Symmetry Condition

14,000,000 Leading Edge Experts on the ideXlab platform

Scan Science and Technology

Contact Leading Edge Experts & Companies

Scan Science and Technology

Contact Leading Edge Experts & Companies

The Experts below are selected from a list of 294 Experts worldwide ranked by ideXlab platform

Neri Merhav - One of the best experts on this subject based on the ideXlab platform.

Joe Sato - One of the best experts on this subject based on the ideXlab platform.

  • Gauge-Higgs Unification Models in Six Dimensions with Extra Space and GUT Gauge Symmetry
    Advances in High Energy Physics, 2012
    Co-Authors: Cheng-wei Chiang, Takaaki Nomura, Joe Sato
    Abstract:

    We review gauge-Higgs unification models based on gauge theories defined on six-dimensional spacetime with / topology in the extra spatial dimensions. Nontrivial boundary Conditions are imposed on the extra / space. This review considers two scenarios for constructing a four-dimensional theory from the six-dimensional model. One scheme utilizes the SO(12) gauge Symmetry with a special Symmetry Condition imposed on the gauge field, whereas the other employs the E6 gauge Symmetry without requiring the additional Symmetry Condition. Both models lead to a standard model-like gauge theory with the Symmetry and SM fermions in four dimensions. The Higgs sector of the model is also analyzed. The electroweak Symmetry breaking can be realized, and the weak gauge boson and Higgs boson masses are obtained.

  • Gauge-Higgs unification models in six dimensions with $S^2/Z_2$ extra space and GUT gauge Symmetry
    arXiv: High Energy Physics - Phenomenology, 2011
    Co-Authors: Cheng-wei Chiang, Takaaki Nomura, Joe Sato
    Abstract:

    In this article, we review gauge-Higgs unification models based on gauge theories defined on six-dimensional spacetime with $S^2/Z_2$ topology in the extra spatial dimensions. On the extra $S^2/Z_2$ space, non-trivial boundary Conditions are imposed. This review considers two scenarios for constructing a four-dimensional theory from the six-dimensional model. One scheme utilizes the SO(12) gauge Symmetry with a special Symmetry Condition imposed on the gauge field, whereas the other employs the E$_6$ gauge Symmetry without requiring the additional Symmetry Condition. Both models lead to a Standard Model-like gauge theory with the SU(3) $\times$ SU(2)$_L$ $\times$ U(1)$_Y$($\times$ U(1)$^2$) Symmetry and SM fermions in four dimensions. The Higgs sector of the model is also analyzed. The electroweak Symmetry breaking can be realized, and the weak gauge boson and Higgs boson masses are obtained.

Gerard Awanou - One of the best experts on this subject based on the ideXlab platform.

  • rectangular mixed elements for elasticity with weakly imposed Symmetry Condition
    Advances in Computational Mathematics, 2013
    Co-Authors: Gerard Awanou
    Abstract:

    We present new rectangular mixed finite elements for linear elasticity. The approach is based on a modification of the Hellinger---Reissner functional in which the Symmetry of the stress field is enforced weakly through the introduction of a Lagrange multiplier. The elements are analogues of the lowest order elements described in Arnold et al. (Math Comput 76:1699---1723, 2007). Piecewise constants are used to approximate the displacement and the rotation. The first order BDM elements are used to approximate each row of the stress field.

  • rectangular mixed elements for elasticity with weakly imposed Symmetry Condition
    arXiv: Numerical Analysis, 2010
    Co-Authors: Gerard Awanou
    Abstract:

    We present new rectangular mixed finite elements for linear elasticity. The approach is based on a modification of the Hellinger-Reissner functional in which the Symmetry of the stress field is enforced weakly through the introduction of a Lagrange multiplier. The elements are analogues of the lowest order elements described in Arnold, Falk and Winther [ Mixed finite element methods for linear elasticity with weakly imposed Symmetry. Mathematics of Computation 76 (2007), pp. 1699--1723]. Piecewise constants are used to approximate the displacement and the rotation. The first order BDM elements are used to approximate each row of the stress field.

Nuray Candemir - One of the best experts on this subject based on the ideXlab platform.

Cheng-wei Chiang - One of the best experts on this subject based on the ideXlab platform.

  • Gauge-Higgs Unification Models in Six Dimensions with Extra Space and GUT Gauge Symmetry
    Advances in High Energy Physics, 2012
    Co-Authors: Cheng-wei Chiang, Takaaki Nomura, Joe Sato
    Abstract:

    We review gauge-Higgs unification models based on gauge theories defined on six-dimensional spacetime with / topology in the extra spatial dimensions. Nontrivial boundary Conditions are imposed on the extra / space. This review considers two scenarios for constructing a four-dimensional theory from the six-dimensional model. One scheme utilizes the SO(12) gauge Symmetry with a special Symmetry Condition imposed on the gauge field, whereas the other employs the E6 gauge Symmetry without requiring the additional Symmetry Condition. Both models lead to a standard model-like gauge theory with the Symmetry and SM fermions in four dimensions. The Higgs sector of the model is also analyzed. The electroweak Symmetry breaking can be realized, and the weak gauge boson and Higgs boson masses are obtained.

  • Gauge-Higgs unification models in six dimensions with $S^2/Z_2$ extra space and GUT gauge Symmetry
    arXiv: High Energy Physics - Phenomenology, 2011
    Co-Authors: Cheng-wei Chiang, Takaaki Nomura, Joe Sato
    Abstract:

    In this article, we review gauge-Higgs unification models based on gauge theories defined on six-dimensional spacetime with $S^2/Z_2$ topology in the extra spatial dimensions. On the extra $S^2/Z_2$ space, non-trivial boundary Conditions are imposed. This review considers two scenarios for constructing a four-dimensional theory from the six-dimensional model. One scheme utilizes the SO(12) gauge Symmetry with a special Symmetry Condition imposed on the gauge field, whereas the other employs the E$_6$ gauge Symmetry without requiring the additional Symmetry Condition. Both models lead to a Standard Model-like gauge theory with the SU(3) $\times$ SU(2)$_L$ $\times$ U(1)$_Y$($\times$ U(1)$^2$) Symmetry and SM fermions in four dimensions. The Higgs sector of the model is also analyzed. The electroweak Symmetry breaking can be realized, and the weak gauge boson and Higgs boson masses are obtained.