Room temperature quantum hall effect in graphene pdf

We have observed the wellkown quantum hall effect qhe in epitaxial graphene grown on silicon carbide sic by using, for the first time, only commercial ndfeb permanent magnets at low temperature. Another indication of graphene s extreme electronic quality is the quantum hall effect, which can be observed even at room temperature 59, 60, 61,9,62,63. The structure of graphene gives it unique properties such as high theoretical area ratio,31 high carrier mobility at room temperature,30 quantum hall effect, high youngsmodulus,32 and. Model for a quantum hall effect without landau levels. Conference series, volume 568, 27th international conference on low temperature physics lt27 6 august 2014, buenos aires. Quantum hall effect in epitaxial graphene with permanent. Furthermore, their robust plateau plateau transitions allow study of the possible quantum phase transitions in the epitaxial graphene system. Graphene was also the first material in which a member of the marked class of macroscopic quantum phenomena 47, the quantum hall effect qhe, could be observed at room temperature when subject to large magnetic fields. Gatetunable reversible rashbaedelstein effect in a few. Evidence for a quantum spin hall phase in graphene. We experimentally and theoretically study artificially enhanced spinorbit coupling in graphene via.

Robust room temperature quantum spin hall effect in methylfunctionalized inbi honeycomb film shengshi li, 1, 2 weixiao ji, 1 changwen zhang, a, 1 shujun hu, 2 ping li, 1 peiji wang, 1 baomin zhang, 1 and chonglong cao 1. Among many remarkable qualities of graphene, its electronic properties attract particular interest due to a massless chiral character of charge carriers, which leads to such unusual phenomena as metallic conductivity in the limit of no carriers and the halfinteger quantum hall effect qhe observable even at room temperature. Graphene s exceptionally weak spinorbit couplingstemming from carbons low massposes the primary obstacle. Particle exchange and fractional statistics the quantum hall e ect is only observed in twodimensional. Graphene synthesis, characterization and its applications. Its quality is markedly different from conventional graphite and semiconductor material. We report the observation of currentinduced spin polarization, the rashbaedelstein effect ree, and its onsager reciprocal phenomenon, the spin galvanic effect sge, in a fewlayer graphene 2htas2 heterostructure at room temperature. Quantum spin hall effect at room temperature in stanene. Recent developments in graphenebased polymer composite. Correlated electron systems high field magnet laboratory hfml year. Topological insulators tis 1,2,3,4 have generated intensive research and engineering activities in recent years, because they give an alternative and robust platform for obtaining relativistic and spinpolarized fermions in the condensed matter system. Topological insulators tis represent a new quantum state of matter characterized by robust gapless states inside the insulating bulk gap. The quantization of electrical and thermal conductance in.

In addition, the quantum hall effect has been observed in graphene at a relatively low magnetic. One of the most interesting phenomena in this realm is the quantum spin hall qsh effect in twodimensional 2d structures 1,2, characterized by an insulating bulk and gapless edge states at its boundaries due to timereversal symmetry trs, thus providing enticing concepts for novel quantum devices with low energy dissipation 3,4. Halfinteger quantum hall effect singlelayer graphene. Tutuc1, 1microelectronics research center, the university of texas at austin, austin, texas 78758, usa. The signature of qhe is the quantization plateaus in the hall resistance rxy and vanishing magnetoresistance rxx in a magnetic field. Graphene is a twodimensional carbon material with only one carbon atom thickness. Currently, most known 2d tis are based on a hexagonal specifically, honeycomb. Quantum hall effect observed at room temperature 15 february 2007 this image is a scanning electron microscope micrograph of a strongly crumpled graphene sheet on a. In 2007, the integer quantum hall effect was reported in graphene at temperatures as high as room temperature, and in the magnesium zinc oxide znomg x zn 1. Room temperature straininduced landau levels in graphene on. In the quantum hall state, the bulk of the 2deg is insulating and the. The metallic edge states of a twodimensional 2d ti, known as the quantum spin hall qsh effect, are immune to backscattering and carry fully spinpolarized dissipationless currents. The qhe, exclusive to twodimensional 2d metals, has elucidated many important aspects of quantum physics and has deepened our.

Halfinteger quantum hall effect in graphene exceptionally high mobility graphene samples allow us to investigate transport phenomena in the magnetic quantum limit where the qhe manifests itself. Topological insulators are electrically insulating on the inside, but along a thin layer on the outside of the ti, they are perfect conductors. Room temperature straininduced landau levels in graphene. Quantumhall plateauplateau transition in topgated epitaxial. Its charge carriers exhibit intrinsic mobility and can travel micrometerlong distances without scattering at room temperature. The hall conductivity is quantized at halfinter values of 4e 2 h. We studied the breakdown of the quantum hall state in graphene with twofold motivation. Roomtemperature quantum hall effect in graphene arxiv. Twodimensional 2d topological insulators tis, also known as quantum spin hall qsh insulators, are excellent candidates for coherent spin transport related applications because the edge states of 2d tis are robust against nonmagnetic impurities since the only available backscattering channel is forbidden. Room temperature quantum spin hall insulators with a. The unique halfinteger quantum hall effect qhe in monolayer graphene serves as a. Graphene synthesis, characterization and its applications in. Firstly, in graphene the cyclotron gaps are unequally spaced and are much larger than that of a 2dimensional electron gas 2deg at a given magnetic eld, which make it possible to observe the qhe even at room temperature 4.

May 27, 20 the unusual quantum hall effect qhe in graphene is often discussed in terms of dirac fermions moving with a linear dispersion relation. Room temperature quantum hall effect in graphene nasaads. Quantum hall effect an overview sciencedirect topics. Our work demonstrates the feasibility of exploiting straininduced macroscopic quantum phases and. Roomtemperature quantum hall effect in graphene core. Due to its fantastic features such as high mobility, optical transparency, room temperature quantum hall effect, mechanical stiffness, etc. Energy gaps and a zerofield quantum hall effect in graphene. Qhe plateaus observed at landau level spectrum with very high cyclotron energy k bilayer novoselov et al, 2005, zhang et al, 2005 manifestation of relativistic dirac electron properties 42x2 spin and valley degeneracy recently. Therefore it is a promising candidate for a high temperature quantum resistance standard 9 for metrology applications.

The qhe is exclusive to twodimensional 2d metals and has elucidated many important aspects of quantum physics and deepened our understanding of interacting systems. Zerogap semiconductor graphene, for example, is a proven test system for twodimensional 2d charge carrier dynamics in which ballistic transport and quantum hall effect occur at room temperature1. By performing spin precession experiments in appropriately. Columbia university kostya novoselov zhigang jiang horst stormer yuanbo zhang sergey morozov uli zeitler. Quantum hall e ect and electromechanics in graphene.

Roomtemperature quantum hall effect in graphene science. Room temperature straininduced quantum hall effect in. Therefore, we describe graphene electrons at a strong magnetic. Disappointingly, however, the qhe has been observed only at liquid. The inset shows the hall conductivity for bilayer graphene. Graphenebased topological insulator with an intrinsic bulk. Graphenes exceptionally weak spinorbit couplingstemming from carbons low massposes the primary obstacle. Jan 14, 2008 halfinteger quantum hall effect singlelayer graphene. Helical quantum hall phase in graphene on strontium titanate. Roomtemperature quantum hall effect in graphene nasaads. Roomtemperature quantum hall effect high field magnet. Energy gaps, topological insulator state and zerofield. Here, we demonstrate strongly enhanced room temperature spintocharge interconversion in graphene driven by the proximity of ws 2.

Ks novoselov, z jiang, y zhang, sv morozov, hl stormer, u. Graphene, a single atomic layer of carbon arranged in a honeycomb lattice, holds great. Apr 12, 2018 the quantum spin hall effect is a similar but also subtly different state which can arise in certain materials which are often called topological insulators. Energy gaps and a zerofield quantum hall effect in. Disappointingly, however, the qhe has been observed. The same phenomenon will be explained in terms of the more. Quantum hall effect in bernal stacked and twisted bilayer. Note that the spacing between plateaus for graphene is 4e 2 h, i. Ngi, npl and oxford instruments collaborate to develop a. It has also led to the establishment of a new metrological standard, the resistance quantum. Evidence for a quantum spin hall phase in graphene decorated. The quantum hall qh effect in twodimensional electron and hole gas is studied in high quality graphene samples.

Experimental observation of quantum hall effect and berrys phase in graphene by yuanbo zhang 2005 experimental observation of the quantum anomalous hall effect in a magnetic topological insulator by qikun xue, shoucheng zhang 20 attempts to extend haldane model to explain fractional quantum hall effect quantum spin hall effect. The halfinteger quantum hall effect qhe, a hallmark of the 2d dirac fermions in graphene, is welldeveloped in these gated epitaxial graphene samples. Robust roomtemperature quantum spin hall effect in methyl. Tunable roomtemperature spin galvanic and spin hall. Room temperature quantum spin hall insulator in ethynyl. A collaborative project between oxford instrument, the national physical laboratory npl and the national graphene institute ngi at university of manchester for a turnkey quantum hall system for graphene characterization and primary resistance metrology has been successfully completed the project has been partially funded by the innovate uk for development of commercial measurement. Graphene, showing fascinating characteristics of the quantum hall effect at room temperature, extremely high carrier mobility, ambipolar field effect, and sensitive response to single molecules, has become one of the hottest research topics in recent years. Experimental observation of the quantum hall effect and berrys phase in graphene. Hall effect and a nonzero berrys phase have been discovered in graphene. Transitionmetal dichalcogenides imprint their strong spinorbit coupling into graphene via the proximity effect, and it has been predicted that efficient spintocharge conversion due to spin hall and rashbaedelstein effects could be achieved. Graphene is a twodimensional material consisting of single atomic layers of graphite. Surprisingly, this theory implies that the conductance and resistance of a nanostructure is independent of its material and temperature, and only depends on the dimensions of the sample, changing in a stepwise manner with a step of h2e 2 representing the conductance quantum. Graphene is an excellent material for longdistance spin transport but allows little spin manipulation. Experiment results the quantum hall effect qhe is one example of a quantum phenomenon that occurs on a truly macroscopic scale.

Left the hall conductivity red and the longitudinal resistivity green as a function of carrier density. The quantum hall effect qhe is an example of those few quantum phenomena that occur on a truly macroscopic scale, and it has been attracting intense interest since its discovery in 1980. Published 8 december 2014 published under licence by iop publishing ltd journal of physics. The quantum hall effect qhe, one example of a quantum phenomenon thatoccurs on a truly macroscopic scale, has been attracting intense interest since its discovery in 1980 1. Geim1 t he quantum hall effect qhe, one example of a quantum phenomenon that occurs on a truly macroscopic scale, has been attracting intense interest since. Both of these e ects have since been observed in graphene, a single layer of carbon atoms in a hexagonal lattice, at room temperature. Observation of quantumhall effect in gated epitaxial. One of the most interesting phenomena in this realm is the quantum spin hall qsh effect in twodimensional 2d structures 1,2. The strain described by 2 and its crystallographic alignment are shown in fig. Spinsensitive electrical measurements unveil full spinpolarization reversal by an applied gate voltage. Their combined citations are counted only for the first article. At low temperatures, the quantumhall effect in hall resistance is observed along with pronounced shubnikovde haas oscillations in diagonal magnetoresistance of gated epitaxial graphene on sic 0001. Roomtemperature quantumconfined stark effect in atomically. Graphene s quantum hall effect in magnetic fields above 10 teslas or so reveals.

The quantum hall effect qhe is an example of those few quantum phenomena that occur on a truly macroscopic scale, and it has. Spin coherence length above 1 micrometre at room temperature was observed, and control of the spin current polarity with an electrical gate was observed at low temperature. Pdf roomtemperature quantum hall effect in graphene. Helical edge states and fractional quantum hall effect in a graphene electronhole bilayer, nature nanotechnology 2016. The quantum hall effect qhe, one example of a quantum phenomenon that occurs on a truly macroscopic scale, has been attracting intense interest since its discovery in 1980 1. Quantum anomalous hall effect in graphene coupled to.

Quantum hall effect in bernal stacked and twisted bilayer graphene grown on cu by chemical vapor deposition. The quantum hall effect qhe, one example of a quantum phenomenon that occur on a truly macroscopic scale, has been attracting intense interest since its discovery in 1980 and has helped elucidate many important aspects of quantum physics. Novoselov ks1, jiang z, zhang y, morozov sv, stormer hl, zeitler u, maan jc, boebinger gs, kim p, geim ak. Figure 4 experimental observation of the unusual quantum hall effect in graphene. Realization of the quantum spin hall effect in graphene devices has remained an outstanding challenge dating back to the inception of the field of topological insulators. Efforts to extend the qhe temperature range by using semiconductors with small effective masses of.

The mobility of the exfoliated graphene could be as high as 200000 cm 2 v. Room temperature quantum hall effect in graphene k. The quantum hall e ect in graphene physics department. Disappointingly, however, the qhe could only have been. We experimentally and theoretically study artificially enhanced spinorbit coupling in graphene via random. Roomtemperature quantum hall effect in graphene iopscience. Quantum hall effect in bernal stacked and twisted bilayer graphene grown on cu by chemical vapor deposition babak fallahazad, 1yufeng hao,2 kayoung lee, seyoung kim,1 r. Researchers at the university of manchester in the uk have discovered that the hall effect a phenomenon well known for more than a centuryis no longer as universal as it was thought to be. Roomtemperature quantum hall effect in graphene article pdf available in science 3155817.

As many other quantum phenomena, the observation of the qhe requires temperatures t typically below 4k. In the quantum hall state, charge carriers are forced into cyclotron orbits with quantized radii and energies known as. Although, the conclusive evidence for collective behaviour of electrons in graphene is lacking so far, recently scientists have observed the fractional quantum hall effect fqhe in graphene experimentally. Citeseerx document details isaac councill, lee giles, pradeep teregowda. Quantum hall effect in graphene with twisted bilayer stripe.

577 1153 928 380 1140 644 1573 213 987 1508 1531 362 47 1191 740 695 377 1165 817 641 1071 256 539 922 1385 233 1171 1176 464 415 976 445 456 181 289 303 1394 98 132