonication in solvents. For example, functionalization allows the exfoliation of LDHs in alcohols (65). Similarly, acid treatment of metal aluminum carbides/nitrides produces the MXenes—metal carbide nanosheets with fluorinated or hydroxylated surfaces—that can be exfoliated in methanol (66, 67).

A number of advances have been made in the exfoliation of layered materials via ion intercalation. Strano et al. have demonstrated that dispersions of predominately bi- and tri-layer graphene can be produced from graphite intercalation compounds by thermal expansion followed by sonication in surfactant solution (21). Eda et al. have used ion intercalation to exfoliate MoS2 (22), obtaining photoluminescent monolayers. Recently, Zeng et al. demonstrated electrochemical Li insertion followed by exfoliation for MoS2, WS2, TiS2, TaS2, ZrS2, and graphite (68). The resultant nanosheets were fabricated into transistors and sensors. Recently, Xiao et al. (63) reported using exfoliated MoS2 to prepare MoS2/polyethylene oxide nanocomposites as battery electrodes with greatly improved lithiation capacity and cycling behavior. Du et al. (69) prepared MoS2 anode electrodes by means of an exfoliation and restacking process, improving stability and achieving capacities as high as 800 mA h g−1. Additionally, exfoliation by means of ion intercalation has been demonstrated for V-VI layered compounds such as Bi2Te3 and Bi2Se3 (70).

Of particular interest are layered metal oxides owing to their interesting electronic and dielectric properties (9, 10). Because of these properties, their exfoliation has been studied since at least 1990 (35) and mainly involves ion exchange followed by agitation (9). Exfoliated oxide nanosheets are most often wide-bandgap semiconductors, making them promising for applications such as photocatalysts or high-dielectric constant materials (8, 10). Alternatively, exfoliated MnO2 and RuO2 nanosheets are either redox-active or semimetallic (8, 10) and have demonstrated high performance as electrochemical supercapacitors and battery materials (8, 10). Furthermore, the availability of 2D semiconducting nanosheets opens up possibilities for designing more complex nanodevices, such as photoconducting cells, p-n junctions, and field-effect transistors (FETs) (8, 9). Colloidal dispersions of exfoliated Cs4W11O362– nanosheets are photochromic and superior to commonly used materials such as WO3 (8). MnO2 has also been exfoliated by means of ultrasonication in aqueous surfactant solutions (58), suggesting that this facile route can be applied to other layered oxides.

Intercalated layered double hydroxides were first successfully delaminated by Adachi-Pagano et al. by exchanging the interlayer anions with dodecylsulfate under reflux in butanol (71). Recent studies have focused on exfoliating such ion-exchanged materials in solvents such as fomamide (71) and water (72). High-concentration (~40 g/L) dispersions of mono- and few-layer LDHs were reported by Wu et al. (73). Liquid exfoliated LDHs have found applications in areas as diverse as drug delivery and water treatment (8).

Although liquid exfoliation of clay minerals such as montmorillonite or vermiculites is reasonably well known, recent work has focused on dispersing clay nanosheets in hydrophobic polymers for composite applications. This has been achieved by exchanging the charge-balancing ions with organocations so as to form organoclays (74).

It has recently been shown that other layered chalcogenides such as metal phosphorous trichalcogenides (CdPS3 and MnPS3, for example) can also be exfoliated into single layers by means of ion exchange (75). Details of exfoliation strategies for a wide range of layered materials are given in Table 1.

Potential Applications of Liquid-Exfoliated Nanosheets

Liquid exfoliation represents a versatile, scalable, and sustainable route for production of 2D nanosheets. In addition, access to suspensions of nanosheets permits processing in ways that would otherwise be difficult or impossible. For example, processing from liquids allows the deposition of individual nanosheets on surfaces and the formation of thin or free-standing films; facilitates mixing with other nanomaterials to form heterostructured solids; and enables insertion, as fillers, into polymer matrices (Fig. 4).

Fig. 4 Once layered materials have been exfoliated in liquids, they can be easily processed into a range of structures.

(A) TiO2 nanosheets deposited onto a substrate and imaged by means of AFM (10). (B) Solution-processed, free-standing films of randomly arranged nanosheets of h-BN, MoS2, and WS2 (29). Scale bar, 25 mm. (C) A composite film of WS2 nanosheets in a matrix of randomly arranged carbon nanotubes (29). (D) Solvent-exfoliated graphene nanosheets (arrows) embedded in a polymer matrix (17). All images were adapted from the sources as referenced.

The ability to invoke different phases of 2D materials via tuning the exfoliation chemistry opens up an exciting range of possibilities. For example, exfoliation via electrochemical ion intercalation leads to realization of the metallic (1T) phase in layered transition metal chalcogenides, which cannot be accessed through other synthesis techniques (76). Some applications include electrodes for energy-storage devices, high-performance fillers for polymer-based composites, electro- and photocatalysis for hydrogen evolution, nano- and large-area electronics and opto-electronics, and low-friction additives in lubrication systems.

The production of inexpensive 2D nanosheets holds promise for multifunctional polymer composites. Polymer-clay composites can display improved mechanical and barrier properties, usually at loading levels from a few percent to a few tens of percent (77). Because of the potentially high aspect ratio of exfoliated graphene, polymers loaded with graphene display reinforcement (17), conductivity enhancement (78), and barrier properties (79) at loading fractions below 1 volume %. Solvent processing of 2D nanosheets makes composite fabrication straightforward and will extend the suite of 2D fillers beyond clays and graphene (4, 29, 80). Liquid exfoliation also allows the formation of unusual composites consisting of mixtures of nanosheets, nanotubes, and other nanostructures (Fig. 4) (29, 58). This results in synergetic effects; for example, composites of WS2 and carbon nanotubes display very high conductivity but retain much of the character of WS2 films (29, 58, 81). Such composites are promising for applications in photovoltaic or thermoelectric devices and as electrodes for supercapacitors or batteries.

Supercapacitor electrodes formed from chemically exfoliated graphene nanosheets have yielded energy densities of 20 W h kg−1 for packaged devices, approaching those of lead-acid batteries (82). Recent results on restacked nanosheet films indicate that they maintain their structural integrity upon intercalation and deintercalation (58). The wide range of 2D materials available with varying electrochemical properties makes them ideal for energy storage. Initial measurements indicate that their capacitive capability is very high, although issues relating to substantial loss after the first few cycles remain. Choosing the correct combinations of materials will allow multiple properties (such as surface area, conductivity, and electrochemical stability) to be simultaneously improved so as to provide flexibility for designing electrodes for batteries and supercapacitors. For example, materials such as VS2, MoO3, and MnO2 could be useful for efficient energy storage.

The possibility that layered materials could catalyze the production of hydrogen from water, for use as a fuel, is a critically important application. The edge molybdenum sites on TMDs are highly active for hydrogen evolution reactions and thus are being considered as electrodes for water-splitting by using sunlight. With ion-exfoliated 2D TMDs, the presence of a metallic (1T) phase makes the entire basal plane catalytically active, leading to an improvement in the catalytic activity and a substantial increase in the number of active catalytic sites (83). Oxide nanosheets (such as TiO2 and MoO3) are also candidates for hydrogen evolution catalysts (84).

Liquid-phase exfoliation facilitates the integration of the materials into large-area electronics through the well-known solution-based techniques such as inkjet printing (49) and roll-to-roll coating. Recent results have indicated that the electronic structure of the 2D nanosheets is largely preserved after liquid exfoliation so that fundamental processes can be observed in individual sheets. For example, because exfoliated oxides retain their excellent dielectric properties, they can be used as high-k dielectrics in nanoelectronics (10). Alternatively, stacking of different layered perovskites allows the fabrication of artificial multi-ferroic materials for use in future oxide-based electronics and memory devices. Exfoliated oxide nanosheets may also be used in more complex nanodevices, such as photoconducting cells, p-n junctions, and field-effect transistors (8, 10). Alternatively, MoS2 shows exceptionally stable transistor operation under very large mechanical deformation (85). The relatively undisturbed electronic structure coupled with flexibility makes MoS2 and other 2D materials useful for next-generation large-area electronics and opto-electronics on plastic and paper platforms. In particular, large-area, solution-cast, TMD thin-film transistors with mobility of ~10 to 50 cm2/V s could replace doped oxide semiconductors for back-plane switching in flexible and transparent displays.

More exotic applications of layered 2D materials will arise from the stacking and seamless integration of specific combinations of materials in order to access fundamental properties such as superconductivity and condensates (86). The integration could be in the vertical or lateral direction so as to allow for different device concepts. The ability to access metallic and semiconducting phases in 2D materials with electrochemical exfoliation also provides opportunities for designing molecular-scale heterostructures with atomically coherent junctions (24). These types of superlattice structures could be easily synthesized from liquid dispersions.


Our ability to employ straightforward techniques to exfoliate materials points to a productive future in this area. However, a number of substantial challenges remain. Although ultrasonication-assisted solvent exfoliation displays great promise, it also has a number of limitations in its current form. For example, the monolayer yield is generally no more than a few tens of percent by number, which is far too low for many applications. As such, it will be necessary to develop methods to monitor and increase both the monomer yield and indeed the lateral flake size. For ion intercalation–based methods, the time required to achieve exfoliation must be reduced. Crucially, the scale-up of liquid exfoliation must be demonstrated. The ultimate aim must be production on an industrial scale (more than kilograms per day)—a goal that seems relatively far off for defect-free materials. This will almost certainly require exfoliation methods that do not rely on ultrasonication, a method that has limited scalability. However, an achievable early target would be a production rate of grams of exfoliated nanosheets per hour.

It will be important to demonstrate exfoliation of a wider range of layered materials. To date, liquid exfoliation has produced graphene, h-BN, a number of TMDs, a range of clays, many oxides and hydroxides, and a scattering of other exfoliated nanosheets. However, there is a galaxy of other materials (Table 1) offering a rich set of distinct features that have not yet been exfoliated but should be amenable to the methods described above. For example, because layered GaSe and InSe are photoluminescent, liquid exfoliation could lead to next-generation solution-processed, photostable light-emitting diodes. Alternatively, V-VI layered compounds (such as Bi2Te3 and Bi2Se3) could form the basis of solution-processed thermoelectric materials (29, 58).

In addition, exfoliation in liquids will be a good starting point for subsequent chemical modification of nanosheets. For example, chemical functionalization will allow controlled modification of the properties of exfoliated nanosheets for applications in composites, targeted drug delivery, or sensing. It will be critical to develop the chemistry required to attach a wide range of chemical groups to both nanosheet basal plane and edge in a controlled way.

Last, there are a number of cases in which 2D materials might be produced from starting materials that differ considerably from the layered crystals described above. Specifically, we consider materials that lack a clearly defined van der Waals gap. There are entire families of materials that are made of extended layers carrying negative or positive charges and are separated by charge-balancing cations or anions, respectively. Such systems will have just as interesting chemical and physical properties as the neutral layered analogs. Some examples include the semiconducting NaInSe2, K2Cd3S4, K2Fe4Se5, the metallic KCu4S3, BaFe2As2, and the superconducting KFe2As2. Instead of weak van der Waals forces, much stronger electrostatic interactions hold these layers together. In these cases, separation of the layers will require the apportioning of the charge-balancing ions between them to partition evenly on both layers coming apart. This will create surfaces that need to be neutral. Therefore, innovative chemical methods that can dismantle the solid-state lattices and stabilize such surfaces will be required. That such approaches are feasible is evidenced by the chemical modification and subsequent exfoliation of Ti3AlC2—a material without a van der Waals gap—to give nanosheets of Ti3C2F2 and Ti3C2(OH)2 (67).

As exfoliation methods increase in their sophistication and effectiveness, layered materials will yield a host of new 2D systems to explore. The diverse range of properties of known layered crystals means that their exfoliated counterparts will be equally diverse, leading to applications in electronics, photonics, energy storage, structural composites, drug delivery, barrier layers, and coatings, to name but a few. We envisage exfoliated nanosheets becoming central to nanotechnology in the 21st century.

References and Notes

  1. Acknowledgments: J.N.C. and V.N. thank Science Foundation Ireland and the European Research Council for support. At Northwestern, M.G.K.’s research is supported by National Science Foundation grant DMR-1104965. M.S.S. acknowledges support from the Materials Research and Engineering Center program of the National Science Foundation under MIT award DMR-0819762. M.C. acknowledges support from the National Science Foundation Integrative Graduate Education and Research Traineeship program (DGE 0903661).
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