Sufficient Condition for Adjoint Representation Kernel to be Lie Group Center

In summary, an adjoint representation is a mapping between a Lie algebra and its dual space, used for studying the algebra through its action on the dual space. It is closely related to the Lie bracket and has many applications in mathematics and physics. It differs from the fundamental representation in structure and properties and can also be extended to other algebraic structures.
  • #1
kakarukeys
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what is the sufficient condition for the kernel of an adjoint representation to be the center of the Lie group?

Does the Lie group have to be non-compact and connected, etc?
 
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  • #2
If the Lie group is connected, the claim holds. So I heard. Is there any chance that you are studying automorphic representations and their L-functions? If so, please let me know good references to start with. Also, references for representation theory. Thanks.:smile:
 
  • #3


The sufficient condition for the kernel of an adjoint representation to be the center of the Lie group is that the Lie group must be compact and connected. This means that the group is a closed and connected set, and all its elements can be continuously connected to the identity element. Additionally, the Lie group must also have a trivial center, meaning that the only element in the center is the identity element.

If these conditions are met, then the kernel of the adjoint representation will be the center of the Lie group. This is because the kernel of the adjoint representation consists of all elements that commute with all other elements in the Lie group. Therefore, if the center of the Lie group is trivial, the only element that satisfies this condition is the identity element, making it the kernel of the adjoint representation.

It is important to note that this is not the only sufficient condition for the kernel of the adjoint representation to be the center of the Lie group. Other conditions may exist, but the compactness and connectedness of the Lie group are commonly used and well-known conditions.

In summary, the sufficient condition for the kernel of an adjoint representation to be the center of the Lie group is that the group must be compact, connected, and have a trivial center.
 

What is an adjoint representation?

An adjoint representation is a mathematical concept used in the study of Lie algebras. It refers to a mapping between a Lie algebra and its dual space, which allows for the study of the algebra through its action on the dual space.

How is the adjoint representation related to the Lie bracket?

The adjoint representation is closely related to the Lie bracket, which is a mathematical operation defined on elements of a Lie algebra. The adjoint representation maps each element of the Lie algebra to a linear transformation on the dual space, and this transformation is determined by the Lie bracket.

What are the applications of the adjoint representation?

The adjoint representation has many applications in mathematics and physics. It is used in the study of Lie algebras, which have applications in quantum mechanics, differential geometry, and other areas of mathematics. It is also used in the study of group representations and Lie groups.

How is the adjoint representation different from the fundamental representation?

The adjoint representation and the fundamental representation are both ways of representing a Lie algebra, but they are different in their structure and properties. The fundamental representation is a faithful representation, meaning that it preserves the structure of the algebra, while the adjoint representation is not necessarily faithful. Additionally, the fundamental representation is a linear representation, while the adjoint representation is not.

Can the adjoint representation be extended to other algebraic structures?

Yes, the adjoint representation can be extended to other algebraic structures, such as associative algebras and Hopf algebras. In these cases, the adjoint representation maps the algebra to its dual space, and is used to study the algebra's structure and properties through its action on the dual space.

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