184,943 research outputs found

    Weak Gravity Conjecture for the Effective Field Theories with N Species

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    We conjecture an intrinsic UV cutoff for the validity of the effective field theory with a large number of species coupled to gravity. In four dimensions such a UV cutoff takes the form Λ=λ/NMp\Lambda=\sqrt{\lambda/ N}M_p for NN scalar fields with the same potential λϕi4\lambda \phi_i^4, i=1,...,Ni=1,...,N. This conjecture implies that the assisted chaotic inflation or N-flation might be in the swampland, not in the landscape. Similarly a UV cutoff Λ=gMp/N\Lambda=gM_p/\sqrt{N} is conjectured for the U(1) gauge theory with NN species.Comment: 12 pages; refs added and some statements clarifie

    Limits from Weak Gravity Conjecture on Dark Energy Models

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    The weak gravity conjecture has been proposed as a criterion to distinguish the landscape from the swampland in string theory. As an application in cosmology of this conjecture, we use it to impose theoretical constraint on parameters of two types of dark energy models. Our analysis indicates that the Chaplygin-gas-type models realized in quintessence field are in the swampland, whereas the aa power-low decay model of the variable cosmological constant can be viable but the parameters are tightly constrained by the conjecture.Comment: Revtex4, 8 pages, 5 figures; References, minor corrections in content, and acknowledgement adde

    Thermochemical Conversion of Biomass in Smouldering Combustion across Scales: the Roles of Heterogeneous Kinetics, Oxygen and Transport Phenomena

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    AbstractThe thermochemical conversion of biomass in smouldering combustion is investigated here by combining experiments and modeling at two scales: matter (1mg) and bench (100g) scales. Emphasis is put on the effect of oxygen (0–33vol.%) and oxidation reactions because these are poorly studied in the literature in comparison to pyrolysis. The results are obtained for peat as a representative biomass for which there is high-quality experimental data published previously. Three kinetic schemes are explored, including various steps of drying, pyrolysis and oxidation. The kinetic parameters are found using the Kissinger–Genetic Algorithm method, and then implemented in a one-dimensional model of heat and mass transfer. The predictions are validated with thermogravimetric and bench-scale experiments and then analyzed to unravel the role of heterogeneous reaction. This is the first time that the influence of oxygen on biomass smouldering is explained in terms of both chemistry and transport phenomena across scales

    Two-component Fermi gas with a resonant interaction

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    We consider a two-component Fermi gas interacting via a Feshbach molecular state. It is shown that an important energy scale is Eg=g4m3/(64π2)E_g=g^4m^3/(64\pi^2) where gg is the Feshbach coupling constant and mm the mass of the particles. Only when Eg≫ϵFE_g\gg \epsilon_{\rm F} where ϵF\epsilon_{\rm F} is the Fermi energy can the gas be expected to enter a universal state in the unitarity limit on the atomic side of the resonance where there are no molecules present. The universal state is distinct from the molecular gas state on the other side of the resonance. We furthermore calculate the energy of the gas for this universal state and our results are related to current experiments on 6^{6}Li and 40^{40}K.Comment: 4 pages, 2 figure

    Weak gravity conjecture constraints on inflation

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    We consider the gravitational correction to the coupling of the scalar fields. Weak gravity conjecture says that the gravitational correction to the running of scalar coupling should be less than the contribution from scalar fields. For instance, a new scale Λ=λ41/2Mp\Lambda=\lambda_4^{1/2}M_p sets a UV cutoff on the validity of the effective λ4ϕ4\lambda_4 \phi^4 theory. Furthermore, this conjecture implies a possible constraint on the inflation model, e.g. the chaotic inflation model might be in the swampland.Comment: 11 pages, 3 figs; monor corrections; some clarifying remarks added and the final version for publication in JHE
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