13,116 research outputs found

    Neutral minima in two-Higgs doublet models

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    We study the neutral minima of two-Higgs doublet models, showing that these potentials can have at least two such minima with different depths. We analyse the phenomenology of these minima for the several types of two-Higgs doublet potentials, where CP is explicitly broken, spontaneously broken or preserved. We discover that it is possible to have a neutral minimum in these potentials where the masses of the known particles have their standard values, with another deeper minimum where those same particles acquire different masses.Comment: 20 pages, 3 figure

    Explicit Formulas for Relaxed Disarrangement Densities Arising from Structured Deformations

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    Structured deformations provide a multiscale geometry that captures the contributions at the macrolevel of both smooth geometrical changes and non-smooth geometrical changes (disarrangements) at submacroscopic levels. For each (first-order) structured deformation (g,G)(g,G) of a continuous body, the tensor field GG is known to be a measure of deformations without disarrangements, and M:=gGM:=\nabla g-G is known to be a measure of deformations due to disarrangements. The tensor fields GG and MM together deliver not only standard notions of plastic deformation, but MM and its curl deliver the Burgers vector field associated with closed curves in the body and the dislocation density field used in describing geometrical changes in bodies with defects. Recently, Owen and Paroni [13] evaluated explicitly some relaxed energy densities arising in Choksi and Fonseca's energetics of structured deformations [4] and thereby showed: (1) (trM)+(trM)^{+}, the positive part of trMtrM, is a volume density of disarrangements due to submacroscopic separations, (2) (trM)(trM)^{-}, the negative part of trMtrM, is a volume density of disarrangements due to submacroscopic switches and interpenetrations, and (3) trM|trM|, the absolute value of trMtrM, is a volume density of all three of these non-tangential disarrangements: separations, switches, and interpenetrations. The main contribution of the present research is to show that a different approach to the energetics of structured deformations, that due to Ba\'ia, Matias, and Santos [1], confirms the roles of (trM)+(trM)^{+}, (trM)(trM)^{-}, and trM|trM| established by Owen and Paroni. In doing so, we give an alternative, shorter proof of Owen and Paroni's results, and we establish additional explicit formulas for other measures of disarrangements.Comment: 17 pages; http://cvgmt.sns.it/paper/2776

    Decompositions of the higher order polars of plane branches

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    \noindent In \cite{Casas} Casas-Alvero found decompositions of higher order polars of an irreducible plane curve generalizing the results of Merle. We improve his result giving a finer decomposition where we determine the topological type and the number of a kind of branches that we call {\em threshold semi-roots}.Comment: 15 page
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