45,677 research outputs found

    Study of the double non linear quantum resonances in diatomic molecules

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    We study the quantum dynamics of diatomic molecule driven by a circularly polarized resonant electric field. We look for a quantum effect due to classical chaos appearing due to the overlapping of nonlinear resonances associated to the vibrational and rotational motion. We solve the Schr\"odinger equation associated with the wave function expanded in term of proper stationary states, n>lm>|n>\otimes|lm> (vibrational\otimesangular momentum states). Looking for quantum-classic correspondence, we consider the Liouville dynamics in the two dimensional phase space defined by the coherent -like state of vibrational states, and it is found some similarities when the quantum dynamics is pictured in terms of number and phase operators.Comment: 15 pages, 4 figure

    Boron determination in steels by Inductively-Coupled Plasma spectometry (ICP)

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    The sample is treated with 5N H2SO4 followed by concentrated HNO3 and the diluted mixture is filtered. Soluble B is determined in the filtrate by Inductively-Coupled Plasma (ICP) spectrometry after addition HCl and extraction of Fe with ethyl-ether. The residue is fused with Na2CO3 and, after treatment with HCl, the insoluble B is determined by ICP spectrometry as before. The method permits determination of ppm amounts of B in steel

    An ab-initio converse NMR approach for pseudopotentials

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    We extend the recently developed converse NMR approach [T. Thonhauser, D. Ceresoli, A. Mostofi, N. Marzari, R. Resta, and D. Vanderbilt, J. Chem. Phys. \textbf{131}, 101101 (2009)] such that it can be used in conjunction with norm-conserving, non-local pseudopotentials. This extension permits the efficient ab-initio calculation of NMR chemical shifts for elements other than hydrogen within the convenience of a plane-wave pseudopotential approach. We have tested our approach on several finite and periodic systems, finding very good agreement with established methods and experimental results.Comment: 11 pages, 2 figures, 4 tables; references expande

    Biofuels - At what cost? Government support for biodiesel in Malaysia

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    One of a series of reports addressing subsidies for biofuels in selected developing countrie

    New Precision Electroweak Tests in Supergravity Models

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    We update the analysis of the precision electroweak tests in terms of 4 epsilon parameters, ϵ1,2,3,b\epsilon_{1,2,3,b}, to obtain more accurate experimental values of them by taking into account the new LEP data released at the 28th ICHEP (1996, Poland). We also compute ϵ1\epsilon_1 and ϵb\epsilon_b in the context of the no-scale SU(5)×U(1)SU(5)\times U(1) supergravity model to obtain the updated constraints by imposing the correlated constraints in terms of the experimental ellipses in the ϵ1ϵb\epsilon_1-\epsilon_b plane and also by imposing the new bound on the lightest chargino mass, mχ1±79m_{\chi^\pm_1}\gtrsim 79 GeV GeV. Upon imposing these new experimental results, we find that the situations in the no-scale model are much more favorable than those in the standard model, and if mt170m_t\gtrsim 170 GeV GeV, then the allowed regions at the 95% C.~L. in the no-scale model are tanβ4\tan\beta\gtrsim 4 and mχ1±120(82)m_{\chi^\pm_1}\lesssim 120 (82) GeV GeV for μ>0(μ<0)\mu>0 (\mu<0), which are in fact much more stringent than in our previous analysis. Therefore, assuming that mt170m_t\gtrsim 170 GeV GeV, if the lightest chargino mass bound were to be pushed up only by a few GeV, the sign on the Higgs mixing term μ\mu in the no-scale model could well be determined from the ϵ1ϵb\epsilon_1-\epsilon_b constraint to be positive at the 95% C.~L. At any rate, better accuracy in the measured mtm_t from the Tevatron in the near future combined with the LEP data is most likely to provide a decisive test of the no-scale SU(5)×U(1)SU(5)\times U(1) supergravity model.Comment: 15 pages, REVTEX, 1 figure (not included but available as a ps file from [email protected]

    Observational Constraints on Transverse Gravity: a Generalization of Unimodular Gravity

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    We explore the hypothesis that the set of symmetries enjoyed by the theory that describes gravity is not the full group of diffeomorphisms Diff(M), as in General Relativity, but a maximal subgroup of it, TransverseDiff(M), with its elements having a jacobian equal to unity; at the infinitesimal level, the parameter describing the coordinate change, xi^mu (x), is transverse, i.e., partial_mu(xi^mu)=0. Incidentally, this is the smaller symmetry one needs to propagate consistently a graviton, which is a great theoretical motivation for considering these theories. Also, the determinant of the metric, g, behaves as a "transverse scalar", so that these theories can be seen as a generalization of the better-known unimodular gravity. We present our results on the observational constraints on transverse gravity, in close relation with the claim of equivalence with general scalar-tensor theory. We also comment on the structure of the divergences of the quantum theory to the one-loop order.Comment: Prepared for the First Mediterranean Conference on Classical and Quantum Gravity, MCCQG, Kolymbari (Crete, Greece), 14-18 September, 2009; also, ERE2009: Gravitation in the Large, Bilbao (Spain), 7-11 September, 200

    Wannier-based calculation of the orbital magnetization in crystals

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    We present a first-principles scheme that allows the orbital magnetization of a magnetic crystal to be evaluated accurately and efficiently even in the presence of complex Fermi surfaces. Starting from an initial electronic-structure calculation with a coarse ab initio k-point mesh, maximally localized Wannier functions are constructed and used to interpolate the necessary k-space quantities on a fine mesh, in parallel to a previously-developed formalism for the anomalous Hall conductivity [X.Wang, J. Yates, I. Souza, and D. Vanderbilt, Phys. Rev. B 74, 195118 (2006)]. We formulate our new approach in a manifestly gauge-invariant manner, expressing the orbital magnetization in terms of traces over matrices in Wannier space. Since only a few (e.g., of the order of 20) Wannier functions are typically needed to describe the occupied and partially occupied bands, these Wannier matrices are small, which makes the interpolation itself very efficient. The method has been used to calculate the orbital magnetization of bcc Fe, hcp Co, and fcc Ni. Unlike an approximate calculation based on integrating orbital currents inside atomic spheres, our results nicely reproduce the experimentally measured ordering of the orbital magnetization in these three materials.Comment: 13 pages, 3 figures, 4 table

    SUSY signals at HERA in the no-scale flipped SU(5) supergravity model

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    Sparticle production and detection at HERA are studied within the recently proposed no-scale flipped SU(5)SU(5) supergravity model. Among the various reaction channels that could lead to sparticle production at HERA, only the following are within its limit of sensitivity in this model: epe~L,Rχi0+X,ν~eχ1+Xe^-p\to \tilde e^-_{L,R}\chi^0_i+X, \tilde \nu_e\chi^-_1+X, where χi0(i=1,2)\chi^0_i(i=1,2) are the two lightest neutralinos and χ1\chi^-_1 is the lightest chargino. We study the elastic and deep-inelastic contributions to the cross sections using the Weizs\"acker-Williams approximation. We find that the most promising supersymmetric production channel is right-handed selectron (e~R\tilde e_{R}) plus first neutralino (χ10\chi^0_1), with one hard electron and missing energy signature. The ν~eχ1\tilde\nu_e\chi^-_1 channel leads to comparable rates but also allows jet final states. A right-handedly polarized electron beam at HERA would shut off the latter channel and allow preferentially the former one. With an integrated luminosity of {\cal L}=100\ipb, HERA can extend the present LEPI lower bounds on me~R,mν~e,mχ10m_{\tilde e_R}, m_{\tilde\nu_e},m_{\chi^0_1} by \approx25\GeV, while {\cal L}=1000\ipb will make HERA competitive with LEPII. We also show that the Leading Proton Spectrometer (LPS) at HERA is an excellent supersymmetry detector which can provide indirect information about the sparticle masses by measuring the leading proton longitudinal momentum distribution.Comment: 11 pages, 8 figures (available upon request as uuencoded file or separate ps files), tex (harvmac) CTP-TAMU-15/93, CERN/LAA/93-1
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