18,169 research outputs found

    Analytical ground state for the three-band Hubbard model

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    For the calculation of charge excitations as those observed in, e.g., photo-emission spectroscopy or in electron-energy loss spectroscopy, a correct description of ground-state charge properties is essential. In strongly correlated systems like the undoped cuprates this is a highly non-trivial problem. In this paper we derive a non-perturbative analytical approximation for the ground state of the three-band Hubbard model on an infinite, half filled CuO_2 plane. By comparison with Projector Quantum Monte Carlo calculations it is shown that the resulting expressions correctly describe the charge properties of the ground state. Relations to other approaches are discussed. The analytical ground state preserves size consistency and can be generalized for other geometries, while still being both easy to interpret and to evaluate.Comment: REVTeX, 8 pages, 6 figures, to appear in Phys. Rev.

    Topological Aspects of Spin and Statistics in Nonlinear Sigma Models

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    We study the purely topological restrictions on allowed spin and statistics of topological solitons in nonlinear sigma models. Taking as space the connected dd-manifold XX, and considering nonlinear sigma models with the connected manifold MM as target space, topological solitons are given by elements of pid(M)pi_d(M). Any topological soliton απd(M)\alpha \in \pi_d(M) determines a quotient \Stat_n(X,\alpha) of the group of framed braids on XX, such that choices of allowed statistics for solitons of type α\alpha are given by unitary representations of \Stat_n(X,\alpha) when nn solitons are present. In particular, when M=S2M = S^2, as in the O(3)O(3) nonlinear sigma model with Hopf term, and απ2(S2)\alpha \in \pi_2(S^2) is a generator, we compute that \Stat_n(\R^2,\alpha) = \Z, while \Stat_n(S^2,\alpha) = \Z_{2n}. It follows that phase exp(iθ)\exp(i\theta) for interchanging two solitons of type α\alpha on S2S^2 must satisfy the constraint θ=kπ/n\theta = k\pi/n, kZk \in \Z, when nn such solitons are present.Comment: 14 page

    Large magnetoresistance effect due to spin-injection into a non-magnetic semiconductor

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    A novel magnetoresistance effect, due to the injection of a spin-polarized electron current from a dilute magnetic into a non-magnetic semiconductor, is presented. The effect results from the suppression of a spin channel in the non-magnetic semiconductor and can theoretically yield a positive magnetoresistance of 100%, when the spin flip length in the non-magnetic semiconductor is sufficiently large. Experimentally, our devices exhibit up to 25% magnetoresistance.Comment: 3 figures, submitted for publicatio

    A compact 90 kilowatt electric heat source for heating inert gases to 1700 F

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    Design and fabrication of compact electric heat source for heating inert gase

    Design and fabrication of a low-specific-weight parabolic dish solar concentrator

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    A segmented design and fabrication and assembly techniques were developed for a 1.8 m (6 ft) diameter parabolic concentrator for space application. This design and these techniques were adaptable to a low cost, mass-produced concentrator. Minimal machining was required. Concentrator segments of formed magnesium were used. The concentrator weighed only 1.6 kg sq m (0.32 lbm/sq ft)

    Theoretical investigation into the possibility of very large moments in Fe16N2

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    We examine the mystery of the disputed high-magnetization \alpha"-Fe16N2 phase, employing the Heyd-Scuseria-Ernzerhof screened hybrid functional method, perturbative many-body corrections through the GW approximation, and onsite Coulomb correlations through the GGA+U method. We present a first-principles computation of the effective on-site Coulomb interaction (Hubbard U) between localized 3d electrons employing the constrained random-phase approximation (cRPA), finding only somewhat stronger on-site correlations than in bcc Fe. We find that the hybrid functional method, the GW approximation, and the GGA+U method (using parameters computed from cRPA) yield an average spin moment of 2.9, 2.6 - 2.7, and 2.7 \mu_B per Fe, respectively.Comment: 8 pages, 3 figure
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