14,805 research outputs found

    Standard Model With Higgs As Gauge Field On Fourth Homotopy Group

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    Based upon a first principle, the generalized gauge principle, we construct a general model with GL×GR′×Z2G_L\times G'_R \times Z_2 gauge symmetry, where Z2=π4(GL)Z_2=\pi_4(G_L) is the fourth homotopy group of the gauge group GLG_L, by means of the non-commutative differential geometry and reformulate the Weinberg-Salam model and the standard model with the Higgs field being a gauge field on the fourth homotopy group of their gauge groups. We show that in this approach not only the Higgs field is automatically introduced on the equal footing with ordinary Yang-Mills gauge potentials and there are no extra constraints among the parameters at the tree level but also it most importantly is stable against quantum correlation.Comment: 19 pages, Latex, ASITP-94-2

    General Volume-Preserving Mechanical Systems

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    In this letter, we present the general form of equations that generate a volume-preserving flow on a symplectic manifold (M, \omega). It is shown that every volume-preserving flow has some 2-forms acting the role of the Hamiltonian functions in the Hamiltonian mechanics and the ordinary Hamilton equations are included as a special case with a 2-form \frac{1}{n-1} H \omega where H is the corresponding Hamiltonian.Comment: Plain LaTeX, 13 pages, no figure

    Brane worlds in gravity with auxiliary fields

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    Recently, Pani, Sotiriou, and Vernieri explored a new theory of gravity by adding nondynamical fields, i.e., gravity with auxiliary fields [Phys. Rev. D 88, 121502(R) (2013)]. In this gravity theory, higher-order derivatives of matter fields generically appear in the field equations. In this paper we extend this theory to any dimensions and discuss the thick braneworld model in five dimensions. Domain wall solutions are obtained numerically. The stability of the brane system under the tensor perturbation is analyzed. We find that the system is stable under the tensor perturbation and the gravity zero mode is localized on the brane. Therefore, the four-dimensional Newtonian potential can be realized on the brane.Comment: 7 pages, 4 figure
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