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A self-consistent theory for graphene transport
We demonstrate theoretically that most of the observed transport properties of graphene sheets at zero magnetic field can be explained by scattering from charged impurities. We find that, contrary toExpand
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Majorana fermions and a topological phase transition in semiconductor-superconductor heterostructures.
We propose and analyze theoretically an experimental setup for detecting the elusive Majorana particle in semiconductor-superconductor heterostructures. The experimental system consists ofExpand
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Generic new platform for topological quantum computation using semiconductor heterostructures.
We show that a film of a semiconductor in which s-wave superconductivity and Zeeman splitting are induced by the proximity effect, supports zero-energy Majorana fermion modes in the ordinary vortexExpand
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High temperature ferromagnetism with a giant magnetic moment in transparent co-doped SnO(2-delta).
The occurrence of room temperature ferromagnetism is demonstrated in pulsed laser deposited thin films of Sn(1-x)Co(x)O(2-delta) (x<0.3). Interestingly, films of Sn(0.95)Co(0.05)O(2-delta) grown onExpand
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Measurement of scattering rate and minimum conductivity in graphene.
The conductivity of graphene samples with various levels of disorder is investigated for a set of specimens with mobility in the range of 1-20x10(3) cm2/V sec. Comparing the experimental data withExpand
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Collective modes of the massless dirac plasma.
We develop a theory for the long-wavelength plasma oscillation of a collection of charged massless Dirac particles in a solid, as occurring, for example, in doped graphene layers, interacting via theExpand
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Tuning the effective fine structure constant in graphene: opposing effects of dielectric screening on short- and long-range potential scattering.
We reduce the dimensionless interaction strength alpha in graphene by adding a water overlayer in ultrahigh vacuum, thereby increasing dielectric screening. The mobility limited by long-rangeExpand
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Topologically protected qubits from a possible non-Abelian fractional quantum Hall state.
The Pfaffian state is an attractive candidate for the observed quantized Hall plateau at a Landau-level filling fraction nu=5/2. This is particularly intriguing because this state has unusualExpand
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Polaron percolation in diluted magnetic semiconductors.
We theoretically study the development of spontaneous magnetization in diluted magnetic semiconductors as arising from a percolation of bound magnetic polarons. Within the framework of a generalizedExpand
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Why does graphene behave as a weakly interacting system?
We address the puzzling weak-coupling perturbative behavior of graphene interaction effects as manifested experimentally, in spite of the effective fine structure constant being large, by calculatingExpand
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