Group Characters: Definition and Applications

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SUMMARY

The discussion focuses on group characters, defined as the trace of representation matrices in group theory. Group characters facilitate the identification of irreducible representation (irrep) content without the need for detailed matrix calculations. Key equations include the character of an element, given by χ(a) = Tr D(a), and the orthogonality relations that help determine the irrep content of a representation. The character values for irreps form an m*m matrix, where m represents the number of conjugacy classes.

PREREQUISITES
  • Understanding of group theory concepts, particularly representations and characters.
  • Familiarity with linear algebra, specifically matrix traces and orthogonality.
  • Knowledge of irreducible representations (irreps) and their properties.
  • Basic comprehension of complex numbers and their conjugates.
NEXT STEPS
  • Study the orthogonality relations of characters in group theory.
  • Learn about the applications of group characters in physics, particularly in quantum mechanics.
  • Explore the computation of irreducible representations for specific groups, such as symmetric groups.
  • Investigate the relationship between group characters and symmetry operations in molecular structures.
USEFUL FOR

Mathematicians, physicists, and students of abstract algebra who are interested in group theory, representation theory, and their applications in various scientific fields.

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Definition/Summary

The character of a group representation is the trace of its representation matrices.

Group characters are useful for finding the irrep content of a representation without working out the representation matrices in complete detail.

Every element in a conjugacy class has the same character, regardless of representation. The character values for the irreps form a m*m matrix, for m classes, and thus m irreps.

Equations

The character of element a is
\chi(a) = Tr\ D(a)

The character of the identity element is the dimension of the representation:
\chi(e) = n(D)

The character of the inverse of an element is the complex conjugate:
\chi(a^{-1}) = \chi(a)^*

Since all elements a of a conjugacy class A have the same character value,
\chi(A) = \chi(a)

The characters of the irreps have various orthogonality relations.

For irreps k and l:
\sum_A n_A \chi^{(k)}(A) \chi^{(l)}(A)^* = n \delta_{kl}
where n is the order of the group and n(A) is the order of class A.

For classes A and B:
\sum_k \chi^{(k)}(A) \chi^{(k)}(B)^* = \frac{n}{n_A}\delta_{AB}

One can thus find the irrep content of a representation:
n(k) = \frac{1}{n} \sum_A n_A \chi(A) \chi^{(k)}(A)^*

Extended explanation

One can find an irrep's reality in a simple way using its character.
\frac{1}{n}\sum_a \chi(a^2)
is 1 for a real irrep, -1 for a pseudoreal irrep, and 0 for a complex irrep.

n is the order of the group (its number of elements).

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Greg Bernhardt said:
The character of a group representation is the trace of its representation matrices.
This is only an example. A group character is any homomorphism from the group into a multiplicative group of a field, i.e. we have a mapping ##x \longmapsto \sigma(x)## with ##\sigma(xy)=\sigma(x)\sigma(y)##. [Algebra Vol. 1,1970, B.L. van der Waerden].
 

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