Potential applications of graphene

Potential graphene applications include lightweight, thin, flexible, yet durable display screens, electric circuits, and solar cells, as well as various medical, chemical and industrial processes enhanced or enabled by the use of new graphene materials.[1]

In 2008, graphene produced by exfoliation was one of the most expensive materials on Earth, with a sample the area of a cross section of a human hair costing more than $1,000 as of April 2008 (about $100,000,000/cm2).[2] Since then, exfoliation procedures have been scaled up, and now companies sell graphene in large quantities.[3] The price of epitaxial graphene on Silicon carbide is dominated by the substrate price, which was approximately $100/cm2 as of 2009.

Hong and his team in South Korea pioneered the synthesis of large-scale graphene films using chemical vapour deposition (CVD) on thin nickel layers, which triggered research on practical applications,[4] with wafer sizes up to 30 inches (760 mm) reported.[5]

In 2013, the European Union made a €1 billion grant to be used for research into potential graphene applications.[6] In 2013 the Graphene Flagship consortium formed, including Chalmers University of Technology and seven other European universities and research centers, along with Nokia.[7]

Medicine

Tissue engineering

Graphene has been investigated for tissue engineering. It has been used as a reinforcing agent to improve the mechanical properties of biodegradable polymeric nanocomposites for engineering bone tissue applications.[8] Dispersion of low weight % of graphene (~0.02 wt.%) increased in compressive and flexural mechanical properties of polymeric nanocomposites.

Contrast agents/bioimaging

Functionalized and surfactant dispersed graphene solutions have been designed as blood pool MRI contrast agents.[9] Additionally, iodine and manganese incorporating graphene nanoparticles have served as multimodal MRI-CT contrast agents.[10] Graphene micro- and nano-particles have served as contrast agents for photoacoustic and thermoacoustic tomography.[11] Graphene has also been reported to be efficiently taken up cancerous cells thereby enabling the design of drug delivery agents for cancer therapy.[12] Graphene nanoparticles of various morphologies are non-toxic at low concentrations and do not alter stem cell differentiation suggesting that they may be safe to use for biomedical applications.[13]

Polymerase chain reaction

Graphene is reported to have enhanced PCR by increasing the yield of DNA product.[14] Experiments revealed that graphene's thermal conductivity could be the main factor behind this result. Graphene yields DNA product equivalent to positive control with up to 65% reduction in PCR cycles.

Devices

Graphene's modifiable chemistry, large surface area, atomic thickness and molecularly gatable structure make antibody-functionalized graphene sheets excellent candidates for mammalian and microbial detection and diagnosis devices.[15] Graphene is so thin water has near-perfect wetting transparency which is an important property particularly in developing bio-sensor applications.[16] This means that a sensors coated in graphene have as much contact with an aqueous system as an uncoated sensor, while it remains protected mechanically from its environment.

Energy of the electrons with wavenumber k in graphene, calculated in the Tight Binding-approximation. The unoccupied (occupied) states, colored in blue–red (yellow–green), touch each other without energy gap exactly at the above-mentioned six k-vectors.

Integration of graphene (thickness of 0.34 nm) layers as nanoelectrodes into a nanopore[17] can potentially solve a bottleneck for nanopore-based single-molecule DNA sequencing.

On November 20, 2013 the Bill & Melinda Gates Foundation awarded $100,000 'to develop new elastic composite materials for condoms containing nanomaterials like graphene'.[18]

In 2014, graphene-based, transparent (across infrared to ultraviolet frequencies), flexible, implantable medical sensor microarrays were announced that allow the viewing of brain tissue hidden by implants. Optical transparency was >90%. Applications demonstrated include optogenetic activation of focal cortical areas, in vivo imaging of cortical vasculature via fluorescence microscopy and 3D optical coherence tomography.[19][20]

Drug delivery

Biomicrorobotics

Researchers demonstrated a nanoscale biomicrorobot (or cytobot) made by cladding a living endospore cell with graphene quantum dots. The device acted as a humidity sensor.[25]

Testing

In 2014 a graphene based blood glucose testing product was announced.[26][27]

Electronics

For integrated circuits, graphene has a high carrier mobility, as well as low noise, allowing it to be used as the channel in a field-effect transistor. Single sheets of graphene are hard to produce and even harder to make on an appropriate substrate.[28]

In 2008, the smallest transistor so far, one atom thick, 10 atoms wide was made of graphene.[29] IBM announced in December 2008 that they had fabricated and characterized graphene transistors operating at GHz frequencies.[30] In May 2009, an n-type transistor was announced meaning that both n and p-type graphene transistors had been created.[31][32] A functional graphene integrated circuit was demonstrated – a complementary inverter consisting of one p- and one n-type graphene transistor.[33] However, this inverter suffered from a very low voltage gain.

According to a January 2010 report,[34] graphene was epitaxially grown on SiC in a quantity and with quality suitable for mass production of integrated circuits. At high temperatures, the quantum Hall effect could be measured in these samples. IBM built 'processors' using 100 GHz transistors on 2-inch (51 mm) graphene sheets.[35]

In June 2011, IBM researchers announced that they had succeeded in creating the first graphene-based integrated circuit, a broadband radio mixer.[36] The circuit handled frequencies up to 10 GHz. Its performance was unaffected by temperatures up to 127 °C.

In June 2013 an 8 transistor 1.28 GHz ring oscillator circuit was described.[37]

Transistors

Graphene exhibits a pronounced response to perpendicular external electric fields, potentially forming field-effect transistors (FET). A 2004 paper documented FETs with an on-off ratio of ~30 at room temperature. A 2006 paper announced an all-graphene planar FET with side gates.[38] Their devices showed changes of 2% at cryogenic temperatures. The first top-gated FET (on–off ratio of <2) was demonstrated in 2007.[39] Graphene nanoribbons may prove generally capable of replacing silicon as a semiconductor.[40]

US patent 7015142 for graphene-based electronics was issued in 2006. In 2008, researchers at MIT Lincoln Lab produced hundreds of transistors on a single chip[41] and in 2009, very high frequency transistors were produced at Hughes Research Laboratories.[42]

A 2008 paper demonstrated a switching effect based on a reversible chemical modification of the graphene layer that gives an on–off ratio of greater than six orders of magnitude. These reversible switches could potentially be employed in nonvolatile memories.[43]

In 2009, researchers demonstrated four different types of logic gates, each composed of a single graphene transistor.[44]

Practical uses for these circuits are limited by the very small voltage gain they exhibit. Typically, the amplitude of the output signal is about 40 times less than that of the input signal. Moreover, none of these circuits operated at frequencies higher than 25 kHz.

In the same year, tight-binding numerical simulations[45] demonstrated that the band-gap induced in graphene bilayer field effect transistors is not sufficiently large for high-performance transistors for digital applications, but can be sufficient for ultra-low voltage applications, when exploiting a tunnel-FET architecture.[46]

In February 2010, researchers announced transistors with an on/off rate of 100 gigahertz, far exceeding the rates of previous attempts, and exceeding the speed of silicon transistors with an equal gate length. The 240 nm devices were made with conventional silicon-manufacturing equipment.[47][48][49]

In November 2011, researchers used 3d printing (additive manufacturing) as a method for fabricating graphene devices.[50]

In 2013, researchers demonstrated graphene's high mobility in a detector that allows broad band frequency selectivity ranging from the THz to IR region (0.76–33 THz)[51] A separate group created a terahertz-speed transistor with bistable characteristics, which means that the device can spontaneously switch between two electronic states. The device consists of two layers of graphene separated by an insulating layer of boron nitride a few atomic layers thick. Electrons move through this barrier by quantum tunneling. These new transistors exhibit “negative differential conductance,” whereby the same electrical current flows at two different applied voltages.[52]

Graphene does not have an energy band-gap, which presents a hurdle for its applications in digital logic gates. The efforts to induce a band-gap in graphene via quantum confinement or surface functionalization have not resulted in a breakthrough. The negative differential resistance experimentally observed in graphene field-effect transistors of "conventional" design allows for construction of viable non-Boolean computational architectures with the gap-less graphene. The negative differential resistance — observed under certain biasing schemes — is an intrinsic property of graphene resulting from its symmetric band structure. The results present a conceptual change in graphene research and indicate an alternative route for graphene's applications in information processing.[53]

In 2013 researchers reported the creation of transistors printed on flexible plastic that operate at 25 gigahertz, sufficient for communications circuits and that can be fabricated at scale. The researchers first fabricate the non-graphene-containing structures—the electrodes and gates—on plastic sheets. Separately, they grow large graphene sheets on metal, then peel it off and transfer it to the plastic. Finally, they top the sheet with a waterproof layer. The devices work after being soaked in water, and are flexible enough to be folded.[54]

Trilayer graphene

An electric field can change trilayer graphene's crystal structure, transforming its behavior from metal-like to semiconductor-like. A sharp metal scanning tunneling microscopy tip was able to move the domain border between the upper and lower graphene configurations. One side of the material behaves as a metal, while the other side behaves as a semiconductor. Trilayer graphene can be stacked in either Bernal or rhombohedral configurations, which can exist in a single flake. The two domains are separated by a precise boundary at which the middle layer is strained to accommodate the transition from one stacking pattern to the other.[55]

Silicon transistors function as either p-type or n-type semiconductors, whereas graphene could operate as both. This lowers costs and is more versatile. The technique provides the basis for a field-effect transistor. Scalable manufacturing techiques have yet to be developed.[55]

In trilayer graphene, the two stacking configurations exhibit very different electronic properties. The region between them consists of a localized strain soliton where the carbon atoms of one graphene layer shift by the carbon–carbon bond distance. The free-energy difference between the two stacking configurations scales quadratically with electric field, favoring rhombohedral stacking as the electric field increases.[55]

This ability to control the stacking order opens the way to new devices that combine structural and electrical properties.[55][56]

Graphene-based transistors could be much thinner than modern silicon devices, allowing faster and smaller configurations.

Transparent conducting electrodes

Graphene's high electrical conductivity and high optical transparency make it a candidate for transparent conducting electrodes, required for such applications as touchscreens, liquid crystal displays, organic photovoltaic cells, and organic light-emitting diodes. In particular, graphene's mechanical strength and flexibility are advantageous compared to indium tin oxide, which is brittle. Graphene films may be deposited from solution over large areas.[57][58]

Large-area, continuous, transparent and highly conducting few-layered graphene films were produced by chemical vapor deposition and used as anodes for application in photovoltaic devices. A power conversion efficiency (PCE) up to 1.71% was demonstrated, which is 55.2% of the PCE of a control device based on indium tin oxide.[59]

Organic light-emitting diodes (OLEDs) with graphene anodes have been demonstrated.[60] The electronic and optical performance of graphene-based devices are similar to devices made with indium tin oxide.

A carbon-based device called a light-emitting electrochemical cell (LEC) was demonstrated with chemically-derived graphene as the cathode and the conductive polymer PEDOT as the anode.[61] Unlike its predecessors, this device contains only carbon-based electrodes, with no metal.

In 2014 a prototype graphene-based flexible display was demonstrated.[62]

Frequency multiplier

In 2009, researchers built experimental graphene frequency multipliers that take an incoming signal of a certain frequency and output a signal at a multiple of that frequency.[63]

Optoelectronics

Graphene strongly interacts with photons, with the potential for direct band-gap creation. This is promising for optoelectronic and nanophotonic devices. Light interaction arises due to the Van Hove singularity. Graphene displays different time scales in response to photon interaction, ranging from femtoseconds (ultra-fast) to picoseconds. Potential uses include transparent films, touch screens and light emitters or as a plasmonic device that confines light and alters wavelengths.[64]

Hall effect sensors

Due to extremely high electron mobility, graphene may be used for production of highly sensitive Hall effect sensors.[65] Potential application of such sensors is connected with DC current transformers for special applications.

Quantum dots

Graphene quantum dots (GQDs) keep all dimensions less than 10 nm. Their size and edge crystallography govern their electrical, magnetic, optical and chemical properties. GQDs can be produced via graphite nanotomy[66] or via bottom-up, solution-based routes (Diels-Alder, cyclotrimerization and/or cyclodehydrogenation reactions).[67] GQDs with controlled structure can be incorporated into applications in electronics, optoelectronics and electromagnetics. Quantum confinement can be created by changing the width of graphene nanoribbons (GNRs) at selected points along the ribbon.[29][68] It is studied as a catalyst for fuel cells.[69]

Organic electronics

A semiconducting polymer (poly(3-hexylthiophene)[70] placed on top of single-layer graphene vertically conducts electric charge better than on a thin layer of silicon. A 50 nm thick polymer film conducted charge about 50 times better than a 10 nm thick film, potentially because the former consists of a mosaic of variably-oriented crystallites forms a continuous pathway of interconnected crystals. In a thin film or on silicon,[70] plate-like crystallites are oriented parallel to the graphene layer. Uses include solar cells.[71]

Light processing

Optical modulator

When the Fermi level of graphene is tuned, its optical absorption can be changed. In 2011, researchers reported the first graphene-based optical modulator. Operating at 1.2 GHz without a temperature controller, this modulator has a broad bandwidth (from 1.3 to 1.6 μm) and small footprint (~25 μm2).[72]

Infrared light detection

Graphene reacts to the infrared spectrum at room temperature, albeit with sensitivity 100 to 1000 times too low for practical applications. However, two graphene layers separated by an insulator allowed an electric field produced by holes left by photo-freed electrons in one layer to affect a current running through the other layer. The process produces little heat, making it suitable for use in night-vision optics. The sandwich is thin enough to be integrated in handheld devices, eyeglass-mounted computers and even contact lenses.[73]

Energy

Generation

Ethanol distillation

Graphene oxide membranes allow water vapor to pass through, but are impermeable to other liquids and gases.[74] This phenomenon has been used for further distilling of vodka to higher alcohol concentrations, in a room-temperature laboratory, without the application of heat or vacuum as used in traditional distillation methods.[75] Further development and commercialization of such membranes could revolutionize the economics of biofuel production and the alcoholic beverage industry.

Solar cells

Graphene has a unique combination of high electrical conductivity and optical transparency, which make it a candidate for use in solar cells. A single sheet of graphene is a zero-bandgap semiconductor whose charge carriers are delocalized over large areas, implying that carrier scattering does not occur. Because this material only absorbs 2.6% of green light and 2.3% of red light,[76] it is a candidate for applications requiring a transparent conductor. Graphene can be assembled into a film electrode with low roughness. However, graphene films produced via solution processing contain lattice defects and grain boundaries that act as recombination centers and decrease the material's electrical conductivity. Thus, these films must be made thicker than one atomic layer to obtain useful sheet resistances. This added resistance can be combatted by incorporating conductive filler materials, such as a silica matrix. Reduced graphene film's electrical conductivity can be improved by attaching large aromatic molecules such as pyrene-1-sulfonic acid sodium salt (PyS) and the disodium salt of 3,4,9,10-perylenetetracarboxylic diimide bisbenzenesulfonic acid (PDI). These molecules, under high temperatures, facilitate better π-conjugation of the graphene basal plane. Graphene films have high transparency in the visible and near-infrared regions and are chemically and thermally stable.[77]

For graphene to be used in commercial solar cells, large-scale production is required. However, no scalable process for producing graphene is available, including the peeling of pyrolytic graphene or thermal decomposition of silicon carbide.[77]

Graphene's high charge mobilities recommend it for use as a charge collector and transporter in photovoltaics (PV). Using graphene as a photoactive material requires its bandgap to be 1.4–1.9 eV. In 2010, single cell efficiencies of nanostructured graphene-based PVs of over 12% were achieved. According to P. Mukhopadhyay and R. K. Gupta organic photovoltaics could be "devices in which semiconducting graphene is used as the photoactive material and metallic graphene is used as the conductive electrodes".[77]

In 2010, Xinming Li and Hongwei Zhu from Tsinghua University first reported graphene-silicon heterojunction solar cell, where graphene served as a transparent electrode and introduced a built-in electric field near the interface between the graphene and n-type silicon to help collect photo-generated carriers. More studies promote this new type of photovoltaic device.[78] For example, in 2012 researchers from the University of Florida reported efficiency of 8.6% for a prototype cell consisting of a wafer of silicon coated with a layer of graphene doped with trifluoromethanesulfonyl-amide (TFSA). Furthermore, Xinming Li found chemical doping could improve the graphene characteristics and significantly enhance the efficiency of graphene-silicon solar cell to 9.6% in 2013.[79] In 2015 researchers reported efficiency of 15.6% by choosing the optimal oxide thickness on the silicon.[80]

In 2013 another team claimed to have reached 15.6% percent using a combination of titanium oxide and graphene as a charge collector and perovskite as a sunlight absorber. The device is manufacturable at temperatures under 150 °C (302 °F) using solution-based deposition. This lowers production costs and offers the potential using flexible plastics.[81]

Large scale production of highly transparent graphene films by chemical vapor deposition was achieved in 2008. In this process, ultra-thin graphene sheets are created by first depositing carbon atoms in the form of graphene films on a nickel plate from methane gas. A protective layer of thermoplastic is laid over the graphene layer and the nickel underneath is dissolved in an acid bath. The final step is to attach the plastic-protected graphene to a flexible polymer sheet, which can then be incorporated into an OPV cell. Graphene/polymer sheets range in size up to 150 square centimeters and can be used to create dense arrays of flexible OPV cells. It may eventually be possible to run printing presses covering extensive areas with inexpensive solar cells, much like newspaper presses print newspapers (roll-to-roll).[82]

Silicon generates only one current-driving electron for each photon it absorbs, while graphene can produce multiple electrons. Solar cells made with graphene could offer 60% conversion efficiency – double the widely accepted maximum efficiency of silicon cells.[83]

Fuel cells

Appropriately perforated graphene (and hexagonal boron nitride hBN) can allow protons to pass through it, offering the potential for using graphene monolayers as a barrier that blocks hydrogen atoms but not protons/ionized hydrogen (hydrogen atoms with their electrons stripped off). They could even be used to extract hydrogen gas out of the atmosphere that could power electric generators with ambient air.[84]

The membranes are more effective at elevated temperatures and when covered with catalytic nanoparticles such as platinum.[84]

Graphene could solve a major problem for fuel cells: fuel crossover that reduces efficiency and durability.[84]

At room temperature, proton conductivity with monolayer hBN, outperforms graphene, with resistivity to proton flow of about 10 Ω cm2 and a low activation energy of about 0.3 electronvolts. At higher temperatures, graphene outperforms with resistivity estimated to fall below 10−3 Ω cm2 above 250 degrees Celsius.[85]

In another project, protons easily pass through slightly imperfect graphene membranes on fused silica in water.[86] The membrane was exposed to cycles of high and low pH. Protons transferred reversibly from the aqueous phase through the graphene to the other side where they undergo acid–base chemistry with silica hydroxyl groups. Computer simulations indicated energy barriers of 0.61–0.75 eV for hydroxyl-terminated atomic defects that participate in a Grotthuss-type relay, while pyrylium-like ether terminations did not.[87]

Storage

Supercapacitor

Due to graphene's high surface area to mass ratio, one potential application is in the conductive plates of supercapacitors.[88]

In February 2013 researchers announced a novel technique to produce graphene supercapacitors based on the DVD burner reduction approach.[89]

In 2014 a supercapacitor was announced that was claimed to achieve energy density comparable to current lithium-ion batteries.[26][27]

In 2015 the technique was adapted to produce stacked, 3-D supercapacitors. Laser-induced graphene was produced on both sides of a polymer sheet. The sections were then stacked, separated by solid electrolytes, making multiple microsupercapacitors. The stacked configuration substantially increased the energy density of the result. In testing, the researchers charged and discharged the devices for thousands of cycles with almost no loss of capacitance.[90] The resulting devices were mechanically flexible, surviving 8,000 bending cycles. This makes them potentially suitable for rolling in a cylindrical configuration.  Solid-state polymeric electrolyte-based devices exhibit areal capacitance of >9 mF/cm2 at a current density of 0.02 mA/cm2, over twice that of conventional aqueous electrolytes.[91]

Also in 2015 another project announced a microsupercapacitor that is small enough to fit in wearable or implantable devices. Just one-fifth the thickness of a sheet of paper, it is capable of holding more than twice as much charge as a comparable thin-film lithium battery. The design employed laser-scribed graphene, or LSG with manganese dioxide. They can be fabricated without extreme temperatures or expensive “dry rooms”. Their capacity is six times that of commercially available supercapacitors.[92] The device reached volumetric capacitance of over 1,100 F/cm3. This corresponds to a specific capacitance of the constituent MnO2 of 1,145 F/g, close to the theoretical maximum of 1,380 F/g. Energy density varies between 22 and 42 Wh/l depending on device configuration.[93]

Electrode for Li-ion batteries

Stable Li-ion cycling has recently been demonstrated in bi- and few layer graphene films grown on nickel substrates,[94] while single layer graphene films have been demonstrated as a protective layer against corrosion in battery components such as the battery case.[95] This creates possibilities for flexible electrodes for microscale Li-ion batteries where the anode acts as the active material as well as the current collector.[96]

There are also silicon-graphene anode Li-ion batteries.[97]

Hydrogen storage

Hydrogenation-assisted graphene origami (HAGO) was used to cause approximately square graphene sheets to fold into a cage can store hydrogen at 9.5 percent by weight. The U.S. Department of Energy had set a goal of 7.5 percent hydrogen by 2020. An electric field causes the box to open and close.[98]

Rechargeable battery

Researchers at Northwestern University built a lithium-ion battery made of graphene and silicon, which was claimed to last over a week on a single charge and only took 15 minutes to charge.[99]

Sensors

Molecular adsorbtion

Theoretically graphene makes an excellent sensor due to its 2D structure. The fact that its entire volume is exposed to its surrounding environment makes it very efficient to detect adsorbed molecules. However, similar to carbon nanotubes, graphene has no dangling bonds on its surface. Gaseous molecules cannot be readily adsorbed onto graphene surfaces, so intrinsically graphene is insensitive.[100] The sensitivity of graphene chemical gas sensors can be dramatically enhanced by functionalization, for example, coating the film with a thin layer of certain polymers. The thin polymer layer acts like a concentrator that absorbs gaseous molecules. The molecule absorption introduces a local change in electrical resistance of graphene sensors. 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.[101]

Piezoelectric effect

Density functional theory simulations predict that depositing certain adatoms on graphene can render it piezoelectrically responsive to an electric field applied in the out-of-plane direction. This type of locally engineered piezoelectricity is similar in magnitude to that of bulk piezoelectric materials and makes graphene a candidate for control and sensing in nanoscale devices.[102]

Body motion

Rubber bands infused with graphene("G-bands") can be used as inexpensive body sensors. The bands remain pliable and can be used as a sensor to measure breathing, heart rate, or movement. Lightweight sensor suits for vulnerable patients could make it possible to remotely monitor subtle movement. These sensors display 10-fold increases in resistance and work at strains exceeding 800%. Gauge factors of up to 35 were observed. Such sensors can function at vibration frequencies of at least 160 Hz. At 60 Hz, strains of at least 6% at strain rates exceeding 6000%/s can be monitored.[103]

Environmental

Contaminant removal

Graphene oxide is non-toxic and biodegradable. Its surface is covered with epoxy, hydroxyl, and carboxyl groups that interact with cations and anions. It is soluble in water and forms stable colloid suspensions in other liquids because it is amphiphilic (able to mix with water or oil). Dispersed in liquids it shows excellent sorption capacities. It can remove copper, cobalt, cadmium, arsenate and organic solvents.[104]

In 2013 it was shown to be able to remove radioactive nuclides from water, including radioactive isotopes of actinides (elements with atomic numbers 89 to 103, including thorium, uranium, neptunium, plutonium and americium) and lanthanides (the ‘rare earths’ with atomic numbers 57 to 71, including europium).[104]

Even at concentrations < 0.1 g/L, radionuclide sorption proceeds rapidly. At pH between 4 and 8, graphene oxide removes over 90% of nuclides, including uranium and europium.  At pH >7, more than 70% of strontium and technicium are removed with up to 20% of neptunium.[104]

Water filtration

Research suggests that graphene filters could outperform other techniques of desalination by a significant margin.[105]

Other

Plasmonics and metamaterials

Graphene accommodates a plasmonic surface mode, observed recently via near field infrared optical microscopy techniques.[106][107] and infrared spectroscopy [108] Potential applications are in the terahertz to midinfrared frequencies,[109] such as terahertz and midinfrared light modulators, passive terahertz filters, midinfrared photodetectors and biosensors.

Lubricant

Scientists discovered using graphene as a lubricant works better than traditionally used graphite. A one atom thick layer of graphene in between a steel ball and steel disc lasted for 6,500 cycles. Conventional lubricants lasted 1,000 cycles.[110]

Radio wave absorption

Stacked graphene layers on a quartz substrate increased the absorption of millimeter (radio) waves by 90 per cent over 125 – 165 GHz bandwidth, extensible to microwave and low-terahertz frequencies, while remaining transparent to visible light. For example, graphene could be used as a coating for buildings or windows to block radio waves. Absorption is a result of mutually coupled Fabry–Perot resonators represented by each graphene-quartz substrate. A repeated transfer-and-etch process was used to control surface resistivity.[111][112]

Redox

Graphene oxide can be reversibly reduced and oxidized using electrical stimulus. Controlled reduction and oxidation in two-terminal devices containing multilayer graphene oxide films are shown to result in switching between partially reduced graphene oxide and graphene, a process that modifies electronic and optical properties. Oxidation and reduction are related to resistive switching.[113]

Nanoantennas

A graphene-based plasmonic nano-antenna (GPN) can operate efficiently at millimeter radio wavelengths. The wavelength of surface plasmon polaritons for a given frequency is several hundred times smaller than the wavelength of freely propagating electromagnetic waves of the same frequency. These speed and size differences enable efficient graphene-based antennas to be far smaller than conventional alternatives. The latter operate at frequencies 100-1000 times larger than GPNs, producing .01-.001 as many photons.[114]

An electromagnetic (EM) wave directed vertically onto a graphene surface excites the graphene into oscillations that interact with those in the dielectric on which the graphene is mounted, thereby forming surface plasmon polaritons (SPP). When the antenna becomes resonant (an integral number of SPP wavelengths fit into the physical dimensions of the graphene), the SPP/EM coupling increases greatly, efficiently transferring energy between the two.[114]

A phased array antenna 100 µm in diameter could produce 300 GHz beams only a few degrees in diameter, instead of the 180 degree radiation from tsa conventional metal antenna of that size. Potential uses include smart dust, low-power terabit wireless networks[114] and photonics.[115]

A nanoscale gold rod antenna captured and transformed EM energy into graphene plasmons, analogous to a radio antenna converting radio waves into electromagnetic waves in a metal cable. The plasmon wavefronts can be directly controlled by adjusting antenna geometry. The waves were focused (by curving the antenna) and refracted (by a prism-shaped graphene bilayer because the conductivity in the two-atom-thick prism is larger than in the surrounding one-atom-thick layer.)[115]

Sound transducers

Graphene provides relatively good frequency response, suggesting uses in audio speakers. Its light weight may make it suitable for microphones as well.[116]

Waterproof coating

Graphene could potentially usher in a new generation of waterproof devices whose chassis may not need to be sealed like today's devices.[99]

Coolant additive

Graphene's high thermal conductivity suggests that it could be used as an additive in coolants. Preliminary research work showed that 5% graphene by volume can enhance the thermal conductivity of a base fluid by 86%.[117] Another application due to graphene's enhanced thermal conductivity was found in PCR.[14]

Reference material

Graphene's properties suggest it as a reference material for characterizing electroconductive and transparent materials. One layer of graphene absorbs 2.3% of red light.[118]

This property was used to define the conductivity of transparency that combines sheet resistance and transparency. This parameter was used to compare materials without the use of two independent parameters.[119]

Thermal management

In 2011, researchers reported that a three-dimensional, vertically aligned, functionalized multilayer graphene architecture can be an approach for graphene-based thermal interfacial materials (TIMs) with superior thermal conductivity and ultra-low interfacial thermal resistance between graphene and metal.[120]

Graphene-metal composites can be utilized in thermal interface materials.[121]

Adding a layer of graphene to each side of a copper film increased the metal's heat-conducting properties up to 24%. This suggests the possibility of using them for semiconductor interconnects in computer chips. The improvement is the result of changes in copper’s nano- and microstructure, not from graphene’s independent action as an additional heat conducting channel. High temperature chemical vapor deposition stimulates grain size growth in copper films. The larger grain sizes improve heat conduction. The heat conduction improvement was more pronounced in thinner copper films, which is useful as copper interconnects shrink.[122]

Structural material

Graphene's strength, stiffness and lightness suggested it for use with carbon fiber. Graphene has been used as a reinforcing agent to improve the mechanical properties of biodegradable polymeric nanocomposites for engineering bone tissue.[123]

Catalyst

In 2014, researchers at The University of Western Australia discovered nano sized fragments of graphene can speed up the rate of chemical reactions.[124]

Footnotes

  1. ↑ Monie, Sanjay. "Developments in Conductive Inks". Industrial & Specialty Printing. Retrieved 2010-04-26.
  2. ↑ Geim, A. K.; Kim, P. (April 2008). "Carbon Wonderland". Scientific American. ... bits of graphene are undoubtedly present in every pencil mark
  3. ↑ Segal, M. (2009). "Selling graphene by the ton". Nature Nanotechnology 4 (10): 612–4. Bibcode:2009NatNa...4..612S. doi:10.1038/nnano.2009.279. PMID 19809441.
  4. ↑ Patel, P. (15 January 2009). "Bigger, Stretchier Graphene". MIT Technology Review.
  5. ↑ Bae, S. et al. (2010). "Roll-to-roll production of 30-inch graphene films for transparent electrodes". Nature Nanotechnology 5 (8): 574–578. Bibcode:2010NatNa...5..574B. doi:10.1038/nnano.2010.132. PMID 20562870.
  6. ↑ "EUROPA – PRESS RELEASES – Press Release – Graphene and Human Brain Project win largest research excellence award in history, as battle for sustained science funding continues". Europa.eu. 28 January 2013.
  7. ↑ Thomson, Iain. "Nokia shares $1.35bn EU graphene research grant". The Register.
    "FET Graphene Flagship". Graphene-flagship.eu. Retrieved 2013-08-24.
  8. ↑ Lalwani, G; Henslee, A. M.; Farshid, B; Lin, L; Kasper, F. K.; Qin, Y. X.; Mikos, A. G.; Sitharaman, B (2013). "Two-dimensional nanostructure-reinforced biodegradable polymeric nanocomposites for bone tissue engineering". Biomacromolecules 14 (3): 900–9. doi:10.1021/bm301995s. PMC 3601907. PMID 23405887.. Full Text PDF.
  9. ↑ Kanakia, S; Toussaint, J. D.; Chowdhury, S. M.; Lalwani, G; Tembulkar, T; Button, T; Shroyer, K. R.; Moore, W; Sitharaman, B (2013). "Physicochemical characterization of a novel graphene-based magnetic resonance imaging contrast agent". International Journal of Nanomedicine 8: 2821–33. doi:10.2147/IJN.S47062. PMC 3742530. PMID 23946653.. Full Text PDF
  10. ↑ Lalwani, G; Sundararaj, J. L.; Schaefer, K; Button, T; Sitharaman, B (2014). "Synthesis, Characterization, In Vitro Phantom Imaging, and Cytotoxicity of a Novel Graphene-Based Multimodal Magnetic Resonance Imaging - X-Ray Computed Tomography Contrast Agent". Journal of Materials Chemistry B 2 (22): 3519–3530. doi:10.1039/C4TB00326H. PMC 4079501. PMID 24999431.. Full Text PDF
  11. ↑ Lalwani, G; Cai, X; Nie, L; Wang, L. V.; Sitharaman, B (2013). "Graphene-based contrast agents for photoacoustic and thermoacoustic tomography". Photoacoustics 1 (3-4): 62–67. doi:10.1016/j.pacs.2013.10.001. PMC 3904379. PMID 24490141.. Full Text PDF
  12. ↑ Mullick Chowdhury, S; Lalwani, G; Zhang, K; Yang, J. Y.; Neville, K; Sitharaman, B (2013). "Cell specific cytotoxicity and uptake of graphene nanoribbons". Biomaterials 34 (1): 283–93. doi:10.1016/j.biomaterials.2012.09.057. PMC 3489471. PMID 23072942.. Full Text PDF
  13. ↑ Talukdar, Y; Rashkow, J. T.; Lalwani, G; Kanakia, S; Sitharaman, B (2014). "The effects of graphene nanostructures on mesenchymal stem cells". Biomaterials 35 (18): 4863–77. doi:10.1016/j.biomaterials.2014.02.054. PMC 3995421. PMID 24674462.. Full Text PDF
  14. ↑ 14.0 14.1 Abdul Khaliq, R; Kafafy, R.; Salleh, H. M.; Faris, W. F. (2012). "Enhancing the efficiency of polymerase chain reaction using graphene nanoflakes". Nanotechnology 23 (45): 455106. doi:10.1088/0957-4484/23/45/455106. PMID 23085573.
  15. ↑ Mohanty, Nihar; Berry, Vikas (2008). "Graphene-based Single-Bacterium Resolution Biodevice and DNA-Transistor – Interfacing Graphene-Derivatives with Nano and Micro Scale Biocomponents". Nano Letters 8 (12): 4469–76. Bibcode:2008NanoL...8.4469M. doi:10.1021/nl802412n. PMID 18983201.
  16. ↑ Donaldson, L. (2012). "Graphene: Invisible to water". Materials Today 15 (3): 82. doi:10.1016/S1369-7021(12)70037-8.
  17. ↑ Xu, M. S. Xu; Fujita, D.; Hanagata, N. (2009). "Perspectives and Challenges of Emerging Single-Molecule DNA Sequencing Technologies". Small 5 (23): 2638–49. doi:10.1002/smll.200900976. PMID 19904762.
  18. ↑ "Bill Gates condom challenge 'to be met' by graphene scientists". BBC News. 20 November 2013.
  19. ↑ Park, Dong-Wook, et. al. (20 October 2014). "Graphene-based carbon-layered electrode array technology for neural imaging and optogenetic applications". Nature Communications 5: 5258. doi:10.1038/ncomms6258. Retrieved December 2014.
  20. ↑ "Transparent graphene-based sensors open new window into the brain". KurzweilAI. October 21, 2014. Retrieved December 2014.
  21. ↑ Press Release (6 August 2014). "Surprise discovery could see graphene used to improve health". Monash University.
  22. ↑ Majumder, M; Tkacz, R; Oldenbourg, R; Mehta, S; Miansari, M; Verma, A (2014). "pH dependent isotropic to nematic phase transitions in graphene oxide dispersions reveal droplet liquid crystalline phases". Chemical Communications (Royal Society of Chemistry) 50 (50): 6668–6671. doi:10.1039/C4CC00970C. PMID 24828948.
  23. ↑ Press Release (6 January 2015). "’Flying Carpet’ Technique Uses Graphene to Deliver One-Two Punch of Anticancer Drugs". North Carolina State University.
  24. ↑ Gu, Zhen et al. (15 December 2014). "Furin-Mediated Sequential Delivery of Anticancer Cytokine and Small-Molecule Drug Shuttled by Graphene". Advanced Materials (Wiley-VCH Veriag GmbH K& Co.) 27: 1021–1028. doi:10.1002/adma.201404498.
  25. ↑ Jeffrey, Colin (March 25, 2015). "Robobug: Scientists clad bacterium with graphene to make a working cytobot". Gizmag. Retrieved March 2015.
  26. ↑ 26.0 26.1 Martin, Steve (18 September 2014). "Purdue-based startup scales up graphene production, develops biosensors and supercapacitors". Purdue University. Retrieved October 4, 2014.
  27. ↑ 27.0 27.1 "Startup scales up graphene production, develops biosensors and supercapacitors". R&D Magazine. 19 September 2014. Retrieved 4 October 2014.
  28. ↑ Chen, J.; Ishigami, M.; Jang, C.; Hines, D. R.; Fuhrer, M. S.; Williams, E. D. (2007). "Printed graphene circuits". Advanced Materials 19 (21): 3623–3627. doi:10.1002/adma.200701059.
  29. ↑ 29.0 29.1 Ponomarenko, L. A.; Schedin, F.; Katsnelson, M. I.; Yang, R.; Hill, E. W.; Novoselov, K. S.; Geim, A. K. (2008). "Chaotic Dirac Billiard in Graphene Quantum Dots". Science 320 (5874): 356–8. arXiv:0801.0160. Bibcode:2008Sci...320..356P. doi:10.1126/science.1154663. PMID 18420930. Lay summary.
  30. ↑ "Graphene transistors clocked at 26 GHz Arxiv article". Arxivblog.com. 11 December 2008.
  31. ↑ Wang, X.; Li, X.; Zhang, L.; Yoon, Y.; Weber, P. K.; Wang, H.; Guo, J.; Dai, H. (2009). "N-Doping of Graphene Through Electrothermal Reactions with Ammonia". Science 324 (5928): 768–71. Bibcode:2009Sci...324..768W. doi:10.1126/science.1170335. PMID 19423822. Lay summary.
  32. ↑ "Nanotechnology Information Center: Properties, Applications, Research, and Safety Guidelines". American Elements.
  33. ↑ Traversi, F.; Russo, V.; Sordan, R. (2009). "Integrated complementary graphene inverter". Appl. Phys. Lett. 94 (22): 223312. arXiv:0904.2745. Bibcode:2009ApPhL..94v3312T. doi:10.1063/1.3148342. Lay summary.
  34. ↑ "European collaboration breakthrough in developing graphene". NPL. 19 January 2010.
  35. ↑ Lin, Y.-M.; Dimitrakopoulos, C.; Jenkins, K. A.; Farmer, D. B.; Chiu, H.-Y.; Grill, A.; Avouris, Ph. (2010). "100-GHz Transistors from Wafer-Scale Epitaxial Graphene". Science 327 (5966): 662–662. arXiv:1002.3845. Bibcode:2010Sci...327..662L. doi:10.1126/science.1184289. PMID 20133565.
  36. ↑ Lin, Y.-M.; Valdes-Garcia, A.; Han, S.-J.; Farmer, D. B.; Meric, I.; Sun, Y.; Wu, Y.; Dimitrakopoulos, C.; Grill, A.; Avouris, P.; Jenkins, K. A. (2011). "Wafer-Scale Graphene Integrated Circuit". Science 332 (6035): 1294–1297. Bibcode:2011Sci...332.1294L. doi:10.1126/science.1204428. PMID 21659599.
  37. ↑ "Graphene circuit breaks the gigahertz barrier". 2013.
  38. ↑ "Carbon-Based Electronics: Researchers Develop Foundation for Circuitry and Devices Based on Graphite". 14 March 2006.
  39. ↑ Lemme, M. C.; Echtermeyer, Tim J. et al. (2007). "A graphene field-effect device". IEEE Electron Device Letters 28 (4): 282–284. arXiv:cond-mat/0703208. Bibcode:2007IEDL...28..282L. doi:10.1109/LED.2007.891668.
  40. ↑ Bullis, K. (28 January 2008). "Graphene Transistors". Cambridge: MIT Technology Review, Inc.
  41. ↑ Kedzierski, J.; Hsu, Pei-Lan; Healey, Paul; Wyatt, Peter W.; Keast, Craig L.; Sprinkle, Mike; Berger, Claire; De Heer, Walt A. (2008). "Epitaxial Graphene Transistors on SiC Substrates". IEEE Transactions on Electron Devices 55 (8): 2078–2085. arXiv:0801.2744. Bibcode:2008ITED...55.2078K. doi:10.1109/TED.2008.926593.
  42. ↑ Moon, J.S.; Curtis, D.; Hu, M.; Wong, D.; McGuire, C.; Campbell, P.M.; Jernigan, G.; Tedesco, J.L.; Vanmil, B.; Myers-Ward, R.; Eddy, C.; Gaskill, D.K. (2009). "Epitaxial-Graphene RF Field-Effect Transistors on Si-Face 6H-SiC Substrates". IEEE Electron Device Letters 30 (6): 650–652. Bibcode:2009IEDL...30..650M. doi:10.1109/LED.2009.2020699.
  43. ↑ Echtermeyer, Tim. J.; Lemme, M.C. et al. (2008). "Nonvolatile Switching in Graphene Field-Effect Devices". IEEE Electron Device Letters 29 (8): 952–954. arXiv:0805.4095. Bibcode:2008IEDL...29..952E. doi:10.1109/LED.2008.2001179.
  44. ↑ Sordan, R.; Traversi, F.; Russo, V. (2009). "Logic gates with a single graphene transistor". Appl. Phys. Lett. 94 (7): 073305. Bibcode:2009ApPhL..94g3305S. doi:10.1063/1.3079663.
  45. ↑ Fiori G., Iannaccone G., "On the possibility of tunable-gap bilayer graphene FET", IEEE Electr. Dev. Lett., 30, 261 (2009)
  46. ↑ Fiori G., Iannaccone G., "Ultralow-Voltage Bilayer graphene tunnel FET", IEEE Electr. Dev. Lett., 30, 1096 (2009)
  47. ↑ Bourzac, Katherine (5 February 2010). "Graphene Transistors that Can Work at Blistering Speeds". MIT Technology Review.
  48. ↑ "IBM shows off 100GHz graphene transistor". Techworld News. Retrieved 2010-12-10.
  49. ↑ Lin; Dimitrakopoulos, C; Jenkins, KA; Farmer, DB; Chiu, HY; Grill, A; Avouris, P (2010). "100-GHz Transistors from Wafer-Scale Epitaxial Graphene". Science (Science) 327 (5966): 662. arXiv:1002.3845. Bibcode:2010Sci...327..662L. doi:10.1126/science.1184289. PMID 20133565.
  50. ↑ Torrisi, F.; Hasan, T.; Wu, W.; Sun, Z.; Lombardo, A.; Kulmala, T.; Hshieh, G. W.; Jung, S. J.; Bonaccorso, F.; Paul, P. J.; Chu, D. P.; Ferrari, A. C. (2011). "Ink-Jet Printed Graphene Electronics". ACS Nano , (2012) (Cornell University Library) 6 (2992): 4970. arXiv:1111.4970. Bibcode:2011arXiv1111.4970T.
  51. ↑ Kawano, Yukio (2013). "Wide-band frequency-tunable terahertz and infrared detection with graphene". Nanotechnology 24 (21): 214004. Bibcode:2013Nanot..24u4004K. doi:10.1088/0957-4484/24/21/214004. PMID 23618878.
  52. ↑ Britnell, L.; Gorbachev, R. V.; Geim, A. K.; Ponomarenko, L. A.; Mishchenko, A.; Greenaway, M. T.; Fromhold, T. M.; Novoselov, K. S.; Eaves, L. (2013). "Radical new graphene design operates at terahertz speed". Nature Communications (KurzweilAI) 4 (4): 1794–. arXiv:1303.6864. Bibcode:2013NatCo...4E1794B. doi:10.1038/ncomms2817. PMC 3644101. PMID 23653206. Retrieved 2013-05-02.
    Britnell, L.; Gorbachev, R. V.; Geim, A. K.; Ponomarenko, L. A.; Mishchenko, A.; Greenaway, M. T.; Fromhold, T. M.; Novoselov, K. S.; Eaves, L. (2013). "Resonant tunnelling and negative differential conductance in graphene transistors". Nature Communications 4: 1794–. arXiv:1303.6864. Bibcode:2013NatCo...4E1794B. doi:10.1038/ncomms2817. PMC 3644101. PMID 23653206.
  53. ↑ Liu, Guanxiong; Ahsan, Sonia; Khitun, Alexander G.; Lake, Roger K.; Balandin, Alexander A. (2013). "Graphene-Based Non-Boolean Logic Circuits". Journal of Applied Physics 114 (10): 4310. arXiv:1308.2931. Bibcode:2013JAP...114o4310L. doi:10.1063/1.4824828.
  54. ↑ Bourzac, Katherine. "Superfast, Bendable Electronic Switches Made from Graphene | MIT Technology Review". Technologyreview.com. Retrieved 2013-08-24.
  55. ↑ 55.0 55.1 55.2 55.3 "How to change the crystal structure of graphene from metal to semiconductor". KurzweilAI. 2014-05-06. Retrieved 2014-06-15.
  56. ↑ Yankowitz, M.; Wang, J. I. J.; Birdwell, A. G.; Chen, Y. A.; Watanabe, K.; Taniguchi, T.; Jacquod, P.; San-Jose, P.; Jarillo-Herrero, P.; Leroy, B. J. (2014). "Electric field control of soliton motion and stacking in trilayer graphene". Nature Materials. doi:10.1038/nmat3965.
  57. ↑ Wang, X.; Zhi, L; Müllen, Klaus (2007). "Transparent, Conductive Graphene Electrodes for Dye-Sensitized Solar Cells". Nano Letters 8 (1): 323–7. Bibcode:2008NanoL...8..323W. doi:10.1021/nl072838r. PMID 18069877.
  58. ↑ Eda, G; Fanchini, G; Chhowalla, M (2008). "Large-area ultrathin films of reduced graphene oxide as a transparent and flexible electronic material". Nat Nanotechnol 3 (5): 270–4. doi:10.1038/nnano.2008.83. PMID 18654522.
  59. ↑ Wang, Yu; Chen, Xiaohong; Zhong, Yulin; Zhu, Furong; Loh, Kian Ping (2009). "Large area, continuous, few-layered graphene as anodes in organic photovoltaic devices". Applied Physics Letters 95 (6): 063302. Bibcode:2009ApPhL..95f3302W. doi:10.1063/1.3204698.
  60. ↑ Wu, J.B.; Agrawal, Mukul; Becerril, HéCtor A.; Bao, Zhenan; Liu, Zunfeng; Chen, Yongsheng; Peumans, Peter (2010). "Organic Light-Emitting Diodes on Solution-Processed Graphene Transparent Electrodes". ACS Nano 4: 43–48. doi:10.1021/nn900728d.
  61. ↑ Matyba, P.; Yamaguchi, H et al. (2010). "Graphene and Mobile Ions: The Key to All-Plastic, Solution-Processed Light-Emitting Devices". ACS Nano 4 (2): 637–42. doi:10.1021/nn9018569. PMID 20131906.
  62. ↑ Jeffrey, Colin (September 11, 2014). "First flexible graphene-based display created". Gizmag. Retrieved December 2014.
  63. ↑ Wang, H.; Nezich, D.; Kong, J.; Palacios, T. (2009). "Graphene Frequency Multipliers". IEEE Electr. Device. L. 30 (5): 547–549. doi:10.1109/LED.2009.2016443. Lay summary.
    Cricchio, D.; Corso, P. P.; Fiordilino, E.; Orlando, G.; Persico, F. (2009). "A paradigm of fullerene". J. Phys. B 42 (8): 085404. Bibcode:2009JPhB...42h5404C. doi:10.1088/0953-4075/42/8/085404.
  64. ↑ Kusmartsev, F. V.; Wu, W. M.; Pierpoint, M. P.; Yung, K. C. (2014). "Application of Graphene within Optoelectronic Devices and Transistors". arXiv:1406.0809 [cond-mat.mtrl-sci].
  65. ↑ Petruk, O.; Szewczyk, R.; Ciuk, T. et al. (2014). "Sensitivity and Offset Voltage Testing in the Hall-Effect Sensors Made of Graphene". Advances in Intelligent Systems and Computing. Advances in Intelligent Systems and Computing (Springer) 267: 631–640. doi:10.1007/978-3-319-05353-0_60. ISBN 978-3-319-05352-3.
  66. ↑ Mohanty, Nihar; Moore, David; Xu, Zhiping; Sreeprasad, T. S.; Nagaraja, Ashvin; Rodriguez, Alfredo A.; Berry, Vikas (2012). "Nanotomy Based Production of Transferrable and Dispersible Graphene-Nanostructures of Controlled Shape and Size". Nature Communications 3 (5): 844. Bibcode:2012NatCo...3E.844M. doi:10.1038/ncomms1834.
  67. ↑ Jinming, Cai; Ruffieux, Pascal; Jaafar, Rached; Bieri, Marco; Braun, Thomas; Blankenburg, Stephan; Muoth, Matthias; Seitsonen, Ari P.; Saleh, Moussa; Feng, Xinliang; Müllen, Klaus; Fasel, Roman (2010). "Atomically precise bottom-up fabrication of graphene nanoribbons". Nature 466 (7305): 470–473. Bibcode:2010Natur.466..470C. doi:10.1038/nature09211.
  68. ↑ Wang, Z. F.; Shi, Q. W.; Li, Q.; Wang, X.; Hou, J. G.; Zheng, H.; Yao, Yao; Chen, Jie (2007). "Z-shaped graphene nanoribbon quantum dot device". Applied Physics Letters 91 (5): 053109. arXiv:0705.0023. Bibcode:2007ApPhL..91e3109W. doi:10.1063/1.2761266.
  69. ↑ Fei, Huilong; Ye, Ruquan; Ye, Gonglan; Gong, Yongji; Peng, Zhiwei; Fan, Xiujun; Samuel, Errol L. G.; Ajayan, Pulickel M.; Tour, James M. (2014). "Boron- and Nitrogen-Doped Graphene Quantum Dots/Graphene Hybrid Nanoplatelets as Efficient Electrocatalysts for Oxygen Reduction". ACS Nano 8 (10): 141001091116007. doi:10.1021/nn504637y. ISSN 1936-0851.
  70. ↑ 70.0 70.1 Vasyl Skrypnychuk et al. (February 4, 2015). "Abstract of Enhanced vertical charge transport in a semiconducting P3HT thin film on single layer graphene". Advanced Functional Materials volume =25 issue =5 pp= 664–670. doi:10.1002/adfm.201403418.
  71. ↑ "Discovery could lead to more powerful graphene-based organic electronic devices". KurzweilAI. February 23, 2015. Retrieved March 2015.
  72. ↑ Liu, Ming; Yin; Xiaobo; Ulin-Avila; Erick; Geng; Baisong; Zentgraf; Thomas; Ju; Long; Wang; Feng; Zhang; Xiang (8 May 2011). "A graphene-based broadband optical modulator". Nature 474 (7349): 64–67. Bibcode:2011Natur.474...64L. doi:10.1038/nature10067. PMID 21552277.
  73. ↑ Scott, Cameron (March 29, 2014). "Contact Lenses with Infrared Vision? Ultra-thin Graphene Opens Up The Possibilities". Singularity Hub. Retrieved 2014-04-06.
  74. ↑ Nair, R. R.; Wu, H. A.; Jayaram, P. N.; Grigorieva, I. V.; Geim, A. K. (2012). "Unimpeded permeation of water through helium-leak-tight graphene-based membranes". Science 335 (6067): 442–4. arXiv:1112.3488. Bibcode:2012Sci...335..442N. doi:10.1126/science.1211694. PMID 22282806.
  75. ↑ Waugh, Rob. "Hi-tech 'wonder material' graphene has an unexpected use – it can distill vodka at room temperature". Daily Mail (London).
  76. ↑ Zhu, Shou-En; Yuan, Shengjun; Janssen, G. C. A. M. (1 October 2014). "Optical transmittance of multilayer graphene". EPL (Europhysics Letters) 108 (1): 17007. doi:10.1209/0295-5075/108/17007.
  77. ↑ 77.0 77.1 77.2 Mukhopadhyay, Prithu (2013). Graphite, Graphene and their Polymer Nanocomposites. Boca Raton, Florida: Taylor & Francis Group. pp. 202–213. ISBN 978-1-4398-2779-6.
  78. ↑ "Graphene-On-Silicon Schottky Junction Solar Cells". 9 April 2010. doi:10.1002/adma.200904383.
  79. ↑ Li, Xinming; Xie, Dan; Park, Hyesung; Zeng, Tingying Helen; Wang, Kunlin; Wei, Jinquan; Zhong, Minlin; Wu, Dehai; Kong, Jing; Zhu, Hongwei (19 April 2013). "Anomalous Behaviors of Graphene Transparent Conductors in Graphene–Silicon Heterojunction Solar Cells". Advanced Energy Materials 3 (8): 1029–1034. doi:10.1002/aenm.201300052.
    "Ion doping of graphene for high-efficiency heterojunction solar cells". 3 January 2013.
  80. ↑ "Role of Interfacial Oxide in High-Efficiency Graphene–Silicon Schottky Barrier Solar Cells". 16 February 2015.
  81. ↑ "Graphene-based solar cell hits record 15.6 percent efficiency". Gizmag.com. Retrieved 2014-01-23.
    Wang, J. T. W.; Ball, J. M.; Barea, E. M.; Abate, A.; Alexander-Webber, J. A.; Huang, J.; Saliba, M.; Mora-Sero, I. N.; Bisquert, J.; Snaith, H. J.; Nicolas, R. J. (2013). "Low-temperature processed electron collection layers of Graphene/TiO2 nanocomposites in thin film perovskite solar cells". Nano Letters 14 (2): 724–730. doi:10.1021/nl403997a.
  82. ↑ "Graphene organic photovoltaics: Flexible material only a few atoms thick may offer cheap solar power". ScienceDaily. 24 July 2010.
    Walker, Sohia (4 August 2010). "Use of graphene photovoltaics as alternate source of energy". Computer Talks.
  83. ↑ inhabitat.com cooperating with ICFO (Institute of Photonic Sciences)(2013-04-03)
  84. ↑ 84.0 84.1 84.2 "Protons found to pass through graphene, raising hopes for efficient fuel cells". KurzweilAI. December 1, 2014. Retrieved December 2014.
  85. ↑ Hu, S.; Lozada-Hidalgo, M.; Wang, F. C.; Mishchenko, A.; Schedin, F.; Nair, R. R.; Hill, E. W.; Boukhvalov, D. W.; Katsnelson, M. I.; Dryfe, R. A. W.; Grigorieva, I. V.; Wu, H. A.; Geim (November 26, 2014). "Proton transport through one-atom-thick crystals". Nature 516: 227–230. doi:10.1038/nature14015. Retrieved December 2014. |first13= missing |last13= in Authors list (help)
  86. ↑ "Imperfect graphene may lead to fast-charging batteries for vehicles". March 17, 2015. Retrieved April 2015.
  87. ↑ Achtyl, Jennifer L.; Unocic, Raymond R.; Xu, Lijun; Cai, Yu; Raju, Muralikrishna; Zhang, Weiwei; Sacci, Robert L.; Vlassiouk, Ivan V.; Fulvio, Pasquale F.; Ganesh, Panchapakesan; Wesolowski, David J.; Dai, Sheng; Duin, Adri C. T. van; Neurock, Matthew; Geiger, Franz M. (17 March 2015). "Aqueous proton transfer across single-layer graphene". Nature Communications 6. doi:10.1038/ncomms7539.
  88. ↑ Stoller, Meryl D.; Park, Sungjin; Zhu, Yanwu; An, Jinho; Ruoff, Rodney S. (2008). "Graphene-Based Ultracapacitors" (PDF). Nano Lett 8 (10): 3498–502. Bibcode:2008NanoL...8.3498S. doi:10.1021/nl802558y. PMID 18788793.
  89. ↑ Malasarn, Davin (19 February 2013). "UCLA researchers develop new technique to scale up production of graphene micro-supercapacitors / UCLA Newsroom". Newsroom.ucla.edu.
  90. ↑ Williams, Mike (2015-01-14). "Laser-induced graphene "super" for electronics". R&D Magazine. Retrieved 2015-02-20.
  91. ↑ "Flexible 3D graphene supercapacitors may power portables and wearables". Kurzweil Accelerating Intelligence. February 9, 2015. Retrieved April 2015.
  92. ↑ Mason, Shaun (04/01/2015). "Quick-charging hybrid supercapacitors". R&D. Check date values in: |date= (help);
  93. ↑ Maher F. El-Kadya,b, Melanie Ihnsa, Mengping Lia, Jee Youn Hwanga, Mir F. Mousavia,c, Lindsay Chaneya, Andrew T. Lecha, and Richard B. Kaner (March 4, 2015). "Engineering three-dimensional hybrid supercapacitors and microsupercapacitors for high-performance integrated energy storage". PNAS. Retrieved April 2015.
  94. ↑ David, L.; Bhandavat, R.; Kulkarni, G.; Pahwa, S.; Zhong, Z.; Singh, G. (2013). "Synthesis of Graphene Films by Rapid Heating and Quenching at Ambient Pressures and Their Electrochemical Characterization". ACS Applied Materials & Interfaces 5 (3): 546. doi:10.1021/am301782h.
    "Fabrication and Electrochemical Characterization of Single and Multi-Layer Graphene Anodes for Lithium-Ion Batteries". Jes.ecsdl.org. Retrieved 2013-06-24.
  95. ↑ Yao, F.; Güneş, F.; Ta, H. Q.; Lee, S. M.; Chae, S. J.; Sheem, K. Y.; Cojocaru, C. S.; Xie, S. S.; Lee, Y. H. (2012). "Diffusion Mechanism of Lithium Ion through Basal Plane of Layered Graphene". Journal of the American Chemical Society 134 (20): 8646–8654. doi:10.1021/ja301586m. PMID 22545779.
  96. ↑ Johnson, Dexter (17 January 2013). "Faster and Cheaper Process for Graphene in Li-ion Batteries – IEEE Spectrum". Spectrum.ieee.org.
  97. ↑ Johnson, Dexter (21 March 2012). "Graphene-Silicon Anodes for Li-ion Batteries Go Commercial – IEEE Spectrum". Spectrum.ieee.org.
    "XGS presents new silicon-graphene anode materials for lithium-ion batteries". Phys.org. Retrieved 2014-02-26.
  98. ↑ "Nanoscale graphene origami cages set world record for densest hydrogen storage". KurzweilAI. Retrieved 2014-04-05.
    Zhu, S.; Li, T. (2014). "Hydrogenation-Assisted Graphene Origami and Its Application in Programmable Molecular Mass Uptake, Storage, and Release". ACS Nano 8 (3): 2864–72. doi:10.1021/nn500025t. PMID 24564284.
  99. ↑ 99.0 99.1 5 Ways Graphene Will Change Gadgets Forever, Laptop, 14 April 2014, Michael Andronico
  100. ↑ Dan, Yaping; Lu, Ye; Kybert, Nicholas J.; Luo, Zhengtang; Johnson, A. T. Charlie (April 2009). "Intrinsic Response of Graphene Vapor Sensors". Nano Letters 9 (4): 1472–1475. arXiv:0811.3091. Bibcode:2009NanoL...9.1472D. doi:10.1021/nl8033637. PMID 19267449.
  101. ↑ Schedin, F.; Geim, A. K.; Morozov, S. V.; Hill, E. W.; Blake, P.; Katsnelson, M. I.; Novoselov, K. S. (2007). "Detection of individual gas molecules adsorbed on graphene". Nature Materials 6 (9): 652–655. Bibcode:2007NatMa...6..652S. doi:10.1038/nmat1967. PMID 17660825.
  102. ↑ "Straintronics: Stanford engineers create piezoelectric graphene". Stanford University. 3 April 2012.
    Ong, M.; Reed, Evan J. (2012). "Engineered Piezoelectricity in Graphene". ACS Nano 6 (2): 1387–94. doi:10.1021/nn204198g. PMID 22196055.
  103. ↑ Boland, C. S.; Khan, U.; Backes, C.; o’Neill, A.; McCauley, J.; Duane, S.; Shanker, R.; Liu, Y.; Jurewicz, I.; Dalton, A. B.; Coleman, J. N. (2014). "Sensitive, High-Strain, High-Rate Bodily Motion Sensors Based on Graphene–Rubber Composites". ACS Nano: 140819080104000. doi:10.1021/nn503454h.
  104. ↑ 104.0 104.1 104.2 "Graphene Oxide for Nuclear Decontamination". Institute of Science In Society. 17/07/13. Retrieved February 2015. Check date values in: |date= (help)
  105. ↑ Cohen-Tanugi, David; Grossman, Jeffrey C. (2012). "Water Desalination across Nanoporous Graphene". Nano Letters 12 (7): 3602–3608. Bibcode:2012NanoL..12.3602C. doi:10.1021/nl3012853. PMID 22668008.
  106. ↑ Chen, J.; Badioli, M.; Alonso-González, P.; Thongrattanasiri, S.; Huth, F.; Osmond, J.; Spasenović, M.; Centeno, A.; Pesquera, A.; Godignon, P.; Zurutuza Elorza, A.; Camara, N.; De Abajo, F. J. G. A.; Hillenbrand, R.; Koppens, F. H. L. (2012). "Optical nano-imaging of gate-tunable graphene plasmons". Nature. doi:10.1038/nature11254.
  107. ↑ Fei, Z.; Rodin, A. S.; Andreev, G. O.; Bao, W.; McLeod, A. S.; Wagner, M.; Zhang, L. M.; Zhao, Z.; Thiemens, M.; Dominguez, G.; Fogler, M. M.; Neto, A. H. C.; Lau, C. N.; Keilmann, F.; Basov, D. N. (2012). "Gate-tuning of graphene plasmons revealed by infrared nano-imaging". Nature. doi:10.1038/nature11253.
  108. ↑ Yan, H.; Low, T.; Zhu, W.; Wu, Y.; Freitag, M.; Li, X.; Guinea, F.; Avouris, P.; Xia, F. (2013). "Damping pathways of mid-infrared plasmons in graphene nanostructures". Nature Photonics 7 (5): 394. doi:10.1038/nphoton.2013.57.
  109. ↑ Low, T.; Avouris, P. (2014). "Graphene Plasmonics for Terahertz to Mid-Infrared Applications". ACS Nano 8 (2): 1086. doi:10.1021/nn406627u. PMID 24484181.
  110. ↑ Graphene proves a long-lasting lubricant, Phys.org, 14 October 2014, Jared Sagoff
  111. ↑ "Graphene found to efficiently absorb radio waves". KurzweilAI. Retrieved 2014-02-26.
  112. ↑ Wu, B.; Tuncer, H. M.; Naeem, M.; Yang, B.; Cole, M. T.; Milne, W. I.; Hao, Y. (2014). "Experimental demonstration of a transparent graphene millimetre wave absorber with 28% fractional bandwidth at 140 GHz". Scientific Reports 4. doi:10.1038/srep04130.
  113. ↑ Ekiz, O.O.; Urel, M et al. (2011). "Reversible Electrical Reduction and Oxidation of Graphene Oxide". ACS Nano 5 (4): 2475–2482. doi:10.1021/nn1014215. PMID 21391707.
    Ekiz, O.O.; Urel, M et al. (2011). "Supporting information for Reversible Electrical Reduction and Oxidation of Graphene Oxide". ACS Nano 5 (4): 2475–2482. doi:10.1021/nn1014215. PMID 21391707.
  114. ↑ 114.0 114.1 114.2 Dodson, Brian (February 3, 2014). "Graphene-based nano-antennas may enable cooperating smart dust swarms". Gizmag.com. Retrieved 2014-04-06.
  115. ↑ 115.0 115.1
  116. ↑ "World’s first graphene speaker already superior to Sennheiser MX400". Gizmag.com. 2014-04-16. Retrieved 2014-04-24.
  117. ↑ Yu, W.; Xie, H.; Wang, X.; Wang, X. (2011). "Significant thermal conductivity enhancement for nanofluids containing graphene nanosheets". Physics Letters A 375 (10): 1323. doi:10.1016/j.physleta.2011.01.040.
  118. ↑ Nair, R. R.; Blake, P.; Grigorenko, A. N.; Novoselov, K. S.; Booth, T. J.; Stauber, T.; Peres, N. M. R.; Geim, A. K. (2008). "Fine Structure Constant Defines Visual Transparency of Graphene". Science 320 (5881): 1308. Bibcode:2008Sci...320.1308N. doi:10.1126/science.1156965. PMID 18388259.
  119. ↑ Eigler, S. (2009). "A new parameter based on graphene for characterizing transparent, conductive materials". Carbon 47 (12): 2936–2939. doi:10.1016/j.carbon.2009.06.047.
  120. ↑ Liang, Qizhen; Yao, Xuxia; Wang, Wei; Liu, Yan; Wong, Ching Ping (2011). "A Three-Dimensional Vertically Aligned Functionalized Multilayer Graphene Architecture: An Approach for Graphene-Based Thermal Interfacial Materials". ACS Nano 5 (3): 2392–2401. doi:10.1021/nn200181e. PMID 21384860.
  121. ↑ Amini, Shaahin; Garay, Javier; Liu, Guanxiong; Balandin, Alexander A.; Abbaschian, Reza (2010). "Growth of Large-Area Graphene Films from Metal-Carbon Melts". Journal of Applied Physics 108 (9): 094321. arXiv:1011.4081. Bibcode:2010JAP...108i4321A. doi:10.1063/1.3498815.
  122. ↑ Nealon, Sean (March 12, 2014). "Graphene-copper sandwich may improve, shrink electronics". Rdmag.com. Retrieved 2014-04-06.
  123. ↑ Lalwani, G; Henslee, A. M.; Farshid, B; Lin, L; Kasper, F. K.; Qin, Y. X.; Mikos, A. G.; Sitharaman, B (2013). "Two-dimensional nanostructure-reinforced biodegradable polymeric nanocomposites for bone tissue engineering". Biomacromolecules 14 (3): 900–9. doi:10.1021/bm301995s. PMC 3601907. PMID 23405887.
  124. ↑ Research unlocks potential of super-compound, Phys.org, 22 October 2014, David Stacey