10,388 research outputs found

    Hodge numbers for the cohomology of Calabi-Yau type local systems

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    We use Higgs cohomology to determine the Hodge numbers of the first intersection cohomology group of a local system V arising from the third direct image of a family of Calabi-Yau 3-folds over a smooth, quasi-projective curve. We give applications to Rhode's families of Calabi-Yau 3-folds without MUM.Comment: Some signs corrected. This article draws heavily from arXiv:0911.027

    Hadron-Hadron Interactions from Nf=2+1+1N_f=2+1+1 Lattice QCD: isospin-1 KKKK scattering length

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    We present results for the interaction of two kaons at maximal isospin. The calculation is based on Nf=2+1+1N_f=2+1+1 flavour gauge configurations generated by the European Twisted Mass Collaboration with pion masses ranging from about 230230 to 450MeV450\,\textrm{MeV} at three values of the lattice spacing. The elastic scattering length a0I=1a_0^{I=1} is calculated at several values of the bare strange and light quark masses. We find MKa0=0.385(16)stat(12+0)ms(5+0)ZP(4)rfM_K a_0 = -0.385(16)_{\textrm{stat}} (^{+0}_{-12})_{m_s}(^{+0}_{-5})_{Z_P}(4)_{r_f} as the result of a combined extrapolation to the continuum and to the physical point, where the first error is statistical, and the three following are systematical. This translates to a0=0.154(6)stat(5+0)ms(2+0)ZP(2)rffma_0 = -0.154(6)_{\textrm{stat}}(^{+0}_{-5})_{m_s} (^{+0}_{-2})_{Z_P}(2)_{r_f}\,\textrm{fm}.Comment: 28 pages, 18 tables, 14 figure

    Challenges in experimental data integration within genome-scale metabolic models

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    A report of the meeting "Challenges in experimental data integration within genome-scale metabolic models", Institut Henri Poincar\'e, Paris, October 10-11 2009, organized by the CNRS-MPG joint program in Systems Biology.Comment: 5 page

    Ground-state energy and Wigner crystallization in thick 2D-electron systems

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    The ground state energy of the 2-D Wigner crystal is determined as a function of the thickness of the electron layer and the crystal structure. The method of evaluating the exchange-correlation energy is tested using known results for the infinitely-thin 2D system. Two methods, one based on the local-density approximation(LDA), and another based on the constant-density approximation (CDA) are established by comparing with quantum Monte-Carlo (QMC) results. The LDA and CDA estimates for the Wigner transition of the perfect 2D fluid are at rs=38r_s=38 and 32 respectively, compared with rs=35±5r_s=35\pm5 from QMC. For thick-2D layers as found in Hetero-junction-insulated-gate field-effect transistors, the LDA and CDA predictions of the Wigner transition are at rs=20.5r_s=20.5 and 15.5 respectively. Impurity effects are not considered here.Comment: Last figure and Table are modified in the revised version. Conclusions regarding the Wigner transition in thick layers are modified in the revised version. Latex manuscript, four figure

    Representation of Markov chains by random maps: existence and regularity conditions

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    We systematically investigate the problem of representing Markov chains by families of random maps, and which regularity of these maps can be achieved depending on the properties of the probability measures. Our key idea is to use techniques from optimal transport to select optimal such maps. Optimal transport theory also tells us how convexity properties of the supports of the measures translate into regularity properties of the maps via Legendre transforms. Thus, from this scheme, we cannot only deduce the representation by measurable random maps, but we can also obtain conditions for the representation by continuous random maps. Finally, we present conditions for the representation of Markov chain by random diffeomorphisms.Comment: 22 pages, several changes from the previous version including extended discussion of many detail

    CPT Violation Implies Violation of Lorentz Invariance

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    An interacting theory that violates CPT invariance necessarily violates Lorentz invariance. On the other hand, CPT invariance is not sufficient for out-of-cone Lorentz invariance. Theories that violate CPT by having different particle and antiparticle masses must be nonlocal.Comment: Minor changes in the published versio
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