Antifundamental representation

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In mathematics differential geometry, an antifundamental representation of a Lie group is the complex conjugate of the fundamental representation, [1] although the distinction between the fundamental and the antifundamental representation is a matter of convention. However, these two are often non-equivalent, because each of them is a complex representation.

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Simple Lie group Connected non-abelian Lie group lacking nontrivial connected normal subgroups

In mathematics, a simple Lie group is a connected non-abelian Lie group G which does not have nontrivial connected normal subgroups. The list of simple Lie groups can be used to read off the list of simple Lie algebras and Riemannian symmetric spaces.

G<sub>2</sub> (mathematics)

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F<sub>4</sub> (mathematics)

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E<sub>6</sub> (mathematics) 78-dimensional exceptional simple Lie group

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Table of Lie groups

This article gives a table of some common Lie groups and their associated Lie algebras.

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In mathematics, a matrix group is a group G consisting of invertible matrices over a specified field K, with the operation of matrix multiplication. A linear group is a group that is isomorphic to a matrix group.

In physics, a charge is any of many different quantities, such as the electric charge in electromagnetism or the color charge in quantum chromodynamics. Charges correspond to the time-invariant generators of a symmetry group, and specifically, to the generators that commute with the Hamiltonian. Charges are often denoted by the letter Q, and so the invariance of the charge corresponds to the vanishing commutator , where H is the Hamiltonian. Thus, charges are associated with conserved quantum numbers; these are the eigenvalues q of the generator Q.

References

  1. Burgess, Cliff; Moore, Guy (2006-12-07), The Standard Model: A Primer, Cambridge University Press, p. 492, ISBN   9781139460460 .