581 research outputs found

    The LHC Experimental Programme

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    Monte Carlo Renormalization of the 3-D Ising model: Analyticity and Convergence

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    We review the assumptions on which the Monte Carlo renormalization technique is based, in particular the analyticity of the block spin transformations. On this basis, we select an optimized Kadanoff blocking rule in combination with the simulation of a d=3 Ising model with reduced corrections to scaling. This is achieved by including interactions with second and third neighbors. As a consequence of the improved analyticity properties, this Monte Carlo renormalization method yields a fast convergence and a high accuracy. The results for the critical exponents are y_H=2.481(1) and y_T=1.585(3).Comment: RevTeX, 4 PostScript file

    Surface and bulk transitions in three-dimensional O(n) models

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    Using Monte Carlo methods and finite-size scaling, we investigate surface criticality in the O(n)(n) models on the simple-cubic lattice with n=1n=1, 2, and 3, i.e. the Ising, XY, and Heisenberg models. For the critical couplings we find Kc(n=2)=0.4541655(10)K_{\rm c}(n=2)=0.454 1655 (10) and Kc(n=3)=0.693002(2)K_{\rm c}(n=3)= 0.693 002 (2). We simulate the three models with open surfaces and determine the surface magnetic exponents at the ordinary transition to be yh1(o)=0.7374(15)y_{h1}^{\rm (o)}=0.7374 (15), 0.781(2)0.781 (2), and 0.813(2)0.813 (2) for n=1n=1, 2, and 3, respectively. Then we vary the surface coupling K1K_1 and locate the so-called special transition at κc(n=1)=0.50214(8)\kappa_{\rm c} (n=1)=0.50214 (8) and κc(n=2)=0.6222(3)\kappa_{\rm c} (n=2)=0.6222 (3), where κ=K1/K1\kappa=K_1/K-1. The corresponding surface thermal and magnetic exponents are yt1(s)=0.715(1)y_{t1}^{\rm (s)} =0.715 (1) and yh1(s)=1.636(1)y_{h1}^{\rm (s)} =1.636 (1) for the Ising model, and yt1(s)=0.608(4)y_{t1}^{\rm (s)} =0.608 (4) andyh1(s)=1.675(1)y_{h1}^{\rm (s)} =1.675 (1) for the XY model. Finite-size corrections with an exponent close to -1/2 occur for both models. Also for the Heisenberg model we find substantial evidence for the existence of a special surface transition.Comment: TeX paper and 10 eps figure

    Estimating nitrogen fluxes at the European scale by upscaling INTEGRATOR model outputs from selected sites

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    A comparison was made between upscaled model results of nitrogen (N) fluxes to air and water from 450 sites within the EU-27 and results derived for the entire EU-27 area using the model INTEGRATOR. The 450 sites were selected using stratified random sampling, dividing the EU-27 into 150 strata and selecting three sites at random within each stratum. The strata were based on important environmental factors influencing N fluxes. Hierarchical divisive cluster analysis was used to reduce the numerous combinations of environmental factors to the required total of 150, such that the heterogeneity of environmental factors within strata was as small as possible. Modelled NH<sub>3</sub>, N<sub>2</sub>O and NO<sub>x</sub> emissions and N leaching/runoff obtained were scaled up from the 450 sites to the entire EU-27 and were within 10% of results obtained by running the model for the whole of the EU-27 using about 36 500 sites. This implies that a reliable estimate of N fluxes for EU-27 can be made by upscaling results of the 450 selected sites suggesting that dramatic reduction in computation time can be achieved without substantial deterioration of result

    Analysis of Bose-Einstein correlations in e+e- -> W+W- events including final state interactions

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    Recently DELPHI Collaboration reported new data on Bose-Einstein correlations (BEC) measured in e+e- -> W^+W^- events. Apparently no enhancement has been observed. We have analyzed these data including final state interactions (FSI) of both Coulomb and strong (s-wave) origin and found that there is enhancement in BEC but it is overshadowed by the FSI which are extremely important for those events. We have found the following values for the size of the interaction range beta and the degree of coherence lambda: beta=0.87 +/- 0.31fm and lambda=1.19 +/- 0.48, respectively.Comment: 7pages, 4 figure

    Pion Mass Effects in the Large NN Limit of \chiPT

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    We compute the large NN effective action of the O(N+1)/O(N)O(N+1)/O(N) non-linear sigma model including the effect of the pion mass to order mπ2/fπ2m^2_{\pi}/f_{\pi}^2. This action is more complex than the one corresponding to the chiral limit not only because of the pion propagators but also because chiral symmetry produce new interactions proportional to mπ2/fπ2m^2_{\pi}/f_{\pi}^2. We renormalize the action by including the appropriate counter terms and find the renormalization group equations for the corresponding couplings. Then we estudy the unitarity propierties of the scattering amplitudes. Finally our results are applied to the particular case of the linear sigma model and also are used to fit the pion scattering phase shifts.Comment: FT/UCM/18/9
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