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11.
Castro EV Novoselov KS Morozov SV Peres NM dos Santos JM Nilsson J Guinea F Geim AK Neto AH 《Physical review letters》2007,99(21):216802
We demonstrate that the electronic gap of a graphene bilayer can be controlled externally by applying a gate bias. From the magnetotransport data (Shubnikov-de Haas measurements of the cyclotron mass), and using a tight-binding model, we extract the value of the gap as a function of the electronic density. We show that the gap can be changed from zero to midinfrared energies by using fields of less, approximately < 1 V/nm, below the electric breakdown of SiO2. The opening of a gap is clearly seen in the quantum Hall regime. 相似文献
12.
Novoselov KS 《Angewandte Chemie (International ed. in English)》2011,50(31):6986-7002
Much like the world described in Abbott's "Flatland", graphene is a two-dimensional object. And, as "Flatland" is "A Romance of Many Dimensions", graphene is much more than just a flat crystal. It possesses a number of unusual properties which are often unique or superior to those in other materials. In this brief lecture I would like to explain the reason for my (and many other people's) fascination with this material, and invite the reader to share some of the excitement I've experienced while researching it. 相似文献
13.
Solutions of fibroin-poly-3-hydroxybutyrate polymer blends in hexafluoro-2-propanol and films obtained after removal of the solvent are experimentally studied at various polymer ratios.__________Translated from Zhurnal Prikladnoi Khimii, Vol. 78, No. 1, 2005, pp. 155–160.Original Russian Text Copyright © 2005 by Sashina, Novoselov, Heinemann. 相似文献
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E.V. Kurganova A.J.M. Giesbers R.V. Gorbachev A.K. Geim K.S. Novoselov J.C. Maan U. Zeitler 《Solid State Communications》2010,150(45-46):2209-2211
We have measured the quantum Hall activation gaps in bilayer graphene at filling factors and in high magnetic fields up to 30 T. We find that energy levels can be described by a 4-band relativistic hyperbolic dispersion. The Landau level width is found to contain a field independent background due to an intrinsic level broadening and a component which increases linearly with magnetic field. 相似文献
18.
A. M. Potapova G. V. Zimina I. N. Smirnova A. V. Novoselov F. M. Spiridonov S. Yu. Stefanovich 《Russian Journal of Inorganic Chemistry》2008,53(2):174-180
Subsolidus sections in the systems Li3PO4-InPO4 (950°C) and Na3PO4-InPO4 (800, 900, and 1000°C) have been studied by X-ray powder diffraction. The compound Li3In(PO4)2 has been synthesized, and the nasicon-type solid solution Li3(1 ? x)In2 + x(PO4)3 (0.67 ≤ x ≤ 0.80). has been found to exist. In the system Na3PO4-InPO4, the solid solution Na3(1 ? x)Inx/3PO4 (0 ≤ x ≤ 0.2) and two complex phosphates exist: Na3In(PO4)2 and Na3In2(PO4)3. These complex phosphates are dimorphic, with the irreversible-transition temperature equal to 675 and 820°C, respectively. Na3In(PO4)2 degrades at 920°C. Ionic conductivity has been measured in some phases in the system. 相似文献
19.
Yu. N. Khanin E. E. Vdovin A. Mishchenko J. S. Tu A. Kozikov R. V. Gorbachev K. S. Novoselov 《JETP Letters》2016,103(5):334-340
The spectral and total electron densities of states in two-dimensional FeAs clusters, which simulate iron-based superconductors, have been calculated using the generalized quantum Monte Carlo algorithm within the full two-orbital model. Spectra have been reconstructed by solving the integral equation relating the Matsubara Green’s function and spectral density by the method combining the gradient descent and Monte Carlo algorithms. The calculations have been performed for clusters with dimensions up to 10 × 10 FeAs cells. The profiles of the Fermi surface for the entire Brillouin zone have been presented in the quasiparticle approximation. Data for the total density of states near the Fermi level have been obtained. The effect of the interaction parameter, size of the cluster, and temperature on the spectrum of excitations has been studied. 相似文献
20.
We analyze and study the asymptotic behavior (asn→∞) of the general solutionx
n
of the equationx
n+2
=Ax
n
+Bx
n+1
,A≠0,n=0,1,2,..., for various possible values of coefficients and initial data.
Translated fromMatematicheskie Zametki, Vol. 66, No. 2, pp. 211–215, August, 99. 相似文献