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Graphene is a one-atom-thick planar sheet of sp2-bonded carbon atoms that are densely packed in a honeycomb crystal lattice. It can be visualized as an atomic-scale chicken wire made of carbon atoms and their bonds. The name comes from graphite + -ene; graphite itself consists of many graphene sheets stacked together.
The carbon-carbon bond length in graphene is about 0.142 nm. Graphene is the basic structural element of some carbon allotropes including graphite, carbon nanotubes and fullerenes. It can also be considered as an infinitely large aromatic molecule, the limiting case of the family of flat polycyclic aromatic hydrocarbons called graphenes.
Image of graphene in a transmission electron microscope.
Description
A simple, non-technical definition has been given in a recent review on graphene:
Graphene is a flat monolayer of carbon atoms tightly packed into a two-dimensional (2D) honeycomb lattice, and is a basic building block for graphitic materials of all other dimensionalities. It can be wrapped up into 0D fullerenes, rolled into 1D nanotubes or stacked into 3D graphite.[1]
Previously, graphene was also defined in the chemical literature as follows:
A single carbon layer of the graphitic structure can be considered as the final member of the series naphthalene, anthracene, coronene, etc. and the term graphene should therefore be used to designate the individual carbon layers in graphite intercalation compounds. Use of the term "graphene layer" is also considered for the general terminology of carbons.[2]
The IUPAC compendium of technology states: "previously, descriptions such as graphite layers, carbon layers, or carbon sheets have been used for the term graphene...it is not correct to use for a single layer a term which includes the term graphite, which would imply a three-dimensional structure. The term graphene should be used only when the reactions, structural relations or other properties of individual layers are discussed." In this regard, graphene has been referred to as an infinite alternant (only six-member carbon ring) polycyclic aromatic hydrocarbon (PAH). The largest molecule of this type consists of 222 atoms and is 10 benzene rings across.[3] It has proven difficult to synthesize even slightly bigger molecules, and they still remain "a dream of many organic and polymer chemists".[4] Furthermore, ab initio calculations show that a graphene sheet is thermodynamically unstable with respect to other fullerene structures if its size is less than about 10 nm (“graphene is the least stable structure until about 6000 atoms”[5]).[improper synthesis?]
Also, a definition of "isolated or free standing graphene" has recently been proposed: "graphene is a single atomic plane of graphite, which—and this is essential—is sufficiently isolated from its environment to be considered free-standing."[6] This definition is narrower than the definitions given above and refers to cleaved, transferred and suspended graphene monolayers. Other forms of graphene, such as graphene grown on various metals, can also become free-standing if transferred to, e.g., SiO2 or suspended. A new example of isolated graphene is graphene on SiC after its passivation with hydrogen.[7]
Occurrence and production
Graphene is essentially an isolated atomic plane of graphite. Therefore, from this perspective, graphene has been known since the invention of X-ray crystallography. Graphene planes become even better separated in intercalated graphite compounds. In 2004 physicists from University of Manchester and Institute for Microelectronics Technology, Chernogolovka, Russia, found a way to isolate individual graphene planes by using Scotch tape and they also measured electronic properties of the obtained flakes and showed their fantastic quality.[8] In 2005 the same Manchester group together with researchers from the Columbia University (see the History chapter below) demonstrated that quasiparticles in graphene were massless Dirac fermions. These discoveries led to the explosion of interest in graphene.
Since then, hundreds of researchers have entered the area and, naturally, they carried out the extensive search for relevant earlier papers. The first literature review was given by the Manchester pioneers themselves[1]. They cite several papers in which graphene or ultra-thin graphitic layers were epitaxially grown on various substrates. Also, they point out at a number of pre-2004 reports in which intercalated graphite compounds were studied in a transmission electron microscope. In the latter case, researchers occasionally observed extremely thin graphitic flakes ("few-layer graphene" and possibly even individual layers). The oldest such observation was recently discovered by Rodney Ruoff in a 1962 German-language magazine [9]. It is now well known that tiny fragments of graphene sheets are produced (along with quantities of other debris) whenever graphite is abraded, such as when drawing a line with a pencil.[10] There was little interest in this graphitic residue before 2004/05 and, therefore, the discovery of graphene is often attributed to Andre Geim and colleagues [11] who introduced graphene in its modern incarnation, although it may be argued that this is as accurate as attributing the discovery of America to Columbus.
A couple of years ago, graphene produced by exfoliation was one of the most expensive materials on Earth, with a sample that can be placed at the cross section of a human hair costing more than $1,000 as of April 2008 (about $100,000,000/cm2).[10] Since then, exfoliation procedures were scaled up, and now companies sell graphene by ton.[12] On the other hand, the price of epitaxial graphene on silicon carbide is dominated by the substrate price, which is approximately $100/cm2 as of 2009. Even cheaper graphene has been produced by transfer from nickel by Korean researchers,[13] with wafer sizes up to 30" reported.[citation needed]
In the literature, specifically that of surface science community, graphene has also been commonly referred to as monolayer graphite. This community has intensely studied epitaxial graphene on various surfaces (over 300 articles prior to 2004). In some cases, these graphene layers are coupled to the surfaces weakly enough (by Van der Waals forces) to retain the two dimensional electronic band structure of isolated graphene,[14][15] as also happens[8] with exfoliated graphene flakes with regard to silicon dioxide. An example of weakly coupled epitaxial graphene is the one grown on silicon carbide (see below).
Drawing method
In 2004, the British researchers obtained graphene by mechanical exfoliation of graphite. They used Scotch tape to repeatedly split graphite crystals into increasingly thinner pieces. The tape with attached optically transparent flakes was dissolved in acetone and, after a few further steps, the flakes including monolayers were sedimented on a Si wafer. Individual atomic planes were then hunted in an optical microscope. A year later, the researchers simplified the technique and started using dry deposition, avoiding the stage when graphene floated in a liquid. Relatively large crystallites (first, only a few microns in size but, eventually, larger than 1 mm and visible by a naked eye) were obtained by the technique. It is often referred to as a scotch tape or drawing method. The latter name appeared because the dry deposition resembles drawing with a piece of graphite.[16] The key for the success probably was the use of high throughput visual recognition of graphene on a proper chosen substrate, which provides a small but noticeable optical contrast. For an example of what graphene looks like, see its photograph below.
The isolation of graphene led to the current research boom. Previously, free-standing atomic planes were often "presumed not to exist"[8] because they are thermodynamically unstable on a nm scale[5] and, if unsupported, have a tendency to scroll and buckle[4]. It is currently believed that intrinsic microscopic roughening on the scale of 1 nm could be important for the stability of purely 2D crystals.[17].
It is interesting to note (see Talk:Graphene) that there were a number of previous attempts to make atomically thin graphitic films by using exfoliation techniques similar to the drawing method. Multilayer samples down to 10 nm in thickness were obtained. These efforts were reviewed in [1]. Furthermore, a couple of very old papers was recently unearthed,[9] in which researchers tried to isolate graphene, starting with intercalated compounds (see History and experimental discovery). These papers reported the observation of very thin graphitic fragments (possibly, monolayers) by transmission electron microscopy. Neither of the earlier observations was sufficient to "spark the graphene gold rush", until the Science paper did so by reporting not only macroscopic samples of extracted atomic planes but, importantly, their unusual properties such as the bipolar transistor effect, ballistic transport of charges, large quantum oscillations, etc. The discovery of such interesting qualities intrinsic to graphene gave an immediate boost to further research, and several groups quickly repeated the initial result and moved further. These breakthroughs also helped to attract attention to other production techniques such as epitaxial growth of ultra-thin graphitic films. In particular, it has later been found that graphene monolayers grown on SiC and Ir are weakly coupled to these substrates (how weakly remains debated) and the graphene-substrate interaction can be passivated further.
Not only graphene but also free-standing atomic planes of boron nitride, mica, dichalcogenides and complex oxides were obtained by using the drawing method Unlike graphene, the other 2D materials have so far attracted surprisingly little attention.
Yet another method is to heat silicon carbide to high temperatures (>1100 °C) to reduce it to graphene.[19] This process produces a sample size that is dependent upon the size of the SiC substrate used. The face of the silicon carbide used for graphene creation, the silicon-terminated or carbon-terminated, highly influences the thickness, mobility and carrier density of the graphene.
Many important graphene properties have been identified in graphene produced by this method. For example, the electronic band-structure (so-called Dirac cone structure) has been first visualized in this material. Weak anti-localization is observed in this material and not in exfoliated graphene produced by the pencil trace method. Extremely large, temperature independent mobilities have been observed in SiC epitaxial graphene. They approach those in exfoliated graphene placed on silicon oxide but still much lower than mobilities in suspended graphene produced by the drawing method. It was recently shown that even without being transferred graphene on SiC exhibits the properties of massless Dirac fermions such as the anomalous quantum Hall effect[24][25][26][27][28].
The weak van der Waals forces that provide the cohesion of multilayer graphene stacks do not always affect the electronic properties of the individual graphene layers in the stack. That is, while the electronic properties of certain multilayered epitaxial graphenes are identical to that of a single graphene layer,[29] in other cases the properties are affected [20][21] as they are for graphene layers in bulk graphite. This effect is theoretically well understood and is related to the symmetry of the interlayer interactions.[29]
Epitaxial graphene on silicon carbide can be patterned using standard microelectronics methods. The possibility of large integrated electronics on SiC epitaxial graphene was first proposed in 2004[30] by researchers at the Georgia Institute of Technology, only a couple of months after the discovery of isolated graphene made the drawing method. (A patent for graphene based electronics was applied for in 2003 and issued in 2006). Since then, important advances have been made. In 2008, researchers at MIT Lincoln Lab have produced hundreds of transistors on a single chip and in 2009, very high frequency transistors have been produced at the Hughes Research Laboratories on monolayer graphene on silicon carbide.
Epitaxial growth on metal substrates
This method uses the atomic structure of a metal substrate to seed the growth of the graphene (epitaxial growth). Graphene grown on ruthenium doesn't typically yield a sample with a uniform thickness of graphene layers, and bonding between the bottom graphene layer and the substrate may affect the properties of the carbon layers. Graphene grown on iridium on the other hand is very weakly bonded, uniform in thickness, and can be made highly ordered. Like on many other substrates, graphene on iridium is slightly rippled. Due to the long-range order of these ripples generation of minigaps in the electronic band-structure (Dirac cone) becomes visible.[34] High-quality sheets of few layer graphene exceeding 1 cm2 (0.2 sq in) in area have been synthesized via chemical vapor deposition on thin nickel films. These sheets have been successfully transferred to various substrates, demonstrating viability for numerous electronic applications. An improvement of this technique has been found in copper foil where the growth automatically stops after a single graphene layer, and arbitrarily large graphene films can be created.[35]
Hydrazine reduction
Researchers have developed a method of placing graphene oxide paper in a solution of pure hydrazine (a chemical compound of nitrogen and hydrogen), which reduces the graphene oxide paper into single-layer graphene.[36]
Sodium reduction of ethanol
A recent publication has described a process for producing gram-quantities of graphene, by the reduction of ethanol by sodium metal, followed by pyrolysis of the ethoxide product, and washing with water to remove sodium salts.[37]
From nanotubes
Experimental methods for the production of graphene ribbons are reported consisting of cutting open nanotubes.[38] In one such method multi walled carbon nanotubes are cut open in solution by action of potassium permanganate and sulfuric acid.[39] In another method graphene nanoribbons are produced by plasma etching of nanotubes partly embedded in a polymer film [40]
Atomic structure
The atomic structure of isolated, single-layer graphene was studied by transmission electron microscopy (TEM) on sheets of graphene suspended between bars of a metallic grid.[17] Electron diffraction patterns showed the expected hexagonal lattice of graphene. Suspended graphene also showed "rippling" of the flat sheet, with amplitude of about one nanometer. These ripples may be intrinsic to graphene as a result of the instability of two-dimensional crystals,[1][41][42] or may be extrinsic, originating from the ubiquitous dirt seen in all TEM images of graphene. Atomic resolution real-space images of isolated, single-layer graphene on silicon dioxide substrates were obtained[43][44] by scanning tunneling microscopy. Graphene processed using lithographic techniques is covered by photoresist residue, which must be cleaned to obtain atomic-resolution images.[43] Such residue may be the "adsorbates" observed in TEM images, and may explain the rippling of suspended graphene. Rippling of graphene on the silicon dioxide surface was determined by conformation of graphene to the underlying silicon dioxide, and not an intrinsic effect.[43]
Graphene sheets in solid form (density > 1 g/cm3) usually show evidence in diffraction for graphite's 0.34 nm (002) layering. This is true even of some single-walled carbon nanostructures.[45] However, unlayered graphene with only (hk0) rings has been found in the core of presolar graphite onions.[46] Transmission electron microscope studies show faceting at defects in flat graphene sheets,[47] and suggest a possible role in this unlayered-graphene for two-dimensional dendritic crystallization from a melt.
Electronic properties
GNR band structure for zig-zag type. Tightbinding calculations show that zigzag type is always metallic.
GNR band structure for arm-chair type. Tightbinding calculations show that armchair type can be semiconducting or metallic depending on width (chirality).
Graphene is quite different from most conventional three-dimensional materials. Intrinsic graphene is a semi-metal or zero-gap semiconductor. Understanding the electronic structure of graphene is the starting point for finding the band structure of graphite. It was realized early on that the E-k relation is linear for low energies near the six corners of the two-dimensional hexagonal Brillouin zone, leading to zero effective mass for electrons and holes.[48] [49] Due to this linear (or “conical") dispersion relation at low energies, electrons and holes near these six points, two of which are inequivalent, behave like relativistic particles described by the Dirac equation for spin 1/2 particles.[50][51] Hence, the electrons and holes are called Dirac fermions, and the six corners of the Brillouin zone are called the Dirac points.[50] The equation describing the E-k relation is 
; where the Fermi velocity vF ~ 106 m/s.[51]
Electronic transport
Experimental results from transport measurements show that graphene has a remarkably high electron mobility at room temperature, with reported values in excess of 15,000 cm2V−1s−1.[1] Additionally, the symmetry of the experimentally measured conductance indicates that the mobilities for holes and electrons should be nearly the same.[49] The mobility is nearly independent of temperature between 10 K and 100 K,[52][53][54] which implies that the dominant scattering mechanism is defect scattering. Scattering by the acoustic phonons of graphene places intrinsic limits on the room temperature mobility to 200,000 cm2V−1s−1 at a carrier density of 1012 cm−2.[54][55] The corresponding resistivity of the graphene sheet would be 10−6 Ω·cm, less than the resistivity of silver, the lowest resistivity substance known at room temperature.[56] However, for graphene on silicon dioxide substrates, scattering of electrons by optical phonons of the substrate is a larger effect at room temperature than scattering by graphene’s own phonons, and limits the mobility to 40,000 cm2 V−1s−1.[54]
Despite the zero carrier density near the Dirac points, graphene exhibits a minimum conductivity on the order of 4e2/h. The origin of this minimum conductivity is still unclear. However, rippling of the graphene sheet or ionized impurities in the SiO2 substrate may lead to local puddles of carriers that allow conduction.[49] Several theories suggest that the minimum conductivity should be 4e2/πh; however, most measurements are of order 4e2/h or greater[1] and depend on impurity concentration.[57]
Recent experiments have probed the influence of chemical dopants on the carrier mobility in graphene.[57][58] Schedin et al. doped graphene with various gaseous species (some acceptors, some donors), and found the initial undoped state of a graphene structure can be recovered by gently heating the graphene in vacuum. They reported that even for chemical dopant concentrations in excess of 1012 cm−2 there is no observable change in the carrier mobility.[58] Chen, et al. doped graphene with potassium in ultra high vacuum at low temperature. They found that potassium ions act as expected for charged impurities in graphene,[59] and can reduce the mobility 20-fold.[57] The mobility reduction is reversible on heating the graphene to remove the potassium.
Due to its two-dimensional property, charge fractionalization (where the apparent charge of individual psuedoparticles in low-dimensional systems is less than a single quantum[60]) is thought to occur in graphene. It may therefore be a suitable material for the construction of quantum computers using anyonic circuits.[61][62]
Optical properties
Photograph of graphene in transmitted light. This one atom thick crystal can be seen with the naked eye because it absorbs approximately 2.3% of white light, which is π times fine-structure constant.
Graphene's unique electronic properties produce an unexpectedly high opacity for an atomic monolayer, with a startlingly simple value: it absorbs πα ≈ 2.3% of white light, where α is the fine-structure constant.[63] This is "a consequence of the unusual low-energy electronic structure of monolayer graphene that features electron and hole conical bands meeting each other at the Dirac point ... [which] is qualitatively different from more common quadratic massive bands".[64] Based on the Slonczewski-Weiss-McClure (SWMcC) band model of graphite, the interatomic distance, hopping value and frequency cancel when the optical conductance is calculated using the Fresnel equations in the thin-film limit.
This has been confirmed experimentally, but the measurement is not precise enough to improve on other techniques for determining the fine-structure constant.[65]
Recently it has been demonstrated that the bandgap of graphene can be tuned from 0 to 0.25 eV (about 5 micron wavelength) by applying voltage to a dual-gate bilayer graphene field-effect transistor (FET) at room temperature.[66]. The optical response of graphene nanoribbons has also been shown to be tunable into the terahertz regime by an applied magnetic field [67]
Saturable absorption
It is further confirmed that such unique absorption could become saturated when the input optical intensity is above a threshold value. This nonlinear optical behavior is termed saturable absorption and the threshold value is called the saturation fluency. Graphene can be saturated readily under strong excitation over the visible to near-infrared region, due to the universal optical absorption and zero band gap. This has relevance for the mode locking of fiber lasers, where fullband mode locking has been achieved by graphene based saturable absorber. Due to this special property, graphene has wide application in ultrafast photonics.[68][69]
Spin transport
Graphene is thought to be an ideal material for spintronics due to small spin-orbit interaction and near absence of nuclear magnetic moments in carbon. Electrical spin-current injection and detection in graphene was recently demonstrated up to room temperature.[70][71][72] Spin coherence length above 1 micron at room temperature was observed,[70] and control of the spin current polarity with an electrical gate was observed at low temperature.[71]
Anomalous quantum Hall effect
The quantum Hall effect is relevant for accurate measuring standards of electrical quantities, and in 1985 Klaus von Klitzing received the Nobel prize for its discovery. The effect concerns the dependence of a transverse conductivity on a magnetic field, which is perpendicular to a current-carrying stripe. Usually the phenomenon, the quantization of the so-called Hall conductivity σxy at integer multiples of the basic quantity e2/h (where e is the elementary electric charge and h is Planck's constant) can be observed only in very clean Si or GaAs solids, and at very low temperatures around 3 K, and at very high magnetic fields.
Graphene in contrast, besides its high mobility and minimum conductivity, and because of certain pseudo-relativistic peculiarities to be mentioned below, shows particularly interesting behavior just in the presence of a magnetic field and just with respect to the conductivity-quantization: it displays an anomalous quantum Hall effect with the sequence of steps shifted by 1/2 with respect to the standard sequence, and with an additional factor of 4. Thus, in graphene the Hall conductivity is 
, where n is the above-mentioned integer "Landau level" index, and the double valley and double spin degeneracies give the factor of 4.[1] Moreover, in graphene these remarkable anomalies can even be measured at room temperature, i.e. at roughly 20 °C.[52] This anomalous behavior is a direct result of the emergent massless Dirac electrons in graphene. In a magnetic field, their spectrum has a Landau level with energy precisely at the Dirac point. This level is a consequence of the Atiyah-Singer index theorem. and is half-filled in neutral graphene,[50] leading to the "+1/2" in the Hall conductivity.[73] Bilayer graphene also shows the quantum Hall effect, but with the standard sequence, i.e. with 
i.e. with only one of the two anomalies. Interestingly, concerning the second anomaly, the first plateau at N = 0 is absent, indicating that bilayer graphene stays metallic at the neutrality point.[1]
Unlike normal metals, the longitudinal resistance of graphene shows maxima rather than minima for integral values of the Landau filling factor in measurements of the Shubnikov-de Haas oscillations, which show a phase shift of π, known as Berry’s phase.[49][52] The Berry’s phase arises due to the zero effective carrier mass near the Dirac points.[74] Study of the temperature dependence of the Shubnikov-de Haas oscillations in graphene reveals that the carriers have a non-zero cyclotron mass, despite their zero effective mass from the E-k relation.[52]
Nanostripes: Spin-polarized edge currents
Nanostripes of graphene (in the "zig-zag" orientation), at low temperatures, show spin-polarized metallic edge currents, which also suggests applications in the new field of spintronics. (In the "armchair" orientation, the edges behave like semiconductors.[75])
Graphene oxide
Further information: Graphite Oxide
By disbursing oxidized and chemically processed graphite in water, and using paper-making techniques, the monolayer flakes form a single sheet and bond very powerfully. These sheets, called graphene oxide paper have a measured tensile modulus of 32 GPa.[76] The peculiar chemical property of graphite oxide is related to the functional groups attached to graphene sheets. They even can significantly change the pathway of polymerization and similar chemical processes.[77]
Chemical modification
Soluble fragments of graphene can be prepared in the laboratory[78] through chemical modification of graphite. First, microcrystalline graphite is treated with a strongly acidic mixture of sulfuric acid and nitric acid. A series of steps involving oxidation and exfoliation result in small graphene plates with carboxyl groups at their edges. These are converted to acid chloride groups by treatment with thionyl chloride; next, they are converted to the corresponding graphene amide via treatment with octadecylamine. The resulting material (circular graphene layers of 5.3 angstrom thickness) is soluble in tetrahydrofuran, tetrachloromethane, and dichloroethane.
Full hydrogenation from both sides of graphene sheet results in graphane, but partial hydrogenation leads to hydrogenated graphene[79]
Thermal properties
The near-room temperature thermal conductivity of graphene was recently measured to be between (4.84±0.44) ×103 to (5.30±0.48) ×103 Wm−1K−1. These measurements, made by a non-contact optical technique, are in excess of those measured for carbon nanotubes or diamond. It can be shown by using the Wiedemann-Franz law, that the thermal conduction is phonon-dominated.[80] However, for a gated graphene strip, an applied gate bias causing a Fermi energy shift much larger than kBT can cause the electronic contribution to increase and dominate over the phonon contribution at low temperatures. The ballistic thermal conductance of graphene is isotropic.[81]
Potential for this high conductivity can be seen by considering graphite, a 3D version of graphene that has basal plane thermal conductivity of over a 1000 W/mK (comparable to diamond). In graphite, the c-axis (out of plane) thermal conductivity is over a factor of ~100 smaller due to the weak binding forces between basal planes as well as the larger lattice spacing.[82] In addition, the ballistic thermal conductance of a graphene is shown to give the lower limit of the ballistic thermal conductances, per unit circumference, length of carbon nanotubes.[83]
Despite its 2-D nature, graphene has 3 acoustic phonon modes. The two in-plane modes (LA, TA) have a linear dispersion relation, whereas the out of plane mode (ZA) has a quadratic dispersion relation. Due to this, the T2 dependent thermal conductivity contribution of the linear modes is dominated at low temperatures by the T1.5 contribution of the out of plane mode.[83] Some graphene phonon bands display negative Grüneisen parameters.[84] At low temperatures (where most optical modes with positive Grüneisen parameters are still not excited) the contribution from the negative Grüneisen parameters will be dominant and thermal expansion coefficient (which is directly proportional to Grüneisen parameters) negative. The lowest negative Grüneisen parameters correspond to the lowest transversal acoustic ZA modes. Phonon frequencies for such modes increase with the in-plane lattice parameter since atoms in the layer upon stretching will be less free to move in the z direction. This is similar to the behavior of a string which is being stretched will have vibrations of smaller amplitude and higher frequency. This phenomenon, named "membrane effect", was predicted by Lifshitz in 1952.[85]
Mechanical properties
As of 2009, graphene appears to be one of the strongest materials ever tested. Measurements have shown that graphene has a breaking strength 200 times greater than steel.[86] However, the process of separating it from graphite, where it occurs naturally, will require some technological development before it is economical enough to be used in industrial processes,[87] though this may be changing soon.[88]
Using an atomic force microscope (AFM), the spring constant of suspended graphene sheets has been measured. Graphene sheets, held together by van der Waals forces, were suspended over silicon dioxide cavities where an AFM tip was probed to test its mechanical properties. Its spring constant was in the range 1-5 N/m and the Young's modulus was 0.5 TPa, which differs from that of the bulk graphite. These high values make graphene very strong and rigid. These intrinsic properties could lead to using graphene for NEMS applications such as pressure sensors and resonators.[89]
As is true of all materials, regions of graphene are subject to thermal and quantum fluctuations in relative displacement. Although the amplitude of these fluctuations is bounded in 3D structures (even in the limit of infinite size), the Mermin-Wagner theorem shows that the amplitude of long-wavelength fluctuations will grow logarithmically with the scale of a 2D structure, and would therefore be unbounded in structures of infinite size. Local deformation and elastic strain are negligibly affected by this long-range divergence in relative displacement. It is believed that a sufficiently large 2D structure, in the absence of applied lateral tension, will bend and crumple to form a fluctuating 3D structure. Researchers have observed ripples in suspended layers of graphene,[17] and it has been proposed that the ripples are caused by thermal fluctuations in the material. As a consequence of these dynamical deformations, it is debatable whether graphene is truly a 2D structure.[1][41][42]
Single molecule gas detection
Graphene makes an excellent sensor due to its 2D structure. The fact that its entire volume is exposed to its surrounding makes it very efficient to detect adsorbed molecules. Molecule detection is indirect: as a gas molecule adsorbs to the surface of graphene, the location of adsorption experiences a local change in electrical resistance. While this effect occurs in other materials, graphene is superior due to its high electrical conductivity (even when few carriers are present) and low noise which makes this change in resistance detectable.[58]
Graphene nanoribbons
Graphene nanoribbons (GNRs) are essentially single layers of graphene that are cut in a particular pattern to give it certain electrical properties. Depending on how the un-bonded edges are configured, they can either be in a zigzag or armchair configuration. Calculations based on tight binding predict that zigzag GNRs are always metallic while armchairs can be either metallic or semiconducting, depending on their width. However, recent density functional theory calculations show that armchair nanoribbons are semiconducting with an energy gap scaling with the inverse of the GNR width.[90] Indeed, experimental results show that the energy gaps do increase with decreasing GNR width.[91] However, as of February 2008, no experimental results have measured the energy gap of a GNR and identified the exact edge structure. Zigzag nanoribbons are also semiconducting and present spin polarized edges. Their 2D structure, high electrical and thermal conductivity, and low noise also make GNRs a possible alternative to copper for integrated circuit interconnects. Some research is also being done to create quantum dots by changing the width of GNRs at select points along the ribbon, creating quantum confinement.[92]
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で ある。ここでNはラ ンダウ準位のインデックスで、二つの谷とスピンの二重縮退により4の 因子が生ずる。この特徴的な振る舞いは室温でも観測されうる。二重層グラフェンも量子ホール効果を示すが、二重層グラフェンで起こるのは正常量子ホール効 果であり、
で ある。最初のプ ラトーであるN = 0は存在しないことから、二重層グラフェンは中性点で金属的になっていることが示唆される。
の 電子のエネルギーは次のように書ける。
は 最近接原子にホップするエネルギー、格 子定数
。分 散関係のプラスとマイナスの符号は、それぞれ伝導帯と価 電子帯に対応している。伝導帯と価電子帯は、K-valuesと呼ばれる6点で接しているが、6点のうち独立なの は2点のみで、残りは対称性から等価である。K点の近傍ではエネルギーは波数に線形となるが、これは相 対論的粒子の分散関係に類似している。さらに、格子の単位胞が 2原子からなるため、波動関数は実効的に2ス ピノル構造まで持つ。結果として、低エネルギーで電子はディ ラック方程式と形式的に等価な方程式で書き表せる。さらにこの擬相対論的な記述はカ イラル極限、すなわち静 止質量M0が ゼロの極限に制限されているため、興味深いさまざまな特性が生ずる。
は グラフェンのフェ ルミ速度であり、ディラック理論の光速に 代わるものである。
はパ ウリ行列のベクトルであり、
は 電子の二成分波動関数。Eはエネルギーである。
Bewise Inc.
Bewise Inc.
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