7,875 research outputs found

    The Inflation-Output Volatility Tradeoff and Exchange Rate Shocks in Mexico and Turkey

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    Using a standard Vector Autorregresion with Autocorrelated Time Varying Covariances this paper finds evidence of a vertical inflation-output volatility tradeoff in Mexico and Turkey. It is found, contrary to common economic wisdom, that there is no tradeoff between output and inflation so that monetary policy affects only prices. In addition, it is observed that the exchange rate crucially affects the dynamics of prices, inflation and output. The pass-through from exchange rate to inflation is high and significant in both economies and periods of high exchange rate volatility are associated with unstable rates of inflation. Also, in agreement with many other studies, it is shown here that nominal depreciations are contractionary.Inflation-output Tradeoff, Exchange Rates, BEKK Models

    Structure of 3-(3,5-Dimethylpiperidino)-\u3cem\u3eN\u3c/em\u3e-(\u3cem\u3ep\u3c/em\u3e-Chlorophenyl)Succinimide

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    In the title molecule, 3-(3,5-dimethylpiperidino )-1-(4-chlorophenyl)-2,5-pyrrolidinedione (1), the N-(p-chlorophenyl) substituent is rotated by 68.8° relative to the succinimide plane. The piperidinyl ring has a chair conformation with all substituents in equatorial positions; the conformation around the piperidino-succinimide C--N bond is staggered

    \u3cem\u3eβ\u3c/em\u3e-Homopipitzolone

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    The structure of β-homopipitzolone (one of the two isomers of an intermediate product in the homocedrole synthesis) has been unequivocally established as 1 O-hydroxy-2,6,9-trimetbyltricyclo[6.3.1.01,6] dodeca-9-ene-5, II, 12-trione with relative IR,2R,6R,8S configuration

    Fully dissipative relativistic lattice Boltzmann method in two dimensions

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    In this paper, we develop and characterize the fully dissipative Lattice Boltzmann method for ultra-relativistic fluids in two dimensions using three equilibrium distribution functions: Maxwell-J\"uttner, Fermi-Dirac and Bose-Einstein. Our results stem from the expansion of these distribution functions up to fifth order in relativistic polynomials. We also obtain new Gaussian quadratures for square lattices that preserve the spatial resolution. Our models are validated with the Riemann problem and the limitations of lower order expansions to calculate higher order moments are shown. The kinematic viscosity and the thermal conductivity are numerically obtained using the Taylor-Green vortex and the Fourier flow respectively and these transport coefficients are compared with the theoretical prediction from Grad's theory. In order to compare different expansion orders, we analyze the temperature and heat flux fields on the time evolution of a hot spot

    A Lloyd-model generalization: Conductance fluctuations in one-dimensional disordered systems

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    We perform a detailed numerical study of the conductance GG through one-dimensional (1D) tight-binding wires with on-site disorder. The random configurations of the on-site energies ϵ\epsilon of the tight-binding Hamiltonian are characterized by long-tailed distributions: For large ϵ\epsilon, P(ϵ)1/ϵ1+αP(\epsilon)\sim 1/\epsilon^{1+\alpha} with α(0,2)\alpha\in(0,2). Our model serves as a generalization of 1D Lloyd's model, which corresponds to α=1\alpha=1. First, we verify that the ensemble average lnG\left\langle -\ln G\right\rangle is proportional to the length of the wire LL for all values of α\alpha, providing the localization length ξ\xi from lnG=2L/ξ\left\langle-\ln G\right\rangle=2L/\xi. Then, we show that the probability distribution function P(G)P(G) is fully determined by the exponent α\alpha and lnG\left\langle-\ln G\right\rangle. In contrast to 1D wires with standard white-noise disorder, our wire model exhibits bimodal distributions of the conductance with peaks at G=0G=0 and 11. In addition, we show that P(lnG)P(\ln G) is proportional to GβG^\beta, for G0G\to 0, with βα/2\beta\le\alpha/2, in agreement to previous studies.Comment: 5 pages, 5 figure
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