346 research outputs found

    Crossover from Luttinger liquid to Coulomb blockade regime in carbon nanotubes

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    We develop a theoretical approach to the low-energy properties of 1D electron systems aimed to encompass the mixed features of Luttinger liquid and Coulomb blockade behavior observed in the crossover between the two regimes. For this aim we extend the Luttinger liquid description by incorporating the effects of a discrete single-particle spectrum. The intermediate regime is characterized by a power-law behavior of the conductance, but with an exponent oscillating with the gate voltage, in agreement with recent experimental observations. Our construction also accounts naturally for the existence of a crossover in the zero-bias conductance, mediating between two temperature ranges where the power-law behavior is preserved but with different exponent.Comment: 5 pages, 3 figure

    Az alvĂĄsidƑ felmĂ©rĂ©se MagyarorszĂĄgon Ă©s RomĂĄniĂĄban Ă©lƑ iskolĂĄskorĂș gyermekek körĂ©ben

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    Introduction: Children's sleep duration is decreasing in the last decade. Despite of the well known negative consequences, there are no data on children's sleep duration in Hungary and Romania. Aim: The aim of the authors was to assess sleep duration of school-age children in Hungary and Romania. Method: A self-edited questionnaire was used for the study. 2446 children were enrolled. All elementary and secondary schools in a Hungarian city, and one elementary and secondary school in a Romanian city took part in the study. Results: Mean sleep duration was 8.3+/-1.2 hours on weekdays. There was a significant difference between the two countries (Hungary vs. Romania, 8.5+/-1.2 hours vs. 7.8+/-0.9 hours, p = 0.001). Age correlated with sleep duration on weekdays (r= -0.605, p = 0.001), but not during weekend. Conclusions: this is the first study on children's sleep duration in Hungary and Romania. The difference between countries may be due to the difference in mean age or cultural and/or geographical differences. Orv. Hetil., 2013, 154, 1592-1596

    Coulomb Gaps in One-Dimensional Spin-Polarized Electron Systems

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    We investigate the density of states (DOS) near the Fermi energy of one-dimensional spin-polarized electron systems in the quantum regime where the localization length is comparable to or larger than the inter-particle distance. The Wigner lattice gap of such a system, in the presence of weak disorder, can occur precisely at the Fermi energy, coinciding with the Coulomb gap in position. The interplay between the two is investigated by treating the long-range Coulomb interaction and the random disorder potential in a self-consistent Hartree-Fock approximation. The DOS near the Fermi energy is found to be well described by a power law whose exponent decreases with increasing disorder strength.Comment: 4 pages, revtex, 4 figures, to be published in Phys. Rev. B as a Rapid Communicatio

    Enhanced Local Moment Formation in a Chiral Luttinger Liquid

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    We derive here a stability condition for a local moment in the presence of an interacting sea of conduction electrons. The conduction electrons are modeled as a Luttinger liquid in which chirality and spin are coupled. We show that an Anderson-U defect in such an interacting system can be transformed onto a nearly-Fermi liquid problem. We find that correlations among the conduction electrons stabilize the local moment phase. A Schrieffer-Wolff transformation is then performed which results in an anisotropic exchange interaction indicative of the Kondo effect in a Luttinger liquid. The ground-state properties of this model are then equivalent to those of the Kondo model in a Luttinger liquid.Comment: 11 pages, no figure

    Spin-charge separation at small lengthscales in the 2D t-J model

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    We consider projected wavefunctions for the 2D t−Jt-J model. For various wavefunctions, including correlated Fermi-liquid and Luttinger-type wavefunctions we present the static charge-charge and spin-spin structure factors. Comparison with recent results from a high-temperature expansion by Putikka {\it et al.} indicates spin-charge separation at small lengthscales.Comment: REVTEX, 5 pages, 5 figures hardcopies availabl

    Renormalization group approach to Fermi Liquid Theory

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    We show that the renormalization group (RG) approach to interacting fermions at one-loop order recovers Fermi liquid theory results when the forward scattering zero sound (ZS) and exchange (ZSâ€Č') channels are both taken into account. The Landau parameters are related to the fixed point value of the ``unphysical'' limit of the forward scattering vertex. We specify the conditions under which the results obtained at one-loop order hold at all order in a loop expansion. We also emphasize the similarities between our RG approach and the diagrammatic derivation of Fermi liquid theory.Comment: 4 pages (RevTex) + 1 postcript file, everything in a uuencoded file, uses epsf (problem with the figure in the first version

    Quasi-Particles in Two-Dimensional Hubbard Model: Splitting of Spectral Weight

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    It is shown that the energy (Δ)(\varepsilon) and momentum (k)(k) dependences of the electron self-energy function ÎŁ(k,Δ+i0)≡ΣR(k,Δ) \Sigma (k, \varepsilon + i0) \equiv \Sigma^{R}(k, \varepsilon) are, ImÎŁR(k,Δ)=−aΔ2âˆŁÎ”âˆ’ÎŸk∣−γ(k) {\rm Im} \Sigma^{R} (k, \varepsilon) = -a\varepsilon^{2}|\varepsilon - \xi_{k}|^{- \gamma (k)} where aa is some constant, Οk=Δ(k)−Ό,Δ(k)\xi_{k} = \varepsilon(k)-\mu, \varepsilon(k) being the band energy, and the critical exponent Îł(k) \gamma(k) , which depends on the curvature of the Fermi surface at k k , satisfies, 0≀γ(k)≀1 0 \leq \gamma(k) \leq 1 . This leads to a new type of electron liquid, which is the Fermi liquid in the limit of Δ,Οk→0 \varepsilon, \xi_{k} \rightarrow 0 but for Οk≠0 \xi_{k} \neq 0 has a split one-particle spectra as in the Tomonaga-Luttinger liquid.Comment: 8 pages (LaTeX) 4 figures available upon request will be sent by air mail. KomabaCM-preprint-O

    Coulomb gap in one-dimensional disordered electron systems

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    The density of states of one-dimensional disordered electron systems with long range Coulomb interaction is studied in the weak pinning limit. The density of states is found to follow a power law with an exponent determined by localization length, and this power law behavior is consistent with the existing numerical results.Comment: RevTeX4 file, 5 pages, no figures To appear in Physical Reviews

    Renormalization group study of interacting electrons

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    The renormalization-group (RG) approach proposed earlier by Shankar for interacting spinless fermions at T=0T=0 is extended to the case of non-zero temperature and spin. We study a model with SU(N)SU(N)-invariant short-range effective interaction and rotationally invariant Fermi surface in two and three dimensions. We show that the Landau interaction function of the Fermi liquid, constructed from the bare parameters of the low-energy effective action, is RG invariant. On the other hand, the physical forward scattering vertex is found as a stable fixed point of the RG flow. We demonstrate that in d=2d=2 and 3, the RG approach to this model is equivalent to Landau's mean-field treatment of the Fermi liquid. We discuss subtleties associated with the symmetry properties of the scattering amplitude, the Landau function and the low-energy effective action. Applying the RG to response functions, we find the compressibility and the spin susceptibility as fixed points.Comment: 11 pages, RevTeX 3.0, 2 PostScript figure
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